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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-25-6283-2021</article-id><title-group><article-title>Optimizing a backscatter forward operator using Sentinel-1 data over irrigated land</article-title><alt-title>Optimizing a backscatter forward operator using Sentinel-1 data over irrigated land</alt-title>
      </title-group><?xmltex \runningtitle{Optimizing a backscatter forward operator using Sentinel-1 data over irrigated land}?><?xmltex \runningauthor{S.~Modanesi~et~al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2 aff4">
          <name><surname>Modanesi</surname><given-names>Sara</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-4720-5233</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Massari</surname><given-names>Christian</given-names></name>
          <email>christian.massari@irpi.cnr.it</email>
        <ext-link>https://orcid.org/0000-0003-0983-1276</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Gruber</surname><given-names>Alexander</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3280-7023</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Lievens</surname><given-names>Hans</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Tarpanelli</surname><given-names>Angelica</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3487-1659</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Morbidelli</surname><given-names>Renato</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>De Lannoy</surname><given-names>Gabrielle J. M.</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Research Institute for Geo-hydrological Protection, National Research Council, Via della Madonna Alta 126,<?xmltex \hack{\break}?> 06128 Perugia, Italy</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Earth and Environmental Sciences, KU Leuven, Heverlee, Belgium</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Civil and Environmental Engineering of Perugia, Via G. Duranti 93, 06125 Perugia, Italy</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>DICEA Department of Civil and Environmental Engineering, University of Florence, Via di S. Marta 3, 50139 Florence, Italy</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Christian Massari (christian.massari@irpi.cnr.it)</corresp></author-notes><pub-date><day>13</day><month>December</month><year>2021</year></pub-date>
      
      <volume>25</volume>
      <issue>12</issue>
      <fpage>6283</fpage><lpage>6307</lpage>
      <history>
        <date date-type="received"><day>21</day><month>May</month><year>2021</year></date>
           <date date-type="accepted"><day>26</day><month>October</month><year>2021</year></date>
           <date date-type="rev-recd"><day>18</day><month>September</month><year>2021</year></date>
           <date date-type="rev-request"><day>14</day><month>June</month><year>2021</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2021 </copyright-statement>
        <copyright-year>2021</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://hess.copernicus.org/articles/.html">This article is available from https://hess.copernicus.org/articles/.html</self-uri><self-uri xlink:href="https://hess.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://hess.copernicus.org/articles/.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e158">Worldwide, the amount of water used for agricultural purposes is rising, and the quantification of irrigation is becoming a crucial topic. Because of   the limited availability of in situ observations, an increasing number of studies is focusing on the synergistic use of models and satellite data to detect and quantify irrigation. The parameterization of irrigation in large-scale land surface models (LSMs) is improving, but it is still hampered by the lack of information about dynamic crop rotations, or the extent of irrigated areas, and the mostly unknown timing and amount of irrigation. On the other hand, remote sensing observations offer an opportunity to fill this gap as they are directly affected by, and hence potentially able to detect, irrigation. Therefore, combining LSMs and satellite information through data assimilation can offer the optimal way to quantify the water used for irrigation.</p>

      <p id="d1e161">This work represents the first and necessary step towards building a reliable LSM data assimilation system which, in future analysis, will   investigate the potential of high-resolution radar backscatter observations from Sentinel-1 to improve irrigation quantification. Specifically, the   aim of this study is to couple the Noah-MP LSM running within the NASA Land Information System (LIS), with a backscatter observation operator for   simulating unbiased backscatter predictions over irrigated lands. In this context, we first tested how well modelled surface soil moisture (SSM) and   vegetation estimates, with or without irrigation simulation, are able to capture the signal of aggregated 1 <inline-formula><mml:math id="M1" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> Sentinel-1 backscatter   observations over the Po Valley, an important agricultural area in northern Italy. Next, Sentinel-1 backscatter observations, together with simulated SSM and leaf area index (LAI), were used to optimize a Water Cloud Model (WCM), which will represent the observation operator in future data assimilation experiments. The WCM was calibrated with and without an irrigation scheme in Noah-MP and considering two different cost functions. Results demonstrate that using an irrigation scheme provides a better calibration of the WCM, even if the simulated irrigation estimates are inaccurate. The Bayesian optimization is shown to result in the best unbiased calibrated system, with minimal chances of having error cross-correlations between the model and observations. Our time series analysis further confirms that Sentinel-1 is able to track the impact of human activities on the water cycle, highlighting its potential to improve irrigation, soil moisture, and vegetation estimates via future data assimilation.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e181">Over the last century, the global water withdrawal grew 1.7 times faster than the population (FAO, 2006). This aggravates the concern over the sustainability of water use as the demand for agricultural uses continues to increase (Foley et al., 2011; FAO AQUASTAT <uri>http://www.fao.org/nr/water/aquastat/water_use/index.stm</uri>, last access: 20 May 2021). The strong impact of irrigation on the global water budget is<?pagebreak page6284?> highlighted by many studies, and it has been estimated that about 87 % of the global fresh water withdrawals have been used for agriculture (Douglas et al., 2009). Accordingly, the quantification of irrigation on a regional to global scale has become a hot research topic.</p>
      <p id="d1e187">Correctly quantifying irrigation in Earth system models can serve two purposes. On the one hand, it can help improve water management (Le Page et al., 2020, Bretreger et al., 2020); on the other hand, it allows us to quantitatively assess its effects on the terrestrial water, carbon, and energy cycles (Haddeland et al., 2007; Breña-Naranjo et al., 2014; Hu et al., 2016; Qian et al. 2020). Indeed, results of large-scale irrigation studies using land surface models (LSMs) have demonstrated that irrigation increases soil moisture and evapotranspiration (ET) and, consequently, latent heat flux with a decrease in sensible heat flux (i.e. Badger and Dirmeyer, 2015; Lawston et al., 2015; Ozdogan et al., 2010).</p>
      <p id="d1e190">Despite the significant impact of irrigation on the water and energy cycles, its simulation within LSMs is not yet common practice (Girotto et al.,
2017). In earlier studies, attempts to simulate irrigation in LSMs have relied on different
parameterizations of well-known irrigation systems (like sprinkler, flood, and drip systems; Ozdogan et al., 2010; Evans and Zaitchik, 2008), making
simplified assumptions. For instance, in Ozdogan et al. (2010), irrigation water is not withdrawn from a source (such as a river) but instead added
as fictitious rainfall. In contrast, Nie et al. (2018) accounted for source water partitioning, albeit only partially, by considering groundwater
irrigation. Irrigation is normally applied when soil moisture drops below a user-defined threshold (Ozdogan et al., 2010) and is typically dependent on the soil properties obtained via soil texture maps.</p>
      <p id="d1e193">Moreover, LSMs equipped with irrigation schemes need to be provided with auxiliary information about crop types and whether or not the crops are
irrigated. This is because different crop types are characterized by different rooting depths, which means they require more or less water to restore root zone field capacity. This information is normally gathered from static maps derived from statistical analysis and/or remote sensing (Ozdogan
et al., 2010; Monfreda et al., 2008; Salmon et al., 2015) collected during specific historical periods, which are normally different to the desired
period of analysis. It is thus clear that the modelling of irrigation is subject to many simplifying assumptions, which span from neglecting the
year-to-year crop variability and the irrigation system used to the definition of irrigation application times based on water availability and crop conditions rather than actual farmer decisions.</p>
      <p id="d1e197">Remote sensing (RS) technologies offer the opportunity to observe the Earth's surface and its changes directly and, hence, are potentially able to
monitor irrigated lands worldwide (Ambika et al., 2016; Gao et al., 2018; Bousbih et al., 2018; Bazzi
et al., 2019; Le Page et al., 2020; Dari et al., 2020). In the last decade, some authors used visible and near-infrared RS observations jointly with
in situ data collected from inventories to map areas equipped for irrigation (Ambika et al., 2016; Ozdogan and Gutman, 2008). S. V. Kumar
et al. (2015) were the first to propose the use of coarse resolution satellite microwave (MW) sensors
to detect irrigation. The authors compared different coarse-scale active and passive MW surface soil moisture (SSM) retrievals with SSM simulations
from the Noah LSM (version 3.3; Ek et al., 2003) without activating an irrigation scheme over a continental USA domain. Areas where the distributions of model and RS data sets deviated (based on a Kolmogorov–Smirnov test) were assumed to be irrigated. Even though some of the products showed a potential ability to detect irrigation, the authors concluded that the spatial mismatch between the satellite footprint and the irrigated fields, radio frequency interference (RFI), vegetation, and topography could all deteriorate the accuracy of the results. Similar conclusions were found over the same area by Zaussinger et al. (2019), who compared coarse-scale satellite SSM products with soil moisture predictions from the Modern-Era
Retrospective analysis for Research and Applications, version 2 (MERRA-2) in the absence of precipitation, and Escorihuela and Quintana-Seguí (2016), who
additionally compared a downscaled version of the Soil Moisture and Ocean Salinity (SMOS) mission SSM to SURFEX LSM simulations. Brocca et al. (2018),
Jalilvand et al. (2019), and Dari et al. (2020) used a conceptually different approach, with the same coarse scale MW SSM products, and estimated
irrigation by directly inverting a simple water balance equation (Brocca et al., 2014).</p>
      <p id="d1e200">The Copernicus Sentinel-1 satellites (Sentinel-1A and Sentinel-1B) offer a new perspective for agricultural applications thanks to the finer spatial
resolution (up to 10–20 <inline-formula><mml:math id="M2" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>) of the synthetic aperture radar (SAR) backscatter (<inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>) data. For instance, Gao et al. (2018) proposed an
approach to map irrigated lands over the Urgell region in Catalonia (Spain), and Le Page et al. (2020) proposed a methodology to detect irrigation
timing in southwestern France by comparing the SSM signal at the plot scale, derived using Sentinel-1 <inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and NDVI from Sentinel-2 (El Hajj
et al., 2017), with a water budget model forced by Sentinel-2 optical data for the detection of irrigation timing.</p>
      <p id="d1e233">Despite the high potential demonstrated by RS in detecting, mapping, and quantifying irrigation, the uncertainties of the satellite retrievals, the
relatively low revisit time of high-resolution active MW products, and the too coarse spatial resolution of passive MW products with respect to the
mean size of irrigated fields represent main limitations for irrigation information retrieval (Romaguera et al., 2010; La Page et al., 2020). Data assimilation (DA) could reduce some uncertainties by optimally integrating LSM estimates and RS
observations. Indeed, the LSM estimates resolve processes at desired spatiotemporal scales, while the RS observations can track, in a more realistic way, human processes like irrigation and their interactions with the water and energy cycles. Contrasting LSM simulations with RS observations offers an opportunity to correct for unmodelled processes or missed<?pagebreak page6285?> events, such as irrigation (S. V. Kumar et al., 2015; Girotto et al., 2017). More generally, DA of satellite-based observations has shown the potential to update soil moisture (De Lannoy and Reichle, 2016; Kolassa et al., 2017) and vegetation (Albergel et al., 2018; Kumar et al., 2020), and important impacts have been reported over agricultural areas (Kumar et al., 2020).</p>
      <p id="d1e236">The assimilation of MW RS observations in LSMs often involves retrieval assimilation. However, assimilating retrievals (i.e. SSM or vegetation
optical depth rather than MW brightness temperature or <inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> measurements) can be problematic as the retrievals may have been produced with ancillary data that are inconsistent with those used in the LSM (De Lannoy et al., 2016). This is particularly true for passive MW retrievals,  while active MW retrievals generally rely on change detection methods that lack land-specific ancillary information altogether. An alternative approach,
which we follow in this study, is to directly assimilate MW observations and equip the LSM with an observation operator that links the land surface
variables of interest (e.g. soil moisture and vegetation) with RS data. This allows us to obtain consistent parameters and to reduce the chance of
cross-correlated errors between model states and corresponding geophysical satellite retrievals. The direct assimilation of MW observations has
already been demonstrated successfully for the update of soil moisture by using brightness temperature (Tb) derived from the SMOS and SMAP (Soil Moisture Active Passive) missions (De Lannoy et al., 2016;
Carrera et al., 2019; Reichle et al. 2019), as well as using radar <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> from ASCAT (Advanced Scatterometer; Lievens et al., 2017b), and <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> from Sentinel-1 in synergy with SMAP Tb (Lievens et al., 2017a). However, to our knowledge, none of these studies considered the joint updating of soil moisture and vegetation, and none specifically focused on the performance over irrigated areas. The <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> from Sentinel-1 contains information on both soil moisture (Zribi et al., 2011; Liu and Shi, 2016; Li and Wang, 2018; Bauer-Marschallinger et al., 2018) and vegetation (Vreugdenhil et al., 2018, 2020), and assimilating this data could allow us to update both soil moisture and vegetation in a land data assimilation system and, in doing so, correct for missed irrigation events.</p>
      <p id="d1e283">To that end, the LSM needs to be coupled to a backscatter forward model as an observation operator. Different SAR <inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> models have been
proposed to simulate the backscattering contributions of soil and vegetation (Attema and Ulaby, 1978; Oh, 2004; Zribi et al., 2005; Bai et al.,
2015; Baghdadi et al., 2017). Most commonly used, the Water Cloud Model (WCM hereafter) developed by Attema and Ulaby (1978) is a <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> model
that represents the vegetation canopy as a homogeneous cloud containing randomly distributed water droplets. In order to use the WCM as the forward
operator in a <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> data assimilation system, it first needs to be calibrated to account for biases between the LSM simulations and the
satellite observations. However, calibrating a WCM to simulate <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> over irrigated areas is not a straightforward process, and it represents
a key research problem if the same <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> signal is used for the calibration of WCM parameters and later for assimilation and updating of the state. In fact, if the objective is to assimilate radar <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> to realistically inform the model about irrigation applications, the WCM parameters have to maintain a certain degree of independence from the irrigation signal contained in the observed <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> as, otherwise, the assumption of uncorrelated errors between model and observations typical of classical Bayesian-based filters is violated. More specifically, if the LSM provides unrealistic simulations as input (i.e. the absence of irrigation), then the WCM calibration with observed <inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> would compensate for this
bias. This would, in turn, lead to a biased backscatter model with undesirable calibrated parameters for the subsequent data assimilation
experiments. Therefore, different strategies can be adopted, for instance by calibrating the model during non-irrigated periods or over non-irrigated
areas or equipping the LSM with an irrigation module that makes the WCM less constrained by inconsistencies between simulated and observed <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> during irrigation periods. The efficacy of these strategies has, so far, never been explored.</p>
      <p id="d1e386">The main objective of this study is to simulate radar <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> using a LSM coupled with a WCM and to provide solutions and recommendations for the
optimization of the WCM as an observation operator. This is a major stepping stone towards the development of a reliable system for the assimilation of high-resolution Sentinel-1 <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> observations over irrigated areas. Additionally, we aim at the following:
<list list-type="order"><list-item>
      <p id="d1e413">testing the ability of a sprinkler irrigation system coupled with a LSM to simulate irrigation so as to highlight the potential and limitations of such a tool to optimize a backscatter forward operator over heavily irrigated areas</p></list-item><list-item>
      <p id="d1e417">demonstrating that Sentinel-1 <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> observations contain valuable information to improve both SM and vegetation predictions over
irrigated land (i.e. soil moisture and vegetation consistent with human alterations in the water cycle due to intensive irrigation).</p></list-item></list></p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e434">The study area and the two test sites of <bold>(a)</bold> Budrio and <bold>(b)</bold> Formellino. Data on the topography are obtained from ETOPO1 Arc-Minute Global Relief Model (Amante and Eakins, 2009). Map data © 2015 Google.</p></caption>
        <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://hess.copernicus.org/articles/25/6283/2021/hess-25-6283-2021-f01.png"/>

      </fig>

      <p id="d1e449">The analysis is carried out over the Po Valley, one of the most important agricultural areas in Italy and also one of the more intensively
irrigated areas in Europe (water withdrawal in the Po basin is estimated to be 20.5 <inline-formula><mml:math id="M21" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">billion</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, of which 16.5 <inline-formula><mml:math id="M22" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">billion</mml:mi></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M23" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> is withdrawn for irrigation; Po River Watershed Authority, 2016). We use the Noah-MP v.3.6 LSM (Noah-MP hereafter) as part of the NASA Land Information System (LIS) framework, together with the WCM from Attema and Ulaby (1978), for the simulation of both <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> vertical send and receive (VV) and vertical send and horizontal receive (VH) polarization. Level 1 Sentinel-1 <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> observations are used to calibrate the WCM at 1 <inline-formula><mml:math id="M26" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> resolution, using simulated SSM and leaf area index (LAI) estimates from Noah-MP. The WCM is calibrated for a total of four calibration experiments for each polarization,<?pagebreak page6286?> namely (1) with or without activating an irrigation scheme within Noah-MP and (2) considering two different cost functions. Specifically, we want to demonstrate that activating an – even poor – irrigation scheme is needed to obtain long-term unbiased <inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations and uncorrelated errors between the WCM and Sentinel-1, and that the calibration process can be sensitive to different cost functions.</p>
      <p id="d1e545">The paper is organized as follows. Section 2 provides information on the study area, the selected data sets, and methods used for our analysis. Specifically, Sect. 2.3 and 2.4 provide a detailed description of the Noah-MP LSM and the WCM. Section 2.5 describes the cost functions used for the WCM calibration, while Sect. 2.6 is a description of the experimental set-up designed for the calibration. Finally, Sect. 2.7 provides insights on the Noah-MP and WCM evaluations. Section 3 presents the results, with an assessment of the Noah-MP evaluation, both regional (Sect. 3.1) and over the test sites (Sect. 3.2). The WCM calibration and evaluation results are described in Sect. 3.3 and 3.4, respectively. We provide a discussion in Sect. 4, while conclusions are reported in Sect. 5.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data and methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Study area and in situ data</title>
      <p id="d1e563">The analysis was carried out over an area of 24 000 <inline-formula><mml:math id="M28" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> located within the Po Valley, one of the most important agricultural areas
in Europe (Fig. 1; 44<inline-formula><mml:math id="M29" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 10.5<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W – bottom left; 45.5<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 12.2<inline-formula><mml:math id="M32" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W – top right). The Po Valley is part of the Po basin district (<inline-formula><mml:math id="M33" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 74 000 <inline-formula><mml:math id="M34" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>), a mountain-fed catchment which extends from the Alps in the west to the Adriatic Sea in the east. The Po district is one of the eight districts mentioned in the Water Framework Directive (WFD; EC, 2000) initiated by the European Commission and has been hit by seasonal drought events which impacted all water use sectors, in particular agriculture (Strosser et al., 2012). The water assessment and impact evaluation of human activities over the Po Valley is thus a topic of major interest, considering the significant requirements from the agricultural management sector.</p>
      <p id="d1e632">According to the Köppen–Geiger climate classes (Peel et al., 2007) the study area is classified as Cfa (temperate climate, without a dry season,
and with hot summers). From a geographical point of view, the Po river flows from the west to the east, splitting the area of interest in northern and
southern areas, respectively. North of the Po river, the agricultural plain area can additionally be subdivided into the Veneto region to the east and
the Lombardy region to the west (Fig. 1). Lombardy lands have a high water availability, thanks to the presence of several Alpine lakes and reservoirs
(Musolino et al., 2017), as does the Veneto region. Wine cultivation plays an important role, especially in the Lake Garda surroundings (located to
the northwest of the study area). In the south, the Emilia Romagna region is an agricultural and urbanized industrialized area. Compared to Lombardy and Veneto, Emilia Romagna is much poorer both in water availability and storage capacity, but its irrigation system is considered the most technologically advanced and efficient in the Po river basin (Musolino et al., 2017). Specifically, it hosts the Canale Emiliano Romagnolo (CER;
<uri>https://consorziocer.it/it/</uri>, last<?pagebreak page6287?> access: 20 May 2021), which is one of the most important Italian hydraulic systems for agricultural water supply. The main crops in the study region include general summer and winter crops, orchards (i.e. peach, pear, and kiwi), olive groves, and vineyards
(<uri>https://sites.google.com/drive.arpae.it/servizio-climatico-icolt/home</uri>; last access: 20 May 2021). The plain area is surrounded by a forested hilly and mountainous area of the Tuscan–Emilian Apennines to the south/southwest.</p>
      <p id="d1e641">In situ data were collected over two test sites located in the Emilia Romagna region.
<list list-type="bullet"><list-item>
      <p id="d1e646">For an analysis at plot scale, we selected the Budrio test site (Fig. 1a), an experimental farm managed by the CER authority, which  includes two plots of 0.39–0.49 <inline-formula><mml:math id="M35" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ha</mml:mi></mml:mrow></mml:math></inline-formula>. The main crops are maize for field 1 (in yellow) and tomatoes in field 2 (red). Daily irrigation data, in millimetres, were collected for the summer of 2015–2016 over field 1, whereas daily irrigation water amounts were collected for the summer of 2017 over field 2. Additionally, for field 2, hourly in situ soil moisture data, aggregated here at a daily scale, were made available from the Department of Physics and Earth Science of the University of Ferrara. The soil moisture data were derived from an innovative proximal gamma-ray (PGR SM hereafter; Filippucci et al., 2020, Strati et al., 2018) station, equipped with a 1 L NaI(Tl) detector placed at 2.25 <inline-formula><mml:math id="M36" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> above ground  and a commercial agro-meteorological station (MeteoSense 2.0, Netsens; Strati et al., 2018). The PGR is a nuclear non-invasive and non-contact  technique, which allows us to overcome the issue connected to in situ point measurements, probing soil moisture with a field-scale footprint
(<inline-formula><mml:math id="M37" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M39" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>) up to a depth of <inline-formula><mml:math id="M40" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 30 <inline-formula><mml:math id="M41" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula>. The quantification of PGR soil moisture is derived from measurements of gamma signals emitted by the decay of <inline-formula><mml:math id="M42" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">40</mml:mn></mml:msup></mml:math></inline-formula>K, which is extremely sensitive to different soil water contents in agricultural soils (for more information on the PGR soil moisture deriving procedure, the reader can refer to Baldoncini et al., 2019). Finally, daily rainfall data were collected from the national rainfall network, managed by the Department of Civil and Environmental Protection (DPC) of Italy, for the irrigated periods.</p></list-item><list-item>
      <p id="d1e718">The second test site (Fig. 1b) is located around the city of Faenza (hereafter the Faenza test site) and has a total extent of 1051 <inline-formula><mml:math id="M43" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ha</mml:mi></mml:mrow></mml:math></inline-formula>, consisting of two fields which allow analysis at the small-district spatial scale. The first one is called San Silvestro (290 <inline-formula><mml:math id="M44" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ha</mml:mi></mml:mrow></mml:math></inline-formula>), and it is located north of the city. The second one is called Formellino (760 <inline-formula><mml:math id="M45" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ha</mml:mi></mml:mrow></mml:math></inline-formula>), located east of the San Silvestro field and northeast of the city of Faenza. Fruit trees are prevalent on the fields; in particular, pear trees and kiwi dominate the area. The water used for irrigation was provided by CER, at an hourly timescale and in millimetres, for the 2-year time period of 2016–2017. Daily rainfall data were collected from the national   rainfall network managed from the DPC.</p></list-item></list></p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><?xmltex \opttitle{Sentinel-1 $\sigma^{{0}}$ and reference remote sensing products}?><title>Sentinel-1 <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and reference remote sensing products</title>
      <p id="d1e765">The Copernicus-ESA Sentinel-1 <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> observations were used in this study for the calibration of the WCM. The Sentinel-1 constellation consists
of two satellites, Sentinel-1A and Sentinel-1B, launched in 2014 and 2016, respectively. Each satellite carries a synthetic aperture radar (SAR)
operating at the C band (5.4 <inline-formula><mml:math id="M48" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">GHz</mml:mi></mml:mrow></mml:math></inline-formula>) in the microwave portion of the electromagnetic spectrum. The processing of the ground-range detected (GRD)
interferometric wide swath (IW) observations in VV and VH polarization was done using Google Earth Engine's Python interface and included standard
techniques, namely precise orbit file application, border noise removal, thermal noise removal, radiometric calibration, and range Doppler terrain
correction. Furthermore, the <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> observations acquired at 5 <inline-formula><mml:math id="M50" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M51" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 20 <inline-formula><mml:math id="M52" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> resolution were aggregated and projected on the 1 <inline-formula><mml:math id="M53" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> Equal-Area Scalable Earth version 2 (EASE-2) grid (Brodzik et al., 2012). After applying an orbit bias correction (Lievens et al., 2019), the observations from different orbits, either from Sentinel-1A or Sentinel-1B and ascending or descending tracks, were combined at the daily timescale.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e832">Regridded and reclassified input data used in the LIS framework. <bold>(a)</bold> The PROBA-V land cover (LC) map. <bold>(b)</bold> The Harmonized World Soil Database (HWSD) soil texture map.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://hess.copernicus.org/articles/25/6283/2021/hess-25-6283-2021-f02.png"/>

        </fig>

      <p id="d1e847">Additionally, RS observations were used for the evaluation of the SSM and LAI simulated in Noah-MP LSM for the period 31 March 2015–December 2019.
<list list-type="bullet"><list-item>
      <p id="d1e852">The NASA Soil Moisture Active Passive (SMAP; Entekhabi et al., 2010) is an orbiting observatory launched in January 2015 carrying two
instruments, namely a SAR, which suffered a failure in early July 2015, and a radiometer measuring Tb at the L band, with a native spatial resolution of   40 <inline-formula><mml:math id="M54" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula>, a revisit time of 2–3 <inline-formula><mml:math id="M55" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">d</mml:mi></mml:mrow></mml:math></inline-formula>, and ascending and descending overpasses at 18:00 and 06:00 LT (local time), respectively. For  this study, the 9 <inline-formula><mml:math id="M56" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> SMAP Enhanced Level-2 SSM version 4 (0–5 <inline-formula><mml:math id="M57" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula>; SMAP L2 hereafter) product was used (O'Neill et al., 2020; Chan   et al., 2018). The product is derived from SMAP Level-1B (L1B) interpolated antenna temperatures using the Backus–Gilbert optimal interpolation technique. Both ascending and descending tracks were collected.</p></list-item><list-item>
      <p id="d1e888">The Metop ASCAT SSM Climate Data Record (CDR) H115 and its extension H116 are provided by the European Organization for the Exploitation of  Meteorological Satellites (EUMETSAT) Support to Operational Hydrology and Water Management (H SAF, 2021). The SSM is retrieved from <inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, using a change detection algorithm (Wagner et al., 2013), and is characterized by a spatial sampling of 12.5 <inline-formula><mml:math id="M59" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> and a temporal resolution of one to two observations per day, depending on the latitude.</p></list-item><list-item>
      <p id="d1e911">The PROBA-V LAI is derived from the PROBA-V satellite mission (Francois et al., 2014; Dierckx et al., 2014) and provided by the Copernicus  Global Land Service (CGLS) programme (Copernicus Global Land Service Site, 2021). The CGLS product at   1 <inline-formula><mml:math id="M60" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> spatial resolution and 10 d temporal resolution is developed based on the work by Verger et al. (2014).</p></list-item></list></p>
      <p id="d1e923">In order to compare Noah-MP simulations and reference data at the same spatial resolution, Sentinel-1 observations (<inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VV and <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VH) and ASCAT SSM, SMAP L2 SSM, and PROBA-V LAI were extracted over the study domain (44<inline-formula><mml:math id="M63" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 10.5<inline-formula><mml:math id="M64" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W – bottom left; 45.5<inline-formula><mml:math id="M65" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 12.2<inline-formula><mml:math id="M66" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W – top right) and regridded over the LIS grid domain (0.01<inline-formula><mml:math id="M67" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>) using the nearest neighbour approach.</p>
</sec>
<?pagebreak page6288?><sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Land surface and irrigation modelling</title>
<sec id="Ch1.S2.SS3.SSS1">
  <label>2.3.1</label><title>Noah-MP v.3.6</title>
      <p id="d1e1009">The analysis was carried out using the Noah-MP (Niu et al., 2011) LSM, running within NASA's LIS version 7.2 (Kumar et al., 2008). LIS is a software
framework for terrestrial hydrology modelling and DA, which supports different LSMs that can be conditioned on multiple remote sensing products from active and/or passive microwave sensors. The Noah-MP LSM, which was chosen for this study, is an evolution of the baseline Noah LSM (Mahrt and Ek, 1984; Chen et al., 1996; Chen and Dudhia, 2001), where the main improvements and augmentations are
(1) the presence of four soil layers, (2) up to three snow layers, (3) one canopy layer, which allows us to dynamically simulate the vegetation and to
compute separately the ground surface temperature, (4) a two-stream radiation transfer scheme based on the canopy layer sub-grid scheme, (5) a
Ball–Berry-type stomatal resistance scheme, and, (6) finally, a simple groundwater model with a TOPMODEL-based runoff scheme (Niu et al.,
2005, 2007). The model was set up by selecting four soil layers at depths of 0–10, 10–40, 40–100, and
100–200 <inline-formula><mml:math id="M68" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula>, a dynamic vegetation model with a Ball–Berry-type canopy stomatal resistance model (Ball et al., 1987), and TOPMODEL-based
runoff.</p>
      <p id="d1e1020">The parameterization followed the recommended options provided in the LIS documentation
(<uri>https://lis.gsfc.nasa.gov/documentation/lis</uri>, last access: 30 November 2021). A model
time step of 15 min and a 6 h output interval were selected, together with a spatial resolution of 0.01<inline-formula><mml:math id="M69" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. The meteorological forcings used
for running Noah-MP LSM were obtained from MERRA-2 (Gelaro et al. 2017). The MERRA-2 original spatial resolution of 0.5<inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M71" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.625<inline-formula><mml:math id="M72" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> was remapped to 0.01<inline-formula><mml:math id="M73" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> through bilinear interpolation. Land model data and parameters were preprocessed and adapted to the LIS longitude/latitude projection using the Land Surface Data Toolkit (LDT; Arsenault et al., 2018) in order to run Noah-MP at the chosen spatial resolution.</p>
      <p id="d1e1070">For this study, the default LIS land cover (LC) map from the University of Maryland (UMD) global land cover product (Hansen et al., 2000), based on the
Advanced Very High Resolution Radiometer (AVHRR) data, was replaced with the 2015 global LC map, available from the CGLS at 100 <inline-formula><mml:math id="M74" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> spatial
resolution (Buchhorn et al., 2020; available at <uri>https://land.copernicus.eu/global/products/lc</uri>,
last access: 20 May 2021). The CGLS provides dynamic land cover layers at 100 <inline-formula><mml:math id="M75" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> spatial resolution (CGLS-LC100), obtained by combining
information derived from the vegetation instrument on board the PROBA-V satellite, a database of high-quality LC reference sites, and several
ancillary data sets. For a more detailed explanation of the LC maps generation process we refer to the Algorithm Theoretical Basis Document (ATBD; Buchorn et al., 2020). The 23 classes of the PROBA-V LC map were reclassified to the 14 classes used<?pagebreak page6289?> in the UMD-AVHRR classification supported by LIS. Additionally, the LC map was regridded at 0.01<inline-formula><mml:math id="M76" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (Fig. 2a) by identifying the most representative class over each LIS grid cell. For
additional information on the reclassification process, we refer the reader to Table S1 in the Supplement. Similarly, the default Food and Agriculture Organization (FAO) Soil Map (FAO, 1971) was replaced by the Harmonized Soil World Database (HWSD v1.21; 1 <inline-formula><mml:math id="M77" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula>; Fig. 2b) and mapped to five soil classes over the study region. Other model preprocessed parameters inputs were (1) the Shuttle Radar Topography Mission elevation data (SRTM30;
30 <inline-formula><mml:math id="M78" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> spatial resolution); (2) the climatological global Greenness Vegetation Fraction (GVF) data (0.144<inline-formula><mml:math id="M79" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>; Gutman and Ignatov, 1998),
derived from 5 years (1985–1989) of normalized difference vegetation index (NDVI) data from the AVHRR (Miller et al., 2006), (3) a snow-free
albedo and a Noah-specific maximum snow albedo product from NCEP (National Centers for Environmental Prediction; original resolution 1<inline-formula><mml:math id="M80" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and regridded), and, finally, (4) soil, vegetation, and other general parameter tables for Noah-MP from the official LIS Data Portal (<uri>https://portal.nccs.nasa.gov/lisdata_pub/data/</uri>, last access:
20 May 2021).</p>
</sec>
<sec id="Ch1.S2.SS3.SSS2">
  <label>2.3.2</label><title>Irrigation modelling</title>
      <p id="d1e1147">The ability of Noah-MP to dynamically simulate the vegetation and the option to activate irrigation are particularly important when considering an
extensively irrigated area such as the Po Valley. Indeed, in a recent study by Nie et al. (2018), Noah-MP was coupled with a sprinkler
irrigation scheme (Ozdogan et al., 2010; where irrigation is applied as supplementary rainfall), which requires the following three pieces of information:
<list list-type="bullet"><list-item>
      <p id="d1e1152">The irrigation location, which only occurs over potentially irrigated croplands (expanding over grassland if the intensity exceeds the grid cell's total crop fraction). This information is extracted from a LC map associated with an additional data set providing information on the percent of irrigated area per grid cell. In this study, the reclassified PROBA-V LC map was coupled with the information contained in the 500 <inline-formula><mml:math id="M81" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> global rain-fed, irrigated, and paddy croplands data set (GRIPC; Salmon et al., 2015).</p></list-item><list-item>
      <p id="d1e1164">The timing of irrigation, which is determined by checking the start and end of the growing season, based on a GVF threshold, separately at each grid cell. Following Ozdogan et al. (2010), we set this threshold to 40 % of the GVF.</p></list-item><list-item>
      <p id="d1e1168">The amount of water which is used for irrigation. This quantity is derived from the root zone soil moisture (RZSM) availability (MA) as   <inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:mtext>MA</mml:mtext><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>=</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>(</mml:mo><mml:mtext>RZSM</mml:mtext><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>-</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SM</mml:mi><mml:mi mathvariant="normal">WP</mml:mi></mml:msub></mml:mrow><mml:mo>)</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>/</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>(</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SM</mml:mi><mml:mi mathvariant="normal">FC</mml:mi></mml:msub></mml:mrow><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>-</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SM</mml:mi><mml:mi mathvariant="normal">WP</mml:mi></mml:msub></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, where RZSM is the current RZSM, <inline-formula><mml:math id="M83" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SM</mml:mi><mml:mi mathvariant="normal">WP</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the wilting point, and <inline-formula><mml:math id="M84" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SM</mml:mi><mml:mi mathvariant="normal">FC</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the field capacity. When the MA falls below a user-defined threshold, irrigation is triggered, and the quantity is defined by calculating the amount of irrigation needed to raise the RZSM to the <inline-formula><mml:math id="M85" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SM</mml:mi><mml:mi mathvariant="normal">FC</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. For this study, the MA threshold was defined as the 50 % of <inline-formula><mml:math id="M86" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SM</mml:mi><mml:mi mathvariant="normal">FC</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> as in Ozdogan et al. (2010). MA is calculated at each time step, but the irrigation is only applied between 06:00 and 10:00 LT. Following Ozdogan et al. (2010), this time frame is typically chosen by farmers to reduce evaporative losses. In this context, the maximum rooting depth becomes a crucial information to compute the amount of irrigation water. This information is related to an assigned crop type, cultivated over the study area, through a maximum rooting depth table. Considering the high crop variability over the Po Valley and the lack of high-resolution dynamic crop maps for the entire study area, a generic crop type with 1 <inline-formula><mml:math id="M87" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> root depth was selected for the irrigation simulations. The reference rooting depth was verified to be feasible over the study area, based on the European Soil Data Centre (ESDAC; available at   <uri>https://esdac.jrc.ec.europa.eu/content/european-soil-database-derived-data</uri>, last access: 20 May 2021) rooting depths map (Fig. S1 in the   Supplement).</p></list-item></list></p>
</sec>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Water Cloud Model</title>
      <p id="d1e1289">The WCM allows us to simulate the top-of-vegetation <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> as a function of SSM and vegetation, using empirical fitting parameters. <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> is modelled as the sum of the backscatter from the vegetation (<inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>veg</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>; in decibels, hereafter dB) and from the bare soil (<inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>soil</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>; in dB), attenuated by the <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:msup><mml:mi>t</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> coefficient that describes the two-way attenuation from the vegetation layer. Scattering interactions between the ground and the vegetation are not accounted for. As reported in Baghdadi et al. (2017), for a given
polarization pq (i.e. VV and VH), the WCM can be written as follows:
            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M93" display="block"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>pq</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup><mml:mo>=</mml:mo><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>veg</mml:mtext><mml:mo>,</mml:mo><mml:mtext>pq</mml:mtext></mml:mrow><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>t</mml:mi><mml:mtext>pq</mml:mtext><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>soil</mml:mtext><mml:mo>,</mml:mo><mml:mtext>pq</mml:mtext></mml:mrow><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where, in the following,

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M94" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E2"><mml:mtd><mml:mtext>2</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>veg</mml:mtext><mml:mo>,</mml:mo><mml:mtext>pq</mml:mtext></mml:mrow><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi>A</mml:mi><mml:mtext>pq</mml:mtext></mml:msub><mml:msub><mml:mi>V</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mi>cos⁡</mml:mi><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msubsup><mml:mi>t</mml:mi><mml:mtext>pq</mml:mtext><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E3"><mml:mtd><mml:mtext>3</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msubsup><mml:mi>t</mml:mi><mml:mtext>pq</mml:mtext><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>=</mml:mo><mml:mi>exp⁡</mml:mi><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi>B</mml:mi><mml:mtext>pq</mml:mtext></mml:msub><mml:msub><mml:mi>V</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mrow><mml:mi>cos⁡</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E4"><mml:mtd><mml:mtext>4</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>soil</mml:mtext><mml:mo>,</mml:mo><mml:mtext>pq</mml:mtext></mml:mrow><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mtext>pq</mml:mtext></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>D</mml:mi><mml:mtext>pq</mml:mtext></mml:msub><mml:mo>⋅</mml:mo><mml:mtext>SSM</mml:mtext><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula></p>
      <p id="d1e1544">Equations (2) and (3) describe the vegetation-related terms. <inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M96" display="inline"><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> represent two bulk vegetation descriptors, with the first one accounting for the direct vegetation <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and the second one representing the attenuation. <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mtext>pq</mml:mtext></mml:msub><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>(</mml:mo><mml:mo>-</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:msub><mml:mi>B</mml:mi><mml:mtext>pq</mml:mtext></mml:msub><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>(</mml:mo><mml:mo>-</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> are the two related fitting parameters. Common vegetation descriptors used in previous studies are the vegetation water content (VWC; Paloscia et al., 2013), the NDVI<?pagebreak page6290?> (El Hajj et al., 2016; Li and Wang, 2018), and LAI (K. Kumar et al., 2015; Bai and He, 2015), while <inline-formula><mml:math id="M100" display="inline"><mml:mi mathvariant="italic">θ</mml:mi></mml:math></inline-formula> represents the incidence angle, which is assumed to be 37<inline-formula><mml:math id="M101" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> for Sentinel-1. Following previous studies (see Lievens et al., 2017b; Baghdadi et al. 2017; Li and Wang, 2018), we assumed <inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>V</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> represented by the dynamically simulated LAI vegetation descriptor.</p>
      <p id="d1e1651">Equation (4) describes the soil-related term. Following the work by Lievens et al. (2017b), the <inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>soil</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula> can be described, in a simple linear approach, as a function of the SSM. There are several semi-empirical models (e.g. the Oh model; Oh et al., 1992) or theoretical models (e.g. the Integral Equation Model – IEM; Fung, 1994), which describe the scattering processes related to the bare soil, but their application as a forward operator coupled to a LSM has two main limitations. The first one lies in the difficulty in retrieving soil roughness values over extended reference areas required to parameterize these models. The second one is their saturation of <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> in moist conditions, which causes low variability in simulated <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> if the LSM soil moisture simulations are biased wet (for more information, see Lievens et al., 2017b). Those limitations justify the use of a linear fitted  approach. In Eq. (4), the <inline-formula><mml:math id="M106" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M107" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> parameters (here fitted in <inline-formula><mml:math id="M108" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">dB</mml:mi></mml:mrow></mml:math></inline-formula> and decibels per cubic metre per cubic metre, <inline-formula><mml:math id="M109" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">dB</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, respectively, but <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>soil</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula> is transformed back to the linear scale in Eq. 1) describe the linear relation between <inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>soil</mml:mtext><mml:mo>,</mml:mo><mml:mtext>pq</mml:mtext></mml:mrow><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula> and SSM. Those parameters, together with <inline-formula><mml:math id="M112" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M113" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula> (–), need to be calibrated separately for each polarization.</p>
</sec>
<sec id="Ch1.S2.SS5">
  <label>2.5</label><title>Calibration algorithms</title>
      <p id="d1e1792">We considered the following two different objective functions to optimize the <inline-formula><mml:math id="M114" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M115" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M116" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M117" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> parameters:
<list list-type="bullet"><list-item>
      <p id="d1e1825">A Bayesian solution, which minimizes the sum of squared errors (SSEs) between <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> observations from Sentinel-1 and WCM simulations. The SSE Bayesian calibration solution aims at identifying the optimal parameter vector <inline-formula><mml:math id="M119" display="inline"><mml:mi mathvariant="bold-italic">α</mml:mi></mml:math></inline-formula>, which maximizes the probability of the resulting <inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations <inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:msup><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>-</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:msup><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>-</mml:mo></mml:msup><mml:mi mathvariant="normal">|</mml:mi><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mo>)</mml:mo><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the prior parameter distribution and <inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:msup><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>-</mml:mo></mml:msup><mml:mi mathvariant="normal">|</mml:mi><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the likelihood. Starting from the assumption of an independent and identically distributed normal error model, the posterior probability can be maximized by maximizing the following:<disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M124" display="block"><mml:mtable class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mi>p</mml:mi></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>(</mml:mo><mml:msup><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>-</mml:mo></mml:msup><mml:mi mathvariant="normal">|</mml:mi><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mo>)</mml:mo><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msubsup><mml:mo>∏</mml:mo><mml:mi>i</mml:mi><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:msubsup><mml:mfenced close="}" open="{"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:msub><mml:mi>s</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msqrt><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">π</mml:mi></mml:mrow></mml:msqrt></mml:mrow></mml:mfrac></mml:mstyle><mml:mi>exp⁡</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>-</mml:mo><mml:msup><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>-</mml:mo></mml:msup><mml:msubsup><mml:mo>)</mml:mo><mml:mi>i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:msubsup><mml:mi>s</mml:mi><mml:mi>i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>⋅</mml:mo><mml:msubsup><mml:mo>∏</mml:mo><mml:mi>j</mml:mi><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="bold-italic">α</mml:mi></mml:msub></mml:mrow></mml:msubsup><mml:mfenced open="{" close="}"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:msub><mml:mi>s</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:msqrt><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">π</mml:mi></mml:mrow></mml:msqrt></mml:mrow></mml:mfrac></mml:mstyle><mml:mi>exp⁡</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:mi mathvariant="bold-italic">α</mml:mi><mml:msubsup><mml:mo>)</mml:mo><mml:mi>j</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:msubsup><mml:mi>s</mml:mi><mml:mi>j</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>i.e. the combination of the likelihood and a prior parameter constraint. The latter helps in reducing problems of equifinality. In Eq. (<xref ref-type="disp-formula" rid="Ch1.E5"/>),
<inline-formula><mml:math id="M125" display="inline"><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover></mml:math></inline-formula> represents the observed <inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:msup><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> is the simulated <inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M129" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> is the time step, and <inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:msub><mml:mi>s</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the standard deviation of the residual differences between the observed and simulated <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> values for <inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> time steps. <inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="bold-italic">α</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the number of parameters to be calibrated, <inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the prior parameter constraint, and the parameter deviation is limited by <inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:msubsup><mml:mi>s</mml:mi><mml:mi>j</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>, which is the variance of a uniform distribution <inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:msubsup><mml:mi>s</mml:mi><mml:mi>j</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mrow><mml:mo>max⁡</mml:mo><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mrow><mml:mo>min⁡</mml:mo><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>/</mml:mo><mml:mn mathvariant="normal">12</mml:mn></mml:mrow></mml:math></inline-formula>, with determined boundaries of the parameters [<inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mo>min⁡</mml:mo></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>]. The maximum likelihood solution is found by minimizing the following cost function <inline-formula><mml:math id="M138" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>:<disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M139" display="block"><mml:mtable rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mi>J</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msubsup><mml:mo>∑</mml:mo><mml:mi>i</mml:mi><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:msubsup><mml:mfenced close="}" open="{"><mml:mrow><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>s</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>-</mml:mo><mml:msup><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>-</mml:mo></mml:msup><mml:msubsup><mml:mo>)</mml:mo><mml:mi>i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:msubsup><mml:mi>s</mml:mi><mml:mi>i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:msubsup><mml:mo>∑</mml:mo><mml:mi>j</mml:mi><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="bold-italic">α</mml:mi></mml:msub></mml:mrow></mml:msubsup><mml:mfenced close="}" open="{"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:mi mathvariant="bold-italic">α</mml:mi><mml:msubsup><mml:mo>)</mml:mo><mml:mi>j</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:msubsup><mml:mi>s</mml:mi><mml:mi>j</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>=</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="bold-italic">α</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>where <inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:msub><mml:mi>s</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is assumed to be constant in time and represented by a target accuracy of 1 <inline-formula><mml:math id="M141" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">dB</mml:mi></mml:mrow></mml:math></inline-formula>, leaving the SSEs in the first term of <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to
minimize. The second term (<inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="bold-italic">α</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) constrains the optimal solution by avoiding strong deviations from initial parameter guesses.</p></list-item><list-item>
      <p id="d1e2520">A solution that maximizes the Kling–Gupta efficiency (KGE; Gupta et al., 2009). Even though this objective function does not ensure Bayesian optimality, it is a widely used metric which could help to better tune the dynamic <inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> behaviour, as follows:<disp-formula id="Ch1.E7" content-type="numbered"><label>7</label><mml:math id="M145" display="block"><mml:mtable class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mtext>KGE</mml:mtext></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{8.5}{8.5}\selectfont$\displaystyle}?><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msqrt><mml:mrow><mml:mo>(</mml:mo><mml:mi>r</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>〈</mml:mo><mml:msup><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>-</mml:mo></mml:msup><mml:mo>〉</mml:mo></mml:mrow><mml:mrow><mml:mo>〈</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>〉</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>s</mml:mi><mml:mo>[</mml:mo><mml:msup><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>-</mml:mo></mml:msup><mml:mo>]</mml:mo><mml:mo>/</mml:mo><mml:mo>〈</mml:mo><mml:msup><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>-</mml:mo></mml:msup><mml:mo>〉</mml:mo></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mo>[</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>]</mml:mo><mml:mo>/</mml:mo><mml:mo>〈</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>〉</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt><?xmltex \hack{$\egroup}?><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p>
      <p id="d1e2674">The KGE formulation embeds three terms. (1) The first term accounts for the Pearson correlation (Pearson <inline-formula><mml:math id="M146" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>) between the observed
(<inline-formula><mml:math id="M147" display="inline"><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover></mml:math></inline-formula>) and simulated (<inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:msup><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> time series. (2) A second term accounts for the bias, where the long-term mean is represented
as <inline-formula><mml:math id="M150" display="inline"><mml:mo>〈</mml:mo></mml:math></inline-formula>.<inline-formula><mml:math id="M151" display="inline"><mml:mo>〉</mml:mo></mml:math></inline-formula>. Finally, (3) there is a term accounting for the variability in the simulated and observed signal through the use of the
standard deviation <inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:mi>s</mml:mi><mml:mo>[</mml:mo><mml:mo>.</mml:mo><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>. KGE <inline-formula><mml:math id="M153" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1 indicates a perfect agreement between simulations and observations. Note that KGE
redistributes the weight of the bias, variance, and correlation components compared to <inline-formula><mml:math id="M154" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> in Eq. (6), which can help in reducing differences between
simulated and observed <inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, and also in terms of temporal dynamics, during the calibration. On the other hand, in the KGE, cost function parameters are not constrained by prior values <inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">α</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. This could possibly result in overfitting and a larger prediction uncertainty.</p></list-item></list></p>
      <p id="d1e2784">The particle swarm optimization (PSO; Kennedy and Eberhart, 1995) was used to minimize <inline-formula><mml:math id="M157" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> and maximize KGE. For our case study, the PSO
parameters were set as in De Lannoy et al. (2013).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e2796">Flow chart of the experimental set-up used in this study to calibrate the WCM <inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> signal. A natural and an irrigation experimental line was performed coupling either Noah-MP natural or irrigation simulations with the WCM. For each experimental line, <inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations are driven by the Sentinel-1 signal using two different cost functions (<inline-formula><mml:math id="M160" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> and KGE) in order to provide eight different calibration experiments.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://hess.copernicus.org/articles/25/6283/2021/hess-25-6283-2021-f03.png"/>

        </fig>

</sec>
<?pagebreak page6291?><sec id="Ch1.S2.SS6">
  <label>2.6</label><title>Experimental set-up</title>
      <p id="d1e2842">An optimal DA system requires long-term unbiased <inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations (with respect to the assimilated observations). The risk, over an
intensively irrigated area, is that an unmodelled irrigation signal would manifest itself as a predominant bias in the <inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations. The
calibration would then inadvertently correct for this supposed bias (i.e. the irrigation signal), thus preventing the DA system from propagating the
missing irrigation signal from the observations into the model. Even though existing irrigation schemes are evidently unrealistic and inaccurate, we
conjecture that using such a scheme when calibrating the WCM will more likely yield optimal WCM parameters than when neglecting irrigation.</p>
      <p id="d1e2867">To that end, we considered two different experiment lines (referred to as <italic>natural</italic> and <italic>irrigation</italic>, respectively) that produced a total of eight different <inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulation runs (see Fig. 3). The natural experiment line differs from the irrigation line by
the activation of an irrigation module in Noah-MP, and both are subjected to the calibration algorithms described in Sect. 2.5. The natural
line was used as a diagnostic experiment against which to compare irrigation, which, according to our initial hypothesis, should minimize the
impact of the irrigation signal contained in the <inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> observations on WCM parameters.</p>
      <p id="d1e2898">As a first step, a model spin up was performed, starting in January 1982 and ending in December 2014. Then, a study period from January 2015 to December 2019 was selected for the different model runs, based on the availability of the processed Sentinel-1 <inline-formula><mml:math id="M165" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and reference irrigation
data (see Sect. 2.1 and 2.2). Daily surface model and irrigation outputs were produced. Considering that the main source of irrigation in the Po Valley is related to surface water abstraction, the sprinkler irrigation scheme did not account for groundwater withdrawals (see Nie et al., 2018).</p>
      <p id="d1e2912">The <inline-formula><mml:math id="M166" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M167" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M168" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M169" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> parameters of the WCM (see Sect. 2.4) were fitted separately to Sentinel-1 <inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VV and <inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VH observations during the
period of January 2017– December 2019. Following previous literature (Lievens et al., 2017b; De Lannoy et al., 2014, 2013), we performed a grid-cell-based calibration to account for the spatial variability in the simulated and observed <inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> signals that stems from specific features
within the observed footprints and from the soil and vegetation parameterization of Noah-MP. Both the calibration using the SSEs with prior
constraint (Bayesian <inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:mi>J</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and the KGE were applied to the natural and irrigation runs, providing eight different experiments named
<inline-formula><mml:math id="M174" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV natural, <inline-formula><mml:math id="M175" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VH natural, <inline-formula><mml:math id="M176" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV irrigation, <inline-formula><mml:math id="M177" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VH irrigation, KGE-VV natural, KGE-VH natural, KGE-VV irrigation, and KGE-VH irrigation.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e3020">Lower boundaries (LB), upper boundaries (UB), and prior guess values of the WCM parameters for both VV and VH polarization.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="9">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">A-VV</oasis:entry>
         <oasis:entry colname="col3">A-VH</oasis:entry>
         <oasis:entry colname="col4">B-VV</oasis:entry>
         <oasis:entry colname="col5">B-VH</oasis:entry>
         <oasis:entry colname="col6">C-VV</oasis:entry>
         <oasis:entry colname="col7">C-VH</oasis:entry>
         <oasis:entry colname="col8">D-VV</oasis:entry>
         <oasis:entry colname="col9">D-VH</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(–)</oasis:entry>
         <oasis:entry colname="col3">(–)</oasis:entry>
         <oasis:entry colname="col4">(–)</oasis:entry>
         <oasis:entry colname="col5">(–)</oasis:entry>
         <oasis:entry colname="col6">(<inline-formula><mml:math id="M178" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">dB</mml:mi></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col7">(<inline-formula><mml:math id="M179" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">dB</mml:mi></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col8">(<inline-formula><mml:math id="M180" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">dB</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col9">(<inline-formula><mml:math id="M181" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">dB</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">UB</oasis:entry>
         <oasis:entry colname="col2">0.4</oasis:entry>
         <oasis:entry colname="col3">0.4</oasis:entry>
         <oasis:entry colname="col4">0.4</oasis:entry>
         <oasis:entry colname="col5">0.4</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M182" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M183" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10</oasis:entry>
         <oasis:entry colname="col8">80</oasis:entry>
         <oasis:entry colname="col9">80</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">LB</oasis:entry>
         <oasis:entry colname="col2">0</oasis:entry>
         <oasis:entry colname="col3">0</oasis:entry>
         <oasis:entry colname="col4">0</oasis:entry>
         <oasis:entry colname="col5">0</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M184" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>35</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M185" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>35</oasis:entry>
         <oasis:entry colname="col8">15</oasis:entry>
         <oasis:entry colname="col9">15</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Guess</oasis:entry>
         <oasis:entry colname="col2">0</oasis:entry>
         <oasis:entry colname="col3">0</oasis:entry>
         <oasis:entry colname="col4">0</oasis:entry>
         <oasis:entry colname="col5">0</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M186" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>20</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M187" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>30</oasis:entry>
         <oasis:entry colname="col8">40</oasis:entry>
         <oasis:entry colname="col9">40</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e3311">Lower and upper boundaries and prior guess values of the WCM parameters were defined based on the work of Lievens et al. (2017b) and on a
sensitivity analysis (not shown here). The selected values are displayed in Table 1. Finally, it should be noted that all the calibration experiments
were realized by considering daily values of <inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations and observations.</p>
</sec>
<?pagebreak page6292?><sec id="Ch1.S2.SS7">
  <label>2.7</label><title>Noah-MP LSM and WCM evaluations</title>
      <p id="d1e3333">The validation aims at (i) evaluating the performance of Noah-MP in simulating irrigation, soil moisture, and vegetation, and the ability of the WCM to simulate radar <inline-formula><mml:math id="M189" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, and (ii) unveiling the information about irrigation contained in Sentinel-1 radar <inline-formula><mml:math id="M190" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> in order to assess its
potential to improve both soil moisture and vegetation representation within Noah-MP.</p>
      <p id="d1e3358">The evaluation was carried out on both the regional scale (i.e. over the entire study area) and on the two selected sites, Faenza (small district
scale) and Budrio (plot scale), where irrigation data were available. Considering the lack of benchmark data for irrigation evaluation (Foster et al.,
2020), we decided to use in situ data for the small Budrio fields spatial scale (i.e.
0.45–049 <inline-formula><mml:math id="M191" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ha</mml:mi></mml:mrow></mml:math></inline-formula>), even though model simulations are made at a much coarser resolution (i.e. <inline-formula><mml:math id="M192" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 1 <inline-formula><mml:math id="M193" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula>). We are aware that differences in the spatial scale can increase the uncertainty of our evaluation, but the 0.01<inline-formula><mml:math id="M194" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> LSM spatial resolution is still a good compromise for an analysis at the regional, small district, and plot scale. Additionally, limitations are partly reduced by the low chance of including non-irrigated fields within the 1 <inline-formula><mml:math id="M195" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> LIS grid cells within the Po Valley, as the latter is almost entirely irrigated (Salmon et al., 2015). We compared Noah-MP (with and without using the irrigation module) SSM and LAI simulations with satellite SSM from ASCAT and SMAP and LAI from PROBA-V, respectively, during the period 2015–2019. Furthermore, these land surface simulations were compared to Sentinel-1 <inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> to understand how much of the SSM and LAI signal was captured by Sentinel-1.</p>
      <p id="d1e3413">As the irrigation timing is often driven by the stakeholders' turns to withdraw water and by water availability rather than by the conditions of the
soil and crops themselves, the comparisons between simulated SSM and satellite SSM were carried out by aggregating the two variables over a biweekly time window. On the other hand, the LAI from Noah-MP was aggregated to 10 daily values in order to match the PROBA-V LAI values. We used the Pearson <inline-formula><mml:math id="M197" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> for SSM and LAI evaluation. For SSM, we also computed the root mean square error (RMSE), calculated considering the original temporal
resolution of the satellite products, while for LAI, we also tested the ratio bias, i.e. the ratio between the long-term mean of the simulations and
the long-term mean of observations. In particular, this additional score for LAI was used to provide a further evaluation of the ability of the
Noah-MP to simulate crop phenology during the irrigated vs. non-irrigated periods so as to not rely solely on the evaluation of temporal dynamics,
which, due to the uncertainty in the Noah-MP crop type parameterization, could be affected by time shifts in the LAI climatology. This
parameterization uncertainty comes from the lack of knowledge of the spatial crop type information and is difficult to reduce without additional
information. Our assumption is that the radar <inline-formula><mml:math id="M198" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> assimilation can also correct for this with future data assimilation.</p>
      <p id="d1e3434">Following Vreugdenhil et al. (2018) and Vreugdenhil et al. (2020), Noah-MP LAI and PROBA-V LAI were also compared with the Sentinel-1
<inline-formula><mml:math id="M199" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mtext>VH</mml:mtext><mml:mo>/</mml:mo><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mtext>VV</mml:mtext></mml:mrow></mml:math></inline-formula> cross ratio (CR), which was demonstrated to have a high agreement with the vegetation signal. Though the
<inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mtext>VH</mml:mtext></mml:mrow></mml:math></inline-formula> was demonstrated to increase with the vegetation signal (Macelloni et al., 2001), the CR will be more sensitive to vegetation
changes as the ratio is less sensitive to changes in soil moisture and soil–vegetation interaction (Veloso et al., 2017; Vreugdenhil et al., 2020).</p>
      <p id="d1e3476">To evaluate WCM simulations, we used biweekly values of <inline-formula><mml:math id="M201" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations and observations considering a 2-year period independent from the
calibration period (i.e. 2015–2016). Statistical metrics, such as grid-based temporal Pearson <inline-formula><mml:math id="M202" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>, KGE, and bias, were calculated between Sentinel-1
<inline-formula><mml:math id="M203" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and calibrated WCM simulations. The analysis of the parameters was restricted to the cropland area as no difference between our
experiment lines exists over other land cover types (i.e. the irrigation module is active only over grid points classified as crop).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e3510">Maps of temporal Pearson <inline-formula><mml:math id="M204" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> between biweekly values of SSM from Noah-MP and satellite retrievals. <bold>(a)</bold> Natural run and SMAP L2. <bold>(b)</bold> Irrigation run and SMAP L2. <bold>(d)</bold> Natural run and ASCAT. <bold>(e)</bold> Irrigation run and ASCAT. Maps of the Pearson <inline-formula><mml:math id="M205" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> differences display the grid-based difference between <bold>(c)</bold> map <bold>b</bold> and map <bold>a</bold> and <bold>(f)</bold> map <bold>e</bold> and map <bold>d</bold>. The reference period is April 2015–December 2019.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://hess.copernicus.org/articles/25/6283/2021/hess-25-6283-2021-f04.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Noah MP regional evaluation</title>
      <p id="d1e3581">Figure 4 shows maps of the Pearson <inline-formula><mml:math id="M206" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> between biweekly Noah-MP SSM natural and irrigation simulations and biweekly ASCAT and SMAP L2 SSM retrievals, respectively, for April 2015 to December 2019. The Noah-MP SSM irrigation run provides a higher agreement with both satellite SSM data sets compared to the natural run. Indeed, the median Pearson <inline-formula><mml:math id="M207" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> between SMAP L2 SSM and Noah-MP SSM increases from 0.68 to 0.73, for the natural run (Fig. 4a) and the irrigation run (Fig. 4b), respectively. A similar improvement can be observed considering the ASCAT reference SSM, with an improvement in the median Pearson <inline-formula><mml:math id="M208" display="inline"><mml:mi>R<?pagebreak page6293?></mml:mi></mml:math></inline-formula> of 0.08 when irrigation is activated in the model (from 0.7 to 0.78; Fig. 4e). Areas characterized by higher correlation when irrigation is simulated are represented in blue in the Pearson correlation difference map of Fig. 4f (obtained by subtracting the map in Fig. 4d from the map in Fig. 4e). Almost all cropland areas are characterized by a higher agreement between observations and simulations for the irrigation run. Note that, for the evaluation of Noah-MP against SMAP, we relaxed the retrieval
quality flags, which would otherwise mask out almost the entire study area. Figure S2 in the Supplement shows the coverage when using the recommended quality flags. The results in Fig. 4 were confirmed by analysing the RMSE between satellite SSM products and Noah-MP simulations for both the natural and irrigation runs, after rescaling them based on their mean and standard deviation, because SSM retrievals and SSM simulations do not have the same units. The results are displayed in Fig. S3 and show, for both the satellite
products, a general reduction in RMSE when compared with the irrigation run. An improvement in performances can be observed over the entire
cropland area, in particular over the central triangle feature where a  sandy loam soil texture is present and where, consequently, more irrigation is
simulated in the model due to the higher permeability of the soil.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e3607">Maps of temporal Pearson <inline-formula><mml:math id="M209" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> between 10 d LAI values from PROBA-V LAI and Noah-MP LAI. <bold>(a)</bold> Natural run. <bold>(b)</bold> Irrigation run. Map of Pearson <inline-formula><mml:math id="M210" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> differences between <bold>(c)</bold> map <bold>b</bold> and map <bold>a</bold>. Map of the ratio bias of LAI from PROBA-V and Noah-MP, showing the <bold>(d)</bold> natural run and <bold>(e)</bold> irrigation run. Additional histogram distributions from <bold>(f)</bold> map <bold>d</bold> and map <bold>e</bold>. The reference period is January 2015–October 2019.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://hess.copernicus.org/articles/25/6283/2021/hess-25-6283-2021-f05.png"/>

        </fig>

      <p id="d1e3662">The evaluation of the LAI simulation was limited to the regional-scale analysis due to a lack of in situ vegetation data over the selected test
sites. The comparison between the 10 d values of Noah-MP LAI, from both model runs, and the PROBA-V LAI product was carried out over the reference period of January 2015 to October 2019, using the temporal Pearson <inline-formula><mml:math id="M211" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> and the ratio bias, as shown in Fig. 5.</p>
      <p id="d1e3673">Figure 5a and b show that the Pearson <inline-formula><mml:math id="M212" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> for vegetation has a lower median value of 0.67 when irrigation is simulated in
Noah-MP, whereas this value equals 0.72 for the natural run. The difference between the two Pearson <inline-formula><mml:math id="M213" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> maps is shown in Fig. 5c, providing
evidence of the areas facing a deterioration of the performance in terms of Pearson <inline-formula><mml:math id="M214" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> related to the irrigation run. This deterioration is
particularly strong over cropland areas south of the Po river (red), while the northern area also shows grid cells where the performance
improves (blue)<inline-formula><mml:math id="M215" display="inline"><mml:mo>.</mml:mo></mml:math></inline-formula></p>
      <p id="d1e3703">In contrast, the ratio bias evaluation score (Fig. 5d–f) highlights an improvement in the long-term mean vegetation simulations when irrigation is
included (Fig. 5e). Here the optimal condition is represented by a ratio bias equal to 1 when the mean of the simulated LAI is equal to the mean of
the observed LAI. In this context, Fig. 5d displays ratio bias values lower than 1 over a large central triangle-shaped cropland area and a median
ratio bias value of 0.73, highlighting an underestimation of the LAI simulation related to the natural run. Conversely, Fig. 5e shows ratio
bias values close to 1 when irrigation is simulated over an extended cropland area and a median bias value of 0.99. The improvement given by the
irrigation run is emphasized in Fig. 5f, where the histograms of the ratio bias distributions related to both model runs show the higher
performance of the irrigation run (red) compared to the natural run (blue) for which the distribution is more skewed to the zero
value.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e3708"><bold>(a)</bold> Evaluation of SSM over the Budrio field 2, with (green) in situ PGR SM data, (light blue) SSM from Noah-MP natural and (orange) SSM from Noah-MP irrigation. Additional information is provided in panel <bold>(b)</bold>, with observed irrigation (green), simulated irrigation (orange), and observed rainfall (magenta) in millimetres per day (<inline-formula><mml:math id="M216" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">d</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>).</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://hess.copernicus.org/articles/25/6283/2021/hess-25-6283-2021-f06.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e3741">Sentinel-1 <inline-formula><mml:math id="M217" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VV and <inline-formula><mml:math id="M218" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VH data for the Budrio field 1 test site compared with Noah-MP SSM, for <bold>(a)</bold> natural and irrigation runs. Sentinel-1 CR (VH/VV) compared with PROBA-V LAI and Noah-MP LAI for <bold>(b)</bold> natural and irrigation runs. Also shown are the <bold>(c)</bold> observed irrigation (green) and simulated irrigation from Noah-MP (orange).</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://hess.copernicus.org/articles/25/6283/2021/hess-25-6283-2021-f07.png"/>

        </fig>

</sec>
<?pagebreak page6295?><sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Noah MP site evaluation</title>
      <p id="d1e3789">The Noah-MP SSM was evaluated at the Budrio test site field 2 (Fig. 1a), using the daily reference PGR SM for the year 2017. Comparisons between the
SSM simulations of the natural and irrigation runs with in situ PGR SM are shown in Fig. 6a, while daily observed irrigation and
rainfall data are compared with daily irrigation simulations in Fig. 6b. Soil moisture data are plotted at their original temporal resolution (i.e.
daily) to illustrate an issue related to the irrigation timing, namely that SSM simulations in Fig. 6a show the ability of the sprinkler irrigation scheme to simulate irrigation in the summer season, but there is an inevitable problem in reproducing the correct timing and magnitude of irrigation. Indeed, the total amount of simulated irrigation is 604 <inline-formula><mml:math id="M219" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> for the 2017 summer season, which overestimates the total amount of observed irrigation that is 349.5 <inline-formula><mml:math id="M220" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula>. Furthermore, the model simulations not only miss irrigation but also suffer from erroneous precipitation input, such as on the 11 July 2017, where the observed precipitation event in the growing season is not found in the model SSM simulations. In any case, biweekly Pearson <inline-formula><mml:math id="M221" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> between simulated SSM and in situ PGR SM are higher for the irrigation run than for the natural run (0.54 vs. 0.42), suggesting the benefit of activating irrigation.</p>
      <p id="d1e3815"><?xmltex \hack{\newpage}?>For the Budrio field 1 test site (Fig. 1a), two summer seasons of irrigation data were available. To assess the irrigation information contained in
Sentinel-1 <inline-formula><mml:math id="M222" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> observations (and the potential added value for a forthcoming DA experiment), we compared biweekly values of Sentinel-1
<inline-formula><mml:math id="M223" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VV and <inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VH with SSM estimates from both the natural run and irrigation run (Fig. 7a) for this site. Although the
<inline-formula><mml:math id="M225" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VV is generally used to retrieve SSM (Wagner et al., 2013; Gruber et al., 2013;
Bauer-Marschallinger et al., 2018), data at both polarizations were analysed in order to understand the soil contribution contained in the two
signals. Information related to the irrigation periods are shown in Fig. 7c, where irrigation observations and irrigation simulations from Noah-MP are
compared. Figure 7a indicates that the SSM simulations are better reflected in the Sentinel-1 <inline-formula><mml:math id="M226" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VV than <inline-formula><mml:math id="M227" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VH data, particularly
when irrigation is simulated (orange line). The SSM estimates from the natural run (light blue line) agree poorly with the Sentinel-1 data,
with Pearson <inline-formula><mml:math id="M228" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> values equal to 0.32 and <inline-formula><mml:math id="M229" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.1 for the <inline-formula><mml:math id="M230" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VV (blue dots) and <inline-formula><mml:math id="M231" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VH (cyan dots), respectively. When irrigation is
simulated, the <inline-formula><mml:math id="M232" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VV data better follow the modelled SSM signal (Pearson <inline-formula><mml:math id="M233" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> of 0.53), especially during the summer irrigation season when
the backscatter signal remains higher and stable. On the other hand, <inline-formula><mml:math id="M234" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VH seems to provide poor performances, also when irrigation is
simulated, with a Pearson <inline-formula><mml:math id="M235" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> value equal to 0.06, confirming findings by Baghdadi et al<?pagebreak page6296?>. (2017), which highlighted how the use of VH alone to retrieve
SSM is suboptimal when vegetation cover is well developed.</p>
      <p id="d1e3959">In Fig. 7b, the Sentinel-1 <inline-formula><mml:math id="M236" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> CR (VH/VV) is compared with Noah-MP LAI from the natural run (light-blue line) and
irrigation run (orange line). The performance in terms of Pearson <inline-formula><mml:math id="M237" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> decreases from 0.76 to 0.65 when the irrigation is simulated. This
is due to a time shift of the Noah-MP LAI growing season in the irrigation run. PROBA-V LAI (in green) was additionally compared with the
Sentinel-1 CR (blue dots), showing a Pearson <inline-formula><mml:math id="M238" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> of 0.84. The higher agreement between the RS products (Sentinel-1 and PROBA-V) highlights the strong relation between the <inline-formula><mml:math id="M239" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> CR and the vegetation signal, suggesting a potential benefit of the Sentinel-1 assimilation for correcting the simulated vegetation phenology.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e4001">Split violin distributions of the calibrated parameters over the entire study area for the eight calibration experiments. For both the natural (blue) and irrigation (orange) experiments, the distributions are shown for the <inline-formula><mml:math id="M240" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M241" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M242" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M243" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> parameters, <bold>(a–d)</bold> using the KGE objective function for VV polarization, <bold>(e–h)</bold> <inline-formula><mml:math id="M244" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> objective function for VV polarization, <bold>(i–l)</bold> KGE objective function for VH polarization, and <bold>(m–p)</bold> <inline-formula><mml:math id="M245" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> objective function for VH polarization. Note that the areas under the histograms on both left and right sides of the violins are automatically scaled for optimizing the visualization.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://hess.copernicus.org/articles/25/6283/2021/hess-25-6283-2021-f08.png"/>

        </fig>

      <p id="d1e4065">Finally, Fig. 7c shows a comparison between 15 <inline-formula><mml:math id="M246" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">d</mml:mi></mml:mrow></mml:math></inline-formula> accumulated millimetres of simulated irrigation (orange) and observed irrigation (green). The
Pearson <inline-formula><mml:math id="M247" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> is equal to 0.77, indicating that the sprinkler irrigation scheme can provide acceptable irrigation estimates at this temporal resolution
though absolute irrigation amounts are overestimated.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>WCM calibration</title>
      <p id="d1e4091">The WCM parameters <inline-formula><mml:math id="M248" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M249" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula> (vegetation parameters) and <inline-formula><mml:math id="M250" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M251" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> (soil parameters) were calibrated for each grid cell separately, during the
reference period of January 2017 to December 2019 (Fig. 3), using daily <inline-formula><mml:math id="M252" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations and observations. The calibrated parameters related to the entire study area for each of the eight experiments are shown in Fig. 8, where the blue (left) parts of the violin plots identify experiments of the
natural run, while the orange (right) parts of the violin plots are related to the irrigation run.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F9" specific-use="star"><?xmltex \currentcnt{9}?><?xmltex \def\figurename{Figure}?><label>Figure 9</label><caption><p id="d1e4135">Maps of the <bold>(a)</bold> <inline-formula><mml:math id="M253" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> parameter, <bold>(b)</bold> <inline-formula><mml:math id="M254" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula> parameter, <bold>(c)</bold> <inline-formula><mml:math id="M255" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> parameter, and <bold>(d)</bold> <inline-formula><mml:math id="M256" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> parameter for the <inline-formula><mml:math id="M257" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV natural calibration experiment. Maps of the <bold>(e)</bold> <inline-formula><mml:math id="M258" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> parameter, <bold>(f)</bold> <inline-formula><mml:math id="M259" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula> parameter, <bold>(g)</bold> <inline-formula><mml:math id="M260" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> parameter, and <bold>(h)</bold> <inline-formula><mml:math id="M261" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> parameter for the <inline-formula><mml:math id="M262" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV irrigation calibration experiment.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://hess.copernicus.org/articles/25/6283/2021/hess-25-6283-2021-f09.jpg"/>

        </fig>

      <p id="d1e4241">Generally, the <inline-formula><mml:math id="M263" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> calibration provides parameter distributions closer around their prior guess as compared to the KGE calibration for which
the distributions are often multimodal, especially for the <inline-formula><mml:math id="M264" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M265" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> parameters (i.e. Fig. 8d and h). This is due to the prior parameter penalty, which is included in the Bayesian solution but not in the KGE. In general, the calibration of the two functions using the natural run provides wider distributions between the lower and upper boundaries for the <inline-formula><mml:math id="M266" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> vegetation parameter, with a high number of grid cells characterized by <inline-formula><mml:math id="M267" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> values higher than 0.1 (see KGE-VV natural and <inline-formula><mml:math id="M268" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV natural experiments in Fig. 8a and e, respectively). Conversely, the irrigation run provides <inline-formula><mml:math id="M269" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> distributions more skewed to the lower boundary (being also the guess value in each calibration experiment), with a smaller number of grid cells characterized by high <inline-formula><mml:math id="M270" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> values compared to the natural run. In a preliminary sensitivity study (not shown), we observed that high values of the vegetation parameters <inline-formula><mml:math id="M271" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M272" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula>, as obtained for the natural run, have the tendency to generate high peaks in the simulated <inline-formula><mml:math id="M273" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> during the growing season. Indeed, in the summer, the SSM natural signal is low and not consistent with the Sentinel-1 <inline-formula><mml:math id="M274" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, which observes irrigation. In order to follow the temporal dynamics of the Sentinel-1 <inline-formula><mml:math id="M275" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, the calibration algorithms attribute a relatively higher weight (higher <inline-formula><mml:math id="M276" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> values) to the LAI than to SSM to compensate for the underestimated SSM in the natural run. In contrast, the irrigation run provides vegetation parameter distributions more skewed to the lower boundaries (see also Sect. 3.4.2). The <inline-formula><mml:math id="M277" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M278" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> parameter distributions feature a better sensitivity to soil moisture dynamics using the irrigation run input data, which is the expected behaviour, considering that they describe the <inline-formula><mml:math id="M279" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>soil</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>. This is true especially when using the <inline-formula><mml:math id="M280" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> cost function (see parameters distributions for the <inline-formula><mml:math id="M281" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV natural and for the <inline-formula><mml:math id="M282" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV irrigation
experiments in Fig. 8g and h), which results in more spread in the calibrated <inline-formula><mml:math id="M283" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M284" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> distributions for the irrigation simulations (especially in VV polarization), whereas the mode of the <inline-formula><mml:math id="M285" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M286" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> parameter distributions for the natural experiments is more shifted to the upper and lower boundaries, respectively.</p>
      <p id="d1e4435">Figure 9 shows the spatial pattern of the parameters over the study area to better understand the differences between the natural and
irrigation calibration runs. We found a connection between the WCM parameters distribution and model parameters, particularly with the HWSD
soil texture map (shown in Fig. 2). For both the <inline-formula><mml:math id="M287" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV natural and <inline-formula><mml:math id="M288" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV irrigation experiments, the activation of the irrigation
scheme reduces the dependency of the vegetation-related parameters <inline-formula><mml:math id="M289" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M290" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula> on soil texture (see Fig. 9a and b for the <inline-formula><mml:math id="M291" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV natural and
Fig. 9e and f for the <inline-formula><mml:math id="M292" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV irrigation experiment). This is also shown in the parameter maps of the KGE calibration experiments
(Fig. S5). Additionally, the activation of the irrigation scheme, more realistically, shifts the soil texture dependency towards the
soil parameters <inline-formula><mml:math id="M293" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M294" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> (Fig. 9g and h), highlighting another important reason for simulating irrigation.</p>
      <p id="d1e4495">Finally, the different polarization experiments generally provided similar distributions for the vegetation <inline-formula><mml:math id="M295" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M296" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula> parameters and the <inline-formula><mml:math id="M297" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> soil
parameter. The largest differences between the VV and VH polarizations are identified for the <inline-formula><mml:math id="M298" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> parameter distributions. This is due to the lower
<inline-formula><mml:math id="M299" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> signal associated with the VH polarization. Indeed, Fig. 8c and g are characterized by higher values of <inline-formula><mml:math id="M300" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> in the VV polarization, as
compared to the distributions for VH polarization in Fig. 8k and o. In the latter, the <inline-formula><mml:math id="M301" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula>–VH distributions are generally more skewed to the lower
boundary of the parameters, with median values closer to the defined guess parameter value.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><?xmltex \currentcnt{10}?><?xmltex \def\figurename{Figure}?><label>Figure 10</label><caption><p id="d1e4554">Split violin distributions of <bold>(a–d)</bold> Pearson <inline-formula><mml:math id="M302" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>, <bold>(e–h)</bold> KGE, and <bold>(i–l)</bold> bias calculated between <inline-formula><mml:math id="M303" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations and observations for the validation period, for all the calibration experiments and considering only the cropland areas, using simulations from the natural run (left; green) and the irrigation run (right; violet). The results are shown for VV (first two columns) and VH (right two columns) and alternate for both the calibration with a <inline-formula><mml:math id="M304" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> and KGE cost function. Note that the areas under the histograms on both left and right sides of the violins are automatically scaled for optimizing the visualization.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://hess.copernicus.org/articles/25/6283/2021/hess-25-6283-2021-f10.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>WCM evaluation</title>
<sec id="Ch1.S3.SS4.SSS1">
  <label>3.4.1</label><title>Regional evaluation</title>
      <?pagebreak page6298?><p id="d1e4613">The regional evaluation of the calibration experiments was carried out during the period from January 2015 to December 2016 for agricultural areas within
the study domain (almost 15 000 <inline-formula><mml:math id="M305" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>), by comparing biweekly <inline-formula><mml:math id="M306" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations with Sentinel-1 <inline-formula><mml:math id="M307" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> in terms of
Pearson <inline-formula><mml:math id="M308" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>, KGE, and bias. The distribution of the evaluation metrics for the eight experiments is shown in Fig. 10. A comparison of the
metrics for the irrigation and natural runs confirms better results when irrigation is activated, with violin plots skewed towards
more positive values for both KGE and Pearson <inline-formula><mml:math id="M309" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>. When stratified by the cost function, the Pearson <inline-formula><mml:math id="M310" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> distribution in Fig. 10a–d indicates a
slightly higher performance for the KGE (Fig. 10a and c) than for <inline-formula><mml:math id="M311" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> (Fig. 10b and d). In terms of the KGE score, simulations are naturally closer to the observations when the KGE cost function is used. On the other hand, in terms of bias, generally better performances are found when the Bayesian solution is used (Fig. 10i–l). The latter is particularly evident for the VH polarization when comparing the KGE-VH and
<inline-formula><mml:math id="M312" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VH experiments (Fig. 10k and l).</p>
      <p id="d1e4685">The VH simulations exhibit a better performance in the irrigation run than the VV simulations (Fig. 10c and d and 10a and b). Indeed, considering all the statistical scores, the VV polarization is characterized by more similar distributions between the
natural and irrigation run for both cost functions. This suggests a higher sensitivity of the VH polarization to the change in vegetation introduced by irrigation, confirming the Sentinel-1 <inline-formula><mml:math id="M313" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VH to be strongly influenced by irrigation, as witnessed by the larger
score improvement obtained for the calibration experiments KGE-VH irrigation (Fig. 10g) and <inline-formula><mml:math id="M314" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VH irrigation
(Fig. 10h) when compared to the natural run experiments.</p>
      <p id="d1e4706">In summary, (i) VH polarization is more sensitive to the change in the cost function and input data (irrigation or natural run) than
VV polarization, likely due to its higher sensitivity to vegetation change (Vreugdenhil et al., 2018; Macelloni et al. 2001), which, in the area, is
related to the crop development after irrigation, and (ii) the combination of <inline-formula><mml:math id="M315" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> with the activation of the irrigation scheme is able to provide the best
unbiased estimates of simulated <inline-formula><mml:math id="M316" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> for both VV and VH (<inline-formula><mml:math id="M317" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV irrigation and <inline-formula><mml:math id="M318" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VH irrigation experiments) at the
price of generally lower correlations (compared to the KGE cost function). This is, however, beneficial for DA as it minimizes the chance of
potential error cross-correlation between model estimates and observations. Indeed, the match of the temporal dynamic of the signals induced by the
correlation term is stronger in the KGE than in <inline-formula><mml:math id="M319" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>, which, additionally, includes a<?pagebreak page6299?> parameter constraint. The higher weight of the correlation
in the KGE cost function can negatively impact the parameter calibration, even when irrigation is turned on in Noah-MP, because the simulated
irrigation applications are, in general, not temporally consistent with those seen by Sentinel-1 (see Fig. 6).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e4752">Results of the site WCM evaluation considering the test site Faenza San Silvestro for each WCM experiment.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="9">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">KGE-VV</oasis:entry>
         <oasis:entry colname="col3">KGE-VV</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M320" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M321" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VV</oasis:entry>
         <oasis:entry colname="col6">KGE-VH</oasis:entry>
         <oasis:entry colname="col7">KGE-VH</oasis:entry>
         <oasis:entry colname="col8"><inline-formula><mml:math id="M322" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VH</oasis:entry>
         <oasis:entry colname="col9"><inline-formula><mml:math id="M323" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VH</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Natural</oasis:entry>
         <oasis:entry colname="col3">Irrigation</oasis:entry>
         <oasis:entry colname="col4">Natural</oasis:entry>
         <oasis:entry colname="col5">Irrigation</oasis:entry>
         <oasis:entry colname="col6">Natural</oasis:entry>
         <oasis:entry colname="col7">Irrigation</oasis:entry>
         <oasis:entry colname="col8">Natural</oasis:entry>
         <oasis:entry colname="col9">Irrigation</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Pearson <inline-formula><mml:math id="M324" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> (–)</oasis:entry>
         <oasis:entry colname="col2">0.14</oasis:entry>
         <oasis:entry colname="col3">0.27</oasis:entry>
         <oasis:entry colname="col4">0.14</oasis:entry>
         <oasis:entry colname="col5">0.18</oasis:entry>
         <oasis:entry colname="col6">0.33</oasis:entry>
         <oasis:entry colname="col7">0.41</oasis:entry>
         <oasis:entry colname="col8">0.22</oasis:entry>
         <oasis:entry colname="col9">0.38</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">KGE  (–)</oasis:entry>
         <oasis:entry colname="col2">0.12</oasis:entry>
         <oasis:entry colname="col3">0.26</oasis:entry>
         <oasis:entry colname="col4">0.12</oasis:entry>
         <oasis:entry colname="col5">0.03</oasis:entry>
         <oasis:entry colname="col6">0.20</oasis:entry>
         <oasis:entry colname="col7">0.38</oasis:entry>
         <oasis:entry colname="col8">0.22</oasis:entry>
         <oasis:entry colname="col9">0.31</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Bias  (<inline-formula><mml:math id="M325" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">dB</mml:mi></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M326" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.46</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M327" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.55</oasis:entry>
         <oasis:entry colname="col4">0.07</oasis:entry>
         <oasis:entry colname="col5">0.09</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M328" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.82</oasis:entry>
         <oasis:entry colname="col7">0.38</oasis:entry>
         <oasis:entry colname="col8"><inline-formula><mml:math id="M329" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.22</oasis:entry>
         <oasis:entry colname="col9"><inline-formula><mml:math id="M330" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.02</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><?xmltex \currentcnt{11}?><?xmltex \def\figurename{Figure}?><label>Figure 11</label><caption><p id="d1e5010">Comparisons between <inline-formula><mml:math id="M331" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> observations (VV polarization in blue dots and VH polarization light blue dots) and simulations (VV polarization in red and VH polarization in green) in the Faenza (San Silvestro) field, after calibration with a KGE cost function for <bold>(a)</bold> the natural run, <bold>(b)</bold> the irrigation run, and after calibration with the <inline-formula><mml:math id="M332" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> cost function for <bold>(c)</bold> the natural and <bold>(d)</bold> irrigation runs.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://hess.copernicus.org/articles/25/6283/2021/hess-25-6283-2021-f11.png"/>

          </fig>

</sec>
<sec id="Ch1.S3.SS4.SSS2">
  <label>3.4.2</label><title>In situ evaluation</title>
      <p id="d1e5058">The WCM simulations are further analysed in detail at the Faenza test site (specifically for the San Silvestro field) because it has a larger extent
than the Budrio site (see Fig. 1), although the same overall conclusions were found for Budrio. Figure 11 shows the simulated and observed <inline-formula><mml:math id="M333" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>
time series for the different experiments highlighted in Fig. 3, and Table 2 summarizes the statistics (i.e. Pearson <inline-formula><mml:math id="M334" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>, KGE and bias) of each
experiment.</p>
      <p id="d1e5079">The agreement between simulated and observed <inline-formula><mml:math id="M335" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> measured by the Pearson <inline-formula><mml:math id="M336" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> and KGE in Table 2 generally gives better performances after calibration with the KGE cost function than with the <inline-formula><mml:math id="M337" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> cost function. An example is in the higher correlations found for the
KGE-VH irrigation experiment as compared to the <inline-formula><mml:math id="M338" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-VH irrigation (Fig. 11b and d, respectively). On the other hand, in
terms of bias, the cost function <inline-formula><mml:math id="M339" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> significantly outperforms the calibration with KGE in all experiments with surprisingly comparable values between natural and irrigation runs (Table 2).</p>
      <p id="d1e5121">One undesirable feature of natural runs is the presence of high <inline-formula><mml:math id="M340" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> peaks during the summer, clearly detectable over the Faenza test
site, especially in the VH polarization, which are less evident in the irrigation run (see Fig. 11b and d). A similar behaviour was found for
Budrio (not shown). These peaks are likely attributed to the poor estimation of model vegetation parameter values, previously discussed in Sect. 3.3,
when the WCM attempts to compensate for bias in SSM and vegetation input, i.e. input that is not consistent with observations over irrigated
areas. This is particularly true for the KGE calibration, which does not use a prior parameter constraint. In contrast, the <inline-formula><mml:math id="M341" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> calibration
still provides reasonable <inline-formula><mml:math id="M342" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations that are closer to the ones of the irrigation run due to the Bayesian technique itself.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Discussion</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Noah-MP irrigation modelling</title>
      <p id="d1e5170">The Noah-MP LSM, used as input for the WCM calibration, was evaluated in two configurations, either with a sprinkler irrigation scheme activated or
without irrigation (i.e. irrigation run and natural run). Although not all of the Po Valley is irrigated by sprinkler
systems, it most likely still leads to more realistic LSM simulations than not considering irrigation at all.</p>
      <p id="d1e5173">The main limitation found in the irrigation simulations was related to the irrigation timing and magnitude that was inconsistent with
observations. Although this finding is based on only a single study site, it is very likely that it is a widespread issue within the study area for
several reasons. In LSMs, the irrigation application is driven by the RZSM availability and, consequently, by the soil type and the rooting depth
parameterizations. Moreover, it is also influenced by the accuracy of the meteorological forcings (especially precipitation), which can determine errors in the soil moisture representation. The main reason, however, is
likely that irrigation is often the result of subjective farmer decisions rather than objective rules based on the soil state and crop conditions. In
theory, the irrigation timing issue could be partly solved by using temporally consistent high-resolution crop maps, which should provide a more
realistic information of crop phenology and rooting depth. However, in practice, this is unfeasible over many areas of the world given the absence of this information on a large scale. Also, given that irrigation applications are mainly linked to unmodelled processes, like rotation schedules for farmers to withdraw water, the correct simulation of the timing can be unsolvable when using models only.</p>
      <p id="d1e5176">Despite the potential problems related to the unrealistic assumptions in the simulation of irrigation, our results demonstrated that even the use of
simple irrigation schemes within Noah-MP can be beneficial. In the regional evaluation, SSM simulations of the natural and irrigation runs were compared with RS SSM from SMAP and ASCAT (Fig. 4) on a biweekly temporal scale. For both products, we found large improvements in temporal Pearson <inline-formula><mml:math id="M343" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> when irrigation was simulated, which were confirmed by a decrease in the RMSE values over croplands, suggesting that the activation of irrigation modelling provides more realistic SSM estimates. Our findings further confirm the potential of coarse-resolution data sets for providing irrigation-related information over intensively irrigated and relatively large agricultural areas, as was shown by S. V. Kumar
et al. (2015).</p>
      <p id="d1e5186">While the impact of irrigation was clear in terms of SSM, the regional evaluation of the simulated LAI against the PROBA-V-based LAI provided
contradicting results. In this case, the Pearson <inline-formula><mml:math id="M344" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> analysis suggested a deterioration of the Noah-MP-simulated LAI when irrigation was activated
over the cropland area. We interpreted this correlation deterioration from the absence of specific information about the crop phenology in the model
parameterization. In practice, information about the specific crop type is not available, and the rooting depth is the sole parameter controlling water
uptake from the soil layers. Additionally, information on sowing and harvest periods are not included in the current version of Noah-MP, while
irrigated areas are defined based on a global data set (Salmon et al., 2015) which can suffer accuracy limitations. Indeed, the absence of annual dynamic information on irrigated fields, the unknown yearly variability of the crop types, and the impact of the meteorological conditions in the stakeholders' decision-making process (i.e. sowing) make the simulation of Noah-MP prone to LAI peak shifts, as compared to observations, when irrigation is<?pagebreak page6300?> simulated. Another important aspect affecting LAI simulations is its sensitivity to root zone soil moisture, which might be more difficult to simulate than SSM during the irrigation season due to larger impacts of the soil texture and transpiration processes along with the high frequency of the wetting and drying phases caused by irrigation events. This results in a significant performance deterioration (often worse than LAI simulations not including irrigation which are mainly driven by seasonality; see Fig. 7). In contrast, irrigation modeling helps to reduce the bias of the LAI-simulated time series, which, in the cropland area, show a significant underestimation when irrigation is not considered.</p>
      <p id="d1e5197">The limitations found in simulating LAI and vegetation by Noah-MP, even when irrigation was simulated, could potentially be overcome by assimilating
Sentinel-1 <inline-formula><mml:math id="M345" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> data. To explore this potential, we compared the LAI from both model runs, and from PROBA-V, with the observed Sentinel-1
<inline-formula><mml:math id="M346" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> CR (VH/VV), which should provide information about the vegetation dynamics (Vreugdenhil et al., 2018, 2020). We found that the
correlation between <inline-formula><mml:math id="M347" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> CR and LAI from PROBA-V was much higher than that between <inline-formula><mml:math id="M348" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> CR and the simulated LAI by Noah-MP (see
Fig. 7), suggesting that Sentinel-1 <inline-formula><mml:math id="M349" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> DA could help to correct poor LAI model simulations. Additionally, a higher correlation was found
between the <inline-formula><mml:math id="M350" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VV observations and the simulated SSM when irrigation was turned on than in the absence of irrigation, suggesting that the assimilation of <inline-formula><mml:math id="M351" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VV could improve SSM where irrigation is poorly modelled or not modelled. On the other hand, considering the low correlation between the VH signal and SSM in presence of vegetation (Baghdadi et al. 2017), and its close relation with vegetation (Ferrazzoli et al.,
1992; Macelloni et al., 2001), future data assimilation experiments will investigate the contribution
of VH and CR in improving LAI predictions and irrigation quantification.</p>
      <p id="d1e5278">Finally, biweekly accumulated irrigation estimates in Fig. 7 agree well with real irrigation applications, suggesting that the large-scale LSM
irrigation scheme is helpful for intensively irrigated areas. On the other hand, the poor soil and crop parameterization, along with other unknown
parameters related to the irrigation management (e.g. the farmers can apply more water than actually needed), can cause large biases in these
irrigation simulations. Again, ingestion of radar backscatter data could correct for unmodelled processes. More specifically, Sentinel-1 <inline-formula><mml:math id="M352" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>
could correct (i) for the magnitude and timing of the irrigation simulations and (ii) for Noah-MP irrigation predictions over regions that are not irrigated.</p>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>WCM backscatter simulation</title>
      <?pagebreak page6301?><p id="d1e5300">The purpose of the presented WCM observation operator calibration and evaluation was to optimize the parameters for the future assimilation of the
Sentinel-1 <inline-formula><mml:math id="M353" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VV and VH into Noah-MP. Such an optimization would ideally minimize the long-term bias between the simulated and observed
<inline-formula><mml:math id="M354" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> signals. This can be achieved by calibrating the observation operator with long-term observed <inline-formula><mml:math id="M355" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> prior to data assimilation,
but in this process, it is crucial to avoid potential error cross-correlation between model observation predictions and observations. Furthermore, a
good observation operator should not already compensate for missing processes in the LSM by accepting effective, but unrealistic, optimized
parameters because it would then lose its physically based ability to accurately convert misfits between observations and simulations to LSM updates during the data assimilation.</p>
      <p id="d1e5336">One way to avoid parameters compensating for erroneous LSM input into the WCM would be to use observed time series of, e.g., LAI. However, LAI products
from different sensors have different biases themselves, which can add bias to the <inline-formula><mml:math id="M356" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations, and more importantly, replacing simulated
LAI or SSM with external data sets would undermine the possibility of updating these variables in the future assimilation system. Based on that, we
performed the WCM calibration considering the SSM and LAI model input from two different experiments, i.e. a natural run and an irrigation
run, as well as two cost functions, a Bayesian solution <inline-formula><mml:math id="M357" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>, and a KGE solution, which resulted in four calibration experiments for each polarization (i.e. eight calibration experiments in total).</p>
      <p id="d1e5357">The calibration experiments using simulations from the natural run as input showed a limited performance and provided presumably bad vegetation parameter estimates, which resulted in unrealistic peaks in the simulated <inline-formula><mml:math id="M358" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> during the summer when driven by higher modelled LAI during this period. The inclusion of the irrigation within Noah-MP was very beneficial for all the calibration experiments, helping to reduce the bias,  increase the correlation with Sentinel-1 <inline-formula><mml:math id="M359" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, and remove the anomalous <inline-formula><mml:math id="M360" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> increase during warm periods, especially for the KGE-based calibration. This corroborates our initial hypothesis that, over intensively irrigated areas, the simulation of
irrigation is a mandatory task for an optimal calibration of the WCM. Irrigation modeling, even if only done approximately and perhaps with inaccurate timing, reduces obvious land surface (soil moisture and vegetation) bias and avoids that the WCM needs to compensate for this bias.</p>
      <p id="d1e5393">Our results show overall higher performance in terms of KGE and Pearson <inline-formula><mml:math id="M361" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> scores for the KGE-based calibration, whereas the long-term bias
was better reduced for the <inline-formula><mml:math id="M362" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>-based calibration, which is beneficial in anticipation of future DA. This is because, in the <inline-formula><mml:math id="M363" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> cost function, there is (i) a target accuracy term which also takes into account the Sentinel-1 observations, where an error is present, and (ii) a parameter deviation penalty based on the prior parameters constraints is used, which prevents parameters from deviating largely from their prior values.</p>
      <p id="d1e5418">In terms of polarization, we found <inline-formula><mml:math id="M364" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VH simulations much more sensitive to the inclusion of the irrigation (vs. non-inclusion) in Noah-MP,
suggesting that observed <inline-formula><mml:math id="M365" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VH might also contain much more information about irrigation (via the influence of the vegetation change due to irrigation) than that contained in <inline-formula><mml:math id="M366" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VV, which is normally used for SSM retrieval (Vreugdenhil et al., 2020). We believe that the cause of
this is related to a comparatively larger <inline-formula><mml:math id="M367" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> of vegetation with respect to that of the soil when the crops are well developed. This was also
corroborated by the better agreement between CR and LAI from PROBA-V in one of the study sites mentioned above. Despite this, further investigations
are required to confirm this hypothesis, and DA will certainly help to test this aspect.</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d1e5475">With the specific focus on intensively irrigated land, the main objective of this work was to define the optimal calibration of the WCM as an observation
operator for the future ingestion of Sentinel-1 backscatter into the Noah-MP LSM via DA. In this context, we additionally aimed at (1) unveiling the
strengths and limitations of irrigation simulation in LSMs from the perspective of a calibrating the WCM and (2) identifying the potential
irrigation-related information contained in the Sentinel-1 <inline-formula><mml:math id="M368" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> observations to improve soil moisture and vegetation states, as well as
irrigation estimates, in a calibrated DA system.</p>
      <p id="d1e5489">To reach these objectives, we coupled the Noah-MP with a sprinkler irrigation scheme within LIS and performed two different simulation experiments, i.e. one with and one without irrigation (i.e. natural and irrigation runs). Moreover, we coupled a WCM with Noah-MP and tested different
calibration options to prepare for the optimal, future, assimilation of <inline-formula><mml:math id="M369" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> VV and VH to update both soil moisture and vegetation states.</p>
      <p id="d1e5503">The main conclusions drawn from our evaluation are as follows:
<list list-type="bullet"><list-item>
      <p id="d1e5508">Over highly irrigated areas, the simulation of irrigation in LSMs helps to provide better soil moisture and vegetation simulations, which can be used with benefit as input for the WCM calibration. However, the performance of the irrigation simulations is limited by the simplistic model parameterization of this human process and the necessity for considering realistic and updated land cover information (e.g. crop types). This results in poor simulations of the irrigation timing and quantities, as well as vegetation dynamics.</p></list-item><list-item>
      <?pagebreak page6302?><p id="d1e5512">The Sentinel-1 <inline-formula><mml:math id="M370" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> observations contain useful information about SSM and vegetation over highly irrigated areas. This information can be exploited to overcome LSM deficiencies in simulating soil moisture and vegetation over highly irrigated regions, e.g. when irrigation is unmodelled or poorly modelled because of uncertainties due to crop types, irrigation timing, and farmer agricultural practices. In particular, there is a high chance that the assimilation of Sentinel-1 <inline-formula><mml:math id="M371" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> can help in correcting LAI dynamics.</p></list-item><list-item>
      <p id="d1e5538">The optimal assimilation of Sentinel-1 <inline-formula><mml:math id="M372" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> into a LSM must rely upon a well-calibrated WCM as the observation operator to provide unbiased   <inline-formula><mml:math id="M373" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations with a minimal chance of having error cross-correlations between model and observations, while ensuring a realistic operator controllability or realistic connection between observed signals and land surface state variables. We demonstrated that calibrating the WCM by including irrigation modeling consistently led to a better agreement with Sentinel-1 <inline-formula><mml:math id="M374" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>. The modeling of irrigation in the LSM simulations, even if not done optimally, avoids that the WCM calibration compensates for LSM biases.</p></list-item><list-item>
      <p id="d1e5575">We demonstrated that the WCM calibration with a Bayesian cost function, including a prior parameter constraint, provides the optimal WCM parameters, is able to generate the lowest bias in the <inline-formula><mml:math id="M375" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> simulations for both VV and VH. Although slightly higher correlations are obtained when using a KGE cost function, unbiased estimates are particularly beneficial for DA, as this minimizes the chance of potential error cross-correlation between model estimates and observations.</p></list-item></list></p>
      <p id="d1e5589">This study improves the understanding of the LSM limitations in simulating irrigation and highlights the information content in Sentinel-1
<inline-formula><mml:math id="M376" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> data. A natural follow-up of this study is the assimilation of <inline-formula><mml:math id="M377" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> observations within Noah-MP, which should enforce our tested
evidence and provide new insights for a more realistic description of the water and carbon cycles over irrigated areas.</p>
</sec>

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

      <p id="d1e5618">Data from SMAP can be downloaded at <ext-link xlink:href="https://doi.org/10.5067/Q8J8E3A89923" ext-link-type="DOI">10.5067/Q8J8E3A89923</ext-link> (O'Neill et al., 2020). Data from ASCAT are available from the website <uri>https://www.cen.uni-hamburg.de/en/icdc/data/land/docs-land/h115-ascat-ssm-cdr-v5-pum-v0-1.pdf</uri> (EUMETSAT, 2019). The Sentinel-1 backscatter data processing was done using Google Earth Engine's Python interface and including standard processing techniques. Data from PROBA-V are available at <uri>https://land.copernicus.vgt.vito.be/PDF/portal/Application.html#Browse;Root=512260;Collection=1000083;Time=NORMAL,NORMAL,-1,,,-1,,</uri> (Verger et al., 2014). MERRA-2 data are available from MDISC, which is managed by the NASA Goddard Earth Sciences (GES) Data and Information Services Center (DISC; <uri>https://disc.gsfc.nasa.gov/datasets?project=MERRA-2</uri>; Gelaro et al., 2017). The LIS source code and default input parameters are available via <uri>https://lis.gsfc.nasa.gov/</uri> (Kumar, 2021).
The 100 m spatial resolution land cover map from the Copernicus Global Land Service can be downloaded from <uri>https://lcviewer.vito.be/2015</uri> (Buchhorn et al., 2020). In situ data are available upon request to the original providers. The ETOPO1 1 arcmin global relief model used in Fig. 1 can be downloaded at <ext-link xlink:href="https://doi.org/10.7289/V5C8276M" ext-link-type="DOI">10.7289/V5C8276M</ext-link> (Amante and Eakins, 2009).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e5643">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/hess-25-6283-2021-supplement" xlink:title="pdf">https://doi.org/10.5194/hess-25-6283-2021-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e5652">SM designed and coordinated the study and did the analyses. CM, GJMDL, and AG designed, coordinated, and helped with the data analysis and interpretation. HL, AT, and RM helped with the result interpretation and data processing and collection. All authors contributed to the editing of the paper.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e5658">The contact author has declared that neither they nor their co-authors have any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e5664">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e5670">The authors would like to thank the European Space Agency (ESA) for funding support as part of the IRRIGATION+ project. For details, please visit <uri>https://esairrigationplus.org/</uri> (last access: 2 December 2021). Additional acknowledgements go to the Canale Emiliano Romagnolo (CER; Emilia Romagna, Italy), for providing irrigation data over the irrigated test sites. For the Proximal Gamma Ray soil moisture data
at the Budrio test site, the authors would like to thank the Department of Physics and Earth Sciences, University of Ferrara Polo Scientifico e Tecnologico, and, in particular, Martina Natali, Virginia Strati, Alberi Matteo, Kassandra Giulia Raptis, and Fabio Mantovani. Additionally, the authors want to acknowledge  Kristi Arsenault from NASA Goddard Space Flight Center (GFSC) for sharing important technical information on irrigation simulations into the Land Information System (LIS) framework and the Vlaams Supercomputer Centrum (VSC) high-performance computing (HPC) for providing the computational resources needed to realize this study (<uri>https://www.vscentrum.be/</uri>, last access: 2 December 2021). Alexander Gruber
has received funding from the Research Foundation Flanders.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e5681">This research has been supported by the European Space Agency (ESA) as part of the IRRIGATION+ project (contract no. 4000129870/20/I-NB). Alexander Gruber has been supported by  the Research Foundation Flanders (grant no. FWO-1224320N).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e5687">This paper was edited by Louise Slater and reviewed by two anonymous referees.</p>
  </notes><ref-list>
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