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<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0" article-type="research-article"><?xmltex \makeatother\@nolinetrue\makeatletter?>
  <front>
    <journal-meta><journal-id journal-id-type="publisher">HESS</journal-id><journal-title-group>
    <journal-title>Hydrology and Earth System Sciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">HESS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Hydrol. Earth Syst. Sci.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1607-7938</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/hess-26-6311-2022</article-id><title-group><article-title>Simulating carbon and water fluxes using a coupled process-based terrestrial biosphere model and joint assimilation of leaf area index and surface soil moisture</article-title><alt-title>Carbon and water flux simulations through joint assimilation of LAI and SSM​​​​​​​</alt-title>
      </title-group><?xmltex \runningtitle{Carbon and water flux simulations through joint assimilation of LAI and SSM​​​​​​​}?><?xmltex \runningauthor{S. Li et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Li</surname><given-names>Sinan</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff3">
          <name><surname>Zhang</surname><given-names>Li</given-names></name>
          <email>zhangli@aircas.ac.cn</email>
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff4">
          <name><surname>Xiao</surname><given-names>Jingfeng</given-names></name>
          <email>j.xiao@unh.edu</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Ma</surname><given-names>Rui</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Tian</surname><given-names>Xiangjun</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff3">
          <name><surname>Yan</surname><given-names>Min</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Key Laboratory of Digital Earth Science, Aerospace Information
Research Institute, Chinese Academy of Sciences,<?xmltex \hack{\break}?> No. 9 Dengzhuang South Road, Beijing 100094, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>College of Resources and Environment, University of Chinese Academy
of Sciences,<?xmltex \hack{\break}?> No. 19A Yuquan Road, Beijing 100049, China</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>International Research Center of Big Data for Sustainable
Development Goals, Beijing 100094, China</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Earth Systems Research Center, Institute for the Study of Earth,
Oceans, and Space,<?xmltex \hack{\break}?> University of New Hampshire, Durham, New Hampshire 03824, USA</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>School of Remote Sensing and Information Engineering, Wuhan
University, Wuhan 430079, China</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>International Center for Climate and Environment Sciences (ICCES),
Institute of Atmospheric Physics,<?xmltex \hack{\break}?> Chinese Academy of Sciences, Beijing
100029, China</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Li Zhang (zhangli@aircas.ac.cn) and Jingfeng Xiao (j.xiao@unh.edu)</corresp></author-notes><pub-date><day>16</day><month>December</month><year>2022</year></pub-date>
      
      <volume>26</volume>
      <issue>24</issue>
      <fpage>6311</fpage><lpage>6337</lpage>
      <history>
        <date date-type="received"><day>6</day><month>March</month><year>2021</year></date>
           <date date-type="rev-request"><day>12</day><month>May</month><year>2021</year></date>
           <date date-type="rev-recd"><day>9</day><month>August</month><year>2022</year></date>
           <date date-type="accepted"><day>4</day><month>October</month><year>2022</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 Sinan Li et al.</copyright-statement>
        <copyright-year>2022</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022.html">This article is available from https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022.html</self-uri><self-uri xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022.pdf">The full text article is available as a PDF file from https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e171">Reliable modeling of carbon and water fluxes is essential for understanding
the terrestrial carbon and water cycles and informing policy strategies
aimed at constraining carbon emissions and improving water use efficiency.
We designed an assimilation framework (LPJ-Vegetation and soil moisture
Joint Assimilation, or LPJ-VSJA) to improve gross primary production (GPP)
and evapotranspiration (ET) estimates globally. The integrated model, LPJ-PM (LPJ-PT-JPL<inline-formula><mml:math id="M1" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> Model) as the underlying model, was coupled from the
Lund–Potsdam–Jena Dynamic Global Vegetation Model (LPJ-DGVM version 3.01)
and a hydrology module (i.e., the updated Priestley–Taylor Jet Propulsion
Laboratory model, PT-JPL<inline-formula><mml:math id="M2" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>). Satellite-based soil moisture products derived from the Soil Moisture and Ocean Salinity (SMOS) and Soil Moisture Active and Passive (SMAP) and leaf area index (LAI) from the Global LAnd and Surface Satellite (GLASS) product were assimilated into LPJ-PM to improve GPP and ET simulations using a proper orthogonal decomposition (POD)-based ensemble four-dimensional variational assimilation method (PODEn4DVar). The joint assimilation framework LPJ-VSJA achieved the best model performance (with an <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> ( coefficient of determination) of 0.91 and 0.81 and an ubRMSD (unbiased root mean square deviation) reduced by 40.3 % and 29.9 % for GPP and ET, respectively, compared with those of LPJ-DGVM at the monthly scale). The GPP and ET resulting from the assimilation demonstrated a better
performance in the arid and semi-arid regions (GPP: <inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M5" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.73,
ubRMSD <inline-formula><mml:math id="M6" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.05 g C m<inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> d<inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; ET: <inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M10" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.73, ubRMSD <inline-formula><mml:math id="M11" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.61 mm d<inline-formula><mml:math id="M12" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) than in the humid and sub-dry humid regions (GPP: <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M14" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.61, ubRMSD <inline-formula><mml:math id="M15" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.23 g C m<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> d<inline-formula><mml:math id="M17" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; ET: <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M19" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.66; ubRMSD <inline-formula><mml:math id="M20" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.67 mm d<inline-formula><mml:math id="M21" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). The ET simulated by LPJ-PM that assimilated SMAP or SMOS data had a slight difference, and the SMAP soil moisture data performed better than
SMOS data. Our global simulation modeled by LPJ-VSJA was compared
with several global GPP and ET products (e.g., GLASS GPP, GOSIF GPP, GLDAS
ET, and GLEAM ET) using the triple collocation (TC) method. Our products,
especially ET, exhibited advantages in the overall error distribution
(estimated error (<inline-formula><mml:math id="M22" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula>): 3.4 mm per month; estimated standard deviation
of <inline-formula><mml:math id="M23" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula>: 1.91 mm per month). Our research showed that the assimilation
of multiple datasets could reduce model uncertainties, while the model
performance differed across regions and plant functional types. Our
assimilation framework (LPJ-VSJA) can improve the model simulation
performance of daily GPP and ET globally, especially in water-limited
regions.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e401">Gross primary production (GPP) and evapotranspiration (ET) are essential
components of the carbon and water cycles. Carbon and water fluxes are
inherently coupled on multiple spatial and temporal scales (Law et al.,
2002; Sun et al., 2019; Waring and Running, 2010). Terrestrial biosphere
models are the most sophisticated approach for providing a relatively
detailed description of such interdependent relationships regarding water
and carbon fluxes and understanding the response of terrestrial ecosystems
to changes in atmospheric CO<inline-formula><mml:math id="M24" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and climate (Kaminski et al., 2017).
Dynamic global vegetation models (DGVMs) are process-based dynamic
terrestrial biosphere models, which can simulate water, carbon, and energy
exchange between vegetation and the atmosphere under different conditions
accounting for vegetation physiological processes and are widely used to
estimate carbon and water fluxes of terrestrial vegetation. However, there
are still large uncertainties in carbon and water flux estimates at regional
to global scales. Both diagnostic and prognostic models show substantial
differences in the magnitude and spatiotemporal patterns of GPP and ET. For
example, the global annual GPP estimates exhibited a large range (130–169 Pg C yr<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) among 16 process-based terrestrial biosphere models (Anav et al., 2015). The global ET ranged from 70 000 to 75 000 km<inline-formula><mml:math id="M26" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, and the uncertainty of regional or global ET estimates was up to 50 % of the annual mean ET value, especially in the semi-arid regions
(Miralles et al., 2016). These uncertainties mainly arise from the
forcing datasets, simplification of mechanisms or imperfect assumptions in
processes, and uncertain parameters in the processed models and assimilation
methods (Xiao et al., 2019).</p>
      <p id="d1e446">In the last 2 decades, remote sensing products have been assimilated into
DGVMs to reduce the uncertainty in modeled carbon and water fluxes
(MacBean et al., 2016; Scholze et al., 2017; Exbrayat
et al., 2019). Data assimilation (DA) is an effective approach to reduce
uncertainties in terrestrial biosphere models by integrating satellite
products with models to constrain related parameters or state variables. A
DA system contains four main components: a set of observations, an
observation operator, an underlying model, and an assimilation method. The
assimilation method considers the errors from both models and observations
and reduces model uncertainties by minimizing a cost function. The ensemble
Kalman filter (EnKF) has been widely applied in land surface process models
for parameter optimization, which significantly improve simulations by
periodically updating state variables (e.g., leaf area index (LAI) and soil moisture) using
remote sensing data without altering the model structure (Rahman et al.,
2022b; Bonan et al., 2020; Xu et al., 2021). Yet, the EnKF relies on the
instantaneous observations to update the state variable at the current time
and gives the predicted value at the next time based on the forward
integration of the updated state variable. The four-dimensional variational
method (4DVar) assimilation method can obtain the dynamic balance of the
estimation in the time window when it is applied to the long-series forecast
model (Bateni et al., 2014; Xu et al., 2019). In particular, the proper
orthogonal decomposition (POD)-based ensemble 4DVAR assimilation method
(referred to as PODEn4DVar) (Tian and Feng, 2015) requires relatively less
computation and can simultaneously assimilate the observations at different
time intervals. Meanwhile, it maintains the structural information of the
four-dimensional space. This method has a satisfactory performance in land
DA for carbon and water variables (Tian et al., 2009, 2010)
and can better estimate GPP and ET than EnKF (Ma et al., 2017).</p>
      <p id="d1e449">Multiple sources of remote sensing data streams have been used to constrain
models for assimilation. As a critical biophysical parameter of the land,
leaf area index (LAI) is closely related to many land processes, such as
photosynthesis, respiration, precipitation interception, ET, and surface
energy exchange (Fang et al., 2019). LAI has a lot of impact on the
simulation of carbon and water fluxes (Liu et al., 2018), and accurate LAI
estimates can improve the simulations of the carbon and water fluxes
(Bonan et al., 2014; Mu et al., 2007). He et al. (2021) assimilated land
surface temperature and LAI observations into the 4DVar framework and
improved ET and GPP estimates. Soil moisture is a major driving factor
affecting vegetation production in arid ecosystems, especially in semi-arid
areas (Liu et al., 2020). Introducing surface soil moisture (SSM) into
the model can significantly improve GPP and ET simulation, particularly in
water-limited areas (He et al., 2017; Li et al., 2020).</p>
      <p id="d1e452">The advancement of earth observation, machine learning, inversion
algorithms, and computer technology has improved the accuracy of global LAI
products and boosted model–data fusion studies (Fang et al., 2019; Kganyago et al., 2020; Xiao et al., 2017). The Advanced Very High-Resolution
Radiometer (AVHRR) generates global LAI products with the longest historic
record (since the early 1980s). The Global LAnd and Surface Satellite (GLASS) LAI product has been verified to
have a better accuracy than that of MODIS and CYCLOPES and is more
temporally continuous and spatially complete (Xiao et al., 2013). Several
recent studies showed that the assimilation of GLASS LAI into DGVMs enhanced
the performance of the models in simulating carbon cycling (e.g., GPP and net
ecosystem exchange – NEE) and hydrological (e.g., ET and SM) processes (Ling et al., 2019; Ma et al., 2017; Yan et al., 2016).</p>
      <p id="d1e456">Microwave remote sensors are considered effective tools for measuring SM
globally (Petropoulos et al., 2015). For example, SSM products have been
derived from the Soil Moisture and Ocean Salinity (SMOS) and Soil Moisture
Active and Passive (SMAP) satellites equipped with an L-band microwave
instrument. The products from these satellites have been evaluated against
in situ observations and other SSM products and overall have high
accuracy (Burgin et al., 2017; Cui et al., 2018). Additionally, the SMAP
performs better than SMOS and other SSM products (e.g., Advanced
Scatterometer, ASCAT, and Advanced Microwave Scanning Radiometer 2, AMSR2) with an overall lower error and a higher correlation based on the
verification with in situ SSM data from 231 sites (Cui et al., 2018;
Kim et al., 2018). The assimilation of SMAP data can improve the simulation
accuracy of carbon and water fluxes (He et al., 2017; Li et al., 2020)
and hydrological variables (surface soil moisture, root-zone soil moisture
(RZSM), and streamflow) (Blyverket et al., 2019; Koster et al., 2018;
Reichle et al., 2017). In addition, the assimilation of SMAP data performed
slightly better than that of SMOS and ESA CCI data (Blyverket et al.,
2019).</p>
      <p id="d1e459">In the nonlinear model or nonlinear observation operator, only simultaneous
assimilation makes optimal use of observations (MacBean et al., 2016).
Therefore, a joint assimilation of SM and LAI can make full use of the two
variables. From site (Albergel et al., 2010; Rüdiger et al., 2010; Wu
et al., 2019) to regional assimilation (Ines et al., 2013), many studies
showed that joint assimilation of vegetation parameters and SM can improve
the simulation of the carbon and water cycles. Over small regions and at
high spatial resolution, Xie et al. (2017) and Pan et al. (2019) showed that
the joint assimilation of SM and LAI improved the accuracy of crop yield
estimation using high-resolution satellite products from Sentinel-1 and Sentinel-2.
At a large regional scale, Bonan et al. (2020) assimilated LAI and SSM
together into the Interaction between Soil, Biosphere and Atmosphere (ISBA)
land model and improved the modeled GPP, ET, and runoff in the Mediterranean
region. Rahman et al. (2022b) jointly assimilated GLASS LAI and SMAP soil moisture to improve water and carbon flux simulations within the Noah-MP
model over the continental United States domain. Albergel et al. (2020)
jointly assimilated the ASCAT Soil Moisture Index (SMI) and LAI GEOV1 into ISBA through the Global Offline Land Data assimilation system LDAS-Monde to
monitor extreme events such as drought and heat wave events. In conclusion,
the Kalman filter and its variant methods are mostly used to implement joint
assimilation methods at regional scales, which requires many kinds of observation data, and their accuracy directly affects the assimilation
performance.</p>
      <p id="d1e462">This study stems from the research studies discussed above and further explored
the potential of jointly assimilating satellite LAI and soil moisture
products globally. Specifically, it was the first time that an updated
LPJ-DGVM model was used to jointly assimilate GLASS LAI and SMAP soil
moisture for simulating global water and carbon fluxes. The latest global
soil moisture datasets (SMOS and SMAP) were used, and the assimilation
performance of these two observations was analyzed. Since previous work
showed the importance of surface soil moisture in the semi-arid and arid
areas, one of the specific objectives of our study is to compare the
assimilation effect in the humid and arid areas and improve the
understanding of the effect of surface soil moisture on vegetation activity
in wet and dry zones. In addition, compared with the assimilation methods in
previous studies (mostly using Kalman filter variants), the POD-En4DVar
method was used, which greatly improves the computational efficiency.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>LPJ-VSJA framework and assimilation strategy</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Coupled model (LPJ-PM) for assimilation</title>
      <p id="d1e480">In this study, a coupled terrestrial biosphere model, LPJ-PM, was used to
simulate daily GPP and ET by assimilating satellite-derived LAI and SSM. The
LPJ-PM is coupled from LPJ-DGVM and PT-JPL<inline-formula><mml:math id="M28" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>. The original input data in PT-JPL<inline-formula><mml:math id="M29" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> were all inherited from LPJ-DGVM, with the exception of
relative humidity (RH) and surface soil moisture (SMOS and SMAP), including
the initial LAI calculated by the LPJ-DGVM or assimilated LAI obtained
through the LAI assimilation scheme, canopy height, and the fraction of
absorbed photosynthetic active radiation (fPAR). The detailed processes of the LPJ-PM have been described in Li et al. (2020), and the flow
chart for the coupling is shown in Fig. 1.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e503">Flowchart of the LPJ-VSJA assimilation scheme: three
assimilation schemes and the coupled model: LPJ-PM (adapted from Li et al.,
2020). The abbreviations in the model and the assimilation framework are explained in Table 1.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f01.png"/>

        </fig>

<sec id="Ch1.S2.SS1.SSS1">
  <label>2.1.1</label><title>LPJ-DGVM</title>
      <p id="d1e519">The LPJ-DGVM is a process-oriented dynamic model, which considers mutual
interaction of carbon and water cycling and is designed to simulate
vegetation distribution and carbon, soil, and atmosphere fluxes (Sitch et
al., 2003). For each plant functional type (PFT), the GPP is calculated by
implementing coupled photosynthesis and water balance.</p>
      <p id="d1e522">The canopy GPP is updated daily:
              <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M30" display="block"><mml:mrow><mml:mi mathvariant="normal">GPP</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi>E</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mi>C</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msqrt><mml:mrow><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi>E</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mi>C</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn><mml:mi mathvariant="italic">θ</mml:mi><mml:msub><mml:mi>J</mml:mi><mml:mi>E</mml:mi></mml:msub><mml:msub><mml:mi>J</mml:mi><mml:mi>C</mml:mi></mml:msub></mml:mrow></mml:msqrt></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi>C</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the Rubisco limiting rate of photosynthesis, <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi>E</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the
light-limiting rate of photosynthesis, and the empirical parameter <inline-formula><mml:math id="M33" display="inline"><mml:mi mathvariant="italic">θ</mml:mi></mml:math></inline-formula>
represents the common limiting effect between the two terms. <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi>E</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is
related to APAR (absorbed photosynthetic active radiation, product of FPAR and
PAR), while <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi>C</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is related to Vcmax (canopy maximum carboxylation
capacity, <inline-formula><mml:math id="M36" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>mol CO<inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M39" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>):

                  <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M40" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E2"><mml:mtd><mml:mtext>2</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>J</mml:mi><mml:mi>E</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mi mathvariant="normal">APAR</mml:mi></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E3"><mml:mtd><mml:mtext>3</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>J</mml:mi><mml:mi>C</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi>V</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>max⁡</mml:mo></mml:mrow></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              where <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are determined by a variety of photosynthetic
parameters and the intercellular partial pressure of CO<inline-formula><mml:math id="M43" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, which is
related to atmospheric CO<inline-formula><mml:math id="M44" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> content and further altered by leaf stomatal
conductance (Sitch et al., 2003). APAR and FPAR are directly related to LAI.</p>
      <p id="d1e787">In the water cycle module, ET is calculated as the minimum of a plant- and
soil-limited supply function (<inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">supply</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and the atmospheric demand
(<inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">demand</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) (Haxeltine and Prentice, 1996; Sitch et al., 2003). The soil structure is simplified to a “two-layer bucket” model (the top soil layer at a 0–50 cm depth and the bottom layer at a 50–100 cm depth).
              <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M47" display="block"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">S</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="normal">Ep</mml:mi><mml:mo>×</mml:mo><mml:msub><mml:mi mathvariant="normal">Wr</mml:mi><mml:mn mathvariant="normal">20</mml:mn></mml:msub><mml:mo>×</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi>f</mml:mi><mml:mi>v</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>
            In this module, it is assumed that the soil layer above 20 cm produces water
through evaporation, and Wr<inline-formula><mml:math id="M48" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">20</mml:mn></mml:msub></mml:math></inline-formula> is the relative water content of the soil
above 20 cm, which is used as the only soil water limit for calculating
vegetation transpiration and soil evaporation. In the evapotranspiration
estimation, the oversimplification of soil structure and the soil water
limitation lead to a large error (Sitch et al., 2003), while LPJ-DGVM cannot
directly assimilate surface soil water due to the limitation of soil layer
stratification, and therefore, the satellite-derived SSM cannot be assimilated into
LPJ-DGVM directly. The oversimplified soil structure and single soil
moisture limitation inevitably lead to sizable uncertainty in ET
simulation. Additionally, the monthly input caused a daily variation of the
modeled SM, which was also not transmitted to the calculation of GPP and ET.
Thus, the updated PT-JPL model (hereafter referred to as PT-JPL<inline-formula><mml:math id="M49" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>) was
coupled with LPJ-DGVM, and the model structure was modified so that SSM can
be directly assimilated into the coupled model at the daily time step.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS2">
  <label>2.1.2</label><?xmltex \opttitle{PT-JPL${}_{\mathrm{SM}}$}?><title>PT-JPL<inline-formula><mml:math id="M50" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula></title>
      <p id="d1e885">In PT-JPL<inline-formula><mml:math id="M51" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>, three ET components are modeled: soil evaporation (<inline-formula><mml:math id="M52" display="inline"><mml:mi>E</mml:mi></mml:math></inline-formula>), vegetation transpiration (<inline-formula><mml:math id="M53" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula>), and leaf evaporation (<inline-formula><mml:math id="M54" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>). The PT-JPL<inline-formula><mml:math id="M55" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> introduced a constraint (0–1, <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">RSM</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) of SSM for <inline-formula><mml:math id="M57" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M58" display="inline"><mml:mi>E</mml:mi></mml:math></inline-formula>, which was used to avoid the implicit soil water control (represented by <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M60" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> RH<inline-formula><mml:math id="M61" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">VPD</mml:mi></mml:msup></mml:math></inline-formula>) in the PT-JPL model.</p>
      <p id="d1e980">Vegetation transpiration is calculated as follows:

                  <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M62" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E5"><mml:mtd><mml:mtext>5</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mtable rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">RSM</mml:mi></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mfenced open="(" close=")"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msup><mml:mi mathvariant="normal">RH</mml:mi><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="normal">VWC</mml:mi><mml:mo>)</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="normal">RH</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:mfenced><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:mfenced close=")" open="("><mml:mrow><mml:msup><mml:mi mathvariant="normal">RH</mml:mi><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="normal">VWC</mml:mi><mml:mo>)</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="normal">RH</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:mfenced><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">TRSM</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E6"><mml:mtd><mml:mtext>6</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">TRSM</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msup><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">CR</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">CR</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi mathvariant="normal">pwp</mml:mi><mml:mi mathvariant="normal">_</mml:mi><mml:mi mathvariant="normal">CH</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:msqrt><mml:mi mathvariant="normal">CH</mml:mi></mml:msqrt></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              where <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the SMAP SSM, <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">pwp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the water content at the wilting point, and VWC is volumetric water content. <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">CR</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is a crucial parameter in characterizing the extent of SM restriction on ET, and
<inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi mathvariant="normal">pwp</mml:mi><mml:mi mathvariant="normal">_</mml:mi><mml:mi mathvariant="normal">CH</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the canopy height (CH)-adjusted surface
soil moisture wilting point and is related to the potential of roots
capturing water from deeper sources to limit the transpiration rate and
characterize the SM availability (Purdy et al., 2018; Evensen, 2004; Serraj et al., 1999). The specific formula is given in Purdy et al. (2018).</p>
      <p id="d1e1194">Soil evaporation is calculated as follows:
              <disp-formula id="Ch1.E7" content-type="numbered"><label>7</label><mml:math id="M67" display="block"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">RSM</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">pwp</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">fc</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">pwp</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            The proportion of available water limits the soil evapotranspiration to the
maximum available water. This scalar was formulated to represent the
relatively accurate extractable water content for the vegetation, determined
by soil properties and the water available for evaporation, which is
estimated via surface water constraints.</p>
      <p id="d1e1241">The SMAP SSM was applied to model global ET using PT-JPL<inline-formula><mml:math id="M68" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>, and the
results demonstrated the largest improvements for ET estimates in dry
regions (Purdy et al., 2018). Due to the limitation of soil stratification in
LPJ-DGVM, the model was coupled with an updated remote sensing ET algorithm
in the PT-JPL<inline-formula><mml:math id="M69" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> that could better simulate ET in water-limited
regions than in humid regions (Purdy et al., 2018).</p>
</sec>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Assimilation scheme and experiment procedure</title>
      <p id="d1e1271">To improve the prediction capability of LPJ-PM, we designed three
assimilation schemes: assimilating LAI only (LAI-only, output:
ET<inline-formula><mml:math id="M70" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula>, GPP<inline-formula><mml:math id="M71" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula>), assimilating SSM only
(SSM-only, output: GPP<inline-formula><mml:math id="M72" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>,
ET<inline-formula><mml:math id="M73" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>), and joint assimilation of LAI and SSM (Joint LAI and
SSM assimilation, output: ET<inline-formula><mml:math id="M74" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula>,
GPP<inline-formula><mml:math id="M75" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula>), i.e., LPJ-VSJA framework) to test the assimilation
performance for simulating GPP and ET.</p>
      <p id="d1e1329">The proposed LPJ-VSJA framework consists of four main components: the model
operator (the LPJ-PM), the observation operator (to establish the relation
between the assimilation variable and the observed variable), the
observation series (GLASS LAI and SMOS or SMAP products), and the
assimilation algorithm (POD4DVar). With the surface soil moisture constraint
in the PT-JPL<inline-formula><mml:math id="M76" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>, the LPJ-VSJA corrects the output fluxes (GPP and ET in this study).</p>
      <p id="d1e1341">The experiment consisted of six steps.
<list list-type="bullet"><list-item>
      <p id="d1e1346"><italic>Step 1</italic>. Initialize the LPJ-DGVM, and output the reference state variables
without assimilation over the experimental period (2010–2018), referred to
as the “control run” scenario.</p></list-item><list-item>
      <p id="d1e1352"><italic>Step 2</italic>. Implement three assimilation schemes respectively, and the results
represent the assimilation integration state (daily GPP and ET assimilation
results are referred to as the “GPP<inline-formula><mml:math id="M77" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula>” and “ET<inline-formula><mml:math id="M78" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula>” in the LAI-only scheme,“GPP<inline-formula><mml:math id="M79" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>” and “ET<inline-formula><mml:math id="M80" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>” in the SSM-only scheme, and “GPP<inline-formula><mml:math id="M81" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> ” and “ET<inline-formula><mml:math id="M82" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> ” in the Joint LAI and SSM assimilation
scheme. This scenario used the same input data and model parameter scheme
as the control run scenario.</p></list-item><list-item>
      <p id="d1e1413"><italic>Step 3</italic>. Evaluate GPP and ET results (three schemes) by comparing the
parameters, <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> ( coefficient of determination), BIAS, and ubRMSD (unbiased root mean square deviation), for conditions of without-DA (control run
scenario) and with-DA states, and assess the assimilation performance of
separate assimilation and joint assimilation to determine the optimal
assimilation scheme for GPP and ET, respectively.</p></list-item><list-item>
      <p id="d1e1430"><italic>Step 4</italic>. Evaluate the in situ GPP and ET resulting from the assimilation
where the sites are located in wet or dry regions by dividing these
validation sites into four parts (humid, sub-dry humid, semi-arid, and arid
regions), and this step was designed to assess the superiority of the
proposed assimilation scheme in water-limited areas.</p></list-item><list-item>
      <p id="d1e1436"><italic>Step 5</italic>. Compare the ET assimilation performance by assimilating the SMOS data with that by assimilating the SMAP data.</p></list-item><list-item>
      <p id="d1e1442"><italic>Step 6</italic>. Evaluate the simulated GPP and ET maps based on the optimal
assimilation scheme against existing global flux products.</p></list-item></list></p>
<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>LAI-only assimilation scheme</title>
      <p id="d1e1454">In the LAI-only assimilation scheme, the observation operator determines the
relationship between LAI and foliage projective cover (FPC) in the process
model (Eq. 8), and the assimilated LAI will be propagated by energy
transmission and ecosystem processes (e.g., photosynthesis, transpiration of
vegetative process) in the dynamic model to improve GPP and ET simulations
(Bonan et al., 2014; Mu et al., 2007). FPC, the vertically projected
percentage of the land covered by foliage, regulates the rate of
photosynthate conversion and transpiration. In this study, the GLASS LAI
with 8 d interval for the period 2010–2018 was selected as the
observation dataset for assimilation, and the FPC state variable was updated
daily through running the LPJ-PM (FPC<inline-formula><mml:math id="M84" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">DA</mml:mi></mml:msub></mml:math></inline-formula>, GPP<inline-formula><mml:math id="M85" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula>, ET<inline-formula><mml:math id="M86" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula> in this study) as shown below:
              <disp-formula id="Ch1.E8" content-type="numbered"><label>8</label><mml:math id="M87" display="block"><mml:mrow><mml:mi mathvariant="normal">FPC</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn><mml:mi mathvariant="normal">LAI</mml:mi></mml:mrow></mml:msup><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e1509">We set the model and observation errors at a given time as 20 % and 10 %
(scale factor) of the LAI value and the observed LAI value, respectively. By
verifying the assimilation performance (<inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, RMSD, and BIAS) for different
scale factors (<inline-formula><mml:math id="M89" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula>) of model simulation and observations in the range of 0.05
to 0.40, taking a step size of 0.05 (a total of 64 combinations), the
optimal scale factors (0.2 and 0.1) were determined (Bonan et al., 2020). The
model and observation errors was the LAI value multiplied by <inline-formula><mml:math id="M90" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula>. The model
integration generation method described by Pipunic et al. (2008) was
used to determine the minimum number of ensemble members required to achieve
maximum efficiency, and the number of sets was 20.</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <label>2.2.2</label><title>SSM-only assimilation scheme</title>
      <p id="d1e1547">In this scheme, the SSM products (SMOS or SMAP) were assimilated into LPJ-PM
to obtain more accurate ET (ET<inline-formula><mml:math id="M91" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>) estimates in water-limited areas. The observation series was the SMOS or SMAP SSM product, and the observation operator was the PT-JPL<inline-formula><mml:math id="M92" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> model. The ET<inline-formula><mml:math id="M93" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula> (see Table 1) was
estimated by the coupled model (LPJ-PM) introducing SSM as a diagnostic
variable. The ET values resulting from the assimilation were applied to
compute the top layer SM (50 cm) at the next time step (​​​​​​​a nonlinear
soil water availability function described by Zhao et al., 2013),
providing feedback for subsequent hydrologic and carbon cycle processes.
Then, the updated SM values regulated the GPP simulation (output:
GPP<inline-formula><mml:math id="M94" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>). Different from other “constant” ET observations, the ET<inline-formula><mml:math id="M95" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula> (“observation”) at each time <inline-formula><mml:math id="M96" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> was adjusted by absorbing intermediate variables updated after assimilation at time <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:mi>t</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>. The ET<inline-formula><mml:math id="M98" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula> was shown to
be better than ET simulated by LPJ-DGVM but not as good as that simulated by
the model with SMAP SSM assimilated (Li et al., 2020). Thus, it is also
proven that this SSM assimilation scheme could improve the accuracy of ET
simulations (Li et al., 2020).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e1627">Description of the models and outputs in this study. “n/a” stands for “not applicable”.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="2.4cm"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="4.4cm"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="4.5cm"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="3.4cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">acronyms</oasis:entry>
         <oasis:entry colname="col2">Full name</oasis:entry>
         <oasis:entry colname="col3">Description</oasis:entry>
         <oasis:entry colname="col4">Output</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">LPJ-DGVM <?xmltex \hack{\hfill\break}?>(Sitch et al., 2003)</oasis:entry>
         <oasis:entry colname="col2">Lund–Potsdam–Jena Dynamic <?xmltex \hack{\hfill\break}?>Global Vegetation Model</oasis:entry>
         <oasis:entry colname="col3">This model is used as a model <?xmltex \hack{\hfill\break}?>operator to simulated initial ET</oasis:entry>
         <oasis:entry colname="col4">GPP<inline-formula><mml:math id="M99" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula>, ET<inline-formula><mml:math id="M100" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">PT-JPL<inline-formula><mml:math id="M101" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?>(Purdy et al., 2018)</oasis:entry>
         <oasis:entry colname="col2">Updated Priestley–Taylor Jet <?xmltex \hack{\hfill\break}?>Propulsion Laboratory model</oasis:entry>
         <oasis:entry colname="col3">The model is used as a module of <?xmltex \hack{\hfill\break}?>the LPJ-PM and establishes a connection between SMAP SM and ET</oasis:entry>
         <oasis:entry colname="col4">n/a</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">LPJ-PM <?xmltex \hack{\hfill\break}?>(Li et al., 2020)</oasis:entry>
         <oasis:entry colname="col2">Lund–Potsdam–Jena and Updated <?xmltex \hack{\hfill\break}?>Priestley–Taylor Jet Propulsion <?xmltex \hack{\hfill\break}?>Laboratory coupled model</oasis:entry>
         <oasis:entry colname="col3">An integrated model corresponding <?xmltex \hack{\hfill\break}?>to the coupling of the PT-JPL<inline-formula><mml:math id="M102" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?>and LPJ-DGVM</oasis:entry>
         <oasis:entry colname="col4">GPP<inline-formula><mml:math id="M103" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>, ET<inline-formula><mml:math id="M104" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">LPJ-VSJA  <?xmltex \hack{\hfill\break}?>(this study)</oasis:entry>
         <oasis:entry colname="col2">Lund–Potsdam–Jena Vegetation- <?xmltex \hack{\hfill\break}?>Soil moisture-Joint-Assimilation <?xmltex \hack{\hfill\break}?>system</oasis:entry>
         <oasis:entry colname="col3">A process-based assimilation <?xmltex \hack{\hfill\break}?>framework for assimilating LAI <?xmltex \hack{\hfill\break}?>and SSM jointly into LPJ-PM</oasis:entry>
         <oasis:entry colname="col4">GPP<inline-formula><mml:math id="M105" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula>, ET<inline-formula><mml:math id="M106" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula>; GPP<inline-formula><mml:math id="M107" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>, <?xmltex \hack{\hfill\break}?>ET<inline-formula><mml:math id="M108" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>; GPP<inline-formula><mml:math id="M109" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula>; ET<inline-formula><mml:math id="M110" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e1865">All assimilation simulations were conducted between January 2010 and
December 2018. Between January 2010 and April 2015, SMOS data were used for
assimilation, and after May 2015, both SMOS and SMAP data were used for assimilation. An assimilation scheme was conducted when RH and SMOS or SMAP
SSM data existed simultaneously; otherwise, the original simulation of the
LPJ-DGVM was conducted directly without adjustment of assimilation.</p>
      <p id="d1e1869">Similar to the LAI assimilation scheme, the model and observation errors
were set as 15 % and 5 % of ET<inline-formula><mml:math id="M111" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M112" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula>, respectively (LPJ-PM was adopted before assimilation). The number of ensemble members was set to 50. The ET<inline-formula><mml:math id="M113" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula> must be rescaled to the ET<inline-formula><mml:math id="M114" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> distribution via
their corresponding cumulative probabilities using the cumulative
distribution function (CDF) matching to avoid introducing any bias into the LPJ-VSJA system (Li et al., 2020).</p>
</sec>
<sec id="Ch1.S2.SS2.SSS3">
  <label>2.2.3</label><title>Joint LAI and SSM assimilation scheme</title>
      <p id="d1e1916">In this scheme, both LAI from GLASS and SSM from SMOS or SMAP were the
observation datasets. The GLASS LAI was assimilated to obtain the FPC<inline-formula><mml:math id="M115" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">DA</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M116" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula>, and then the FPC<inline-formula><mml:math id="M117" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">DA</mml:mi></mml:msub></mml:math></inline-formula> served as input to LPJ-PM to simulate optimized ET<inline-formula><mml:math id="M118" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula>, and the ET<inline-formula><mml:math id="M119" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> was generated using ET<inline-formula><mml:math id="M120" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M121" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula>. Then, the SM (referred to as SM<inline-formula><mml:math id="M122" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">CO</mml:mi></mml:msub></mml:math></inline-formula> in Fig. S1 in the Supplement) updated by ET<inline-formula><mml:math id="M123" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> and the FPC<inline-formula><mml:math id="M124" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">DA</mml:mi></mml:msub></mml:math></inline-formula> were used as input to correct GPP (ET<inline-formula><mml:math id="M125" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula>).</p>
      <p id="d1e2019">Here, we applied the error regulation in the LAI-only scheme and maintained
the error setting of the LAI observation and model simulation. Considering
the transmission of integrated model error, we recalculated the model error
of LPJ-PM after the LAI assimilation and set model and observation errors of
ET<inline-formula><mml:math id="M126" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M127" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula> to be 15 % and 10 %, respectively.</p>
</sec>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>POD-based ensemble 4D variational assimilation method</title>
      <p id="d1e2049">The proper orthogonal decomposition (POD)-based ensemble four-dimensional
variational (4DVar) assimilation method (referred to as PODEn4DVar)
(Tian and Feng, 2015) has the advantage of avoiding the
calculation of adjoint patterns as its incremental analysis field, which can
be represented linearly by the POD base (transformed OP, observing perturbation, and MP, model perturbation). Moreover, the PODEn4DVar can
simultaneously assimilate multiple-time observation data and provide
flow-dependent (the flow-dependent is the ensembles of forecasting
statistical characteristics in the <inline-formula><mml:math id="M128" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> time) error estimates of the background
errors. It has shown advantages in terrestrial assimilation, the Tan-Tracker
system (a Chinese carbon cycle data-assimilation system; in Chinese, “Tan”
means carbon) and radar assimilation (Tian et al., 2010,
2009, 2014; Zhang and Weng, 2015).</p>
      <p id="d1e2059">By minimizing the following initial incremental format of the cost function
in the 4DVar algorithm, an analysis field can be obtained as follows:
            <disp-formula id="Ch1.E9" content-type="numbered"><label>9</label><mml:math id="M129" display="block"><mml:mtable class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mi mathvariant="bold">J</mml:mi><mml:mo>(</mml:mo><mml:msup><mml:mi mathvariant="bold">x</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mo>=</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:mo>(</mml:mo><mml:msup><mml:mi mathvariant="bold">x</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:msup><mml:mi mathvariant="bold">B</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>(</mml:mo><mml:msup><mml:mi mathvariant="bold">x</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:msup><mml:mfenced open="[" close="]"><mml:mrow><mml:msup><mml:mi mathvariant="bold">y</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:msup><mml:mi mathvariant="bold">x</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="bold">y</mml:mi><mml:mi mathvariant="normal">obs</mml:mi><mml:mo>′</mml:mo></mml:msubsup></mml:mrow></mml:mfenced><mml:mi>T</mml:mi></mml:msup></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:msup><mml:mi mathvariant="bold">R</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mfenced close="]" open="["><mml:mrow><mml:msup><mml:mi mathvariant="bold">y</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:msup><mml:mi mathvariant="bold">x</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="bold">y</mml:mi><mml:mi mathvariant="normal">obs</mml:mi><mml:mo>′</mml:mo></mml:msubsup></mml:mrow></mml:mfenced><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
          Here, the <inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold">x</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>=</mml:mo><mml:mi mathvariant="bold">x</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="bold">x</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold">y</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:msup><mml:mi mathvariant="bold">x</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi mathvariant="bold">y</mml:mi><mml:mo>(</mml:mo><mml:msup><mml:mi mathvariant="bold">x</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="bold">x</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="bold">y</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="bold">x</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>,
<inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="bold">y</mml:mi><mml:mi mathvariant="normal">obs</mml:mi><mml:mo>′</mml:mo></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="bold">y</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi mathvariant="bold">y</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="bold">x</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mi mathvariant="bold">y</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="bold">H</mml:mi><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="bold">M</mml:mi><mml:mrow><mml:mi mathvariant="normal">to</mml:mi><mml:mo>→</mml:mo><mml:mi mathvariant="normal">tk</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="bold">x</mml:mi><mml:mo>)</mml:mo><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>. <inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold">x</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:msubsup><mml:mi mathvariant="bold">x</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mo>′</mml:mo></mml:msubsup><mml:msubsup><mml:mi mathvariant="bold">x</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mo>′</mml:mo></mml:msubsup><mml:msubsup><mml:mi mathvariant="bold">x</mml:mi><mml:mi>N</mml:mi><mml:mo>′</mml:mo></mml:msubsup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the model perturbation (MP) matrix​​​​​​​, and <inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold">y</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:msubsup><mml:mi mathvariant="bold">y</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mo>′</mml:mo></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mi mathvariant="bold">y</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mo>′</mml:mo></mml:msubsup><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:msubsup><mml:mi mathvariant="bold">y</mml:mi><mml:mi>N</mml:mi><mml:mo>′</mml:mo></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula> is the observation perturbation (OP)
matrix with <inline-formula><mml:math id="M136" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> samples. Following Rüdiger et al. (2010), the LAI
perturbation was set to a fraction (0.001) of the LAI itself. The
perturbation of ET<inline-formula><mml:math id="M137" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M138" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> conforms to a Gaussian distribution with a mean of 0 and a specified covariance (10 % and 5 % of the ET<inline-formula><mml:math id="M139" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M140" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> at time <inline-formula><mml:math id="M141" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>). The subscript b represents the background field, the superscript <inline-formula><mml:math id="M142" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> represents a transpose, <inline-formula><mml:math id="M143" display="inline"><mml:mi mathvariant="bold">H</mml:mi></mml:math></inline-formula> is the observation operator of
the LAI-only assimilation scheme as described in Sect. 2.2.1, and the
SSM-only assimilation scheme is the PT-JPL<inline-formula><mml:math id="M144" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> (described in Sect. 2.1.2). <inline-formula><mml:math id="M145" display="inline"><mml:mi mathvariant="bold">M</mml:mi></mml:math></inline-formula> is the forecast model (LPJ-PM in this study), <inline-formula><mml:math id="M146" display="inline"><mml:mi mathvariant="bold">B</mml:mi></mml:math></inline-formula> is the background error covariance, <inline-formula><mml:math id="M147" display="inline"><mml:mi mathvariant="bold">R</mml:mi></mml:math></inline-formula> is the observation error covariance, and obs denotes observation.</p>
      <p id="d1e2509">Assuming the approximately linear relationship between OP<inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:msup><mml:mi>y</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and MP<inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:msup><mml:mi>x</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>,
POD decomposition and transformation were successively conducted for OP and
MP. The transformed OP samples (<inline-formula><mml:math id="M150" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">Φ</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msubsup><mml:mi mathvariant="bold">y</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mo>′</mml:mo></mml:msubsup><mml:msubsup><mml:mi mathvariant="bold">y</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mo>′</mml:mo></mml:msubsup><mml:msubsup><mml:mi mathvariant="bold">y</mml:mi><mml:mi>n</mml:mi><mml:mo>′</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>) are
orthogonal and independent, and the transformed MP samples (<inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">Φ</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msubsup><mml:mi mathvariant="bold">x</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mo>′</mml:mo></mml:msubsup><mml:msubsup><mml:mi mathvariant="bold">x</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mo>′</mml:mo></mml:msubsup><mml:msubsup><mml:mi mathvariant="bold">x</mml:mi><mml:mi>n</mml:mi><mml:mo>′</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>) are orthogonal to the corresponding OP samples,
where <inline-formula><mml:math id="M152" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> is the number of POD modes.</p>
      <p id="d1e2617">The manifestation of the background error covariance is the same as the
ensemble Kalman filter (EnKF; Evensen, 2004), and the incremental
analysis <inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="bold">x</mml:mi><mml:mi mathvariant="normal">a</mml:mi><mml:mo>′</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> was expressed by the <inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">Φ</mml:mi><mml:mrow><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi mathvariant="bold">Φ</mml:mi><mml:mo mathvariant="normal" stretchy="false">̃</mml:mo></mml:mover><mml:mi>y</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi mathvariant="bold">Φ</mml:mi><mml:mo stretchy="false" mathvariant="normal">̃</mml:mo></mml:mover><mml:mi>y</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msup><mml:mfenced close="]" open="["><mml:mrow><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>n</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced><mml:msub><mml:mi>I</mml:mi><mml:mrow><mml:mi>n</mml:mi><mml:mo>×</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="bold">Φ</mml:mi><mml:mrow><mml:mi>y</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow><mml:mi>T</mml:mi></mml:msubsup><mml:msup><mml:mi mathvariant="bold">R</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:msub><mml:mi mathvariant="bold">Φ</mml:mi><mml:mrow><mml:mi>y</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:msubsup><mml:mi mathvariant="bold">Φ</mml:mi><mml:mrow><mml:mi>y</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow><mml:mi>T</mml:mi></mml:msubsup><mml:msup><mml:mi mathvariant="bold">R</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula>. Finally,
the optimal analysis <inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">x</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is calculated as <inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">x</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="bold">x</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="bold">Φ</mml:mi><mml:mrow><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mover accent="true"><mml:mi mathvariant="bold">Φ</mml:mi><mml:mo mathvariant="normal" stretchy="false">̃</mml:mo></mml:mover><mml:mi>y</mml:mi></mml:msub><mml:msubsup><mml:mi mathvariant="bold">y</mml:mi><mml:mi mathvariant="normal">obs</mml:mi><mml:mo>′</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>. The detailed derivation process of the
algorithm is described by a previous study (Tian et al., 2011).</p>
      <p id="d1e2810">In the ensemble-based method (Evensen, 2004), the number of ensemble
members is usually fewer than that of the observation data and the degrees
of freedom of the model variables, and spurious long-range correlations
occur between observation locations and model variables. A practical method,
the localization technique, is applied to address this issue (Mitchell
et al., 2002). The final incremental analysis is rewritten as
            <disp-formula id="Ch1.E10" content-type="numbered"><label>10</label><mml:math id="M158" display="block"><mml:mrow><mml:msubsup><mml:mi mathvariant="bold">x</mml:mi><mml:mi mathvariant="normal">a</mml:mi><mml:mo>′</mml:mo></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="bold">Φ</mml:mi><mml:mrow><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mover accent="true"><mml:mi mathvariant="bold">Φ</mml:mi><mml:mo stretchy="false" mathvariant="normal">̃</mml:mo></mml:mover><mml:mi>y</mml:mi></mml:msub><mml:msubsup><mml:mi mathvariant="bold">y</mml:mi><mml:mi mathvariant="normal">obs</mml:mi><mml:mo>′</mml:mo></mml:msubsup><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi mathvariant="normal">h</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>⋅</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi mathvariant="normal">v</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the horizontal and vertical distances between the spatial positions of state and observed variables, respectively; and <inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi mathvariant="normal">h</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi mathvariant="normal">v</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> are the horizontal and vertical covariance localization Schur radii, respectively. The filtering function <inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is
expressed as
            <disp-formula id="Ch1.E11" content-type="numbered"><label>11</label><mml:math id="M164" display="block"><mml:mtable rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mi>r</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{8.9}{8.9}\selectfont$\displaystyle}?><mml:mfenced close="" open="{"><mml:mtable class="array" columnalign="left left"><mml:mtr><mml:mtd><mml:mrow><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">4</mml:mn></mml:mfrac></mml:mstyle></mml:mstyle><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">5</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mstyle><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">5</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:mfrac></mml:mstyle></mml:mstyle><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">5</mml:mn><mml:mn mathvariant="normal">3</mml:mn></mml:mfrac></mml:mstyle></mml:mstyle><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mn mathvariant="normal">0</mml:mn><mml:mo>≤</mml:mo><mml:mi>r</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">12</mml:mn></mml:mfrac></mml:mstyle></mml:mstyle><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">5</mml:mn></mml:msup><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mstyle><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">5</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:mfrac></mml:mstyle></mml:mstyle><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">5</mml:mn><mml:mn mathvariant="normal">3</mml:mn></mml:mfrac></mml:mstyle></mml:mstyle><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mi>r</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">4</mml:mn><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">2</mml:mn><mml:mn mathvariant="normal">3</mml:mn></mml:mfrac></mml:mstyle></mml:mstyle><mml:msup><mml:mi>r</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>≤</mml:mo><mml:mi>r</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>&lt;</mml:mo><mml:mi>r</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced><?xmltex \hack{$\egroup}?></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
          where <inline-formula><mml:math id="M165" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> is the radius of the filter.</p>
      <p id="d1e3209">The assimilation algorithm is mainly divided into two steps: (1) prediction, by running LPJ-PM in the current assimilation window and generating simulation
results and background field vectors, and (2) update, the algorithm being used to
calculate the optimal assimilation increment <inline-formula><mml:math id="M166" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="bold">x</mml:mi><mml:mi mathvariant="normal">a</mml:mi><mml:mo>′</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> and analysis
solution <inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">x</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. The simulation results and the initial conditions of
the model in the current window are updated using the analysis solution. The
updated initial conditions were applied for model LPJ-PM prediction, and the
above process was repeated.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Validation method for assimilation performance</title>
      <p id="d1e3244">The <inline-formula><mml:math id="M168" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> (coefficient of determination), BIAS, and ubRMSD (unbiased root
mean square deviation) between simulation and tower-based observations were
applied for evaluation. In addition, a Taylor chart was also used to
demonstrate the performance of two ET estimations with different SSM
observations in terms of <inline-formula><mml:math id="M169" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>, ubRMSD, and normalized standard deviation (NSD)
on 2D plots, to display how closely the datasets matched observations in one
diagram (Taylor, 2001). In the Taylor diagram, NSD represents the radial
distance from the origin point and the correlation with the site
observations as an angle in the polar plot. The ubRMSD is the distance
between the observation and the model and is represented in the Taylor chart
as a green semi-circular arc with point A as the center of the circle. The
closer the model point to the reference point (Point A), the better the
performance. This diagram is convenient and visual in evaluating multiple
aspects of various models.</p>
      <p id="d1e3265">The error variance of GPP and ET products was estimated using the triple
collocation (TC) approach (Stoffelen, 1998) to validate the global
simulation in this study. The method has been extensively applied in the
study of hydrology and oceanography (Caires and Sterl, 2003; Khan et al.,
2018; O'Carroll et al., 2008; Stoffelen, 1998), particularly in SM studies
(Chan et al., 2016; Kim et al., 2018). The TC provides a reliable platform
for comparison of spatial assimilation results and in situ measurements. In
this experiment, no calculation was performed on the non-vegetated areas,
where the correlation was lower than 0.2, in order to have independent datasets and
avoid correlated errors (crucial assumptions in TC) (Yilmaz and Crow,
2014).</p>
      <p id="d1e3268">In this study, the five products were divided into three product categories,
including satellite products (MODIS and GOSIF GPP), reanalysis products (GLASS and GLDAS), and data-assimilation products (GLEAM ET and LPJ-VSJA) (C. Li et al., 2018).
One product in each category was selected to form a group to calculate their
error. The LPJ-VSJA product was set as the reference data.</p>
      <p id="d1e3271">For GPP products, GOSIF, GLASS, and LPJ-VSJA were treated as a group, and
MODIS, GLASS and LPJ-VSJA were treated as another group to calculate the
errors; the final errors were determined by the average of these two.</p>
      <p id="d1e3275">Similarly, to calculate the errors for ET, GLEAM, GLASS, and MODIS were
chosen as a group; LPJ-VSJA, GLDAS, and MODIS were treated as a group;
LPJ-VSJA, GLASS, and MODIS were considered a group. In order to reduce the
influence of orthogonality hypothesis of error, the first and third groups
are for indirect and effective comparison between LPJ-VSJA product and GLEAM
product.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Experiment sites and data</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Description of flux tower sites</title>
      <p id="d1e3294">We screened over 300 eddy covariance (EC) flux sites across the globe from the FLUXNET2015 (<uri>https://fluxnet.org/data/fluxnet2015 dataset/</uri>, last access: 10 ​​​​​​​April 2021), AmeriFlux (<uri>https://ameriflux.lbl.gov/data-and-manifest/</uri>​​​​​​​, last access: 10 ​​​​​​​April 2021), and the HeiHe River basin (<ext-link xlink:href="https://doi.org/10.11888/Hydro.tpdc.270888" ext-link-type="DOI">10.11888/Hydro.tpdc.270888</ext-link>, Xie, 2017) for the evaluation of assimilation
performance over the period from January 2010 to December 2018. The in situ
half-hourly latent heat flux (LE) and GPP data from the sites were aggregated into daily data. The daily gap-filled data were excluded if the percentage of gap-filled
half-hourly values was more than 20 %. Then we corrected the data of
energy non-closure using the Bowen ratio closure method (Twine et al.,
2000) to improve the energy closure rate (Huang et al., 2015; Yang et
al., 2020). The data were selected to cover the 2010–2018 period with at
least 1 year of reliable data, and the result from the error of
assimilation is relative to the LE value and seasonal variation (Purdy
et al., 2018; Zou et al., 2017). It is essential to have available data every
month during a 1-year period, and only days with less than 25 % missing
data were processed per month (Feng et al., 2015). In addition, for flux
tower data, the data were also excluded for the analysis if the SMAP/SMOS
SSM data were not of good quality.</p>
      <p id="d1e3306">Finally, we identified a total of 105 sites across the globe encompassing
five major biomes: grassland (18 for GPP and 19 for ET), savanna (11),
shrubland (4), forest (49 and 53), and cropland (13 and 14). In the
comparative analysis of the performance for simulating ET by assimilating
SMOS and SMAP SSM data separately, we selected 46 AmeriFlux sites (Fig. S3) with at least 1 year of reliable data from 2015 to 2018 based on the
simultaneous availability of SMAP and SMOS data, including grassland (19),
savanna (11), shrubland (5), forest (23), and cropland (7). Figures S2 and S3
illustrate the location and distribution of the 105 and 46 EC flux tower
sites, respectively. A more detailed description is summarized in
Table S1 in the Supplement.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Remote sensing datasets: LAI and SSM</title>
      <p id="d1e3317">The GLASS LAI product with an 8 d time step (8 d average) and 5 km
resolution was derived from MODIS and CYCLOPES surface reflectance and
ground observations using general regression neural networks (GRNNs)
(Xiao et al., 2013, 2016). The verification of the product
using the mean values of high-resolution LAI maps showed that the GLASS LAI
values were closer to these high-resolution LAI maps (RMSD <inline-formula><mml:math id="M170" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.78 and
<inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M172" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.81) (Xiao et al., 2016; Liang et al., 2013). Therefore,
the GLASS LAI product has satisfactory performance and can be assimilated
into terrestrial biosphere models.</p>
      <p id="d1e3345">The SMAP mission (Entekhabi et al., 2010) and SMOS mission
(Jacquette et al., 2010), the two dedicated soil moisture satellites
currently in orbit equipped with L-band microwave instruments, provide SSM
retrievals. We chose the SMOS-L2 product and the SMAP-L3-Enhanced product,
which both provide global coverage every 3 d for soil depth of 5 cm.
Only good-quality SMAP and SMOS data were used. The grid cells with water
areas larger than 10 % and those with less than 50 % good-quality data in 1 year were masked out, which alleviates the undesirable model
simulations caused by the decrease in SMAP retrieval accuracy (Chan
et al., 2016; O'Neill et al., 2010). We only adopted the data with an
uncertainty below 0.1 m<inline-formula><mml:math id="M173" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M174" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, in the actual range (0.00–0.6 m<inline-formula><mml:math id="M175" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M176" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), and the temperature of the Land Surface Module (LSM) observation layer (the second layer) was higher than 2 <inline-formula><mml:math id="M177" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C (Blyverket et al., 2019).</p>
      <p id="d1e3399">The GLASS LAI, SMOS, and SMAP observations were resampled to 9 km for site
simulation and 0.25<inline-formula><mml:math id="M178" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> for regional simulation. The 8 d average
of GLASS LAI was assimilated for each day, and the SMAP or SMOS SSM was
assimilated every 3 d.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Model-forcing and validation datasets</title>
      <p id="d1e3419">In this study, the meteorological, soil property, and CO<inline-formula><mml:math id="M179" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> concentration
datasets were used to drive the LPJ-PM. The climate-driven datasets used for
the initialization of the LPJ-DGVM are the atmospheric CO<inline-formula><mml:math id="M180" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
concentrations (1901–2018) of ice-core measurements and atmospheric
observations at the Mauna Loa Observatory and CRU TS4.03 version Climate
data from 1901 to 1930 provided by the Climatic Research Unit (CRU) of the
Climate Laboratory, University of East Anglia, UK, including monthly
precipitation, surface temperature, cloud cover and wet day. In the
simulation period of 2010–2018, the Modern Era Retrospective-Analysis for
Research and Applications Version 2 (MERRA-2) was adopted, and the variables
used included precipitation, temperature, cloud cover, and relative humidity.
Soil properties (including limited water content of vegetation at wilting
points, field capacity, and soil porosity) from the Harmonized World Soil
Database (HWSD) V1.2 dataset (Wieder et al., 2014) were selected as inputs to
the PT-JPLSM model. Table 2 provides the spatial and temporal
characteristics of the model-forcing datasets in the LPJ-PM (submodule:
LPJ-DGVM and PT-JPL<inline-formula><mml:math id="M181" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e3452">List of the selected forcing and remote sensing datasets
used in this study.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.95}[.95]?><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="3.2cm"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="2.7cm"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="2cm"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:colspec colnum="5" colname="col5" align="justify" colwidth="6.6cm"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Datasets</oasis:entry>
         <oasis:entry colname="col2">Variable</oasis:entry>
         <oasis:entry colname="col3">Period</oasis:entry>
         <oasis:entry colname="col4">Spatial</oasis:entry>
         <oasis:entry colname="col5">References</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">resolution</oasis:entry>
         <oasis:entry colname="col5"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">CRU TS v4.1<inline-formula><mml:math id="M185" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Cloud cover, tem- <?xmltex \hack{\hfill\break}?>perature, precipita- <?xmltex \hack{\hfill\break}?>tion, wet day</oasis:entry>
         <oasis:entry colname="col3">1901–1930</oasis:entry>
         <oasis:entry colname="col4">0.5<inline-formula><mml:math id="M186" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M187" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.5<inline-formula><mml:math id="M188" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">New et al. (2000), <?xmltex \hack{\hfill\break}?> <uri>https://crudata.uea.ac.uk/cru/data/hrg/</uri> <?xmltex \hack{\hfill\break}?>( last access: 10 ​​​​​​​April 2021)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Ice-core measurements <?xmltex \hack{\hfill\break}?>and atmospheric <?xmltex \hack{\hfill\break}?>observations at the <?xmltex \hack{\hfill\break}?>Mauna Loa Observatory<inline-formula><mml:math id="M189" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Atmospheric CO<inline-formula><mml:math id="M190" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?>concentrations</oasis:entry>
         <oasis:entry colname="col3">1901–2018</oasis:entry>
         <oasis:entry colname="col4">n/a</oasis:entry>
         <oasis:entry colname="col5">Etheridge et al. (1996), Keeling et al. (1995), <?xmltex \hack{\hfill\break}?> <uri>https://scrippsco2.ucsd.edu/data/atmospheric_co2/</uri> <?xmltex \hack{\hfill\break}?>(last access: 21 January 2021)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">MERRA-2<inline-formula><mml:math id="M191" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Precipitation, surface temperature, cloud <?xmltex \hack{\hfill\break}?>fraction, relative <?xmltex \hack{\hfill\break}?>humidity</oasis:entry>
         <oasis:entry colname="col3">2010–2018</oasis:entry>
         <oasis:entry colname="col4">0.5<inline-formula><mml:math id="M192" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M193" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.625<inline-formula><mml:math id="M194" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Rienecker et al. (2011), <?xmltex \hack{\hfill\break}?> <uri>https://www.esrl.noaa.gov/psd/</uri> <?xmltex \hack{\hfill\break}?>(last access: 21 January 2021)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">HWSD (v121)<inline-formula><mml:math id="M195" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Soil texture data</oasis:entry>
         <oasis:entry colname="col3">n/a</oasis:entry>
         <oasis:entry colname="col4">1 km <inline-formula><mml:math id="M196" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1 km</oasis:entry>
         <oasis:entry colname="col5">Wieder et al. (2014), <?xmltex \hack{\hfill\break}?> <uri>http://daac.ornl.gov</uri> (last access: 21 January 2021)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">SPL3SMP_E<inline-formula><mml:math id="M197" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Surface soil moisture</oasis:entry>
         <oasis:entry colname="col3">April 2015–present</oasis:entry>
         <oasis:entry colname="col4">9 km <inline-formula><mml:math id="M198" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 9 km</oasis:entry>
         <oasis:entry colname="col5">Entekhabi et al. (2010), <?xmltex \hack{\hfill\break}?> <uri>https://smap.jpl.nasa.gov/</uri> <?xmltex \hack{\hfill\break}?>(last access: 21 January 2021)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">GLASS LAI<inline-formula><mml:math id="M199" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mi mathvariant="normal">a</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">b</mml:mi></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Leaf area index</oasis:entry>
         <oasis:entry colname="col3">2010–2018</oasis:entry>
         <oasis:entry colname="col4">5 km <inline-formula><mml:math id="M200" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 5 km</oasis:entry>
         <oasis:entry colname="col5">Xiao et al. (2016), <?xmltex \hack{\hfill\break}?> <uri>http://www.glass.umd.edu/Download.html</uri> <?xmltex \hack{\hfill\break}?>(last access: 21 January 2021)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SMOS_L3 CATDS<inline-formula><mml:math id="M201" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Surface soil moisture</oasis:entry>
         <oasis:entry colname="col3">2010–present</oasis:entry>
         <oasis:entry colname="col4">25km <inline-formula><mml:math id="M202" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 25 km</oasis:entry>
         <oasis:entry colname="col5">Jacquette et al. (2010), <?xmltex \hack{\hfill\break}?> <uri>https://earth.esa.int/eogateway/missions/smos</uri> <?xmltex \hack{\hfill\break}?>(last access: 21 January 2021)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table><table-wrap-foot><p id="d1e3455"><inline-formula><mml:math id="M182" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula> Forcing dataset for LPJ-DGVM. <inline-formula><mml:math id="M183" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula> External input dataset for PT-JPL<inline-formula><mml:math id="M184" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>.</p></table-wrap-foot></table-wrap>

      <p id="d1e3874">The GLASS LAI product, SMOS-L2 product, and the SMAP-L3-Enhanced product were
assimilated to simulate GPP and ET. For site simulation, in order to maintain
consistency with the SMAP Enhanced 3 Level product (Entekhabi et al., 2010),
model-forcing data were resampled to a 9 km spatial resolution based on
EASE-2 projection grid. In the global spatial simulation, the model-forcing
datasets were resampled to 0.25<inline-formula><mml:math id="M203" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> based on the bilinear method to
ensure the consistency of spatial representation.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><?xmltex \currentcnt{3}?><label>Table 3</label><caption><p id="d1e3890">Global GPP and ET products for comparison in this study.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.99}[.99]?><oasis:tgroup cols="6">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:colspec colnum="5" colname="col5" align="justify" colwidth="5.5cm"/>
     <oasis:colspec colnum="6" colname="col6" align="left"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Product</oasis:entry>
         <oasis:entry colname="col2">Dataset</oasis:entry>
         <oasis:entry colname="col3">Temporal</oasis:entry>
         <oasis:entry colname="col4">Spatial</oasis:entry>
         <oasis:entry colname="col5">Retrieval algorithm</oasis:entry>
         <oasis:entry colname="col6">References</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">resolution</oasis:entry>
         <oasis:entry colname="col4">resolution</oasis:entry>
         <oasis:entry colname="col5"/>
         <oasis:entry colname="col6"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">MOD17A2</oasis:entry>
         <oasis:entry colname="col2">GPP and ET</oasis:entry>
         <oasis:entry colname="col3">8 d average</oasis:entry>
         <oasis:entry colname="col4">1 km <inline-formula><mml:math id="M204" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1 km</oasis:entry>
         <oasis:entry colname="col5">GPP: Based on the light use efficiency <?xmltex \hack{\hfill\break}?>(LUE) model <?xmltex \hack{\hfill\break}?>ET: Improved Penman formula</oasis:entry>
         <oasis:entry colname="col6">Running et al. (2004)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">GLASS</oasis:entry>
         <oasis:entry colname="col2">GPP and ET</oasis:entry>
         <oasis:entry colname="col3">8 d average</oasis:entry>
         <oasis:entry colname="col4">5 km <inline-formula><mml:math id="M205" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 5 km</oasis:entry>
         <oasis:entry colname="col5">GPP: EC-LUE model <?xmltex \hack{\hfill\break}?>ET: Combining five Bayesian averages <?xmltex \hack{\hfill\break}?>based on process models (BMA)</oasis:entry>
         <oasis:entry colname="col6">Yuan et al. (2010)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">GOSIF GPP</oasis:entry>
         <oasis:entry colname="col2">GPP</oasis:entry>
         <oasis:entry colname="col3">8 d average</oasis:entry>
         <oasis:entry colname="col4">0.05<inline-formula><mml:math id="M206" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M207" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.05<inline-formula><mml:math id="M208" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Estimated from solar-induced chlorophyll <?xmltex \hack{\hfill\break}?>fluorescence with GPP–SIF relationships</oasis:entry>
         <oasis:entry colname="col6">Li and Xiao (2019)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">GLDAS ET</oasis:entry>
         <oasis:entry colname="col2">ET</oasis:entry>
         <oasis:entry colname="col3">daily</oasis:entry>
         <oasis:entry colname="col4">0.25<inline-formula><mml:math id="M209" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M210" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.25<inline-formula><mml:math id="M211" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Processed model assimilation</oasis:entry>
         <oasis:entry colname="col6">Fang et al. (2009)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GLEAM v3a ET</oasis:entry>
         <oasis:entry colname="col2">ET</oasis:entry>
         <oasis:entry colname="col3">daily</oasis:entry>
         <oasis:entry colname="col4">0.25<inline-formula><mml:math id="M212" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M213" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.25<inline-formula><mml:math id="M214" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Processed model assimilation</oasis:entry>
         <oasis:entry colname="col6">Martens et al. (2017)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

      <p id="d1e4163">We used four global ET products and three global GPP products (S. Li et al.,
2018; Li and Xiao, 2019; Wang et al., 2017) that was resampled to 0.25<inline-formula><mml:math id="M215" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> to evaluate the performance of the model with the joint
assimilation scheme. <?xmltex \hack{\mbox\bgroup}?>Table 3<?xmltex \hack{\egroup}?> shows the details of these GPP and ET products.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Results</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Performance of LPJ-PM for simulating GPP and ET with the assimilation of LAI and soil moisture</title>
<sec id="Ch1.S4.SS1.SSS1">
  <label>4.1.1</label><title>Accuracy assessment of GPP for separate and joint assimilation</title>
      <p id="d1e4202">In general, the <inline-formula><mml:math id="M216" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> between GPP<inline-formula><mml:math id="M217" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> and GPP<inline-formula><mml:math id="M218" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula> was above 0.4 at most of the sites (62 sites) and was relatively weak for some sites. The LAI assimilation improved the simulations at most sites (<inline-formula><mml:math id="M219" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> value increased at 82 sites), particularly for sites in the United States and Europe
(Fig. S4). The <inline-formula><mml:math id="M220" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> improvement from the LAI assimilation (LAI-only
assimilation) was superior to that from the SSM assimilation (Fig. S4b
and c). The performance of the joint assimilation was similar to that of
LAI-only assimilation. Sites (Fig. S5a) that showed positive BIAS
(GPP<inline-formula><mml:math id="M221" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula>–GPP<inline-formula><mml:math id="M222" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula>) were mainly distributed in the humid and sub-dry humid forest, grassland, and arid cropland regions, showing underestimation for GPP<inline-formula><mml:math id="M223" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula>. The assimilation improved the accuracy for overestimated sites, but there was no significant improvement for underestimated sites. The ubRMSD implied that the SSM assimilation alone had a better performance than the LAI assimilation alone, especially for sites in arid areas (Fig. 2). The analysis of the above three statistical
measures (<inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, BIAS, and ubRMSD) indicated that the accuracy of joint
assimilation was much better than that of each separate assimilation.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e4297"><bold>(a)</bold> The unbiased root mean square error (ubRMSD)
between the GPP<inline-formula><mml:math id="M225" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> and the site observations,
with yellow/blue indicating low/high ubRMSD. <bold>(b)</bold> <inline-formula><mml:math id="M226" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>ubRMSD (GPP<inline-formula><mml:math id="M227" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula>–GPP<inline-formula><mml:math id="M228" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula>). <bold>(c)</bold> <inline-formula><mml:math id="M229" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>ubRMSD (GPP<inline-formula><mml:math id="M230" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>–GPP<inline-formula><mml:math id="M231" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula>). <bold>(d)</bold> <inline-formula><mml:math id="M232" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>ubRMSD (GPP<inline-formula><mml:math id="M233" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">Joint</mml:mi></mml:msub></mml:math></inline-formula>–GPP<inline-formula><mml:math id="M234" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula>). Blue/red represents positive/negative values.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f02.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e4405">Seasonal cycles of tower GPP and simulated gross primary
productivity (GPP) from Lund–Potsdam–Jena (LPJ), LAI-only assimilation,
SSM-only assimilation, and joint assimilation for six sites representing six
PFTs.</p></caption>
            <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f03.png"/>

          </fig>

      <p id="d1e4415">At the seasonal scale, all three assimilation schemes corrected the model
trajectory and significantly improved the growing season simulations,
especially for peak values (IT-Tor, US-NR1, and US-NE1) (Fig. 3). In addition,
the linear fitting of GPP<inline-formula><mml:math id="M235" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> and GPP<inline-formula><mml:math id="M236" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula> on a monthly scale was closer to 1 : 1 (<inline-formula><mml:math id="M237" display="inline"><mml:mrow><mml:mi>y</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.92</mml:mn><mml:mi>x</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">21.66</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M238" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M239" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 0.001) than that of GPP<inline-formula><mml:math id="M240" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula> (<inline-formula><mml:math id="M241" display="inline"><mml:mrow><mml:mi>y</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.89</mml:mn><mml:mi>x</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">28.3</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M242" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M243" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 0.001) and GPP<inline-formula><mml:math id="M244" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> (<inline-formula><mml:math id="M245" display="inline"><mml:mrow><mml:mi>y</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.86</mml:mn><mml:mi>x</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">41.70</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M246" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M247" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 0.001) (Fig. S9). The results in Table S2
support the above analysis, and the joint assimilation showed advantages in
overall accuracy in both arid and humid areas.</p>
      <p id="d1e4552">The residual analysis indicated that the three assimilation schemes for GPP
(Fig. S11 left) were different. For the assimilation results, most of
the errors were distributed around <inline-formula><mml:math id="M248" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>70–60 g C m<inline-formula><mml:math id="M249" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> per month. The high GPP<inline-formula><mml:math id="M250" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula> values were considerably underestimated. The maximum negative error reached 100 g C m<inline-formula><mml:math id="M251" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> per month. The error distribution of GPP<inline-formula><mml:math id="M252" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> was more dispersed than that of GPP<inline-formula><mml:math id="M253" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula> and GPP<inline-formula><mml:math id="M254" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula>. Among the residuals of these three schemes, GPP<inline-formula><mml:math id="M255" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> significantly overestimated the GPP<inline-formula><mml:math id="M256" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula>,
mainly distributed in the 0–200 g C m<inline-formula><mml:math id="M257" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> per month range.
GPP<inline-formula><mml:math id="M258" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula> showed significant improvement in the overestimation of
GPP<inline-formula><mml:math id="M259" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula> compared with GPP<inline-formula><mml:math id="M260" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula>. In general, the GPP<inline-formula><mml:math id="M261" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> with
the most concentrated error distribution had significant improvement.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e4692">Scatter plots of daily GPP<inline-formula><mml:math id="M262" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> <bold>(a)</bold> and GPP<inline-formula><mml:math id="M263" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> <bold>(b)</bold> versus tower GPP for different PFTs.</p></caption>
            <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f04.png"/>

          </fig>

      <p id="d1e4725">After determining the optimal assimilation scheme (Joint LAI and SSM
assimilation scheme), we evaluated the GPP<inline-formula><mml:math id="M264" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> and GPP<inline-formula><mml:math id="M265" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> at the site level (Fig. 4). The results showed that GPP<inline-formula><mml:math id="M266" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> performed better (<inline-formula><mml:math id="M267" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M268" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.83, ubRMSD <inline-formula><mml:math id="M269" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.15 g C m<inline-formula><mml:math id="M270" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> d<inline-formula><mml:math id="M271" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) than
GPP<inline-formula><mml:math id="M272" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> (<inline-formula><mml:math id="M273" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M274" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.69, ubRMSD <inline-formula><mml:math id="M275" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.91 g C m<inline-formula><mml:math id="M276" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> d<inline-formula><mml:math id="M277" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). The
noticeable underestimation in all PFTs and overestimation at most forest
sites for GPP<inline-formula><mml:math id="M278" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> were corrected by joint assimilation (GPP<inline-formula><mml:math id="M279" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula>). Our joint assimilation methods had better performance in forests, shrublands, and grasslands than in croplands and savannas. Except for the cropland, the linear fitting results of other types were all below the 1 : 1
line, showing the overall underestimation. Superior performance in both
the original simulation and assimilation occurred at shrubland (<inline-formula><mml:math id="M280" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M281" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.93, ubRMSD <inline-formula><mml:math id="M282" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.89 g C m<inline-formula><mml:math id="M283" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> d<inline-formula><mml:math id="M284" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) and grassland (<inline-formula><mml:math id="M285" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M286" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.97,
ubRMSD <inline-formula><mml:math id="M287" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.83 g C m<inline-formula><mml:math id="M288" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> d<inline-formula><mml:math id="M289" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) sites. However, the standard
deviation of GPP<inline-formula><mml:math id="M290" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> and GPP<inline-formula><mml:math id="M291" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula> at savanna sites was relatively large, and the GPP<inline-formula><mml:math id="M292" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> at several savanna sites was significantly underestimated.</p>
</sec>
<sec id="Ch1.S4.SS1.SSS2">
  <label>4.1.2</label><title>Accuracy assessment of ET for separate and joint assimilation</title>
      <p id="d1e5017">In general, the coefficient of determination (<inline-formula><mml:math id="M293" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>) between ET<inline-formula><mml:math id="M294" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M295" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula> was generally over 0.4 (the simulations were superior to GPP<inline-formula><mml:math id="M296" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula>) (Fig. S6). ET<inline-formula><mml:math id="M297" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula> showed slightly higher <inline-formula><mml:math id="M298" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, while some sites showed reduced values (41 sites). The ET<inline-formula><mml:math id="M299" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M300" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula>
were significantly improved compared with the ET<inline-formula><mml:math id="M301" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula>. The <inline-formula><mml:math id="M302" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> increased considerably in Australia but declined at some sites in the
United States after assimilation. For ubRMSD, ET<inline-formula><mml:math id="M303" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> performed better than ET<inline-formula><mml:math id="M304" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M305" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula>. The SSM assimilation improved more in humid regions, while the ubRMSD of ET<inline-formula><mml:math id="M306" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> was slightly higher in South
America (Fig. 5). In the original LPJ-DGVM simulation, the sites with a
negative BIAS were mostly located in the humid and sub-dry humid regions,
while most of the sites in arid and semi-arid regions had underestimation
(Fig. S7a, Table S3). The assimilation improved ET at some of the
overestimated sites, but the underestimation over these sites showed little
improvement.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e5156"><bold>(a)</bold> The unbiased root mean square error
(ubRMSE) between the ET simulated by the LPJ-DGVM and the site observations,
with yellow/blue indicating low/high ubRMSD.
<bold>(b)</bold> <inline-formula><mml:math id="M307" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>ubRMSD (ET<inline-formula><mml:math id="M308" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula>–ET<inline-formula><mml:math id="M309" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula>). <bold>(c)</bold> <inline-formula><mml:math id="M310" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>ubRMSD (ET<inline-formula><mml:math id="M311" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>–ET<inline-formula><mml:math id="M312" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula>).
<bold>(d)</bold> <inline-formula><mml:math id="M313" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>ubRMSD (ET<inline-formula><mml:math id="M314" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">Joint</mml:mi></mml:msub></mml:math></inline-formula>–ET<inline-formula><mml:math id="M315" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula>).
Blue/red represents positive/negative values.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f05.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e5255">Seasonal cycles of tower-based and simulated ET
from Lund–Potsdam–Jena (LPJ), LAI-only assimilation, SSM-only
assimilation, and joint assimilation for the six sites representing six PFTs
during the study period.</p></caption>
            <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f06.png"/>

          </fig>

      <p id="d1e5265">At the seasonal scale, the model simulations were able to capture the
temporal trend of ET<inline-formula><mml:math id="M316" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula>, and joint assimilation significantly improved the simulation in the growing season (US-NR1, US-NE1); overall
underestimation was observed for ET<inline-formula><mml:math id="M317" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula>, especially in winter (Fig. 6). Overall, the linear fitting of monthly ET<inline-formula><mml:math id="M318" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M319" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula> was closer to 1 : 1 than that of ET<inline-formula><mml:math id="M320" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M321" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> (Fig. S6). The
simulation accuracy of joint assimilation was better than that of each separate assimilation, and the performance of the SSM assimilation was better than
that of the LAI assimilation.</p>
      <p id="d1e5323">The ET residual analysis (Fig. S11 right) indicated that the three
assimilation scheme errors showed underestimation for ET<inline-formula><mml:math id="M322" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula>. In
general, the error distribution of separate assimilations was more dispersed
than that of the joint assimilation. Similar to the assimilation performance
of GPP, ET<inline-formula><mml:math id="M323" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M324" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> significantly improved the overestimation of ET<inline-formula><mml:math id="M325" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula> but did not significantly improve the underestimation. For the ET<inline-formula><mml:math id="M326" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula>, most of the errors were distributed around <inline-formula><mml:math id="M327" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>30–18 mm per month. The region with high ET<inline-formula><mml:math id="M328" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula> was considerably
underestimated, and the maximum negative error reached <inline-formula><mml:math id="M329" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>57 mm per month.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e5397">Scatter plots of daily ET<inline-formula><mml:math id="M330" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> <bold>(a)</bold> and daily ET<inline-formula><mml:math id="M331" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> <bold>(b)</bold> versus tower
ET for different PFTs.</p></caption>
            <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f07.png"/>

          </fig>

      <p id="d1e5430">We also evaluated the ET assimilation results at the PFT scale (Fig. 7).
The results showed that our ET values resulting from the assimilation
performed better at the site level (<inline-formula><mml:math id="M332" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M333" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.77, ubRMSD <inline-formula><mml:math id="M334" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.65 mm d<inline-formula><mml:math id="M335" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) than that of ET<inline-formula><mml:math id="M336" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> (<inline-formula><mml:math id="M337" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M338" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.67, ubRMSD <inline-formula><mml:math id="M339" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.95 mm d<inline-formula><mml:math id="M340" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). Joint assimilation significantly reduced the errors of those shrubland sites with overestimation for ET<inline-formula><mml:math id="M341" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula>, and the site distribution was closer to the 1 : 1 line. Our assimilation methods had better
performance in forest, savanna, and grassland ecosystems than in cropland
and shrubland (Table S3). The linear fitting results of grassland and
shrubland were all above the 1 : 1 line, showing overall overestimation.
Although the original simulation and assimilation performance were superior
at savanna sites (<inline-formula><mml:math id="M342" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M343" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.95, ubRMSD <inline-formula><mml:math id="M344" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.78 mm d<inline-formula><mml:math id="M345" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), the
standard deviations of ET<inline-formula><mml:math id="M346" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M347" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula> at savanna sites were relatively large, which was similar to the GPP results at savanna sites.</p>
</sec>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Comparison of assimilation performance in semi-arid and arid regions with that in humid and sub-dry humid regions</title>
      <p id="d1e5591">During the period 2010–2014, monthly GPP<inline-formula><mml:math id="M348" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M349" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> performed differently in humid and sub-dry humid regions and semi-arid and arid regions (Fig. 8, Tables S2, S3). Overall, the GPP and ET simulations had good consistency with the tower data in the two regions. For GPP<inline-formula><mml:math id="M350" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula>,
there was no significant difference in the correlation and fitting
coefficients between the two regions. As for ET<inline-formula><mml:math id="M351" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula>, the fitting
results and <inline-formula><mml:math id="M352" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> values in the semi-arid and arid regions performed
better than those in the humid and sub-dry humid regions, which also
suggested the importance of SSM for ET estimation in water-limited areas.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e5643">Scatter plots of daily tower GPP and ET versus
GPP<inline-formula><mml:math id="M353" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M354" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> under arid and humid sites:
<bold>(a, c)</bold> the fitting results of GPP and ET in arid and semi-arid
regions, respectively, and <bold>(b, d)</bold> the fitting results of GPP and ET in
humid and dry sub-humid zone, respectively.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f08.png"/>

        </fig>

      <p id="d1e5676">On the daily scale, the original GPP simulations (GPP<inline-formula><mml:math id="M355" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula>) performed better in the semi-arid and arid regions than in the humid and sub-dry humid regions with higher <inline-formula><mml:math id="M356" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and lower ubRMSD (Table S2).</p>
      <p id="d1e5700">The <inline-formula><mml:math id="M357" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and BIAS implied that the LAI assimilation alone had a better
performance than the SSM assimilation alone. However, for sites in arid and
semi-arid areas, the ubRMSD showed that the GPP<inline-formula><mml:math id="M358" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> improved better than GPP<inline-formula><mml:math id="M359" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula>, which both demonstrated SSM data are essential in water-limited regions. For GPP<inline-formula><mml:math id="M360" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula>, the shrubland in the semi-arid and arid regions had the lowest <inline-formula><mml:math id="M361" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> values and the second lowest ubRMSD. The forest in the semi-arid and arid regions had the largest improvement after assimilation. In the humid and sub-dry humid regions, the GPP<inline-formula><mml:math id="M362" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> of the savanna and cropland showed the largest improvement (<inline-formula><mml:math id="M363" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> increased by 64.7 % and 71.1 %, respectively; ubRMSD decreased by 47.0 % and 31.8 %, respectively). The grassland in the semi-arid and arid regions had
the highest <inline-formula><mml:math id="M364" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, and the savanna by combining all indicators had the
best assimilation results compared to other types in both regions.</p>
      <p id="d1e5784">Similar to ET<inline-formula><mml:math id="M365" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula> (Table S3), the ET<inline-formula><mml:math id="M366" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> in the semi-arid and arid regions was better than that in humid and sub-dry humid regions in terms of four
evaluation indicators (ubRMSD decreased by 34.4 % in semi-arid and arid
regions and the ubRMSD decreased by 30.9 % in humid and sub-dry humid
regions compared with ET<inline-formula><mml:math id="M367" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula>). The <inline-formula><mml:math id="M368" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and ubRMSD implied that the SSM assimilation alone had a better performance than the LAI assimilation
alone, especially for sites in arid areas. and the BIAS showed that the
ET<inline-formula><mml:math id="M369" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LAI</mml:mi></mml:msub></mml:math></inline-formula> improved better than ET<inline-formula><mml:math id="M370" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> for sites in humid and sub-dry humid areas. The performance of the original simulation and assimilation of grassland sites in the semi-arid and arid regions was the best among all five PFTs.</p>
      <p id="d1e5844">To investigate the reasons for better assimilation performance in
water-limited regions, we evaluated the GPP and ET simulated by the LPJ-PM
according to <inline-formula><mml:math id="M371" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, ubRMSD, and BIAS (Fig. 9). Compared with the semi-arid and arid regions, the humid and sub-dry humid region had smaller
<inline-formula><mml:math id="M372" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> mean, larger BIAS, and no significant difference in mean ubRMSD for
GPP<inline-formula><mml:math id="M373" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>. In general, the evaluation results of joint assimilation for ET<inline-formula><mml:math id="M374" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula> were generally consistent with those for GPP<inline-formula><mml:math id="M375" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> and GPP<inline-formula><mml:math id="M376" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>. ET<inline-formula><mml:math id="M377" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula> showed underestimation, which was consistent with the
underestimation in SSM assimilation. These results indicated that both GPP
and ET modeled by LPJ-PM with joint assimilation were less stable and had a
lower performance in the humid and sub-dry regions than in the semi-arid and
arid regions.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9"><?xmltex \currentcnt{9}?><?xmltex \def\figurename{Figure}?><label>Figure 9</label><caption><p id="d1e5917">Box plots of <inline-formula><mml:math id="M378" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, ubRMSD, and BIAS for GPP<inline-formula><mml:math id="M379" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> <bold>(a)</bold> and ET<inline-formula><mml:math id="M380" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula> <bold>(b)</bold>. A represents the sites in arid and semi-arid areas, and B represents the sites in humid and dry sub-humid areas.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f09.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS3">
  <label>4.3</label><title>Comparison of assimilation performance in assimilating SMOS and SMAP soil moisture data</title>
      <p id="d1e5969">The Taylor chart was used to compare the assimilation performance of
ET<inline-formula><mml:math id="M381" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMAP</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M382" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMOS</mml:mi></mml:msub></mml:math></inline-formula> at 46 AmeriFlux sites (Fig. 10 left). The results showed that ET<inline-formula><mml:math id="M383" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMAP</mml:mi></mml:msub></mml:math></inline-formula> performed better than ET<inline-formula><mml:math id="M384" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMOS</mml:mi></mml:msub></mml:math></inline-formula> for most PFTs, except forest. Both ET<inline-formula><mml:math id="M385" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMAP</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M386" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMOS</mml:mi></mml:msub></mml:math></inline-formula> performed well for grassland (closer to point A), and there was little difference between <inline-formula><mml:math id="M387" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and ubRMSD. The NSD of ET<inline-formula><mml:math id="M388" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMAP</mml:mi></mml:msub></mml:math></inline-formula> in grassland was 0.88, which was closer to 1 than that of ET<inline-formula><mml:math id="M389" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMOS</mml:mi></mml:msub></mml:math></inline-formula>. The assimilation of ET had a lower <inline-formula><mml:math id="M390" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and higher ubRMSD (0.7–0.8) in forest than other
PFTs, and the NSD of cropland and shrubland was lower than that of other
PFTs (0.6–0.8), indicating that the assimilation for cropland and shrubland
could not reproduce the variations in ET effectively. However, ET<inline-formula><mml:math id="M391" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMAP</mml:mi></mml:msub></mml:math></inline-formula> showed significant improvement in <inline-formula><mml:math id="M392" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> compared with ET<inline-formula><mml:math id="M393" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMOS</mml:mi></mml:msub></mml:math></inline-formula> for shrubland and cropland. The assimilation performance of ET<inline-formula><mml:math id="M394" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMAP</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M395" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMOS</mml:mi></mml:msub></mml:math></inline-formula> for savanna showed the greatest difference. In general, the ET<inline-formula><mml:math id="M396" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMAP</mml:mi></mml:msub></mml:math></inline-formula> and ET<inline-formula><mml:math id="M397" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMOS</mml:mi></mml:msub></mml:math></inline-formula> were slightly different, and the ET<inline-formula><mml:math id="M398" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMAP</mml:mi></mml:msub></mml:math></inline-formula> was
more improved than ET<inline-formula><mml:math id="M399" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMOS</mml:mi></mml:msub></mml:math></inline-formula>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><?xmltex \currentcnt{10}?><?xmltex \def\figurename{Figure}?><label>Figure 10</label><caption><p id="d1e6154">Taylor diagram (left) comparing ET simulations with
observations at all 46 AmeriFlux sites at the daily time step between April
2015 and December 2018. Blue dots represent results based on assimilation
with SMAP SSM only, and red dots represent results based on assimilation with
SMOS SSM only. Reference points A and B–F correspond to the vegetation
functional types (PFTs). The grid diagram (right) compares the evaluation
indices of ET simulations with those of the observed values at all 46
AmeriFlux sites with different wet and dry zones at the daily time step; the
yellow cells indicate that ET<inline-formula><mml:math id="M400" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMAP</mml:mi></mml:msub></mml:math></inline-formula> performs better in the metric, and green cells indicate that ET<inline-formula><mml:math id="M401" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMOS</mml:mi></mml:msub></mml:math></inline-formula>
performs better in the metric.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f10.png"/>

        </fig>

      <p id="d1e6181">Figure 10 (right) shows the assimilation accuracy of ET<inline-formula><mml:math id="M402" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMOS</mml:mi></mml:msub></mml:math></inline-formula> and
ET<inline-formula><mml:math id="M403" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMAP</mml:mi></mml:msub></mml:math></inline-formula> in different humid and arid regions. The ET<inline-formula><mml:math id="M404" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMAP</mml:mi></mml:msub></mml:math></inline-formula> had significant advantages for the four indicators. The <inline-formula><mml:math id="M405" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> of ET<inline-formula><mml:math id="M406" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMAP</mml:mi></mml:msub></mml:math></inline-formula> was higher than that of ET<inline-formula><mml:math id="M407" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMOS</mml:mi></mml:msub></mml:math></inline-formula> in all the areas. However, ET<inline-formula><mml:math id="M408" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMOS</mml:mi></mml:msub></mml:math></inline-formula> in some evaluation indicators showed a better performance than ET<inline-formula><mml:math id="M409" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SMAP</mml:mi></mml:msub></mml:math></inline-formula>
(BIAS in the humid region; ubRMSD in the sub-dry humid region). This may be
due to the overall more humid nature of SMOS SSM than the SMAP SSM.
Moreover, the sensitivity of deep soil moisture contributed more to the ET
in humid areas than in the water-limited areas.</p>
</sec>
<sec id="Ch1.S4.SS4">
  <label>4.4</label><title>Global simulations of GPP and ET with joint assimilation of LAI and soil moisture data</title>
      <p id="d1e6267">To assess the spatial scalability of the LPJ-VSJA assimilation scheme, we
simulated the global daily GPP and ET for 2010–2018 with a spatial
resolution of 0.25<inline-formula><mml:math id="M410" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. The original results simulated by the
LPJ-DGVM and LPJ-VSJA were referred to as LPJ-DGVM GPP(ET) and LPJ-VSJA
GPP(ET), respectively. We compared the annual spatial GPP and ET values and
the error standard deviation of the LPJ-VSJA with several existing flux
products.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><?xmltex \currentcnt{11}?><?xmltex \def\figurename{Figure}?><label>Figure 11</label><caption><p id="d1e6281">Column A​​​​​​​: spatial distribution of annual LPJ-VSJA GPP and other independent satellite-based datasets. Column B: spatial distribution of the difference between annual LPJ-VSJA GPP and other independent satellite-based datasets. Column C: scatter plots between these products. Black lines show the 1 : 1 line, and red lines show the regression fit.</p></caption>
          <?xmltex \igopts{width=409.719685pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f11.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12" specific-use="star"><?xmltex \currentcnt{12}?><?xmltex \def\figurename{Figure}?><label>Figure 12</label><caption><p id="d1e6292">Column A: spatial distribution of annual LPJ-VSJA ET and
other independent satellite-based datasets. Column B: spatial distribution of the difference between annual LPJ-VSJA ET and other independent satellite-based datasets. Column C: scatter plots between these products are provided on the right of the difference maps. Black lines show the 1 : 1 line, and red lines show the regression fit.</p></caption>
          <?xmltex \igopts{width=409.719685pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f12.png"/>

        </fig>

      <p id="d1e6302">Figures 11 and 12 depict the spatial distribution of the annual mean and the
differences between our simulation results and the global independent
satellite-based products. The developed LPJ-VSJA GPP was the closest to
GOSIF GPP (Li and Xiao, 2019) in most regions with the lowest spatial
mean deviation (LPJ-VSJA-GOSIF) (27.9 g C m<inline-formula><mml:math id="M411" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M412" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), followed by GLASS GPP (51.2 g C m<inline-formula><mml:math id="M413" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M414" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) (Yuan et al., 2010), LPJ-DGVM (<inline-formula><mml:math id="M415" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>73.4 g C m<inline-formula><mml:math id="M416" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M417" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), and MODIS GPP (93.1 g C m<inline-formula><mml:math id="M418" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M419" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>).
LPJ-VSJA had higher GPP values than GOSIF GPP in tropical regions, such as
Amazonia, Central Africa, and Southeast Asia. In general, the annual mean
and differences between MODIS, GOSIF GPP, LPJ-DGVM, and our LPJ-VSJA were in
broad agreement (with higher <inline-formula><mml:math id="M420" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> ranging from 0.74 to 0.95).</p>
      <p id="d1e6420">LPJ-VSJA ET was the closest to GLEAM ET on the spatial average with the
least spatial average deviation (<inline-formula><mml:math id="M421" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>13.9 mm yr<inline-formula><mml:math id="M422" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) and highest <inline-formula><mml:math id="M423" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> (0.88), followed by GLASS ET (<inline-formula><mml:math id="M424" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>23.1 mm yr<inline-formula><mml:math id="M425" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 0.82), GLDAS ET (<inline-formula><mml:math id="M426" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>34.7 mm yr<inline-formula><mml:math id="M427" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 0.73), LPJ-DGVM (<inline-formula><mml:math id="M428" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>48.7 and 0.66 mm yr<inline-formula><mml:math id="M429" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), and MODIS ET (<inline-formula><mml:math id="M430" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>122.1 and 0.54 mm yr<inline-formula><mml:math id="M431" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F13" specific-use="star"><?xmltex \currentcnt{13}?><?xmltex \def\figurename{Figure}?><label>Figure 13</label><caption><p id="d1e6532">Spatial distribution and histograms of error standard
deviation (<inline-formula><mml:math id="M432" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula>) for global GPP products: MODIS <bold>(a)</bold>, GOSIF <bold>(b)</bold>, GLASS <bold>(c)</bold>, LPJ-DGVM <bold>(d)</bold>, and LPJ-VSJA <bold>(e)</bold>.</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f13.png"/>

        </fig>

      <p id="d1e6564">Figure 13a–e represent the spatial error standard deviation (<inline-formula><mml:math id="M433" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula>) distribution of MODIS, GLASS, GOSIF, and LPJ-VSJA GPP, respectively. The
graphs on the right side depict the corresponding histograms. The <inline-formula><mml:math id="M434" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula>
of the MODIS GPP was evenly distributed between 30 and 60 g C m<inline-formula><mml:math id="M435" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> per month, while the average <inline-formula><mml:math id="M436" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> of other products was concentrated
in 0–20 g C m<inline-formula><mml:math id="M437" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> per month (90 %). The high errors of all products
were concentrated in the hot and humid areas of southern North
America, eastern South America, humid and dry sub-humid areas of South Asia,
and the savannas of Africa and Australia. The error histogram of GOSIF GPP
and LPJ-DGVM GPP was in line with the normal distribution, with an average
value of 8.3 and 22.4 g C m<inline-formula><mml:math id="M438" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> per month.
The GLASS GPP product had the lowest mean value (3.6 g C m<inline-formula><mml:math id="M439" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> per
month), followed by LPJ-VSJA (4.7 g C m<inline-formula><mml:math id="M440" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> per month), but the
error variance of the LPJ-VSJA product was the lowest, indicating the stability of the regional error (Table S4). Compared to the LPJ-DGVM, the
joint assimilation results showed improvement in all regions (the average
error reduced by 17.7 g C m<inline-formula><mml:math id="M441" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> per month), especially in the humid
regions of South Asia, Australia, and the United States. Our LPJ-VSJA GPP
was generally proven to have high accuracy and stability for spatial
analysis and could provide a reference for other model products.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F14" specific-use="star"><?xmltex \currentcnt{14}?><?xmltex \def\figurename{Figure}?><label>Figure 14</label><caption><p id="d1e6663">Spatial distribution and histograms of error standard
deviation (<inline-formula><mml:math id="M442" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula>) for global ET products: MODIS <bold>(a)</bold>, GLDAS <bold>(b)</bold>, GLEAM <bold>(c)</bold>, GLASS <bold>(d)</bold>, LPJ-DGVM <bold>(e)</bold>, and LPJ-VSJA <bold>(f)</bold>.</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/6311/2022/hess-26-6311-2022-f14.png"/>

        </fig>

      <p id="d1e6699">Figure 14a–f show the <inline-formula><mml:math id="M443" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> of MODIS, GLDAS, GLEAM, GLASS, and
LPJ-VSJA ET (the units are millimeters per month), and the right graphs are the
corresponding histograms. The <inline-formula><mml:math id="M444" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> values of GLDAS and LPJ-VSJA
represented a normal distribution trend. Except for MODIS, GLASS, and
LPJ-DGVM (0–60 mm per month), the <inline-formula><mml:math id="M445" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> of other products was
generally between 0–20 mm per month. The simulation error was relatively
smaller in the Northern Hemisphere than in the Southern Hemisphere,
especially for GLASS ET and GLDAS ET. Significant improvements in joint
assimilation were observed in the Northern Hemisphere (especially in the
semi-arid areas of the western United States and savanna and cropland areas
of central India) and African savanna areas, and the average error was
reduced by 15.1 mm per month. In general, the error mean and variance of
LPJ-VSJA and GLEAM products were relatively low (Table S4), and there was no
apparent extremely high-value region in the error distribution. Among the five products, LPJ-VSJA had the lowest error mean and variance and the
highest accuracy.</p>
</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Discussion</title>
<sec id="Ch1.S5.SS1">
  <label>5.1</label><title>Advantage of joint assimilation for GPP and ET</title>
      <p id="d1e6740">The benefit of employing multiple data flows in an assimilation system is
the complementarity of the data, which enables constraints on different
components of the underlying process-based terrestrial biosphere model. Due
to the interaction and feedback between the internal components of the
model, the assimilation of multiple observations has a synergistic effect,
and the integrated constraints are greater than the individual constraint
(Kato et al., 2013). The advantage of our joint assimilation is that it
can improve the simulation accuracy of both GPP and ET, especially ET, in
arid and semi-arid regions.</p>
      <p id="d1e6743">In the GPP assimilation experiment, the performance of the LAI assimilation
was better than that of the SSM assimilation possibly for two reasons: (1) the LPJ-VSJA is more controlled by LAI data because the ratio of assimilated LAI (daily input) to SSM observations (3 d interval input) is
approximately 3 : 1, which makes the likelihood function biased to LAI data; and (2) the SM directly influences the simulation of ET, and the corresponding time function (computes the top layer SM – 50 cm) used here by Zhao et al. (2013) will result in the error of the updated top SM and propagating the error to the GPP<inline-formula><mml:math id="M446" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula>. In addition, the 8 d interval LAI has the capability to capture the temporal variability of phenology.</p>
      <p id="d1e6755">Current studies on terrestrial water and carbon flux assimilation mostly
focus on the assimilation between a single model framework and observation
results, lacking the fusion and comparison between multiple models. The
processed models used in DA are simplifications and approximations of
reality, and different models focus on different ecological processes. In
this study, the updated ET module was integrated to compensate for the
simplification of soil stratification and the lack of SM information in the
hydrological module of the LPJ-DGVM. Therefore, the integration of multiple
types of models and multi-source observation data (remotely sensed data,
ecological inventory data; National Ecological Observatory Network, NEON; Keller et al., 2008) and other measurements (Desai et al., 2011;
Hayes et al., 2012) is expected to more objectively and effectively simulate
the real state of ecosystems.</p>
</sec>
<sec id="Ch1.S5.SS2">
  <label>5.2</label><title>Comparison of joint assimilation (LPJ-VSJA) and other models for GPP and ET across regions and vegetation types</title>
      <p id="d1e6766">Global GPP and ET for different products were calculated by multiplying the
global mean GPP density flux by the global vegetation area (<inline-formula><mml:math id="M447" display="inline"><mml:mrow><mml:mn mathvariant="normal">122.4</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M448" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>) that originated from the MODIS land cover product (Friedl et al., 2010). The mean global GPP of the LPJ-VSJA (130.2 Pg C yr<inline-formula><mml:math id="M449" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) was approximately 12 % lower than that of PML-V2 (145.8 Pg C yr<inline-formula><mml:math id="M450" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) and 18 % higher than that of GLASS and MODIS, respectively (Table S6). The GPP
values of LPJ-VSJA and GOSIF were the most similar. The GOSIF GPP was
developed from gridded solar-induced chlorophyll fluorescence (SIF) using simple linear relationships between SIF and
GPP. Our global LPJ-VSJA GPP estimates were within the currently most
plausible 110–150 Pg C yr<inline-formula><mml:math id="M451" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> range.</p>
      <p id="d1e6829">As for ET, our results were similar to those of GLEAM ET and lower than
those of PML-V2, GLDAS-2, and GLASS ET (<inline-formula><mml:math id="M452" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 72 000 km<inline-formula><mml:math id="M453" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M454" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). Joint assimilation improved the overestimation of
LPJ-DGVM ET. At the daily scale, the estimation accuracy of PML-V2 and
GLDAS-2 products, calibrated with flux tower data, was better than that of
our estimates, which suggests underestimation of LPJ-VSJA ET in wet regions. It is likely because the SSM of SMAP or SMOS was underestimated in
the wet region, or the influence of deep SM was underrepresented. According
to Seneviratne et al. (2010), satellite-based ET estimation approaches
often overestimate ET in areas of arid and semi-arid climatic regimes in the
magnitude of 0.50 to 3.00 mm d<inline-formula><mml:math id="M455" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The poor performance of these models
can largely be attributed to the lack of constraints of SSM or RZSM and more
accurate vegetation parameters (Gokmen et al., 2012; Pardo et al., 2014).
For instance, the monthly estimated ET modeled by the
Penman–Monteith–Leuning (PML) model agreed with flux tower data well
(<inline-formula><mml:math id="M456" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M457" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.77; BIAS <inline-formula><mml:math id="M458" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M459" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>9.7 %, approximately 0.2 mm d<inline-formula><mml:math id="M460" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). Our annual ET simulations were lower than other products and slightly underestimated tower ET with a BIAS of 0.19 mm d<inline-formula><mml:math id="M461" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (ET<inline-formula><mml:math id="M462" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">OBS</mml:mi></mml:msub></mml:math></inline-formula>–ET<inline-formula><mml:math id="M463" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">joint</mml:mi></mml:msub></mml:math></inline-formula>).</p>
      <p id="d1e6948">In general, GPP and ET had better assimilation performance in arid and
semi-arid regions than in humid and sub-dry humid regions, likely because of
the following reasons. First, the incorporation of SSM is more important for
vegetation growth in water-limited areas. The module PT-JPL<inline-formula><mml:math id="M464" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> has been proven to have better performance in semi-arid and arid regions (Purdy
et al., 2018). Our integrated model LPJ-PM also performed better in semi-arid
and arid regions by assimilating SMAP soil moisture (Li et al., 2020).
Second, the input performance, including SMOS and SMAP SSM products, is
better in arid and temperate regions than in cold and humid regions
(Zhang et al., 2019). Third, the vegetation types in humid regions are
more complex and relatively less accurately simulated by the LPJ-DGVM within
a single grid cell. For comparison, Zhang et al. (2020) used a
data-driven upscaling approach to estimate GPP and ET in global semi-arid
regions. This data-driven approach (<inline-formula><mml:math id="M465" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M466" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.79, RMSD <inline-formula><mml:math id="M467" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.13 g C m<inline-formula><mml:math id="M468" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> d<inline-formula><mml:math id="M469" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) had slightly higher performance in estimating GPP than our LPJ-VSJA (<inline-formula><mml:math id="M470" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M471" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.73 and RMSD <inline-formula><mml:math id="M472" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.14 g C m<inline-formula><mml:math id="M473" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> d<inline-formula><mml:math id="M474" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), and
the data-driven method (<inline-formula><mml:math id="M475" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M476" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.72 and RMSD <inline-formula><mml:math id="M477" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.72 mm d<inline-formula><mml:math id="M478" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) had identical performance for estimating ET with our LPJ-VSJA (<inline-formula><mml:math id="M479" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M480" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.73 and RMSD <inline-formula><mml:math id="M481" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.72 mm d<inline-formula><mml:math id="M482" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>).</p>
      <p id="d1e7135">Our assimilation performance varied with PFT. The GPP and ET assimilation
results of savanna sites performed well in both dry and wet regions, and
those of shrubland sites showed the most remarkable improvement for
simulations of LPJ-DGVM. The original simulation and assimilation
performance of grassland sites in the semi-arid and arid regions were the
best for all five PFTs. Consistent with our research, previous studies also
showed better GPP or ET simulations for grassland, savannas, and shrublands
biomes. For instance, Feng et al. (2015) validated five satellite-based
ET algorithms for semi-arid ecosystems and concluded that all the models
produced acceptable and relatively better results for most grassland,
savanna, and shrubland sites. Yang et al. (2017) demonstrated that the
GLEAM ET had a superior performance for the grassland sites. The GOSIF GPP
demonstrated better simulation for grassland and woody savannas sites at
8 d time steps with higher <inline-formula><mml:math id="M483" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> (0.77 and 0.83, respectively) and
lower RMSD (1.48 and 1.1 g C m<inline-formula><mml:math id="M484" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> d<inline-formula><mml:math id="M485" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) (Li
and Xiao, 2019). In contrast, our LPJ-VSJA GPP showed an <inline-formula><mml:math id="M486" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> of 0.87 for grassland and 0.75 for savannas and an RMSD of 1.11 and 1.1 g C m<inline-formula><mml:math id="M487" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> d<inline-formula><mml:math id="M488" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively, in semi-arid and arid
regions.</p>
</sec>
<sec id="Ch1.S5.SS3">
  <label>5.3</label><title>Uncertainty analysis of joint assimilation</title>
      <p id="d1e7217">Our validation results at both site and regional scales indicated that
uncertainty existed in LPJ-VSJA daily GPP and ET estimates. The errors from
the tower EC observations, model-driven data, model structure, error of
satellite-based observations (e.g., LAI and SSM), and the spatial scale
mismatch between the ground observed footprint size and satellite-derived
footprint size were the vital factors affecting assimilation performance.</p>
      <p id="d1e7220">First, recent studies have revealed errors in the GLASS LAI and SMOS or SMAP
SSM compared with ground measurements. By computing the RMSD and <inline-formula><mml:math id="M489" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> of each product, the GLASS LAI accuracy was clearly superior to that of
MODIS and Four-Scale Geometric Optical Model-based LAI (FSGOM) in forests,
and GLASS and FSGOM led to much higher annual GPP and ET estimates
compared to MCD15 (Liu et al., 2018). The vegetation type (or land cover)
misclassification caused 15 %–50 % differences in LAI retrieval (Fang and Liang, 2005; Gonsamo and Chen, 2011). Yan et al. (2016) calculated a RMSD of 0.18 for the GLASS LAI over a range of HeiHe River basin sites and
used the error to improve the simulation of LAI and fluxes by assimilating
GLASS LAI data. Previous studies reported an improvement in the performance
of the SMOS and SMAP products (Lievens et al., 2015; Miernecki et al.,
2014), which both provide an accuracy of 0.04 m<inline-formula><mml:math id="M490" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M491" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (Zhang et
al., 2019). However, the actual observation error of these two products
typically depends on the spatial location and time of the year (RMSD varying
between 0.035 and 0.056 m<inline-formula><mml:math id="M492" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M493" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for several retrieval
configurations) (Brocca et al., 2012). According to Purdy et al. (2018), the ET simulated by PT-JPL<inline-formula><mml:math id="M494" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">SM</mml:mi></mml:msub></mml:math></inline-formula> using the 9 km SM_L3_P_E data showed an inferior agreement (<inline-formula><mml:math id="M495" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M496" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.47) but a relatively low RMSD (0.77 mm d<inline-formula><mml:math id="M497" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), due to the
SMAP errors in the grid cell with soil heterogeneity and the climatological
differences between model SM forecasts and SMAP SSM (Reichle and Koster,
2004). We rescaled the ET<inline-formula><mml:math id="M498" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula> to the probability distribution of the ET<inline-formula><mml:math id="M499" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> through a cumulative distribution function (CDF) to correct the potential seasonal biases of ET<inline-formula><mml:math id="M500" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">PM</mml:mi></mml:msub></mml:math></inline-formula> before assimilation.</p>
      <p id="d1e7344">Second, there is large uncertainty in the influence of RZSM as the source of
water available to plants (Albergel et al., 2008; Bonan et al., 2020). Our
GPP results of irrigated sites were largely influenced by US-Ne1, an
irrigated site. This site maintained high annual GPP in 2012 despite the drought (Fig. S4). However, the SMOS SSM in 2012 had a lower SSM annual
mean than the site observations, likely because the detected soil layer (0–50 cm) of the site observation is deeper than that of the satellite retrieval, and the cumulative deep soil moisture due to the regular irrigation was higher than the SSM that could easily be vaporized during the drought period (Fig. S4). Therefore, the influence of deep SM of some cropland sites
during the drought years induced large simulation errors and unsatisfactory
assimilation performance. Moreover, some deep-rooted forests maintain a high
LAI during drought by absorbing deep SM (<inline-formula><mml:math id="M501" display="inline"><mml:mo lspace="0mm">&gt;</mml:mo></mml:math></inline-formula> 2 m) and groundwater
(Zhang et al., 2016). Thus, joint assimilation of the LAI and SSM may
eliminate a portion of the underestimation of GPP of such vegetation in
drought periods. Therefore, further research is needed on how to optimally
utilize satellite SM data for improving GPP and ET simulations.</p>
      <p id="d1e7354">Third, the problem of mixed pixels and mismatches in the observation
footprints may also have an influence on the accuracy of estimated GPP and
ET. The 5 km spatial resolution of the GLASS LAI, 9 km of SMAP, and 25 km of
SMOS products cannot capture the sub-grid-scale condition, especially in
grid cells for complex land surfaces or strong soil heterogeneity. To ensure
the consistency of the grid-cell representativeness for the LAI and SSM, the
interpolation results in errors that propagate through the modeling and
assimilation, causing the accumulation of output errors (Nijssen and
Lettenmaier, 2004). Moreover, the shrubland in the LPJ-DGVM was most likely
simulated as C<inline-formula><mml:math id="M502" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> grassland in the hydrothermal condition of semi-arid and
arid regions. In contrast, the shrubland tended to be hybrid vegetation
types (grassland mixed with other types of forest vegetation) in the
hydrothermal condition of humid and sub-dry humid regions, and the simulated
canopy height is closer to the real condition of shrubland. This might also
be the reason for the superior performance of ET<inline-formula><mml:math id="M503" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">LPJ</mml:mi></mml:msub></mml:math></inline-formula> and assimilation results of shrubland sites in humid and sub-dry humid regions.</p>
      <p id="d1e7376">When assimilating multiple data streams, all data streams could be in the
same optimization (simultaneous assimilation) or use a sequential
(step-by-step) approach. Mathematically, simultaneous optimization is
optimal because strong parametric connections are maintained between
different processes. However, complications may arise due to computational
constraints related to the inversion of large matrices or the requirement of
numerous simulations, particularly for global datasets (e.g., Peylin et
al., 2016), and due to the “weight” of different data streams in the
optimization (e.g., Wutzler and Carvalhais, 2014). This is particularly true
when considering a regional- to global-scale, multiple-site optimization of a
complex model that contains many parameters and which typically takes on
the order of minutes to an hour to run a 1-year simulation. In practice,
it is very difficult to define a probability distribution that properly
characterizes the model structural uncertainty and observation errors,
accounting for biases and non-Gaussian distributions. Nevertheless, a
step-wise assimilation may be useful in dealing with possible
inconsistencies on a temporary basis, since the parameter error covariance
matrix must be propagated at each step. It is worth noting that the deviation
between the model and observational data should be solved in the process of
step-wise assimilation; for example, the joint assimilation in this study, the
satellite observations, and model simulation were integrated using the CDF method so that the first step of the assimilation will strongly constrain the
uncertainty of parameters related to phenology and carbon flux and propagate
to the second step. Alternative solutions were found for water-related
parameters through soil moisture, providing a better fit for all data
streams. The sequence of assimilation is essential in the step-wise
assimilation, and if the first observation contains a strong BIAS, then the
associated error correlation will also propagate through the first
assimilation. If the autocorrelation in the observation error, or the
correlation between the data stream errors is not considered, it is likely
that the posterior simulation has been overturned. That is, we overestimate
the reduction in parametric uncertainty. If two observational data are less uncertain (i.e., high precision of observation data), the model of
deviation is smaller (depending on the spatial scale and inversion method). Moreover, the correlation of these observations is stronger, and they contain
enough spatiotemporal information to limit all the parameters' optimization
accurately, and the step-wise assimilation performance is basically the same as
that of simultaneous assimilation.</p>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Conclusions</title>
      <p id="d1e7388">We developed an assimilation system LPJ-VSJA that integrates GLASS LAI, SMOS
SSM, and SMAP SSM data to improve GPP and ET estimates globally. The system
was designed to assimilate two SSM products (SMOS and SMAP) into the
integrated model – LPJ-PM for both dry and humid regions through separate
and joint assimilation. The results show that the joint constraints provided
by vegetation and soil variable strategies improve model simulations. Both
the original and joint assimilation results for GPP and ET in semi-arid and
arid regions performed better than those in humid and sub-dry humid regions,
and the LPJ-PM that emphasized the SSM information is more suitable for the
water-limited regions. For ET assimilation, the different SSM products
influence assimilation performance, and SMAP SSM possesses a slight
advantage in most vegetation types and in both dry and humid regions. Our
global LPJ-VSJA GPP and ET products have relatively higher accuracy than
other products, especially in water-limited regions with lower ET values.</p>
</sec>

      
      </body>
    <back><notes notes-type="codedataavailability"><title>Code and data availability</title>

      <p id="d1e7395">The LPJ-DGVM v4.1 version code (LPJ-ML) and example configurations are publicly available via the project home page
(<uri>https://github.com/PIK-LPJmL/LPJmL</uri>, last access: 14 December 2022; Müller et al., 2019). We used the 3.01 version of LPJ-DGVM, which removed the agricultural management module. The assimilation method code configured by the Fortran platform can be provided by contacting Xiangjun Tian (tianxj@mail.iap.ac.cn). The modified code of the LPJ-PM model and the underlying and global LPJ-VSJA GPP and ET data can be obtained by contacting the lead author of this paper (zhangli@aircas.ac.cn). These EC datasets were used: FLUXNET2015 (<uri>https://fluxnet.org/data/fluxnet2015-dataset/</uri>, last access: 14 December 2022; Pastorello et al., 2020), AmeriFlux
(<uri>https://ameriflux.lbl.gov/data-and-manifest/</uri>, login required, last access: 4 October 2021; AmeriFlux, 2021), and the HeiHe River basin (<ext-link xlink:href="https://doi.org/10.11888/Hydro.tpdc.270888" ext-link-type="DOI">10.11888/Hydro.tpdc.270888</ext-link>, Xie, 2017). Other input and validation datasets of the assimilation system have been described in Tables 2 and 3.</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e7410">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/hess-26-6311-2022-supplement" xlink:title="pdf">https://doi.org/10.5194/hess-26-6311-2022-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e7419">SL and LZ designed the experiment and wrote the paper with support from all coauthors. SL and RM implemented the codes necessary for the experiments. JX contributed to the structure of the article and comparison of assimilation performance between the SMOS and SMAP experiments. XT provided the POD-En4DVAR method and the code. MY contributed to the
validation and analysis of the results. All the authors contributed to the
synthesis of results and key conclusions.</p>
  </notes><?xmltex \hack{\newpage}?><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e7426">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e7432">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e7438">Sinan Li, Li Zhang, Rui Ma, and Min Yan were funded by the National Natural Science Foundation of China (grant no. 41771392, PI Li Zhang; and grant no. 41901364, PI Min Yan).</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e7444">This research has been supported by the National Natural Science Foundation of China (grant nos. 41771392 and 41901364).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e7450">This paper was edited by Genevieve Ali and reviewed by three anonymous referees.</p>
  </notes><ref-list>
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