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  <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-20-4895-2016</article-id><title-group><article-title><?xmltex \hack{\vspace{5mm}}?>Assimilation of SMOS brightness temperatures or soil moisture retrievals into a land surface model</article-title>
      </title-group><?xmltex \runningtitle{SMOS data assimilation}?><?xmltex \runningauthor{G. J. M. De Lannoy and R. H. Reichle}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>De Lannoy</surname><given-names>Gabriëlle J. M.</given-names></name>
          <email>gabrielle.delannoy@kuleuven.be</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Reichle</surname><given-names>Rolf H.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5513-0150</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>KU Leuven, Department of Earth and Environmental Sciences, Heverlee, Belgium</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>NASA Goddard Space Flight Center, Global Modeling and Assimilation Office, Greenbelt, Maryland, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Gabriëlle J. M. De Lannoy (gabrielle.delannoy@kuleuven.be)</corresp></author-notes><pub-date><day>15</day><month>December</month><year>2016</year></pub-date>
      
      <volume>20</volume>
      <issue>12</issue>
      <fpage>4895</fpage><lpage>4911</lpage>
      <history>
        <date date-type="received"><day>16</day><month>August</month><year>2016</year></date>
           <date date-type="rev-request"><day>23</day><month>August</month><year>2016</year></date>
           <date date-type="rev-recd"><day>8</day><month>November</month><year>2016</year></date>
           <date date-type="accepted"><day>27</day><month>November</month><year>2016</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under a Creative Commons Attribution 3.0 Unported License. To view a copy of this license, visit <ext-link ext-link-type="uri" xlink:href="http://creativecommons.org/licenses/by/3.0/">http://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://hess.copernicus.org/articles/20/4895/2016/hess-20-4895-2016.html">This article is available from https://hess.copernicus.org/articles/20/4895/2016/hess-20-4895-2016.html</self-uri>
<self-uri xlink:href="https://hess.copernicus.org/articles/20/4895/2016/hess-20-4895-2016.pdf">The full text article is available as a PDF file from https://hess.copernicus.org/articles/20/4895/2016/hess-20-4895-2016.pdf</self-uri>


      <abstract>
    <p>Three different data products from the Soil Moisture Ocean
Salinity (SMOS) mission are assimilated separately into the Goddard Earth
Observing System Model, version 5 (GEOS-5) to improve estimates of surface
and root-zone soil moisture. The first product consists of multi-angle,
dual-polarization brightness temperature (Tb) observations at the bottom of the atmosphere
extracted from Level 1 data. The second product is a derived SMOS Tb product
that mimics the data at a 40<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> incidence angle from the Soil Moisture
Active Passive (SMAP) mission. The third product is the operational SMOS
Level 2 surface soil moisture (SM) retrieval product. The assimilation system
uses a spatially distributed ensemble Kalman filter (EnKF) with seasonally
varying climatological bias mitigation for Tb assimilation, whereas a
time-invariant cumulative density function matching is used for SM retrieval
assimilation. All assimilation experiments improve the soil moisture
estimates compared to model-only simulations in terms of unbiased
root-mean-square differences and anomaly correlations during the period from
1 July 2010 to 1 May 2015 and for 187 sites across the US. Especially in
areas where the satellite data are most sensitive to surface soil moisture,
large skill improvements (e.g., an increase in the anomaly correlation by
0.1) are found in the surface soil moisture. The domain-average surface and
root-zone skill metrics are similar among the various assimilation
experiments, but large differences in skill are found locally. The
observation-minus-forecast residuals and analysis increments reveal large
differences in how the observations add value in the Tb and SM retrieval
assimilation systems. The distinct patterns of these diagnostics in the two
systems reflect observation and model errors patterns that are not well
captured in the assigned EnKF error parameters. Consequently, a localized
optimization of the EnKF error parameters is needed to further improve Tb or
SM retrieval assimilation.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>Microwave satellite missions are collecting large amounts of data for soil
moisture monitoring. It is not yet clear, however, how this wealth of data
can be used in the most efficient way to obtain global estimates of soil
moisture that can improve, e.g., weather prediction, flood and drought
modeling, agricultural yield monitoring, or landslide predictions. Many such
applications require knowledge of soil moisture in a deeper layer, where
water is extracted by plant roots or stored to buffer drainage and runoff,
not the approximately 5 cm surface layer to which the current L-band
(<inline-formula><mml:math display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 1.4 GHz) microwave missions are sensitive. Moreover, L-band
satellite observations have a fairly coarse spatial resolution (about 40 km)
and are available only at particular overpass times, typically once every
2–3 days for a given location. The challenge is thus to derive soil profile
moisture information at all times and locations through data assimilation,
that is, through the merger of satellite observations with information from a
dynamical land surface model.</p>
      <p>The Soil Moisture Ocean Salinity <xref ref-type="bibr" rid="bib1.bibx21" id="paren.1"><named-content content-type="pre">SMOS;</named-content></xref> mission and the
Soil Moisture Active Passive <xref ref-type="bibr" rid="bib1.bibx18" id="paren.2"><named-content content-type="pre">SMAP;</named-content></xref> mission are the
two L-band observatories currently orbiting in space with the specific aim of
measuring global soil moisture. These missions supply Level 1 (L1) brightness
temperature (Tb) data, Level 2 (L2) surface soil moisture (SM) retrievals,
and derived Level 3 (L3) products. The SMAP mission also provides an
operational Level 4 surface and root-zone soil moisture product
<xref ref-type="bibr" rid="bib1.bibx18 bib1.bibx36" id="paren.3"><named-content content-type="pre">L4_SM;</named-content></xref> that is based on the
assimilation of L1 SMAP Tb data into Goddard Earth Observing System Model,
version 5 (GEOS-5) land surface simulations. Alternatively, a soil moisture
assimilation system could ingest L2 SM retrievals instead of L1 Tb
observations.</p>
      <p>In this paper, we compare Tb and SM retrieval assimilation using a historical
(5-year) record of SMOS observations over North America in an assimilation
system similar to that of the SMAP L4_SM system. The main differences
between the SMAP L4_SM system and the experiments in this paper pertain to
the differences in assimilated data, to the difference in spatial resolution
of the resulting soil moisture products (36 km in the current paper; see
below; 9 km for the L4_SM product), and to differences in meteorological
forcing input (re-analysis meteorology in the current paper; operational
forecast meteorology corrected with gauge-based precipitation in the L4_SM
product).</p>
      <p>It is more difficult to assimilate Tb observations than SM retrievals because
brightness temperatures are only indirectly connected with the land surface
variables of interest and the Tb data come in multiple polarizations. SMOS Tb
observations are even more complex because of their multi-angular nature.
Some of the SMOS L1 Tb data complexity is reduced in the L3 SMOS Tb product
and further addressed in <xref ref-type="bibr" rid="bib1.bibx29" id="text.4"/> and
<xref ref-type="bibr" rid="bib1.bibx12" id="text.5"/>, who prepared the L1 SMOS Tb data for assimilation
into (quasi-)operational systems.</p>
      <p>Successful examples of SMOS Tb assimilation using a variety of simplifying
assumptions are illustrated in
<xref ref-type="bibr" rid="bib1.bibx26 bib1.bibx8 bib1.bibx22" id="text.6"/>. These studies
use a radiative transfer model (RTM) to dynamically invert Tb information
into corrections to modeled soil moisture estimates. In this paper, we
advance the spatially distributed multi-angle and dual-polarization Tb
assimilation of <xref ref-type="bibr" rid="bib1.bibx8" id="normal.7"/> in the GEOS-5 land surface model
with a new version of Tb observations and an improved spatial support and
forward simulation of the Tb observation predictions. Moreover, to mimic SMAP
Tb assimilation we also assimilate dual-polarization single-angle 40<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
SMOS Tb observations after fitting the multi-angle Tb data
<xref ref-type="bibr" rid="bib1.bibx12" id="paren.8"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><caption><p>Flowchart of Tb assimilation. The forward simulation consists of
<bold>(a)</bold> land surface model simulations and <bold>(b)</bold> Tb simulations
on the 36 km EASEv2 grid. The Tb simulations are subsequently
<bold>(c)</bold> aggregated using weights based on an approximate antenna
pattern. The resulting footprint-scale brightness temperature observation
predictions are compared to <bold>(d)</bold> SMOS observations to calculate
innovations (O–F) at the footprint scale. <bold>(e)</bold> The three-dimensional
EnKF maps the footprint-scale innovations to the 36 km EASEv2 grid based on
the modeled error correlations between the footprint-scale Tb and the 36 km
soil moisture and soil temperature state variables (per
Eqs. <xref ref-type="disp-formula" rid="Ch1.E1"/> and <xref ref-type="disp-formula" rid="Ch1.E2"/>).</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/20/4895/2016/hess-20-4895-2016-f01.png"/>

      </fig>

      <p>A key disadvantage of a system that assimilates SM retrievals is that the SM
retrievals may be produced with inconsistent ancillary data, such as for
example soil temperature simulated by another model than that used in the
assimilation system. The current SMOS SM retrievals by themselves have been
found to be skillful <xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx19" id="paren.9"/>, and research is
ongoing to further improve them
<xref ref-type="bibr" rid="bib1.bibx39 bib1.bibx47 bib1.bibx49 bib1.bibx41 bib1.bibx46" id="paren.10"/>.
The use of these SMOS SM retrievals has been manifold, e.g., to derive
enhanced estimates of precipitation <xref ref-type="bibr" rid="bib1.bibx44 bib1.bibx24" id="paren.11"/>, to
derive offline root-zone soil moisture estimates <xref ref-type="bibr" rid="bib1.bibx20" id="paren.12"/>, or to
offline downscale the data to higher-resolution soil moisture estimates
<xref ref-type="bibr" rid="bib1.bibx30" id="paren.13"/>. Other studies have assimilated SMOS SM retrievals online
into land surface models to possibly downscale the retrievals and
consistently improve soil moisture and other land surface variables
<xref ref-type="bibr" rid="bib1.bibx37 bib1.bibx48 bib1.bibx26" id="paren.14"/>, leading to, e.g., improved
estimates of floods <xref ref-type="bibr" rid="bib1.bibx2" id="paren.15"/> and crop growth
<xref ref-type="bibr" rid="bib1.bibx6" id="paren.16"/>. In this paper, we use a spatially distributed
assimilation system to integrate SMOS SM retrievals into the GEOS-5 land
surface model with the aim of inferring improved surface and root-zone soil
moisture estimates. Our study mainly differs from the above SMOS SM retrieval
studies in the continental and multi-year scale of the experiments, in the
advanced quality screening and spatial support of the SM retrieval
observations, and in the comparison between Tb and SM retrieval assimilation
(also discussed in <xref ref-type="bibr" rid="bib1.bibx26" id="altparen.17"/>).</p>
      <p>To assess the potential of Tb and SM retrieval assimilation, 5 years of SMOS
Tb data or SM data are assimilated into the GEOS-5 land surface model using a
careful data quality control and data preprocessing. The observations are
associated with a realistic antenna pattern, containing 50 % of the
signal power in a circular area with 20 km radius. Special attention is paid
to large-scale patterns of random and persistent forecast and observation
errors in the different assimilation systems, and to the impact of the
different assimilation schemes on the skill of surface and root-zone soil
moisture estimates. Section <xref ref-type="sec" rid="Ch1.S2"/> describes the SMOS
observations, the various modeling components, and the in situ validation
data. Section <xref ref-type="sec" rid="Ch1.S3"/> highlights the technical differences between the
various assimilation schemes, and Sect. <xref ref-type="sec" rid="Ch1.S4"/> presents the
results.</p>
</sec>
<sec id="Ch1.S2">
  <title>Data and model</title>
<sec id="Ch1.S2.SS1">
  <title>SMOS Tb observations</title>
      <p>The Microwave Imaging Radiometer with Aperture Synthesis (MIRAS) onboard SMOS
provides multi-angle Tb data, with a nominal (3 dB) spatial resolution of
43 km and a global coverage approximately every 3 days (at either 06:00 or
18:00 local time, i.e., ascending or descending half-orbits, separately). The
most recent version (v620) of the SCLF1C Tb data is used. Observations are
retained for further processing only (a) in the alias-free zone, (b) when the
data are not contaminated by point source radio frequency interference (RFI)
or tails thereof, (c) when the values fall within the range 100–320 K, and
(d) when valid data are available for both horizontal (<inline-formula><mml:math display="inline"><mml:mi>H</mml:mi></mml:math></inline-formula>) and vertical
(<inline-formula><mml:math display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula>) polarization. The flag for snapshot RFI is not activated, because it is
currently too sensitive (R. Oliva and Y. Kerr, personal communication,
2016). After the initial screening, we correct the
L1 Tb values for geometric and Faraday rotation and for atmospheric and
reflected extraterrestrial radiation <xref ref-type="bibr" rid="bib1.bibx12" id="paren.18"/> using Modern-Era
Retrospective Analysis for Research and Applications (MERRA) version 2
<xref ref-type="bibr" rid="bib1.bibx4" id="paren.19"><named-content content-type="pre">MERRA2;</named-content></xref> background fields. The resulting Tb
values at the bottom of the atmosphere are then binned into 41 evenly spaced
angular bins with the center angle ranging from 20 through 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. Next,
the data are regridded from the 15 km discrete global grid (DGG) on which
they are posted to the 36 km cylindrical Equal-Area Scalable Earth (EASEv2)
grid <xref ref-type="bibr" rid="bib1.bibx5" id="paren.20"/>, and the data are screened for excessive
sub-36 km heterogeneity (spatial standard deviation <inline-formula><mml:math display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 7 K), which is
indicative of open water bodies or RFI. Tb values for a given 36 km EASEv2
grid cell are computed only if at least two valid DGG observations are
available.</p>
      <p>From these preprocessed Tb data, two datasets are derived for assimilation:
(i) a seven-angle Tb dataset, with incidence angles <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> [30, 35, 40,
45, 50, 55, 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>] <xref ref-type="bibr" rid="bib1.bibx9" id="paren.21"/>, and (ii) a fitted Tb dataset
<xref ref-type="bibr" rid="bib1.bibx12" id="paren.22"/> from which only the Tb at a 40<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> incidence
angle is used to mimic the single-angle nature of SMAP Tb observations. We
refer to these datasets as Tb_7ang and Tb_fit, respectively. Tb_fit data
are only retained when the fitting error is less than 5 K and a minimum of
15 data points contribute to the entire fitted angular signature, with at
least 5 data points above and below the 40<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> incidence angle and at
least 10 data points in the incidence angle interval between 30 and
50<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <title>SMOS SM retrieval observations</title>
      <p>The SMOS SM retrievals are extracted from the SMUDP2 product v552. Because
this product version ends in early May 2015, we limit our study period to 1
July 2010–1 May 2015. (The reprocessed v620 version of the SM retrievals was
not yet available at the time we conducted the experiments.) The SMOS
retrieval algorithm simultaneously retrieves soil moisture and vegetation
opacity, by fitting multi-angle Tb observations at both <inline-formula><mml:math display="inline"><mml:mi>H</mml:mi></mml:math></inline-formula>- and
<inline-formula><mml:math display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula>-polarization with simulations of the L-band Microwave Emission of the
Biosphere Model <xref ref-type="bibr" rid="bib1.bibx45" id="paren.23"><named-content content-type="pre">L-MEB,</named-content></xref>. Based on the quality
information provided within the SMOS products, the SM data are retained only
if (a) all retrieved variables fall within a realistic range
(0–0.6 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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 soil moisture), (b) the SM uncertainty estimated
by the SMOS retrieval algorithm is less than 0.1 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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>, (c) the
RFI probability for both <inline-formula><mml:math display="inline"><mml:mi>H</mml:mi></mml:math></inline-formula>- and <inline-formula><mml:math display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula>-polarization is less than 0.3, and
(d) SM retrieval flags are not raised for high topographic complexity, high
urban fraction, high open water fraction, sea ice, coastal areas, and high
total electron content. Further screening for frozen temperature and snow is
based on GEOS-5 model output (Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/>). After the regridding
from the 15 km DGG grid to the 36 km cylindrical EASEv2 grid, the data are
screened for excessive sub-36 km heterogeneity (spatial standard deviation
<inline-formula><mml:math display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 0.2 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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>). SM values for a given 36 km EASEv2 grid cell are
computed only if at least two valid DGG observations are available.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <title>Soil moisture and brightness temperature modeling</title>
      <p>The land data assimilation system used here employs the GEOS-5 catchment land
surface model <xref ref-type="bibr" rid="bib1.bibx25" id="paren.24"><named-content content-type="pre">CLSM;</named-content></xref>, along with an L-band tau-omega
radiative transfer model <xref ref-type="bibr" rid="bib1.bibx9 bib1.bibx11" id="paren.25"><named-content content-type="pre">RTM;</named-content></xref>. The
CLSM simulations use GEOS-5 parameters <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx10" id="paren.26"/>
similar to those used in the SMAP L4_SM product, and are forced with
<inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> GEOS-5 forcing data from MERRA
<xref ref-type="bibr" rid="bib1.bibx38" id="paren.27"/> bilinearly interpolated to the model grid. The study
domain covers most of North America, with the northwestern corner at
(125<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W, 55<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N) and the southeastern corner at
(60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W, 24<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N).</p>
      <p>The computational elements are the 36 km EASEv2 grid cells. The land model
computation time step is 7.5 min, and output is saved at 3 h
intervals. At each grid cell, the surface soil moisture content (sfmc, 0–5 cm) and root-zone soil moisture content (rzmc, 0–100 cm) are diagnosed based
on three prognostic variables: catchment deficit (catdef), root-zone excess
(rzexc), and surface excess (srfexc). Similarly, the surface (skin)
temperature is diagnosed from the prognostic land surface temperatures across
the saturated (tc1), unsaturated (tc2), and wilting (tc4) sub-grid areas.
Finally, the soil temperature (tp1 for the topmost layer) is diagnosed from
the prognostic ground heat content (ght1 for the top layer). An overview of
the model variables is given in <xref ref-type="bibr" rid="bib1.bibx35 bib1.bibx25" id="text.28"/> and
<xref ref-type="bibr" rid="bib1.bibx16" id="text.29"/>.</p>
      <p>The L-band tau-omega RTM converts the 36 km CLSM soil moisture and
temperature simulations into 36 km L-band Tb estimates when the soil is not
frozen or covered with snow, when precipitation is less than
10 mm day<inline-formula><mml:math 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 where the open water fraction is less than 5 %.
For each 36 km grid cell, key parameters of the RTM are estimated by
minimizing Eq. (B.1) in <xref ref-type="bibr" rid="bib1.bibx11" id="text.30"/>, using a 5-year history of
SMOS v620 Tb data, and computing observation predictions (see below) at the
footprint scale. Specifically, all 36 km grid cells within one footprint
area are initially assigned the same set of RTM parameters, while the dynamic
background information is spatially variable. For each 36 km grid cell, the
calibration estimates a spatially homogeneous set of RTM parameters for the
entire associated footprint area, and the resulting values are assigned to
the central (and typically dominant) 36 km grid cell only. For the forward
calculation of the Tb observation predictions during the data assimilation,
all 36 km pixels have a unique set of RTM parameters. The RTM is calibrated
using all 5 years of available Tb data and aims at minimizing climatological
biases. The data assimilation is performed over the same 5 years and aims at
addressing random (or short-term) errors. The methodology is very similar to
that in <xref ref-type="bibr" rid="bib1.bibx8" id="normal.31"/>, but with the difference that, here, the
RTM does not simulate atmospheric contributions (because the Tb observations
are now a priori corrected for atmospheric contributions) and the observation
predictions are now spatially aggregated using a realistic (but approximate)
antenna pattern.</p>
      <p>For the computation of differences between SMOS observations and
footprint-scale model simulations in the RTM calibration and for the
computation of the “observation-minus-forecast” (O–F) residuals in the
assimilation system (Sect. <xref ref-type="sec" rid="Ch1.S3.SS1"/>, Fig. <xref ref-type="fig" rid="Ch1.F1"/>),
the modeled 36 km soil moisture or Tb simulations are aggregated to the
footprint scale by spatial convolution with weights given by an approximation
of the SMOS antenna pattern. We also refer to these spatially aggregated
model estimates as “observation predictions”. The SMOS antenna pattern is
approximated by a two-dimensional Gaussian function containing 50 % of the
signal within a circle with a radius of 20 km. The simulations outside a
radius of 40 km are discarded in the computation of the footprint-scale
estimates.</p>
      <p>The number of 36 km EASEv2 grid cells included in one footprint area varies
with latitude. The circular footprint shape is preserved everywhere on the
globe. In contrast, the shape of the EASEv2 grid cells projected on the globe
varies with the latitude, with an aspect ratio of 1 at 30<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
(north–south) latitude, larger than 1 towards the poles and less than 1
towards the Equator. Therefore, at higher latitudes multiple EASEv2 grid
cells with the same latitude and various longitudes belong to one circular
footprint, whereas towards the Equator, several EASEv2 grid cells with the
same longitude and various latitudes contribute to the footprint. Overall,
the difference between single 36 km simulations and footprint-scale values
is small, but the number of valid Tb observation predictions at the footprint
scale is reduced, because of the increased likelihood of finding a 36 km
grid cell with a non-negligible water fraction, snow amount, or precipitation
within the footprint area.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <title>In situ soil moisture data and metrics</title>
      <p>The assimilation results are evaluated using independent in situ measurements
of surface and root-zone soil moisture from two sparse networks across the
US: the US Natural Resources Conservation Service Soil Climate Analysis
Network <xref ref-type="bibr" rid="bib1.bibx40" id="paren.32"><named-content content-type="pre">SCAN;</named-content></xref> and the US Climate Reference Network
<xref ref-type="bibr" rid="bib1.bibx14 bib1.bibx3" id="paren.33"><named-content content-type="pre">USCRN;</named-content></xref>. Surface soil moisture
measurements are taken at approximately 5 cm depth. Root-zone soil moisture
measurements are a weighted average of measurements at 5, 10, 20, and 50 cm
depth, with respective weights of 0.1, 0.1, 0.27, and 0.53. Given the
difference in spatial support between these point measurements and the 36 km
gridded model and assimilation results, the skill is quantified in terms of
anomaly time series correlation (anomR) and unbiased root-mean-square
difference <xref ref-type="bibr" rid="bib1.bibx17" id="paren.34"><named-content content-type="pre">RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula>;</named-content></xref>, using all 3 h
forecast and analysis time steps in the period 1 July 2010–1 May 2015,
excluding times when the soil is frozen (top layer soil temperature <inline-formula><mml:math display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula>
274.15 K) or snow covered (snow water equivalent <inline-formula><mml:math display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 0 kg m<inline-formula><mml:math 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>). The
anomaly correlation is based on anomaly time series obtained by subtracting a
multi-year smoothed climatology from both the simulations and in situ
observations. Note that the assimilation and open-loop simulations have, by
design, the same climatological variability; the assimilation only corrects
for random errors. Metrics at a single site are only calculated if at least
200 data points are available. Skill metrics across an entire network are
calculated by clustering the sites within SCAN and USCRN to avoid densely
sampled areas dominating the validation metrics and to ensure realistic
confidence intervals <xref ref-type="bibr" rid="bib1.bibx8" id="paren.35"/>. The number of clusters is
estimated a priori after prescribing an average cluster radius of 3<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>,
which approximately reflects the autocorrelation length of large-scale
topographic and meteorological phenomena, or of large-scale soil moisture
patterns <xref ref-type="bibr" rid="bib1.bibx43" id="paren.36"/>. The actual size of the clusters that results
from the clustering algorithm varies strongly in space.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Data assimilation</title>
<sec id="Ch1.S3.SS1">
  <title>Distributed ensemble Kalman filter</title>
      <p>For both Tb and SM retrieval assimilation, a spatially distributed (or
three-dimensional, 3-D) ensemble Kalman filter
<xref ref-type="bibr" rid="bib1.bibx31 bib1.bibx8" id="paren.37"><named-content content-type="pre">EnKF;</named-content></xref> is used. This system
simultaneously assimilates multiple spatially distributed observation sets,
using horizontal and vertical error covariance structures, to update the
simulations at each 36 km model grid cell. The details of the Tb assimilation
system are explained in <xref ref-type="bibr" rid="bib1.bibx8" id="text.38"/> and differ only in that
the observations are here associated with a spatially variable antenna
pattern reaching out to a radius of 40 km.</p>
      <p>During the model integration, a data assimilation step is activated every 3 h. All the SMOS observations <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> collected within 1.5 h of
the analysis time <inline-formula><mml:math display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> are assimilated simultaneously to update the forecasted
state <inline-formula><mml:math display="inline"><mml:mrow><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mrow><mml:mi>j</mml:mi><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> at location <inline-formula><mml:math display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> as follows:</p>
      <p><disp-formula id="Ch1.E1" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mrow><mml:mi>j</mml:mi><mml:mo>+</mml:mo></mml:mrow></mml:msubsup><mml:mo>=</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mrow><mml:mi>j</mml:mi><mml:mo>-</mml:mo></mml:mrow></mml:msubsup><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="bold">K</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>[</mml:mo><mml:msubsup><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mi>i</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>-</mml:mo></mml:mrow></mml:msubsup><mml:mo>]</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          with <inline-formula><mml:math display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula> denoting the ensemble member, <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">K</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> the Kalman gain,
<inline-formula><mml:math display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> the perturbed observations,
<inline-formula><mml:math display="inline"><mml:mrow><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi>i</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>-</mml:mo></mml:mrow></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi>h</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mi>i</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>-</mml:mo></mml:mrow></mml:msubsup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> the observation predictions,
and <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mo>.</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> the observation operator mapping the simulated land surface
variables to observed quantities. Bias in the observation-minus-forecast
residuals is addressed prior to the analysis (Sect. <xref ref-type="sec" rid="Ch1.S3.SS2"/>). The
ensemble is created by perturbing the model forcing, the model forecasts, and
the observations (Sect. <xref ref-type="sec" rid="Ch1.S3.SS3"/>). The Kalman gain is calculated as
            <disp-formula id="Ch1.E2" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi mathvariant="bold">K</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="normal">Cov</mml:mi><mml:mo>(</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mo>-</mml:mo></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mi>i</mml:mi><mml:mo>-</mml:mo></mml:msubsup><mml:mo>)</mml:mo><mml:msup><mml:mfenced close="]" open="["><mml:mi mathvariant="normal">Cov</mml:mi><mml:mo>(</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi>i</mml:mi><mml:mo>-</mml:mo></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi>i</mml:mi><mml:mo>-</mml:mo></mml:msubsup><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="bold">R</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mfenced><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">Cov</mml:mi><mml:mo>(</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mo>-</mml:mo></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi>i</mml:mi><mml:mo>-</mml:mo></mml:msubsup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the
(sample) error covariance (across the ensemble) between the forecasted land
surface state and the forecasted Tb or SM. Similarly, <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">Cov</mml:mi><mml:mo>(</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mi>i</mml:mi><mml:mo>-</mml:mo></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mi>i</mml:mi><mml:mo>-</mml:mo></mml:msubsup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the (sample) error covariance of the Tb or SM
forecasts, and <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">R</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the Tb or SM observation error covariance. The
Kalman gain is identical for all ensemble members.</p>
      <p>In the case of SM retrieval assimilation, the observation operator
<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mo>.</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> performs the spatial aggregation of soil moisture simulations
from the 36 km grid cells to the satellite footprint; in the case of Tb data
assimilation, the observation operator includes both the RTM and the spatial
aggregation of gridded Tb simulations to the footprint
(Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/>). For the Tb_7ang assimilation, one observation set
at location <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">κ</mml:mi></mml:math></inline-formula> contains Tb observations at a maximum of seven angles
and both <inline-formula><mml:math display="inline"><mml:mi>H</mml:mi></mml:math></inline-formula>- and <inline-formula><mml:math display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula>-polarization, i.e., up to 14 individual observations
<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>∈</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mrow><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>. The subscript <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">λ</mml:mi></mml:math></inline-formula> refers to
the polarization and incidence angle of the individual Tb observations. In
the middle part of the swath, all 14 observations are typically available,
whereas slightly fewer observations are available in the outer portions of
the swath, where the observations with lower incidence angles are missing.</p>
      <p>For the Tb_fit assimilation, one observation set usually contains two
observations, i.e., both <inline-formula><mml:math display="inline"><mml:mi>H</mml:mi></mml:math></inline-formula>- and <inline-formula><mml:math display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula>-polarization Tb at a 40<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
incidence angle. For the SM retrieval assimilation, each observation set
contains only one observation. In all cases, the observation vector
<inline-formula><mml:math display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> collects multiple perturbed observation sets that are spatially
distributed within an influence radius of 1.25<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> around the model grid
cell <inline-formula><mml:math display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>, and each observation vector <inline-formula><mml:math display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> has a forecasted
counterpart <inline-formula><mml:math display="inline"><mml:mrow><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mi>i</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>. After removal of the persistent errors
(Sect.  <xref ref-type="sec" rid="Ch1.S3.SS2"/>) from the O–F residuals (or innovations), the
increments <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">K</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>[</mml:mo><mml:msubsup><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mi>i</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>-</mml:mo></mml:mrow></mml:msubsup><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> are
calculated and applied to the state variables. Figure <xref ref-type="fig" rid="Ch1.F1"/>
illustrates the forward simulation from 36 km gridded land surface
simulations to footprint-scale observation predictions of Tb and the
downscaling of the footprint-scale Tb innovations to 36 km gridded land
surface increments.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p>Soil moisture and temperature analysis on 30 April 2015 at 12:00 UTC
for the Tb_fit assimilation system. (<bold>a</bold>, <bold>b</bold>) Tb innovations
(O–F) at a 40<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> incidence angle for <inline-formula><mml:math display="inline"><mml:mi>H</mml:mi></mml:math></inline-formula>- and <inline-formula><mml:math display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula>-polarization
respectively; (<bold>c</bold>, <bold>d</bold>) increments in total profile water
(<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>wtot) and first soil layer temperature (<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>tp1), respectively;
(<bold>e</bold>, <bold>f</bold>, <bold>g</bold>) assimilation analyses of surface soil
moisture (sfmc), root-zone soil moisture (rzmc), and soil temperature (tp1),
respectively.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://hess.copernicus.org/articles/20/4895/2016/hess-20-4895-2016-f02.pdf"/>

        </fig>

      <p>The subset of prognostic variables updated in Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>) differs
depending on the assimilation experiment. The state vector for Tb
assimilation (<inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> [catdef, srfexc, rzexc, tc1, tc2, tc4, ght1]<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mi>T</mml:mi></mml:msup></mml:math></inline-formula>)
includes prognostic variables related to soil moisture and soil temperature
(Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/>), because Tb observations are by definition sensitive
to surface soil moisture and temperature. In contrast, the state vector for
SM retrieval assimilation (<inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> [catdef, srfexc, rzexc]<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mi>T</mml:mi></mml:msup></mml:math></inline-formula>) contains
only model prognostic variables related to soil moisture, because the SM
retrievals do not carry direct information about the soil temperature. The
selected updates will be propagated to all other variables within the land
surface modeling system through energy and water exchange between various
soil layers and land–vegetation–atmosphere compartments. For the discussion
of the soil moisture increments we will focus on the total profile water
increments (<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>wtot=<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>srfexc+<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>rzexc–<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>catdef) in
units of kg m<inline-formula><mml:math 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> (that is, mm of water equivalent). This quantity is
easily understandable and thus simplifies the discussion.</p>
      <p>Figures <xref ref-type="fig" rid="Ch1.F2"/> and <xref ref-type="fig" rid="Ch1.F3"/> illustrate the concept
for Tb assimilation and SM retrieval assimilation, respectively.
Figure <xref ref-type="fig" rid="Ch1.F2"/>a–b show swaths of footprint-scale bias-corrected
Tb_fit innovations (mapped onto the 36 km EASEv2 grid), for <inline-formula><mml:math display="inline"><mml:mi>H</mml:mi></mml:math></inline-formula>- and
<inline-formula><mml:math display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula>-polarization at a 40<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> incidence angle from the single-angle Tb
assimilation system. The Tb innovations are then transformed into soil
moisture and temperature increments using Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>). Where Tb
innovations are warm, the soil water is reduced and the temperature is
increased. Figure <xref ref-type="fig" rid="Ch1.F2"/>c shows the total profile water
increments <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>wtot and Fig. <xref ref-type="fig" rid="Ch1.F2"/>d shows increments to
the first soil layer temperature <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>tp1. Increments to the surface
temperature prognostic variables (Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/>; <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>tc1,
<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>tc2, <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>tc4) are similar (not shown). Finally, the increments
are added to the forecasted fields to create spatially complete analysis maps
of surface and root-zone soil moisture, as well as surface temperature and
soil temperature (Fig. <xref ref-type="fig" rid="Ch1.F2"/>e–g).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><caption><p>Soil moisture analysis on 30 April 2015 at 12:00 UTC for the SM
retrieval assimilation system. <bold>(a)</bold> SM innovations (O–F);
<bold>(b)</bold> increments in total profile water (<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>wtot); (<bold>c</bold>,
<bold>d</bold>) assimilation analyses of surface soil moisture (sfmc) and
root-zone soil moisture (rzmc).</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hess.copernicus.org/articles/20/4895/2016/hess-20-4895-2016-f03.pdf"/>

        </fig>

      <p>Similarly, Fig. <xref ref-type="fig" rid="Ch1.F3"/>a shows the SM innovations from the SM
retrieval assimilation at the same time as in Fig. <xref ref-type="fig" rid="Ch1.F2"/>.
Areas with positive (wet) SM innovations in the SM retrieval assimilation
roughly correspond to negative (cold) Tb innovations in the Tb assimilation
system (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a–b). Note that the color bars for Tb and
SM throughout the paper are chosen according to the rule of thumb that a
2–3 K change in Tb corresponds to a 0.01 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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> change in soil
moisture, but keep in mind that the relationship between Tb and SM is
nonlinear and varies with time, location, and incidence angle. Next, the SM
innovations are converted to soil moisture increments (<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>wtot;
Fig. <xref ref-type="fig" rid="Ch1.F3"/>b); no increment to surface or soil temperature is
calculated. Figures <xref ref-type="fig" rid="Ch1.F2"/>c and <xref ref-type="fig" rid="Ch1.F3"/>b show that
the Tb and SM retrieval assimilation systems produce wtot increments with
somewhat different large-scale patterns, which is further discussed in
Sect. <xref ref-type="sec" rid="Ch1.S4.SS2"/>. Finally, Fig. <xref ref-type="fig" rid="Ch1.F3"/>c–d show the
resulting surface and root-zone soil moisture analysis fields obtained by
adding the increments to the model forecast fields. For both the Tb and SM
retrieval assimilation systems, the analysis increments blend smoothly into
the forecast fields; that is, the analysis maps do not reveal sharp spatial
edges that would reveal the geometry of the assimilated satellite swaths.
Further details about this figure are discussed in Sect. <xref ref-type="sec" rid="Ch1.S4.SS1"/>.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Tb and SM innovation bias</title>
      <p>To limit the long-term biases between Tb observations and simulations, the
RTM was calibrated (Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/>). The 5-year average absolute bias
between SMOS Tb and forecasted Tb is about 2 K across the domain. In
general, slightly warm model biases are found in the boreal zones and cold
model biases over the central part of the US (not shown), but larger seasonal
Tb biases remain, primarily due to systematic errors in the modeled
temperature and vegetation. The seasonally varying climatological Tb bias is
removed prior to data assimilation for each angle, polarization, and overpass
time separately, as described in <xref ref-type="bibr" rid="bib1.bibx8" id="text.39"/>. The Tb
innovation biases are calculated over the period 1 July 2010–1 May 2015 for
each individual 36 km grid cell without spatial sampling.</p>
      <p>The CLSM soil moisture was not calibrated for lack of global observations
that would support such an effort and because modeled soil moisture does not
necessarily represent soil moisture as observed in the field anyway
<xref ref-type="bibr" rid="bib1.bibx23" id="paren.40"/>. Unlike biases in Tb innovations, the biases in the SM
innovations are more stationary and do not depend on seasonal temperature
variations. Therefore, the SM innovation biases are not corrected seasonally,
but instead cumulative distribution function (CDF) matching between the
observations and simulations is performed <xref ref-type="bibr" rid="bib1.bibx32" id="paren.41"/> to
reconcile the differences in long-term mean, variance, and higher moments, as
in earlier retrieval assimilation studies <xref ref-type="bibr" rid="bib1.bibx27 bib1.bibx15" id="paren.42"/>. The
observed and simulated SM CDFs are computed for the entire study period,
i.e., for 1 July 2010–1 May 2015, at each 36 km grid cell individually.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <title>Random forecast and observation error</title>
      <p>The imposed ensemble forecast perturbations for Tb and SM retrieval
assimilation are identical to those of <xref ref-type="bibr" rid="bib1.bibx8" id="text.43"/> and not
repeated here. The total observation error standard deviation for SMOS
Tb_7ang is set to 6 K, which yields near-optimal assimilation diagnostics
on average across the globe. However, the diagnostics are not necessarily
near-optimal in individual regions <xref ref-type="bibr" rid="bib1.bibx8" id="paren.44"/>. The input
observation error standard deviation for SM retrievals is
0.04 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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 line with the soil moisture accuracy requirement
for the recent SMOS and SMAP missions. The SM retrieval error standard
deviation is rescaled following the CDF matching of the SM observations and
results in an effective mean error standard deviation of
0.02 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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>, with larger values in the wetter eastern part, which
exhibits a higher temporal variability in soil moisture simulations, and
lower values in the drier, western part of the study domain (not shown). In
all cases, the spatial observation error correlation length is 0.25<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>.
In the case of multi-angle Tb_7ang assimilation, interangular error
correlations are imposed as in <xref ref-type="bibr" rid="bib1.bibx8" id="text.45"/>.</p>
      <p>Observation errors in Tb data or SM retrievals are a combination of
instrument error and representation error <xref ref-type="bibr" rid="bib1.bibx7 bib1.bibx42" id="paren.46"/>. The
6 K Tb error consists of a radiometric error of about 4 K for individual
incidence angles (instrument error) plus 4.5 K representation inaccuracies
(in our system, i.e., based on the near-optimal 6 K observation error) due
to errors in the RTM, the spatial aggregation, or other discrepancies between
Tb observations and forecasts (<inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">6</mml:mn><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:msup><mml:mn mathvariant="normal">4</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mn>4.5</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt></mml:mrow></mml:math></inline-formula>). For Tb_fit
observations, the instrument error may be slightly reduced compared to that
for Tb_7ang after the angular smoothing, but the representation error
remains similar. SM observations contain retrieval errors due to errors in
the RTM and in the input L1 Tb observations, as well as representation error
due to, e.g., the inherently different nature of simulated and observed soil
moisture <xref ref-type="bibr" rid="bib1.bibx23" id="paren.47"/>. In either case, the representation error
depends on the soil moisture and temperature dynamics and should ideally be
modeled as a function of time and location, but we chose a constant input
observation error standard deviation in this paper for simplicity. For SM
retrieval assimilation, some spatial error variability is introduced after
rescaling in line with the CDF matching.</p>
</sec>
<sec id="Ch1.S3.SS4">
  <title>Tb or SM retrieval assimilation</title>
      <p>In our experiments, we do not expect the SMOS Tb and SM retrieval
assimilation systems to yield the same results. During the SMOS L2 SM
retrieval optimization, the Tb data are used to estimate surface soil
moisture and vegetation opacity, given soil temperature background fields
provided by the European Center for Medium-Range Weather Forecasts (ECMWF)
and look-up parameter information that differs significantly from the NASA
GEOS-5 land data assimilation system. In contrast, our SMOS Tb assimilation
scheme estimates soil moisture and temperature, given vegetation
information. Furthermore, the data screening is necessarily different for Tb
data and SM retrievals, and the approach for bias correction is intentionally
different. The soil moisture information extracted during the L2 retrieval
process or Tb assimilation is thus by design expected to be different.
Finally, differences in the Tb and SM retrieval assimilation results could
also be due to differences in how close each of the systems is to an optimal
calibration of its model and observation error parameters.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><caption><p>Observation-space assimilation diagnostics for the period from 1
July 2010 to 1 May 2015. Number of assimilated observation sets for
<bold>(a)</bold> Tb_7ang assimilation, <bold>(b)</bold> Tb_fit assimilation, and
<bold>(c)</bold> SM retrieval assimilation. Standard deviation of the
<bold>(d)</bold> Tb innovations from Tb_7ang assimilation, <bold>(e)</bold> Tb
innovations from Tb_fit assimilation, and <bold>(f)</bold> SM innovations from
SM retrieval assimilation. (<bold>g</bold>, <bold>h</bold>, <bold>i</bold>) Same as
(<bold>d</bold>, <bold>e</bold>, <bold>f</bold>), but for normalized innovations
(normO–F). Ensemble standard deviation of the (j) Tb forecast error for
Tb_7ang assimilation, <bold>(k)</bold> Tb forecast error for Tb_fit
assimilation, and <bold>(l)</bold> surface soil moisture forecast error for SM
retrieval assimilation. The titles show the spatial mean (m) and standard
deviation (s) across each map.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://hess.copernicus.org/articles/20/4895/2016/hess-20-4895-2016-f04.pdf"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4">
  <title>Results</title>
<sec id="Ch1.S4.SS1">
  <title>Observation and forecast diagnostics</title>
<sec id="Ch1.S4.SS1.SSS1">
  <title>Number of assimilated observations</title>
      <p>Let us revisit Figs. <xref ref-type="fig" rid="Ch1.F2"/>a–b and <xref ref-type="fig" rid="Ch1.F3"/>a to
further highlight some differences between the various assimilated SMOS
observations. First, the swath width for Tb innovations is much narrower than
that of the SM innovations because the assimilated Tb observations are
strictly limited to the alias-free zone within the full swath, while the
assimilated SM retrievals are retained in the extended alias-free zone.
Furthermore, the swath width of the Tb_fit innovations is narrower than that
of the multi-angle assimilation (not shown) because the fitting requires
sufficient data at a range of incidence angles and lower angle data are not
available at the outer edges of the swaths. Note that SMAP provides useable
Tb measurements over a much wider swath (not shown).</p>
      <p>The different swath widths result in different numbers of observation sets
assimilated in each of the three experiments. Figure <xref ref-type="fig" rid="Ch1.F4"/>a–c show
the average number of assimilated observation sets (defined in
Sect. <xref ref-type="sec" rid="Ch1.S3.SS1"/>) over the study period 1 July 2010–1 May 2015. The
number of observation sets is smallest (one every 4 days) for Tb_fit and
largest for SM retrievals (one every 2 days), because the swath width is
narrowest for Tb_fit and widest for SM retrievals. The northern areas and
the western mountain ranges have the fewest observations, because data are
not used when the soil is frozen or snow covered. Tb observations are not
assimilated in many small areas scattered around the study domain, where more
than 5 % of open water is found in the footprint, based on the underlying
GEOS-5 land mask. For the SM retrievals, the screening for an excessive
(<inline-formula><mml:math display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 5 %) water fraction is only based on the product science flags, not
on GEOS-5 information. Data gaps in the SM retrievals are found in the
western mountain ranges and in the vegetated southeastern part of the US. The
data coverage is also different for Tb and SM retrieval assimilation because
the availability of the climatological information needed for the innovation
bias correction (Sect. <xref ref-type="sec" rid="Ch1.S3.SS2"/>) is different for the Tb and SM
retrieval observations.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><caption><p>Hovmüller plots showing the temporal evolution of longitudinally
averaged innovations (O–F) for the period from 1 July 2010 to 1 May 2015.
<bold>(a)</bold> Tb_7ang innovations, averaged over <inline-formula><mml:math display="inline"><mml:mi>H</mml:mi></mml:math></inline-formula>- and <inline-formula><mml:math display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula>-polarization,
ascending and descending swaths, and over seven incidence angles.
<bold>(b)</bold> SM innovations, averaged over ascending and descending
swaths.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://hess.copernicus.org/articles/20/4895/2016/hess-20-4895-2016-f05.pdf"/>

          </fig>

</sec>
<sec id="Ch1.S4.SS1.SSS2">
  <title>Actual observation and forecast errors</title>
      <p>The long-term mean observation-minus-forecast differences (O–F, or
innovations) are unbiased by design (Sect. <xref ref-type="sec" rid="Ch1.S3.SS2"/>). The
Hovmüller plots for two data assimilation cases in
Fig. <xref ref-type="fig" rid="Ch1.F5"/> reveal that the temporal pattern in area-averaged
biases is fairly random for the Tb_7ang assimilation case (very similar for
Tb_fit assimilation, not shown), whereas it shows a slight seasonal pattern
in the SM retrieval assimilation case. This small difference is not
surprising, given that the Tb innovation bias is seasonally corrected,
whereas the SM innovation bias is not.</p>
      <p>The time series standard deviation of the innovations, that is, the
root-mean-square difference (RMSD) between SMOS observations and simulations,
represents the total observation and forecast error that is present in the
assimilation system <xref ref-type="bibr" rid="bib1.bibx13" id="paren.48"/>. The spatial patterns of this
diagnostic are very different for Tb and SM retrieval assimilation.
Figure <xref ref-type="fig" rid="Ch1.F4"/>d–e show values of about 7.4 K for Tb_7ang and
Tb_fit, with larger values (exceeding 10 K) in the central plains and along
the Mississippi, where agricultural practices, such as altering crop rotation
and irrigation, are observed by SMOS, whereas interannual variations in
vegetation are not simulated by the model or provided as input to the model.
Along the eastern coast and in the southeast, the temporal standard deviation
in the innovations is low (2–3 K): forests show a limited interannual
variability, and under dense vegetation Tb is only marginally sensitive to
soil moisture and depends primarily on vegetation characteristics and
(physical) temperature.</p>
      <p>The standard deviation in the SM innovations in the SM retrieval assimilation
(Fig. <xref ref-type="fig" rid="Ch1.F4"/>f) is 0.03 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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>, showing larger values in
the wetter vegetated east and smaller values in the drier west, with the
exception of the western coast. Surprisingly, even though altering crop
rotation and irrigation are not simulated, the values over the central
agricultural area are not higher than elsewhere in the domain. This good
agreement between SMOS SM retrievals and our simulations is partly due to the
bounded nature of SM (unlike Tb) and the CDF matching between both.</p>
      <p>Our current system has a Tb sensitivity to soil moisture of about
1.3 K/0.01 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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> across the domain, averaged over all incidence
angles and polarizations. A standard deviation in SM innovations of
0.03 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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> would thus roughly correspond to a standard deviation
in Tb innovations of about 4 K, but instead we find 7.4 K across the study
domain in the Tb assimilation systems. The Tb observations thus either have a
comparably higher observation (including representation) error or they
contain more information than the SM retrievals. At this point, we anticipate
that the larger Tb innovations in the central plains may indicate that the Tb
observations contain more unfiltered information about soil moisture (e.g.,
irrigation) and that the Tb observation error is higher due to shortcomings,
e.g., in the vegetation modeling (representation error).</p>
</sec>
<sec id="Ch1.S4.SS1.SSS3">
  <title>Actual vs. simulated observation and forecast errors</title>
      <p>In a near-optimal filtering system, that is, a system that correctly
simulates the actual model and observation errors, the standard deviation of
the normalized innovations <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mrow><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mrow><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mo>-</mml:mo></mml:msubsup><mml:msub><mml:mo>]</mml:mo><mml:mi mathvariant="italic">λ</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:msqrt><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="bold">R</mml:mi><mml:mrow><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="normal">Cov</mml:mi><mml:mo>(</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mrow><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mo>-</mml:mo></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mrow><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mo>-</mml:mo></mml:msubsup><mml:mo>)</mml:mo><mml:msub><mml:mo>]</mml:mo><mml:mrow><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msqrt></mml:mrow></mml:math></inline-formula>
is close to unity <xref ref-type="bibr" rid="bib1.bibx34" id="paren.49"/>. Figure <xref ref-type="fig" rid="Ch1.F4"/>g–i show
that, averaged across the domain (and across all angles and polarizations for
Tb assimilation), this metric is 1.14, 1.11, and 1.23 (–) for Tb_7ang,
Tb_fit, and SM retrieval assimilation, respectively. The figure thus suggests that, on
average, the simulated errors in the assimilation system only slightly
underestimate the actual errors. But the figures also show that the metric
varies strongly across the domain and exhibits very different spatial
patterns for Tb and SM retrieval assimilation. For Tb_7ang and Tb_fit
assimilation, values are much larger than 1 in the central area and much
smaller than 1 in the eastern forested area. This indicates that the assigned
observation and forecast errors are severely underestimated in the central
area and overestimated in the eastern forested area. Over forests, it can be
assumed that the assigned representation error (part of the observation
error) should be smaller. The Tb forecast error is already very small (see
below), because the Tb uncertainty is only marginally sensitive to soil
moisture uncertainties under dense vegetation. For SM retrieval assimilation,
the pattern is reversed, with the largest values in the eastern half of the
domain, suggesting that here the simulated errors underestimate the actual
errors. Values less than 1 are found in most of the western half of the
domain, where the SM retrieval assimilation seems to overestimate the actual
errors.</p>
      <p>To further interpret the actual and simulated error magnitudes,
Fig. <xref ref-type="fig" rid="Ch1.F4"/>j–k show the ensemble spread in the Tb forecasts (that
is, the simulated forecast error standard deviation)
<inline-formula><mml:math display="inline"><mml:msqrt><mml:mrow><mml:mo>[</mml:mo><mml:mi mathvariant="normal">Cov</mml:mi><mml:mo>(</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mrow><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mo>-</mml:mo></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mrow><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mo>-</mml:mo></mml:msubsup><mml:mo>)</mml:mo><mml:msub><mml:mo>]</mml:mo><mml:mrow><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msqrt></mml:math></inline-formula>.
Averaged across all angles and polarizations <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">λ</mml:mi></mml:math></inline-formula>, the values are around
2 K when averaged across the entire domain. Larger values (3 K) are found
in the central and dry western part, and smaller values (1 K) in the wetter
eastern part. This pattern is similar for the SM ensemble spread in the SM
retrieval assimilation system (Fig. <xref ref-type="fig" rid="Ch1.F4"/>l). In dry climates, the
root-zone soil moisture often drops to the wilting point, remains stagnant
and no longer replenishes the surface. This results in increased sensitivity
of the surface soil moisture to perturbations in meteorological conditions,
and thus in higher uncertainty estimates for surface soil moisture in dry
climates.</p>
      <p>Given that the Tb observation error
<inline-formula><mml:math display="inline"><mml:msqrt><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="bold">R</mml:mi><mml:mrow><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mo>]</mml:mo><mml:mrow><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msqrt></mml:math></inline-formula> is set to 6 K for each individual
angle, polarization, and overpass time in the Tb assimilation, the
approximate total assigned observation and forecast error is 6.1 K
(<inline-formula><mml:math display="inline"><mml:msqrt><mml:mrow><mml:msup><mml:mn mathvariant="normal">6</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mn mathvariant="normal">2</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt></mml:math></inline-formula>) across the study domain, 6.7 K (<inline-formula><mml:math display="inline"><mml:msqrt><mml:mrow><mml:msup><mml:mn mathvariant="normal">6</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mn mathvariant="normal">3</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt></mml:math></inline-formula>) in the
central area, and 6 K (<inline-formula><mml:math display="inline"><mml:msqrt><mml:mrow><mml:msup><mml:mn mathvariant="normal">6</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt></mml:math></inline-formula>) in the eastern Appalachian area.
Because the assigned observation error is uniformly set to 6 K, the spatial
variability in the total simulated errors is thus too small compared to the
actual errors (Fig. <xref ref-type="fig" rid="Ch1.F4"/>d–e), which ranges from more than 10 K
in the central area to around 2–3 K in the eastern Appalachian area.</p>
      <p>The SM observation error (after rescaling) is 0.02 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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> on
average across the domain, with higher values in the eastern part and lower
values in the western part, with the exception of Mexico, California, and
western Oregon, where higher observation errors are found
(Sect. <xref ref-type="sec" rid="Ch1.S3.SS3"/>). This general pattern is reversed in the SM forecast
errors. Combined, the spatial variability in the SM observation and forecast
errors does not capture the spatial variability in the actual errors
(Fig. <xref ref-type="fig" rid="Ch1.F4"/>f), which leads to an overestimation of the errors in
the west and an underestimation in the east.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F6" specific-use="star"><caption><p>Statistics of the increments, calculated for the period from 1 July
2010 to 1 May 2015. Number of increments per day for <bold>(a)</bold> Tb_7ang
assimilation, <bold>(b)</bold> Tb_fit assimilation, and <bold>(c)</bold> SM
assimilation. Temporal standard deviation of total profile water (wtot)
increments for <bold>(d)</bold> Tb_7ang assimilation, <bold>(e)</bold> Tb_fit
assimilation, and <bold>(f)</bold> SM assimilation. (<bold>g</bold>, <bold>h</bold>,
<bold>i</bold>) Same as (<bold>d</bold>, <bold>e</bold>, <bold>f</bold>) but for srfexc
increments. (<bold>j</bold>, <bold>k</bold>, <bold>l</bold>) Same as (<bold>d</bold>,
<bold>e</bold>, <bold>f</bold>) but for rzexc increments. (<bold>m</bold>, <bold>n</bold>,
<bold>o</bold>) Same as (<bold>d</bold>, <bold>e</bold>, <bold>f</bold>) but for catdef
increments. The titles show the spatial mean (m) and standard deviation (s)
across each map.</p></caption>
            <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://hess.copernicus.org/articles/20/4895/2016/hess-20-4895-2016-f06.pdf"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S4.SS2">
  <title>Analysis increments</title>
<sec id="Ch1.S4.SS2.SSS1">
  <title>Spatio-temporal patterns</title>
      <p>The Kalman filter translates footprint-scale innovations into 36 km
increments. Because of the spatially distributed (3-D) filtering (Sect. <xref ref-type="sec" rid="Ch1.S3.SS1"/>), the number of increments in Fig. <xref ref-type="fig" rid="Ch1.F6"/>a–c is
about 1.4 times the number of assimilated observation sets
(Fig. <xref ref-type="fig" rid="Ch1.F4"/>a–c). Many areas with missing observations (or
observation predictions) are filled through interpolation and extrapolation.
With SM retrieval assimilation, there is almost one increment per day.</p>
      <p>Figure <xref ref-type="fig" rid="Ch1.F6"/>d–f show the temporal standard deviations in the
increments for the total soil profile water
(<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>wtot=<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>srfexc+<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>rzexc–<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>catdef). The area average
(<inline-formula><mml:math display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>standard deviation) values are 6.9 <inline-formula><mml:math display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 3.7 mm for Tb_7ang
assimilation, 5.9 <inline-formula><mml:math display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 3.5 mm for Tb_fit assimilation, and
4.2 <inline-formula><mml:math display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.9 for SM retrieval assimilation. After scaling for the
(variable) profile depth, the area-average values in volumetric soil moisture
units are <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>3.4</mml:mn><mml:mo>±</mml:mo><mml:mn>1.7</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn>10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for Tb_7ang assimilation,
<inline-formula><mml:math display="inline"><mml:mrow><mml:mn>2.9</mml:mn><mml:mo>±</mml:mo><mml:mn>1.7</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn>10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for Tb_fit assimilation, and
<inline-formula><mml:math display="inline"><mml:mrow><mml:mn>2.3</mml:mn><mml:mo>±</mml:mo><mml:mn>1.9</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn>10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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 SM retrieval assimilation.</p>
      <p>The individual components of the wtot increments are shown in
Fig. <xref ref-type="fig" rid="Ch1.F6"/>g–i for the surface excess increments,
Fig. <xref ref-type="fig" rid="Ch1.F6"/>j–l for the root-zone excess increments, and
Fig. <xref ref-type="fig" rid="Ch1.F6"/>m–o for the catchment deficit increments. The patterns in
wtot increments are dominated by catdef increments, and they generally
reflect the patterns in the respective innovations' standard deviations
(Fig. <xref ref-type="fig" rid="Ch1.F4"/>d–f), which are very different for Tb and SM retrieval
assimilation. The catdef increments pertain to the entire profile depth
(which typically ranges between 2 and 3 m) and they presumably have a
relatively small impact on the upper 5 cm soil layer (surface soil
moisture): the domain-averaged magnitude of 5.4, 4.9, and 3.5 mm for catdef
increments due to Tb_7ang, Tb_fit or SM retrieval assimilation,
respectively (Fig. <xref ref-type="fig" rid="Ch1.F6"/>m–o), would linearly scale to about 0.1 mm
for a 5 cm soil layer. This is a rough approximation: in reality the part of
catdef that contributes to the 5 cm soil moisture cannot be calculated
without computing the entire balanced profile. However, the approximate
0.1 mm is considerably less than the 0.6, 0.4, and 0.4 mm for the
corresponding srfexc increments (Fig. <xref ref-type="fig" rid="Ch1.F6"/>g–i), which are directly
applied to the upper 5 cm soil layer. The increments in rzexc
(Fig. <xref ref-type="fig" rid="Ch1.F6"/>j–l) are relatively the smallest, because this variable is not
perturbed by design.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><caption><p>Spatially and temporally collocated analysis increments from
(<bold>a</bold>, <bold>c</bold>, <bold>e</bold>) Tb_fit assimilation and (<bold>b</bold>,
<bold>d</bold>, <bold>f</bold>) SM retrieval assimilation vs. the same from Tb_7ang
assimilation for (<bold>a</bold>, <bold>b</bold>) profile-integrated wtot increments,
(<bold>c</bold>, <bold>d</bold>) srfexc increments, and (<bold>e</bold>–<bold>f</bold>)
rzexc increments. Increments are from the period 1 July 2010 to 1 May 2015.
The plot range is limited to the maximum value of 10 times the standard
deviation in either experiment, and divided into 100 even sample bins. Colors
indicate the number of sample points within each 1.5, 0.13, or
0.44 mm bin for <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>wtot, <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>srfexc, and <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>rzexc, respectively.
<inline-formula><mml:math display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> is the spatio-temporal Pearson correlation coefficient between the
individual increments from two assimilation experiments.
</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://hess.copernicus.org/articles/20/4895/2016/hess-20-4895-2016-f07.pdf"/>

          </fig>

      <p>Both Tb and SM retrieval assimilation show similar spatial patterns in the
standard deviations of srfexc increments (Fig. <xref ref-type="fig" rid="Ch1.F6"/>g–i): the
largest increments are found in the dry west and the smallest in the wetter
east. The patterns in srfexc increments agree with the patterns in the
ensemble forecast uncertainty for this variable (not shown, but implied by
the Tb and soil moisture uncertainty in Fig. <xref ref-type="fig" rid="Ch1.F4"/>j–l). The srfexc
values are small with small uncertainties, and the increments are thus
similarly bounded in both Tb and SM retrieval assimilation, yielding
comparable spatial increment patterns.</p>
      <p>Finally, Fig. <xref ref-type="fig" rid="Ch1.F7"/> compares spatially and temporally
collocated wtot, srfexc, and rzexc increments obtained with Tb_7ang
assimilation, Tb_fit assimilation, and SM retrieval assimilation; i.e., the
figure shows all pairs of increments available from two assimilation cases.
The scatter plots show that the increments are usually small and unbiased.
The correlation between the wtot increments (Fig. <xref ref-type="fig" rid="Ch1.F7"/>a)
obtained by Tb_7ang and Tb_fit assimilation is 0.7, and aligns with the
expectation that either Tb assimilation experiment roughly corrects for the
same events. In contrast, the correlation between the increments obtained by
Tb_7ang and SM retrieval assimilation is only 0.3
(Fig. <xref ref-type="fig" rid="Ch1.F7"/>b). The figure is similar when comparing the
Tb_fit and SM retrieval assimilation (not shown). For srfexc and rzexc
(Fig. <xref ref-type="fig" rid="Ch1.F7"/>c–f), the increments are again similar for
Tb_7ang and Tb_fit assimilation, but different for Tb and SM retrieval
assimilation. For all soil moisture prognostic variables, Tb assimilation
leads to larger increments than SM retrieval assimilation. The different
assimilation systems thus introduce distinct corrections to the modeled soil
moisture trajectories.</p>
</sec>
<sec id="Ch1.S4.SS2.SSS2">
  <title>Discussion</title>
      <p>In a nutshell, Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>) states that the increments are given
by the product of the Kalman gain and the innovations. To explain the
differences in increment patterns between Tb and SM retrieval assimilation,
we must therefore consider each system's innovations and Kalman gains. The
relatively larger magnitude of the Tb innovations compared to the SM
innovations (Sect. <xref ref-type="sec" rid="Ch1.S4.SS1.SSS2"/>) contributes to the fact that the Tb
assimilation results in larger soil moisture increments. This is the case
even though the SM retrieval assimilation (unlike Tb assimilation) applies
increments only to moisture variables and does not adjust modeled
temperatures.</p>
      <p>Furthermore, the Kalman gain matrices <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">K</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> (Eq. <xref ref-type="disp-formula" rid="Ch1.E2"/>) for
Tb and SM retrieval assimilation are different because the two systems employ
different observation operators <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mo>.</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and different observation error
covariances <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">R</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. First, we note that the nonlinear inversion of Tb
innovations to soil moisture increments, driven by the RTM in the observation
operator, is <italic>not</italic> responsible for the larger wtot increments in the central
grass and crop areas, because these areas exhibit low values for the
microwave roughness parameter (<inline-formula><mml:math display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mo>&lt;</mml:mo></mml:mrow></mml:math></inline-formula> 0.2, not shown) and a high sensitivity
of Tb to soil moisture (as confirmed by the high forecast Tb errors in
Fig. <xref ref-type="fig" rid="Ch1.F4"/>j–k). That is, in these areas commensurately large Tb
innovations (O–F) values result in only small updates to soil moisture.</p>
      <p>Second, the choice of a spatially uniform observation error covariance in the
Tb assimilation experiment creates an imprint of the innovation pattern in
the increment pattern. Higher increments are found in the agricultural areas
with large Tb innovation standard deviations (Fig. <xref ref-type="fig" rid="Ch1.F4"/>d–e),
because irrigation is not modeled and vegetation is not accurately
parameterized. Since the filter is not set up to correct the latter,
occasional excessive increments to soil moisture and temperature may be
introduced. Such shortcomings could be mitigated by a more sophisticated
assignment of Tb observation (representation) errors.</p>
      <p>For SM retrieval assimilation, the pattern of the SM innovation standard
deviation (RMSD) is similarly visible in the increments, with smaller values
in the west and higher values in the east. Here again, the true
spatio-temporal nature of the observation errors is not captured in the
assigned observation error covariance and therefore propagated into the
increments. Note also that the 0.03 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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> SM innovation standard
deviation (top 5 cm, Fig. <xref ref-type="fig" rid="Ch1.F4"/>f) is translated into a standard
deviation of profile moisture increments of 0.002 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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>
(Fig. <xref ref-type="fig" rid="Ch1.F6"/>f rescaled by profile depth), but these increments are
not equally distributed; i.e., larger increments are found for surface soil
moisture and smaller increments for the deeper profile.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><caption><p>Unbiased RMSD (RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula>) for the model-only open-loop (OL)
simulation, and change in unbiased RMSD (<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula>) due to
data assimilation at (circles) SCAN and (triangles) USCRN sites for
(<bold>a</bold>, <bold>b</bold>, <bold>c</bold>) surface and (<bold>d</bold>, <bold>e</bold>,
<bold>f</bold>) root-zone soil moisture. The skill of (<bold>a</bold>, <bold>d</bold>)
the open-loop simulation is the reference value for the changes in skill due
to (<bold>b</bold>, <bold>e</bold>) Tb_7ang and (<bold>c</bold>, <bold>f</bold>) SM
retrieval assimilation. Statistically significant changes are marked by
larger symbols (e.g., the southeastern US for SM retrieval assimilation).
Metrics are calculated across 3 h time steps during the period from 1 July
2010 to 1 May 2015. The titles indicate the spatial mean
(<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>)RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula> across all sites with clustering (31 clusters).
The gray background shading marks areas with limited vegetation and
topographic complexity based on model parameters.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://hess.copernicus.org/articles/20/4895/2016/hess-20-4895-2016-f08.pdf"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S4.SS3">
  <title>In situ validation</title>
      <p>The above discussion highlights similarities and stark contrasts in how the
Tb and SM retrieval assimilation systems operate. In this section, we look at
the effect of these differences on the skill of the assimilation estimates
vs. in situ observations. Figure <xref ref-type="fig" rid="Ch1.F8"/> shows the
RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula> (Sect. <xref ref-type="sec" rid="Ch1.S2.SS4"/>) for the model-only open-loop
(OL) simulation, and the change in RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula>
(Sect. <xref ref-type="sec" rid="Ch1.S2.SS4"/>) between the OL simulation and either the Tb_7ang
or SM retrieval data assimilation (DA) experiment
(<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula>(DA) – RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula>(OL))
at individual SCAN and USCRN sites, for the period 1 July 2010–1 May 2015.
The gray background shading indicates areas with modest topographic
complexity and vegetation cover and where the satellite observations are most
sensitive to surface soil moisture <xref ref-type="bibr" rid="bib1.bibx8" id="paren.50"><named-content content-type="pre">details
in</named-content></xref>. The OL simulation has an average
RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula> value of 0.054 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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 surface soil moisture
and 0.039 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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 root-zone soil moisture. Looking more closely,
the RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula> values are generally higher in the central and wetter
eastern regions. In dry areas, the RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula> is limited, because the
time series show a limited variability for lack of much precipitation. On
average, both assimilation experiments introduce improvements at about
80 % of the sites for surface soil moisture, with spatially averaged
<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula> values of <inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.004 and <inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.003 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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
Tb_7ang and SM retrieval assimilation, respectively. (Spatial average
metrics are computed using a cluster-based algorithm,
Sect. <xref ref-type="sec" rid="Ch1.S2.SS4"/>.) The improvements are also propagated to the
root-zone soil moisture (65 % of sites improved) with smaller average
<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula> values of <inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.002 and <inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.001 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math 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>,
respectively.</p>
      <p>The domain-average <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula> values caused by assimilation are
only barely statistically significant for surface soil moisture in
“favorable” areas, i.e., where the satellite observations are most
sensitive to soil moisture (indicated with green background shading in
Fig. <xref ref-type="fig" rid="Ch1.F8"/>). The differences between Tb_7ang, Tb_fit, or SM
retrieval assimilation are not significant. The assimilation contributes an
average relative improvement in surface soil moisture of 7 % of the OL
RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula> in favorable locations and 4 % in non-favorable areas.
Both Tb and SM retrieval assimilation show improvements in the central and
eastern parts of the US, but perform poorly in the western dry mountain
areas, where the RMSD<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mtext>ub</mml:mtext></mml:msub></mml:math></inline-formula> for the OL was small and the assimilation
may have introduced some additional noise. The Tb_7ang assimilation shows
the largest improvements in the central US, whereas the SM retrieval
assimilation shows the largest improvements in the southeastern part, for
both surface and root-zone soil moisture. It is possible that the Tb
assimilation has a larger impact in the central US than the SM retrieval
assimilation, because irrigation events may be filtered in the SM retrievals
(and perhaps partly assigned to vegetation opacity retrievals).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9"><caption><p>Performance of open-loop and data assimilation experiments in terms
of anomaly correlations (anomR) calculated across 3 h analyses and forecast
time steps from 1 July 2010 to 1 May 2015 for <bold>(a)</bold> surface and
<bold>(b)</bold> root-zone soil moisture. The bars show skill metrics averaged
over sites in either favorable or non-favorable areas, where favorable areas
refer to the areas indicated by the gray background shading in
Fig. <xref ref-type="fig" rid="Ch1.F8"/>. The variable <inline-formula><mml:math display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> is the total number of SCAN and
USCRN sites considered for each category, with the number of clusters in
parentheses. The error bars reflect cluster-averaged 95 % confidence
intervals.</p></caption>
          <?xmltex \igopts{width=199.169291pt}?><graphic xlink:href="https://hess.copernicus.org/articles/20/4895/2016/hess-20-4895-2016-f09.pdf"/>

        </fig>

      <p>The bar plots in Fig. <xref ref-type="fig" rid="Ch1.F9"/> summarize the average anomR values
for the open-loop and data assimilation experiments, after stratifying all
SCAN and USCRN sites into “favorable” and “non-favorable” categories
(gray vs. white background in Fig. <xref ref-type="fig" rid="Ch1.F8"/>). The figures show
that the open-loop anomR values for surface soil moisture are similar for
both the favorable and non-favorable areas (0.51 and 0.50, respectively).
However, data assimilation has a larger impact in favorable areas, where all
assimilation schemes introduce significant improvements (anomR <inline-formula><mml:math display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.63,
0.61, and 0.59 for Tb_7ang, Tb_fit, and SM retrieval assimilation). In
non-favorable areas, the improvements are smaller but still significant
(anomR <inline-formula><mml:math display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.57, 0.56, and 0.54, for Tb_7ang, Tb_fit, and SM retrieval
assimilation).</p>
      <p>In the root zone, data assimilation also improves the skill over the
open-loop simulations, but without statistical significance. The open-loop
simulations yield anomR values of 0.56 and 0.50 in favorable and
non-favorable areas, respectively. In favorable areas, the assimilation
increases the anomR to 0.64, 0.64, and 0.62, for Tb_7ang, Tb_fit, and SM
retrieval assimilation. In non-favorable areas, the skill improvement is
limited and the anomR values are 0.54, 0.54, and 0.52, for Tb_7ang, Tb_fit,
and SM retrieval assimilation. In any case, with assimilation, all anomR
values exceed 0.5, meaning that the skill becomes better than a
climatological forecast (Brier skill score larger than 0).</p>
      <p>Overall, the skill metrics are comparable for the Tb_7ang and Tb_fit
assimilation (Fig. <xref ref-type="fig" rid="Ch1.F9"/>). The results from SM retrieval
assimilation are slightly worse than those from Tb assimilation, which may
indicate that Tb observations indeed still contain more information
(Sect. <xref ref-type="sec" rid="Ch1.S4.SS2"/>) than the SM retrievals, which are implicitly
filtered during the retrieval process. However, the differences between the
domain-averaged skill values of the various assimilation schemes are minimal.
Furthermore, when running the assimilation scheme with different spatially
constant Tb observation error parameters, the skill metrics only changed
marginally. This shows that our skill metrics are relatively insensitive to
uniform changes in the data assimilation parameters. One reason for this is
that the skill metrics are presented as (clustered) spatial averages, which
compensate for large local differences. It is expected that the skill of our
data assimilation systems can only be further improved by using a more
localized (in space and time) approach to optimizing the assimilated
observations (e.g., L2 SM retrievals) and the forecast and observation error
parameters in the EnKF.</p>
      <p>Finally, unlike <xref ref-type="bibr" rid="bib1.bibx27" id="text.51"/>, the skill improvements in this study are
smaller when we correct the re-analysis precipitation input with gauge-based
precipitation data <xref ref-type="bibr" rid="bib1.bibx33" id="paren.52"/>. This and other recent
improvements in the GEOS-5 modeling system make it increasingly challenging
to obtain significant skill improvements from the assimilation of microwave
observations over areas for which high-quality forcing data are available,
such as the domain studied here. The benefits of the microwave-based soil
moisture assimilation system are expected to be greater in areas with poorer
ancillary inputs to the modeling system. This aspect will be further
investigated through the validation of the global SMAP L4_SM data product.</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <title>Conclusions</title>
      <p>The SMOS and SMAP satellite missions currently provide a wealth of L-band
data to monitor large-scale soil moisture. A key question is how to make the
best use of these data in current land surface data assimilation systems. The
L1 Tb data from these missions are often complex, because of their
multi-polarization and possibly multi-angle nature and their indirect
connection with soil moisture. In theory, the best approach is to directly
assimilate Tb observations using a consistent data assimilation system, but a
correct global characterization of the Tb forecast and observation errors
remains difficult. The L2 SM retrievals are easily handled products, but
their assimilation is impacted by errors introduced by inconsistent ancillary
information in the SM retrieval algorithm and the assimilation system. With
further improvements in the assimilated retrievals and careful selection of
the ancillary data, SM retrieval assimilation may become a coequal
alternative.</p>
      <p>Three different data products from the SMOS mission are assimilated
separately into the GEOS-5 land surface model to improve estimates of surface
and root-zone soil moisture and to study the workings of each assimilation
system. The first product consists of L1-based data of multi-angle,
dual-polarization Tb observations at the bottom of the atmosphere. The second
product is a derived 40<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> Tb product that mimics SMAP data. The third
product is the operational L2 SM dataset. Special care is taken during
quality control and processing of the satellite observations prior to
assimilation and within the assimilation system. The Tb assimilation uses a
distributed EnKF with a temporally variable Tb bias mitigation, a system that
is also used for the SMAP L4_SM product <xref ref-type="bibr" rid="bib1.bibx36" id="paren.53"/>. The SM
retrieval assimilation uses a similar system, but with CDF matching instead
to eliminate the more stationary SM innovation biases. The study covers most
of North America for the period of 1 July 2010–1 May 2015.</p>
      <p>The Tb and SM innovations show very different spatial patterns and the number
of assimilated observations differs because of different needs for data
screening and bias mitigation. Based on the average sensitivity of Tb to soil
moisture, the magnitude of the Tb innovations is comparably larger than that
of the SM innovations, which may either introduce more information or more
error into the Tb assimilation system. The Tb and SM retrieval assimilation
schemes also yield surprisingly different spatio-temporal increment patterns,
leading to very different adjustments to the modeled soil moisture
trajectories. Despite these stark differences, the various assimilation
schemes yield soil moisture estimates with similar average skill metrics,
computed from a set of 187 SCAN and USCRN sites across the US. Compared to in
situ observations, both Tb and SM retrieval assimilations yield anomaly
correlations around or larger than 0.6 for both the surface and root-zone
soil moisture in “favorable” areas, where the satellite data are expected
to better represent the soil moisture conditions, i.e., in areas with limited
topographic complexity and limited vegetation. The anomaly correlation with
data assimilation is between 0.5 and 0.6 in non-favorable areas. The data
assimilation introduces significant improvements over the model-only
simulations for surface soil moisture everywhere, but the improvements are
much larger in favorable areas. For the root zone, improvements are also
found, but without statistical significance. While no significant differences
in domain-averaged skills can be found between the various assimilation
systems, there are large local differences in performance between the Tb and
SM retrieval assimilation which may be due to differences in information
content and screening of the observations, and differences in how close each
of the systems is to an optimal calibration of its model and observation
error parameters. Therefore, we expect that soil moisture data assimilation
systems can be further improved only if the systems manage to better simulate
the spatial and temporal variations of the actual errors in the model and the
observations. Furthermore, the SM retrieval assimilation results will benefit
from any future improvement in the SM retrievals.</p>
      <p>In line with our findings for the SMOS data assimilation, we anticipate that
future versions of the Tb assimilation system for the SMAP L4_SM product may
benefit from an improved characterization of spatial model and observation
error structures, and from a better representation of some modeling
components, such as, e.g., vegetation. In addition, given that SMOS and SMAP
both provide L-band Tb observations, future assimilation systems should
consider a joint assimilation of SMOS and SMAP Tb data. In such a system, it
is important to consider the different instrument, Tb
processing, and Tb error
characteristics of the two L-band missions <xref ref-type="bibr" rid="bib1.bibx12" id="paren.54"/>.</p>
</sec>
<sec id="Ch1.S6">
  <title>Data availability</title>
      <p>The SMOS data are distributed by ESA.
The model and assimilation results can be obtained from the authors upon request.</p><?xmltex \hack{\newpage}?>
</sec>

      
      </body>
    <back><ack><title>Acknowledgements</title><p>The NASA Soil Moisture Active Passive (SMAP) mission supported this study.
The NASA Center for Climate Simulation (NCCS) at the Goddard Space Flight
Center provided computational resources through the NASA High-End Computing
(HEC) program. The authors thank the editors and reviewers for their input.
<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: B. Su<?xmltex \hack{\newline}?>
Reviewed by: Y. Zeng and two anonymous referees</p></ack><ref-list>
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