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  <front>
    <journal-meta><journal-id journal-id-type="publisher">ESSD</journal-id><journal-title-group>
    <journal-title>Earth System Science Data</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ESSD</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Earth Syst. Sci. Data</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1866-3516</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/essd-14-3673-2022</article-id><title-group><article-title>A global terrestrial evapotranspiration product based on the
three-temperature model with fewer input parameters and no calibration
requirement</article-title><alt-title>A global terrestrial evapotranspiration product based on the
three-temperature model</alt-title>
      </title-group><?xmltex \runningtitle{A global terrestrial evapotranspiration product based on the
three-temperature model}?><?xmltex \runningauthor{L.~Yu et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Yu</surname><given-names>Leiyu</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Qiu</surname><given-names>Guo Yu</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Yan</surname><given-names>Chunhua</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff3">
          <name><surname>Zhao</surname><given-names>Wenli</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Zou</surname><given-names>Zhendong</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Ding</surname><given-names>Jinshan</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Qin</surname><given-names>Longjun</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff5 aff6">
          <name><surname>Xiong</surname><given-names>Yujiu</given-names></name>
          <email>xiongyuj@mail.sysu.edu.cn</email>
        <ext-link>https://orcid.org/0000-0002-5762-3538</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>School of Environment and Energy, Peking University Shenzhen Graduate School, Shenzhen, 518055, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Earth and Environmental Engineering, Columbia University, New York, NY 10027, USA</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Max Planck Institute for Biogeochemistry, Hans-Knöll-Str. 10,
Jena 07745, Germany</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Shenzhen Investment Holdings Co., LTD, Shenzhen, 518048, China</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>School of Civil Engineering, Sun Yat-Sen University, Guangzhou,
510275, China</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Southern Marine Science and Engineering Guangdong Laboratory (Zhuhai),
Zhuhai, 519082, China</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Yujiu Xiong (xiongyuj@mail.sysu.edu.cn)</corresp></author-notes><pub-date><day>12</day><month>August</month><year>2022</year></pub-date>
      
      <volume>14</volume>
      <issue>8</issue>
      <fpage>3673</fpage><lpage>3693</lpage>
      <history>
        <date date-type="received"><day>19</day><month>May</month><year>2022</year></date>
           <date date-type="rev-request"><day>24</day><month>May</month><year>2022</year></date>
           <date date-type="rev-recd"><day>25</day><month>July</month><year>2022</year></date>
           <date date-type="accepted"><day>27</day><month>July</month><year>2022</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 Leiyu Yu et al.</copyright-statement>
        <copyright-year>2022</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022.html">This article is available from https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022.html</self-uri><self-uri xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022.pdf">The full text article is available as a PDF file from https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e180">Accurate global terrestrial evapotranspiration (ET)
estimation is essential to better understand Earth's energy and water
cycles. Although several global ET products exist, recent studies indicate
that ET estimates exhibit high uncertainty. With the increasing trend of
extreme climate hazards (e.g., droughts and heat waves), accurate ET
estimation under extreme conditions remains challenging. To overcome these
challenges, we used 3 h and 0.25<inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> Global Land Data Assimilation
System (GLDAS) datasets (net radiation, land surface temperature (LST), and
air temperature) and a three-temperature (3T) model, without resistance and
parameter calibration, in global terrestrial ET product development. The
results demonstrated that the 3T model-based ET product agreed well with
both global eddy covariance (EC) observations at daily (root mean square
error (RMSE) <inline-formula><mml:math id="M2" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.1 mm d<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">294</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mn mathvariant="normal">058</mml:mn></mml:mrow></mml:math></inline-formula>) and monthly (RMSE <inline-formula><mml:math id="M5" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 24.9 mm month<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">9632</mml:mn></mml:mrow></mml:math></inline-formula>) scales and basin-scale water balance observations (RMSE <inline-formula><mml:math id="M8" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 116.0 mm yr<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">34</mml:mn></mml:mrow></mml:math></inline-formula>). The 3T model-based global terrestrial
ET product was comparable to other common ET products, i.e., MOD16, P-LSH,
PML, GLEAM, GLDAS, and Fluxcom, retrieved from various models, but the 3T
model performed better under extreme weather conditions in croplands than
did the GLDAS, attaining 9.0 %–20 % RMSE reduction. The proposed daily and
0.25<inline-formula><mml:math id="M11" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> ET product covering the period of 2001–2020 could provide periodic and large-scale information to support water-cycle-related studies.
The dataset is freely available at the Science Data Bank
(<ext-link xlink:href="https://doi.org/10.57760/sciencedb.o00014.00001" ext-link-type="DOI">10.57760/sciencedb.o00014.00001</ext-link>, Xiong et al., 2022).</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e311">Evapotranspiration (ET), the second-largest component of the global
hydrological cycle (Trenberth et al., 2007), plays an important role in
linking global energy and water cycles (Trenberth et al., 2009). ET is
usually observed via techniques such as those involving evaporation pans,
sap flowmeters, weighing lysimeters, stable isotopes, Bowen ratio systems,
eddy covariance (EC) systems, and scintillometers (Liu et al., 2022). However, these methods can only reflect ET representing the flux footprint
of a given instrument (normally smaller than 1 km<inline-formula><mml:math id="M12" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>), which cannot
provide spatial ET data for large-scale (e.g., basin and continental)
studies. With the advancement of remote-sensing (RS) technology, which can provide much information in regard to the land surface and atmosphere,
remote estimation remains the most feasible and economic way to obtain
continuous spatial ET data across field to global scales (Han et al., 2021;
K. Zhang et al., 2016). Several global ET estimates have been developed over
the past 2 decades based on various theories, including (1) surface energy balance residual methods, e.g., the ET product based on the Surface Energy
Balance System (SEBS) (EB) (Chen et al., 2021), (2) Penman–Monteith (PM) and Priestley–Taylor (PT) equation-based methods, e.g., MOD16 (Mu et al.,
2011), P-LSH (Zhang et al., 2015), PML (Zhang et al., 2019), and GLEAM
(Martens et al., 2017; Miralles et al., 2011), (3) land surface models, e.g., the Global Land Data Assimilation System (GLDAS) (Rodell et al., 2004), (4) multimodel ensemble approaches, e.g., GLASS (Yao et al., 2014), Hi-GLASS (Yao
et al., 2017), and a synthesized ET product (Elnashar et al., 2021), and (5) empirical methods, e.g., Fluxcom (Jung et al., 2019). Although these ET products have been rigorously evaluated and widely applied, notable
disagreement exists among these ET products. For example, Mueller et al. (2013) reported that the multi-year mean ET value retrieved from 40 ET
products ranged from 423 to 563 mm yr<inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. In addition, while the
interannual variation in some ET products exhibited similar change trends,
inconsistent or even contrasting trends occurred among these ET products
(Kim et al., 2021). The abovementioned phenomena indicate that high
uncertainties remain in ET estimates and products (Fisher et al., 2017).</p>
      <p id="d1e335">The uncertainty in ET estimates mainly originates from the quality of model
input data, model (or algorithm) assumptions, and variable parameterization
(Badgley et al., 2015; Cao et al., 2021; Khan et al., 2018; Vinukollu et
al., 2011). In terms of model input datasets, meteorological data (i.e.,
relative humidity, RH, and wind speed, WS) are essential for most models.
However, gridded meteorological data are generally produced via the data
assimilation method based on limited ground observations, but simulation
results may not necessarily capture real conditions, which could undoubtedly
affect ET estimates (model output). For example, RH, directly affecting the
vapor pressure deficit (VPD), retrieved from three meteorological reanalysis products, exhibited a low correlation with in situ EC tower observations, with the coefficient of determination ranging from 0.005 to
0.09 (Cao et al., 2021). A similar problem exists between simulated and
observed WS datasets (Vinukollu et al., 2011). In terms of model (or
algorithm) assumptions, different descriptions of the ET process within the
soil–plant–atmosphere continuum could yield single-layer versus multilayer models and incorrect but useful paradigms (Bonan et al., 2021; Raupach and
Finnigan, 1988). Even though big-leaf models simplify the land surface as a
homogeneous single layer, which is physically incorrect, they are recognized
as highly computable and applicable models (Cheng et al., 2021). In
contrast, multilayer models can more reasonably represent vertical vegetation and soil structures, but these models require more computational
resources, and additional hypotheses must be introduced to determine the model input or solve the model. This increase in model structure complexity
and parameterization can increase the risk of error propagation or
uncertainty in ET estimates, as revealed in the literature, e.g., Ershadi et
al. (2015) and Zhao et al. (2020). For instance, under varying model
assumptions and data availability levels, the surface resistance can be
parameterized in different ways. In parameterization, several empirical
coefficients and biophysical values required for resistance estimation must
be calibrated. The error in ET estimates based on the PM method and the
difference between surface resistance values with and without calibration
can range from 12 % to 53 % in terms of the mean absolute percentage
error (MAPE) (Zhao et al., 2020). To reduce the above uncertainty in ET
estimates, the PM equation was simplified as the PT model by replacing the resistance terms with an empirical coefficient (<inline-formula><mml:math id="M14" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>) (Priestley and
Taylor, 1972). Eventually, the combined uncertainty due to the model input
data quality, model (or algorithm) assumptions, and variable
parameterization schemes could lead to propagation errors in ET simulation
results (Bengtsson and Shukla, 1988; Rienecker et al., 2011). Therefore,
simpler algorithms without resistance parameterization (Yao et al., 2013, 2015) and variable calibration (Ma et al., 2021) requirements
are necessary to reduce the uncertainty in ET estimates.</p>
      <p id="d1e345">The three-temperature (3T) model, without calibration and resistance
parameterization requirements, was proposed to reduce the uncertainty in ET
estimates (Qiu, 1996). Based on the surface energy balance residual method,
the inputs of the 3T model mainly comprise variables that can be directly
measured or easily determined via RS, such as net radiation, surface
temperature, and air temperature. The 3T model has been evaluated with an
acceptable accuracy considering various land cover types on different
spatial scales (Qiu et al., 1999; Wang et al., 2016; Xiong et al., 2019; Qiu
et al., 2020; Zhao et al., 2020). Specifically, this model typically
performs well in ET rate estimation in water-limited arid regions (Tian et
al., 2013; Xiong et al., 2019), where surface and aerodynamic resistance
values are very difficult to accurately estimate. Consequently, ET in these
arid regions has usually been assumed to be zero in certain ET products (Mu et al., 2011; Jung et al., 2019). In addition, the 3T model is sensitive to the
temperature, and the model could potentially be suitable for ET estimation
under notable temperature fluctuations (i.e., extreme heat or drought
conditions). As such, the 3T model may provide an accurate dataset to
support the attainment of Sustainable Development Goals (SDGs) (Guo et al.,
2021) under increasing frequency and intensity of extreme events (IPCC, 2022).</p>
      <p id="d1e348">The objectives of this study were to (1) propose a global ET product with a
low uncertainty based on the 3T model, (2) evaluate the product performance
with global EC network and catchment water budget methods, (3) compare the
established product to available mainstream ET products, and (4) explore the
product suitability under extreme weather conditions, such as extreme heat
and drought.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Materials and methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Estimation of transpiration, evaporation, and evapotranspiration with
the three-temperature model</title>
      <p id="d1e366">The 3T model, proposed by Qiu (1996), comprises two equations for vegetation
transpiration (<inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and soil evaporation (<inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) calculation. This
model mainly utilizes net solar radiation, surface temperature, and air
temperature as model inputs. In this model, the resistance terms in the
energy balance equation are eliminated via the introduction of a dry surface
without evaporation or transpiration, as detailed in Qiu et al. (1999). In
RS-based applications in which most pixels cannot represent pure vegetation
or soil conditions, ET calculation depends on the fractional vegetation
cover <inline-formula><mml:math id="M17" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula>, as follows (Xiong and Qiu, 2011):

                <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M18" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E1"><mml:mtd><mml:mtext>1</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi>L</mml:mi><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">c</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">cr</mml:mi></mml:mrow></mml:msub><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">cr</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mspace width="1em" linebreak="nobreak"/><mml:mi>f</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E2"><mml:mtd><mml:mtext>2</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi>L</mml:mi><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">s</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>G</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">sr</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>G</mml:mi><mml:mi mathvariant="normal">sr</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">sr</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mi>f</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><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:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi>L</mml:mi><mml:mfenced close=")" open="("><mml:mtext>ET</mml:mtext></mml:mfenced><mml:mo>=</mml:mo><mml:mi>L</mml:mi><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mi>L</mml:mi><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mn mathvariant="normal">0</mml:mn><mml:mo>&lt;</mml:mo><mml:mi>f</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            where <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:mi>L</mml:mi><mml:mi>E</mml:mi></mml:mrow></mml:math></inline-formula> (unit W m<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) is the latent heat flux, <inline-formula><mml:math id="M21" display="inline"><mml:mi>L</mml:mi></mml:math></inline-formula> (J kg<inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) is the latent heat of ET, <inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">c</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">s</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> are the vegetation and soil net radiation components (W m<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), respectively, <inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the
vegetation and soil surface temperatures (K), respectively, <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the
air temperature (K), and <inline-formula><mml:math id="M29" display="inline"><mml:mi>G</mml:mi></mml:math></inline-formula> is the ground heat flux (W m<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). The
subscript “r” denotes the reference vegetation or soil.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Parameterization and datasets</title>
      <p id="d1e763">The variables of the 3T model (Eqs. 1 to 3) can be parameterized as follows.</p>
      <p id="d1e766">The net radiation (<inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) can be calculated by summing <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">ns</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">nl</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (Eq. 4), and the canopy and soil components, <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">c</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">s</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, respectively, can be calculated by partitioning <inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> based on
the fractional vegetation cover via Eqs. (5) to (6) (Mu et al., 2007):

                <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M37" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E4"><mml:mtd><mml:mtext>4</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">ns</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">nl</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E5"><mml:mtd><mml:mtext>5</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">c</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub><mml:mo>×</mml:mo><mml:mi>f</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E6"><mml:mtd><mml:mtext>6</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">s</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub><mml:mo>×</mml:mo><mml:mfenced open="(" close=")"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi>f</mml:mi></mml:mrow></mml:mfenced><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            The fractional vegetation cover, <inline-formula><mml:math id="M38" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula>, can be calculated according to the normalized difference vegetation index (NDVI) with Eq. (7) (Cleugh et al.,
2007):
            <disp-formula id="Ch1.E7" content-type="numbered"><label>7</label><mml:math id="M39" display="block"><mml:mrow><mml:mi>f</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mtext>NDVI</mml:mtext><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="normal">NDVI</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="normal">NDVI</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="normal">NDVI</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where NDVI<inline-formula><mml:math id="M40" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:math></inline-formula> and NDVI<inline-formula><mml:math id="M41" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:math></inline-formula> are threshold values, defined as the mean values
of the upper and lower 5 % positive terrestrial NDVI values, respectively.</p>
      <p id="d1e1008">The ground heat flux, <inline-formula><mml:math id="M42" display="inline"><mml:mi>G</mml:mi></mml:math></inline-formula>, can be directly extracted from net radiation
<inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> according to Su (2002). Vegetation and soil component temperatures, <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, respectively, can be derived from the land surface
temperature (LST) according to Lhomme et al. (1994), as described in Xiong
et al. (2015).</p>
      <p id="d1e1051">In this study, <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">ns</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">nl</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and LST datasets were derived
from the GLDAS (<uri>https://ldas.gsfc.nasa.gov/gldas/</uri>, last access: 12 March 2022) with spatial and temporal
scales of 0.25<inline-formula><mml:math id="M49" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and 3 h (GLDAS_NOAH025_3H_2.1), respectively (Beaudoing and
Rodell, 2020; Rodell et al., 2004). A monthly NDVI dataset with a spatial
resolution of 0.05<inline-formula><mml:math id="M50" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> was obtained from MOD13C2 (version 6) (Didan, 2015) and resampled to 0.25<inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> via the nearest-neighbor method with the HEG tool (HDF-EOS to GeoTIFF Conversion Tool;
<uri>https://lpdaac.usgs.gov/tools/heg/</uri>, last access: 4 February 2021). Each dataset covered the 2001–2020
period (Table 1).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e1125">Input datasets for the three-temperature (3T) model-based global ET
product.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:colspec colnum="5" colname="col5" align="justify" colwidth="3cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1">Model input</oasis:entry>

         <oasis:entry colname="col2">Datasets</oasis:entry>

         <oasis:entry colname="col3">Spatial–temporal resolution</oasis:entry>

         <oasis:entry colname="col4">Available data coverage</oasis:entry>

         <oasis:entry colname="col5">Reference</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>

         <oasis:entry colname="col1"><inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">ns</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">nl</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col2">GLDAS_NOAH025_3H_2.1</oasis:entry>

         <oasis:entry colname="col3">0.25<inline-formula><mml:math id="M57" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> 3-hourly</oasis:entry>

         <oasis:entry colname="col4">2000–2020</oasis:entry>

         <?xmltex \mrwidth{3cm}?><oasis:entry rowsep="1" colname="col5" morerows="2">Beaudoing and Rodell (2020), Rodell et al. (2004)</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">LST</oasis:entry>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4"/>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"><inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4"/>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">NDVI</oasis:entry>

         <oasis:entry colname="col2">MOD13C2</oasis:entry>

         <oasis:entry colname="col3">0.05<inline-formula><mml:math id="M59" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> monthly</oasis:entry>

         <oasis:entry colname="col4">2001–2020</oasis:entry>

         <oasis:entry colname="col5">Didan (2015)</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p id="d1e1128">Note: <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">ns</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>: net shortwave radiation; <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">nl</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>: net longwave radiation; LST: land surface temperature; <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>: air temperature; NDVI: normalized difference vegetation index.</p></table-wrap-foot></table-wrap>

      <p id="d1e1311">To remotely estimate ET at the watershed scale, Xiong and Qiu (2014)
proposed a simple method to determine the reference temperature.
Specifically, a pixel with the maximum temperature within a given watershed
can be defined as the reference pixel. Once the reference pixel has been
determined, the reference vegetation temperature, <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">cr</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (or reference
soil temperature, <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">sr</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), can be obtained with Eq. (8) (or Eq. 9). In
the global-scale application in this study, 31 terrestrial climate regions
based on the Köppen–Geiger climate classification system (Kottek et
al., 2006) were first divided into subregions via the principal component
analysis (PCA) and <inline-formula><mml:math id="M62" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>-means clustering methods, aiming to maintain relatively equivalent climate conditions within each subregion. Specifically, PCA was
used to select major variables to describe regional characteristics from
GLDAS meteorological factors (i.e., net radiation, air temperature,
humidity, wind speed, precipitation, and air pressure) and land surface
conditions (i.e., albedo, land surface temperature, NDVI, soil moisture, and
soil temperature). Thereafter, these variables were used to classify the 31
climate regions through the <inline-formula><mml:math id="M63" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>-means clustering method. Because of
meteorology and land surface variation, the subregions varied from 90 to 110
in different months, and a reference pixel could be determined in each subregion for applying the 3T model.

                <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M64" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E8"><mml:mtd><mml:mtext>8</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">cr</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi mathvariant="normal">c</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">max</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mo movablelimits="false">max⁡</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi mathvariant="normal">c</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi mathvariant="normal">c</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi mathvariant="normal">c</mml:mi><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E9"><mml:mtd><mml:mtext>9</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">sr</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">max</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mo movablelimits="false">max⁡</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            where <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi mathvariant="normal">c</mml:mi><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> denote the vegetation surface and soil
temperatures, respectively, in pixel <inline-formula><mml:math id="M67" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> (<inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, 2, 3…) within each
subregion.</p>
      <p id="d1e1538">The reference net radiation values of the soil and vegetation components,
<inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">sr</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">cr</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, respectively, were assumed to be mean <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">c</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">s</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> values, respectively, within the same subregion corresponding to
pixels of the upper 5 % <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values, respectively.

                <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M75" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E10"><mml:mtd><mml:mtext>10</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><?xmltex \hack{\hbox\bgroup\fontsize{8.5}{8.5}\selectfont$\displaystyle}?><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">sr</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">s</mml:mi></mml:mrow></mml:msub><mml:mfenced close="]" open="["><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">upper</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mn mathvariant="normal">5</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mtext>mean</mml:mtext><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">s</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">s</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">s</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mo>,</mml:mo><?xmltex \hack{$\egroup}?></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E11"><mml:mtd><mml:mtext>11</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><?xmltex \hack{\hbox\bgroup\fontsize{8.5}{8.5}\selectfont$\displaystyle}?><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">cr</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">c</mml:mi></mml:mrow></mml:msub><mml:mfenced open="[" close="]"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi mathvariant="normal">c</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">upper</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mn mathvariant="normal">5</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mtext>mean</mml:mtext><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">c</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">c</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">c</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mo>,</mml:mo><?xmltex \hack{$\egroup}?></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            where <inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">s</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">n</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">c</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> denote the soil and vegetation net radiation
values, respectively, corresponding to pixel <inline-formula><mml:math id="M78" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula> (<inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, 2, 3…) of
the upper 5 % <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values, respectively, within the same
subregion.</p>
      <p id="d1e1922">The daytime ET was considered in this study. In global-scale applications,
the daytime can be defined based on 3-hourly GLDAS net radiation values
higher than 100 W m<inline-formula><mml:math id="M82" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Then, all the 3-hourly LE (or ET) estimates can be arithmetically averaged (or summed) into daily, monthly, and annual values.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Evaluation of the performance of the 3T model</title>
      <p id="d1e1945">ET values estimated with the 3T model were assessed on three scales due to
challenges in the validation of RS-based ET estimates (Vinukollu et al.,
2011; Miralles et al., 2016; Liu et al., 2016). First, ET estimates at daily
and monthly scales were validated against in situ observations retrieved
from global EC flux towers covering various land cover types, as widely
applied in other studies, e.g., Chen et al. (2016) and Ma et al. (2021). Due
to a mismatch between the flux tower footprint and pixel resolution
(0.25<inline-formula><mml:math id="M83" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> in this study), mean ET values in different watersheds were
compared to those obtained from the water balance equation on a yearly
scale. EC-based and basin-scale water-budget-based validation methods are considered the most reliable and commonly used methods. Finally, ET
estimates were compared to several gridded ET products on a multi-year
average scale. Statistical analysis, including Pearson's correlation
coefficient (<inline-formula><mml:math id="M84" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula>), relative bias (RB), and root mean square error (RMSE), was
employed in assessment.</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="d1e1966">Locations of the eddy covariance flux towers <bold>(a)</bold> and catchments <bold>(b)</bold> used for ET validation in this study. In this study, 126 flux towers and
34 catchments are considered. CRO denotes croplands, CSH denotes closed
shrublands, DBF denotes deciduous broadleaf forests, EBF denotes evergreen
broadleaf forests, ENF denotes evergreen needleleaf forests, GRA denotes
grasslands, MF denotes mixed forests, OSH denotes open shrublands, SAV
denotes savannas, WET denotes wetlands, and WSA denotes woody savannas. The multi-year mean aridity index in each catchment is calculated as the mean
annual precipitation divided by the mean annual reference ET (Trabucco and
Zomer, 2018), and the catchment classification refers to the United Nations
Environment Programme (UNEP, 1997).</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022-f01.png"/>

        </fig>

<sec id="Ch1.S2.SS3.SSS1">
  <label>2.3.1</label><title>Evaluation via the global eddy covariance network</title>
      <p id="d1e1988">ET observations of 126 flux towers within the FLUXNET network
(<uri>https://fluxnet.org/</uri>, last access: 5 September 2021) were selected (Fig. 1a), and the selection process
was conducted according to the following criteria. (1) A given flux tower should exhibit stable operation conditions for at least 2 consecutive years
since 2001. (2) The latent heat flux (LE) was subjected to energy closure correction, and the percentage of good-quality measurement and gap-filled data should be higher than 0.7. (3) The land cover within each 0.25<inline-formula><mml:math id="M85" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid pixel containing a tower should be as homogeneous as possible (Zhang et
al., 2019; Ma et al., 2021). The selected 126 EC towers were located at 26
evergreen needle leaf forest (ENF), 25 grassland (GRA), 15 cropland (CRO),
15 wetland (WET), 13 deciduous broadleaf forest (DBF), 8 evergreen broadleaf
forest (EBF), 7 open/closed shrubland (OSH/CSH), 6 mixed forest (MF), 6
woody savanna (WSA), and 5 savanna (SAV) sites globally. Pixel-scale ET
estimates based on the EC tower location were compared to EC tower
observations.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS2">
  <label>2.3.2</label><title>Evaluation considering the water budget in global main catchments</title>
      <p id="d1e2012">The catchment ET (ET<inline-formula><mml:math id="M86" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">wb</mml:mi></mml:msub></mml:math></inline-formula>), based on the water balance equation, has been
recognized as a highly robust and credible method, particularly in
relatively large catchments, on a multi-year (more than 10-year) scale (Liu et al., 2016). Hence, 34 catchments (Fig. 1b) were selected based on the
following two criteria. (1) The basin area should be larger than 100 000 km<inline-formula><mml:math id="M87" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> to minimize uncertainties in the measurement of water balance equation components in relatively small basins. (2) The available basin data
should cover more than 10 years since 2001. ET<inline-formula><mml:math id="M88" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">wb</mml:mi></mml:msub></mml:math></inline-formula> can be calculated with Eq. (12):
              <disp-formula id="Ch1.E12" content-type="numbered"><label>12</label><mml:math id="M89" display="block"><mml:mrow><mml:msub><mml:mtext>ET</mml:mtext><mml:mi mathvariant="normal">wb</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi>P</mml:mi><mml:mo>-</mml:mo><mml:mi>R</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>S</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M90" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M91" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>S</mml:mi></mml:mrow></mml:math></inline-formula> are the precipitation (mm yr<inline-formula><mml:math id="M93" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), runoff (mm yr<inline-formula><mml:math id="M94" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), and terrestrial water storage change (mm yr<inline-formula><mml:math id="M95" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), respectively, in a given catchment. Annual <inline-formula><mml:math id="M96" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>S</mml:mi></mml:mrow></mml:math></inline-formula> can be calculated as
the terrestrial water storage anomaly (TWSA) difference between the Decembers of the target year and its previous year. Monthly 0.25<inline-formula><mml:math id="M97" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>-resolution
<inline-formula><mml:math id="M98" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> data (full monthly data version 2020) were downloaded from the Global
Precipitation Climatology Center (GPCC, <uri>http://gpcc.dwd.de/</uri>, last access: 5 October 2021) (Schneider et
al., 2020). <inline-formula><mml:math id="M99" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> data were acquired from the Global Runoff Data Center (GRDC,
<uri>https://portal.grdc.bafg.de/</uri>, last access: 16 October 2021). Monthly 0.5<inline-formula><mml:math id="M100" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>-resolution TWSA data
were obtained from the JPL Mascon RL06 version 2.0 GRACE dataset (Watkins et
al., 2015).</p>
</sec>
<sec id="Ch1.S2.SS3.SSS3">
  <label>2.3.3</label><title>Evaluation via comparison to other commonly used global ET products</title>
      <p id="d1e2187">At the global scale, six commonly used ET products retrieved from different methods were selected for inter-comparison. Among the selected ET products,
three products were based on the PM model with varying resistance
parameterization schemes, i.e., MOD16 (version 6, Mu et al., 2011), P-LSH
(Zhang et al., 2015), and PML (version 2, Zhang et al., 2019), while the
remaining three products were based on the PT model (GLEAM version 3.5a;
Miralles et al., 2011; Martens et al., 2017), land surface models (GLDAS
version 2.1, Beaudoing and Rodell, 2020; Rodell et al., 2004), and machine
learning (Fluxcom; Jung et al., 2019). All products were first resampled to
0.25<inline-formula><mml:math id="M101" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> via the nearest-neighbor method before comparison. Datasets covering the 2003–2013 period were used to maintain the above ET products.
In the comparison process, non-vegetated areas (please refer to the Fluxcom
product) were excluded due to the absence of ET data in certain products,
such as the Fluxcom and MOD16 products.</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="d1e2201">The temporal variations in daily ET estimated from the 3T model
(green line) using EC observations (gray dot). The scatter plot between EC
observations and ET estimates for 1 selected year (with RMSE values at the average level) at 10 EC sites covering various biomes: <bold>(a)</bold> all 126 sites, <bold>(b1, 2)</bold> EBF_AU-Tum (36<inline-formula><mml:math id="M102" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, 148<inline-formula><mml:math id="M103" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) in
2008, <bold>(c1, 2)</bold> SAV_AU-DaS (14<inline-formula><mml:math id="M104" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, 131<inline-formula><mml:math id="M105" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E)
in 2009, <bold>(d1, 2)</bold> DBF_US-UMB (46<inline-formula><mml:math id="M106" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 85<inline-formula><mml:math id="M107" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W)
in 2006, <bold>(e1, 2)</bold> ENF_US-Me2 (44<inline-formula><mml:math id="M108" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 122<inline-formula><mml:math id="M109" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W) in 2008, <bold>(f1, 2)</bold> OSH_US-Whs (32<inline-formula><mml:math id="M110" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N,
110<inline-formula><mml:math id="M111" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W) in 2012, <bold>(g1, 2)</bold> WSA_US-Ton (38<inline-formula><mml:math id="M112" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 120<inline-formula><mml:math id="M113" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W) in 2010, <bold>(h1, 2)</bold> MF_BE-Bra (51<inline-formula><mml:math id="M114" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 5<inline-formula><mml:math id="M115" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) in 2009, <bold>(i1, 2)</bold> CRO_DE-Geb (51<inline-formula><mml:math id="M116" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 11<inline-formula><mml:math id="M117" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) in 2008, <bold>(j1, 2)</bold> WET_CZ-wet (49<inline-formula><mml:math id="M118" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 15<inline-formula><mml:math id="M119" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) in 2009, <bold>(k1, 2)</bold> GRA_AT-Neu (47<inline-formula><mml:math id="M120" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 11<inline-formula><mml:math id="M121" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) in 2009.</p></caption>
            <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022-f02.png"/>

          </fig>

</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Performance of the 3T product versus the global EC network</title>
      <p id="d1e2445">At the daily scale, the 3T model-based ET estimates agreed well with the
observation (<inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">294</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mn mathvariant="normal">058</mml:mn></mml:mrow></mml:math></inline-formula>), with RMSE of 32 W m<inline-formula><mml:math id="M123" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (or 1.1 mm d<inline-formula><mml:math id="M124" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)
(Fig. 2a), which was comparable to other ET products, such as GLDAS (RMSE:
32 W m<inline-formula><mml:math id="M125" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> or 1.1 mm d<inline-formula><mml:math id="M126" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) (Fig. S1), PML (RMSE: 0.7 mm d<inline-formula><mml:math id="M127" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)
(Zhang et al., 2019), and SEBS (RMSE: 1.6 mm d<inline-formula><mml:math id="M128" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) (Chen et al.,
2021). Moreover, the 3T model could capture the change trend of daily ET
because comparison results at 10 EC sites covering various biomes in both
the Southern Hemisphere (Fig. 2b and c) and Northern Hemisphere (Fig. 2d–k) indicate that interannual variabilities of the estimates were close to that of the
observed ET. A comparison at an instantaneous 3 h scale was also
performed to test the ET estimates. EC observations across the world for the
15th day of each month in 2011 (<inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">6278</mml:mn></mml:mrow></mml:math></inline-formula>) were compared because the data are
too large to perform an entire comparison at a global scale. Although the
RMSE (74 W m<inline-formula><mml:math id="M130" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) was slightly greater than that at the daily scale (Fig. S2a), the 3T model-based ET estimates at the 3 h scale agree well with the GLDAS ET, with an <inline-formula><mml:math id="M131" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> of 0.89 and a RMSE of 21 W m<inline-formula><mml:math id="M132" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (Fig. S2b). The
explanation is likely that high temporal data may encounter missing values,
which complicates the comparison.</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="d1e2581">Comparison of the estimated (3T model) and measured (EC tower)
monthly ET values from 2003 to 2013, where panel <bold>(a)</bold> shows the data for all 126 sites on a multi-year monthly mean (MYM) scale and panel <bold>(b)</bold> shows the data for
all sites on an annual mean (AM) monthly scale. Panels <bold>(c)</bold>–<bold>(l)</bold> show all land use/land cover types on an annual monthly scale. The abbreviations in
panels <bold>(c)</bold>–<bold>(l)</bold> are the same as those in Fig. 1.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022-f03.png"/>

        </fig>

      <p id="d1e2609">At the monthly scale, the paired ET values between the 3T model and EC
observations were generally distributed on both sides of the <inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> line,
revealing relatively large differences at a few points for ET values higher
than 100 mm month<inline-formula><mml:math id="M134" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and resulting in regression line slope and <inline-formula><mml:math id="M135" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> values
of 0.75 and 0.80, respectively (Fig. 3a). The RMSE and RB values between the
ET estimates and EC-based observations reached 22.85 mm month<inline-formula><mml:math id="M136" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and
<inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.2</mml:mn></mml:mrow></mml:math></inline-formula> %, respectively. If monthly data were compared, similar results could
be obtained, with an RMSE value of 24.90 mm month<inline-formula><mml:math id="M138" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, an RB value of
0.7 %, and regression line slope and <inline-formula><mml:math id="M139" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> values of 0.75 and 0.78,
respectively (Fig. 3b). The errors in the 3T model-based ET estimates were
comparable to those in the other ET products (please refer to Sect. 3.3
for details). For example, compared to EC observations, the RMSE and <inline-formula><mml:math id="M140" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> values of an ET product retrieved from the process-based Breathing Earth
System Simulator (BESS) model reached 23.4 mm month<inline-formula><mml:math id="M141" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 0.79,
respectively (Jiang and Ryu, 2016). These results indicate that the ET
product developed based on the 3T model agreed well with global EC
observations at multi-temporal scales.</p>
      <p id="d1e2705">The performance of the 3T model in the different biomes was further analyzed (Fig. 3c–l). Due to data point separation in Fig. 3b, the results shown in Fig. 3c–l are similar to those shown in Fig. 3b, with slight differences
among the various biomes. The 3T model performed the best at forest sites
because the paired data points were more closely distributed along the <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>
line, with slope values ranging from 0.81 to 1.05, whereas the <inline-formula><mml:math id="M143" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> values
ranged from 0.75 to 0.85 (Fig. 3e–h). Among the different forest cover types, the ET estimates at the MF and ENF sites exhibited a lower
uncertainty, with RMSE and RB values of 20.3 mm month<inline-formula><mml:math id="M144" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 13.3 %,
respectively, at the former sites and values of 22.8 mm month<inline-formula><mml:math id="M145" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and
10.4 %, respectively, at the latter sites, followed by DBF (RMSE <inline-formula><mml:math id="M146" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 24.2 mm month<inline-formula><mml:math id="M147" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and RB <inline-formula><mml:math id="M148" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 25.8 %) and EBF sites (RMSE <inline-formula><mml:math id="M149" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 29.7 mm month<inline-formula><mml:math id="M150" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>
and RB <inline-formula><mml:math id="M151" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 4.6 %). The 3T model performance at the shrubland sites was
similar to that at the MF sites (RMSE <inline-formula><mml:math id="M152" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 20.6 mm month<inline-formula><mml:math id="M153" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and
RB <inline-formula><mml:math id="M154" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 9.2 %) but with lower slope and <inline-formula><mml:math id="M155" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> values of 0.53 and 0.60,
respectively (Fig. 3i). At the sites of the remaining land use/land cover
(LULC) types, the 3T model yielded lower ET estimates than the EC
observations as the RB value ranged from <inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6.1</mml:mn></mml:mrow></mml:math></inline-formula> % to <inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">33.8</mml:mn></mml:mrow></mml:math></inline-formula> % (Fig. 3c,
d, and j to l). Among these sites, the 3T model exhibited the lowest bias
at the GRA sites, with slope, <inline-formula><mml:math id="M158" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula>, and RMSE values of 0.71, 0.82, and 21.4 mm month<inline-formula><mml:math id="M159" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively (Fig. 3j), followed by the SAV (slope <inline-formula><mml:math id="M160" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.67, <inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.83</mml:mn></mml:mrow></mml:math></inline-formula>, and RMSE <inline-formula><mml:math id="M162" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 27.7 mm month<inline-formula><mml:math id="M163" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) (Fig. 3k), CRO (slope <inline-formula><mml:math id="M164" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.61,
<inline-formula><mml:math id="M165" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.78</mml:mn></mml:mrow></mml:math></inline-formula>, and RMSE <inline-formula><mml:math id="M166" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 27.9 mm month<inline-formula><mml:math id="M167" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) (Fig. 3c), WET (slope <inline-formula><mml:math id="M168" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.65,
<inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.74</mml:mn></mml:mrow></mml:math></inline-formula>, and RMSE <inline-formula><mml:math id="M170" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 28.3 mm month<inline-formula><mml:math id="M171" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) (Fig. 3d), and WSA sites
(slope <inline-formula><mml:math id="M172" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.49, <inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.70</mml:mn></mml:mrow></mml:math></inline-formula>, and RMSE <inline-formula><mml:math id="M174" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 31.7 mm month<inline-formula><mml:math id="M175" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) (Fig. 3l). The 3T
model performance among the different biomes, with a maximum RMSE value of
31.7 mm month<inline-formula><mml:math id="M176" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, was comparable to that of the other methods based on
the above comparison to EC observations, with RMSE values ranging from 30 to
42.9 mm month<inline-formula><mml:math id="M177" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, as reported by Carter and Liang (2018), Zhang et al. (2019), and Peng et al. (2021). These results suggest that the 3T model
performed with an acceptable accuracy across the various biomes.</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="d1e3059">Comparison of the annual model-estimated (3T model) and
water-balance-based ET values during the 2003–2013 period: <bold>(a)</bold> multi-year
mean annual scale, <bold>(b)</bold> annual scale, and <bold>(c)</bold> relative bias (RB) in each basin.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022-f04.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Performance of the 3T product versus the water budget in global
catchments</title>
      <p id="d1e3085">Multi-year (2003–2013) average ET values for 34 relatively large watersheds
were obtained with the 3T model and compared to water balance ET (ET<inline-formula><mml:math id="M178" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">wb</mml:mi></mml:msub></mml:math></inline-formula>)
data. The estimated mean ET value was 514.5 mm yr<inline-formula><mml:math id="M179" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, with a standard
deviation of 211 mm yr<inline-formula><mml:math id="M180" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, whereas the mean ET<inline-formula><mml:math id="M181" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">wb</mml:mi></mml:msub></mml:math></inline-formula> value reached
<inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:mn mathvariant="normal">476.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">280</mml:mn></mml:mrow></mml:math></inline-formula> mm yr<inline-formula><mml:math id="M183" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The mean ET difference reached only 38 mm yr<inline-formula><mml:math id="M184" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, indicating that the ET estimates obtained with the 3T model were
similar to the ET<inline-formula><mml:math id="M185" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">wb</mml:mi></mml:msub></mml:math></inline-formula> values. The scatter plots shown in Fig. 4a and
b at multi-year and annual scales, respectively, also confirmed that these
two types of ET values agreed well, with r values of 0.94 and 0.91,
respectively. The regression line slope at the multi-year scale was 0.71,
with RMSE and RB values of 116 mm yr<inline-formula><mml:math id="M186" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 8.0 %, respectively (Fig. 4a), whereas the values reached 0.69, 128 mm yr<inline-formula><mml:math id="M187" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, and 9.1 %,
respectively, at the annual scale (Fig. 4b). Figure 4c shows the 3T model
performance in each watershed in terms of RB. The RB values in nearly 70 % of the watersheds were relatively low, within <inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">25</mml:mn></mml:mrow></mml:math></inline-formula> %, indicating
satisfactory performance of the 3T model in these watersheds. However, the
3T model overestimated ET in approximately 21 % of all watersheds, with RB values greater than 60 % (the red color in Fig. 4c). These river basins were mainly located at high latitudes (approximately 60<inline-formula><mml:math id="M189" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N)
with relatively low ET<inline-formula><mml:math id="M190" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">wb</mml:mi></mml:msub></mml:math></inline-formula> values (<inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:mn mathvariant="normal">133</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula> mm yr<inline-formula><mml:math id="M192" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). ET
overestimation in these regions was not only observed in this study, but was also observed in other ET comparison-based studies, such as Ma et al. (2021). A possible reason for the higher uncertainty may be that a higher bias occurs
in the hydrological (e.g., runoff) and gridded meteorological (e.g.,
precipitation) data employed in the water balance equation due to the
scarcity of in situ observational stations in these regions (Ma et al.,
2021). Nonetheless, the above results generally suggest that the 3T model
performance was comparable to that of the water balance equation.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e3255">Validation of six commonly used ET products (GLDAS, PML, P-LSH, GLEAM, Fluxcom, and MOD16) against EC tower observations. The data are
monthly average ET values over the 2003–2013 period and are the same as
those used in Fig. 3a.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022-f05.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Comparison of the 3T product to other global ET products</title>
      <p id="d1e3272">To further assess the performance of the 3T model across the various
terrestrial land types, 3T model-based ET estimates were cross-validated against six global ET products during the 2003–2013 period.</p>
      <p id="d1e3275">When EC observation data were adopted as a reference, 3T model-based ET
estimates were comparable to GLDAS, GLEAM, and MOD16 data in terms of <inline-formula><mml:math id="M193" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> and
RMSE, with values of 0.8 and 22 mm month<inline-formula><mml:math id="M194" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively (Figs. 3a and
5a–c). Although the slope of the regression line (0.75, as shown
in Fig. 3a) between the 3T model-based ET estimates and observations was
slightly lower than that between the ET estimates and GLDAS (0.83, as shown
in Fig. 5a) and GLEAM data (0.79, as shown in Fig. 5b) and slightly higher
than that between the ET estimates and MOD16 data (0.73, as shown in Fig. 5c), the absolute RB value of the 3T model was lower than that of the GLDAS
(1.9 %, as shown in Fig. 5a), GLEAM (2.7 %, as shown in Fig. 5b), and
MOD16 products (<inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4.7</mml:mn></mml:mrow></mml:math></inline-formula> %, as shown in Fig. 5c). The remaining three
products, i.e., Fluxcom, PML, and P-LSH, exhibited limited comparative
advantages, with an <inline-formula><mml:math id="M196" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> value of 0.9, a slope higher than 0.8 (0.92, 0.84, and
0.83, respectively), and an RMSE value ranging from 16.9 to 18.6 mm month<inline-formula><mml:math id="M197" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e3328">Validation of six commonly used ET products (GLDAS, PML, P-LSH, GLEAM, Fluxcom, and MOD16) against values obtained with the catchment water
balance approach. The data are yearly average values over the 2003–2013
period. The left column shows mean annual values, and the right column shows the RB in each catchment.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022-f06.png"/>

        </fig>

      <p id="d1e3338">When ET<inline-formula><mml:math id="M198" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">wb</mml:mi></mml:msub></mml:math></inline-formula> values were adopted as a reference, although the 3T model
performance was slightly lower than that of the PML, GLEAM, and P-LSH
products in terms of RMSE, with a value of 116 mm month<inline-formula><mml:math id="M199" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> versus values
of 96, 111, and 115 mm month<inline-formula><mml:math id="M200" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively (Figs. 4a and 6a–c), the 3T model performed better than did the GLDAS (RMSE <inline-formula><mml:math id="M201" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 120 mm month<inline-formula><mml:math id="M202" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), Fluxcom (RMSE <inline-formula><mml:math id="M203" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 149 mm month<inline-formula><mml:math id="M204" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), and MOD16 products
(RMSE <inline-formula><mml:math id="M205" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 182 mm month<inline-formula><mml:math id="M206" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) (Fig. 6d–f). In terms of the regression
line between the ET estimates and ET<inline-formula><mml:math id="M207" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">wb</mml:mi></mml:msub></mml:math></inline-formula>, except for the relatively low
performance of MOD16, for slope and <inline-formula><mml:math id="M208" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> values of 0.58 and 0.77, respectively,
<inline-formula><mml:math id="M209" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> values of the other ET products were greater than 0.94 and exhibited a
slight difference, with a maximum difference of 0.03, but the slope (0.71,
as shown in Fig. 4a) of the regression line between the ET<inline-formula><mml:math id="M210" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">wb</mml:mi></mml:msub></mml:math></inline-formula> values and
3T model-based ET estimates was lower than that between the ET<inline-formula><mml:math id="M211" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">wb</mml:mi></mml:msub></mml:math></inline-formula> values
and Fluxcom (1.13), P-LSH (0.92), PML (0.83), GLDAS (0.80), and GLEAM data
(0.76) (Fig. 6). However, the absolute RB, with a value of 8 % (Fig. 4a),
of the 3T model was the smallest, while the absolute RB values of the other
six products were greater than 8 %, ranging from 8.2 % to 21.8 % (Fig. 6).</p>
      <p id="d1e3474">Via comparison of the terrestrial (excluding Antarctica) ET values retrieved
from the various ET products, the mean ET value of the 3T model reached 546 mm yr<inline-formula><mml:math id="M212" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> during the 2003–2013 period, whereas the mean ET values
obtained with the MOD16, PML, GLEAM, Fluxcom, GLDAS, and P-LSH products
reached 468, 542, 544, 549, 551, and 551 mm yr<inline-formula><mml:math id="M213" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e3503"><bold>(a)</bold> Monthly variation and <bold>(b)</bold> annual latitudinal distributions of
the multi-year (2003–2013) mean ET value estimated with the 3T model (black
line) and six ET products in vegetated areas (mainly excluding Greenland, Antarctica, and desert areas, according to Jung et al., 2019).</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022-f07.png"/>

        </fig>

      <p id="d1e3517">In terms of interannual variation (excluding Antarctica, Greenland, and
desert areas according to Jung et al., 2019), the 3T model-based estimates
were similar to the other six ET products, with an increasing trend from January (approximately 40 mm month<inline-formula><mml:math id="M214" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) to July (approximately 65 mm month<inline-formula><mml:math id="M215" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)
and then a decreasing trend through the following months (Fig. 7a). The latitudinal distribution of the values obtained with each ET
product was also determined, and the changing trend of the 3T model-based ET
values was similar to that of the values obtained with the six considered ET
products (Fig. 7b). Specifically, the highest terrestrial ET values occurred
at the Equator, with values ranging from 1251 to 1390 mm yr<inline-formula><mml:math id="M216" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (1293 mm yr<inline-formula><mml:math id="M217" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for the 3T model), and the ET value decreased towards the North Pole and South Pole. In the Northern Hemisphere, ET attained a second peak at
approximately 20<inline-formula><mml:math id="M218" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, with values ranging from 934 to 1111 mm yr<inline-formula><mml:math id="M219" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (950 mm yr<inline-formula><mml:math id="M220" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for the 3T model), whereas a third peak occurred
from 37 to 45<inline-formula><mml:math id="M221" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (the third peak varied among
the different ET products) in the Southern Hemisphere, with values ranging
from 562 to 706 mm yr<inline-formula><mml:math id="M222" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (690 mm yr<inline-formula><mml:math id="M223" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for the 3T model). This ET
peak distribution trend was correlated with the global vegetation
distribution. However, it should be noted that the ET values obtained with
the 3T model were generally lower than those obtained with the ET products
between approximately 30<inline-formula><mml:math id="M224" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and 45<inline-formula><mml:math id="M225" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N (except MOD16), and a large discrepancy in ET estimates occurred,
particularly between approximately 17<inline-formula><mml:math id="M226" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and
17<inline-formula><mml:math id="M227" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, where the difference could exceed 350 mm yr<inline-formula><mml:math id="M228" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. These results suggest that even though the ET products are
similar, the ET estimates in certain areas may differ, and uncertainty may
exist in ET estimates in these regions.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e3686">Spatial pattern and pixel-to-pixel comparison of multi-year
(2003–2013) global mean annual ET rates among the 3T model, the GLDAS, and GLEAM. Left column: spatial ET distribution of <bold>(a)</bold> 3T model-, <bold>(b)</bold> GLDAS-, and <bold>(c)</bold> GLEAM-based ET values. Right column: pixel-to-pixel comparison of ET values between <bold>(d)</bold> the 3T model and the GLDAS and <bold>(e)</bold> the 3T model and GLEAM.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022-f08.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9"><?xmltex \currentcnt{9}?><?xmltex \def\figurename{Figure}?><label>Figure 9</label><caption><p id="d1e3713">RMSE and <inline-formula><mml:math id="M229" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> of pixel-to-pixel (0.25<inline-formula><mml:math id="M230" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> resolution)
comparison of multi-year (2003–2013) mean annual ET values among the 3T
model and six products in vegetated areas (mainly excluding Greenland, Antarctica, and desert areas, according to Jung et al., 2019).</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022-f09.png"/>

        </fig>

      <p id="d1e3738">Pixel-by-pixel comparison of the various ET products was also conducted. To
overcome the influence of the resampling method on the obtained ET values,
only GLDAS and GLEAM data, sharing the same spatial resolution as the 3T model-based estimates (0.25<inline-formula><mml:math id="M231" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>), are shown in Fig. 8. The left
column shows the global land ET distribution, and the 3T model-based ET values generally exhibited a similar distribution to that of the ET values
obtained with the two ET products, as shown in Fig. 8. However, obvious
differences existed, especially in arid regions such as the Sahara, the Middle East, Mongolia, and the southeast of the Qinghai–Tibet Plateau, where the 3T model-based ET estimates were higher than the values obtained with the two
ET products. The scatter plots in the right column of Fig. 8 reveal that the 3T model-based ET estimates were very similar to the GLDAS-based ET values.
Moreover, the slope of the regression line between the 3T model- and
GLDAS-based ET values was 0.93, with <inline-formula><mml:math id="M232" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> and RMSE values of 0.95 and 114.6 mm yr<inline-formula><mml:math id="M233" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively (Fig. 8d), whereas the values reached 0.89, 0.94, and 130.6 mm yr<inline-formula><mml:math id="M234" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively, between the 3T model and GLEAM (Fig. 8e).
RMSE and <inline-formula><mml:math id="M235" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> statistics between the 3T model-based ET estimates and the values
obtained with each ET product were visualized in a heatmap (Fig. 9) in which the darker the blue color is, the higher the <inline-formula><mml:math id="M236" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> value and the lower the RMSE value are. Overall, the 3T model-based ET product is consistent with
the other six products, with <inline-formula><mml:math id="M237" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> ranging from 0.89 (compared to MOD16) to 0.96 (compared to GLDAS) and RMSE ranging from 108.5 (compared to the GLDAS) to 177.7 (compared to MOD16) mm yr<inline-formula><mml:math id="M238" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Interestingly, it was obvious that the 3T
model-based, GLDAS, and PML products with the same model inputs were highly
consistent according to the higher <inline-formula><mml:math id="M239" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> and lower RMSE values (the
corresponding blue cubes are in the bottom left of Fig. 9), while the ET
products calibrated or upscaled based on EC towers, i.e., PML, P-LSH, and
Fluxcom, were highly consistent (the corresponding blue cubes are in the top
right of Fig. 9).</p>
      <p id="d1e3822">The abovementioned results indicate that the 3T model-based ET estimates
were comparable to the data obtained with the commonly used global ET
products.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e3828">Information on the typical ET products used to cross-validate the ET estimates of the 3T model in this study.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="4cm"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="3cm"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1">ET products</oasis:entry>

         <oasis:entry colname="col2">Method</oasis:entry>

         <oasis:entry colname="col3">Spatial–temporal resolution</oasis:entry>

         <oasis:entry colname="col4">Reference</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>

         <oasis:entry colname="col1">Fluxcom</oasis:entry>

         <oasis:entry colname="col2">Machine learning</oasis:entry>

         <oasis:entry colname="col3">0.083<inline-formula><mml:math id="M240" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> monthly</oasis:entry>

         <oasis:entry colname="col4">Jung et al. (2019)</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">GLDAS</oasis:entry>

         <oasis:entry colname="col2">Land surface models</oasis:entry>

         <oasis:entry colname="col3">0.25<inline-formula><mml:math id="M241" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?>3-hourly and monthly</oasis:entry>

         <oasis:entry colname="col4">Beaudoing and Rodell (2020), Rodell et al. (2004)</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">GLEAM</oasis:entry>

         <oasis:entry colname="col2">Priestley–Taylor equation</oasis:entry>

         <oasis:entry colname="col3">0.25<inline-formula><mml:math id="M242" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> monthly</oasis:entry>

         <oasis:entry colname="col4">Martens et al. (2017), Miralles et al. (2011)</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">MOD16</oasis:entry>

         <?xmltex \mrwidth{4cm}?><oasis:entry colname="col2" morerows="2">Penman–Monteith equation with different resistance parameterization methods</oasis:entry>

         <oasis:entry colname="col3">0.05<inline-formula><mml:math id="M243" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> monthly</oasis:entry>

         <oasis:entry colname="col4">Mu et al. (2011)</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">P-LSH</oasis:entry>

         <oasis:entry colname="col3">0.05<inline-formula><mml:math id="M244" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> monthly</oasis:entry>

         <oasis:entry colname="col4">Zhang et al. (2015)</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">PML</oasis:entry>

         <oasis:entry colname="col3">0.083<inline-formula><mml:math id="M245" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> 8 d</oasis:entry>

         <oasis:entry colname="col4">Zhang et al. (2019)</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3"><?xmltex \currentcnt{3}?><label>Table 3</label><caption><p id="d1e4010">Multi-year (2003–2013) average ET values considering the water
depth (mm yr<inline-formula><mml:math id="M246" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) and volume (km<inline-formula><mml:math id="M247" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M248" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) of the different
products used in this study for the global land surface.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <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:thead>
       <oasis:row>
         <oasis:entry colname="col1">ET products</oasis:entry>
         <oasis:entry colname="col2">ET rate</oasis:entry>
         <oasis:entry colname="col3">ET volume</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(mm yr<inline-formula><mml:math id="M251" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3">(<inline-formula><mml:math id="M252" display="inline"><mml:mrow><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M253" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M254" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">3T</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M255" display="inline"><mml:mrow><mml:mn mathvariant="normal">546</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">22</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M256" display="inline"><mml:mrow><mml:mn mathvariant="normal">73.8</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">3.0</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Fluxcom</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M257" display="inline"><mml:mrow><mml:mn mathvariant="normal">549</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M258" display="inline"><mml:mrow><mml:mn mathvariant="normal">74.2</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GLDAS</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M259" display="inline"><mml:mrow><mml:mn mathvariant="normal">551</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M260" display="inline"><mml:mrow><mml:mn mathvariant="normal">74.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.3</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GLEAM</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M261" display="inline"><mml:mrow><mml:mn mathvariant="normal">544</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M262" display="inline"><mml:mrow><mml:mn mathvariant="normal">73.6</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MOD16</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M263" display="inline"><mml:mrow><mml:mn mathvariant="normal">468</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M264" display="inline"><mml:mrow><mml:mn mathvariant="normal">63.3</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">P-LSH</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M265" display="inline"><mml:mrow><mml:mn mathvariant="normal">551</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M266" display="inline"><mml:mrow><mml:mn mathvariant="normal">74.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PML</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M267" display="inline"><mml:mrow><mml:mn mathvariant="normal">542</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">12</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M268" display="inline"><mml:mrow><mml:mn mathvariant="normal">73.2</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.7</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p id="d1e4046">Note: the global land surface has an area of <inline-formula><mml:math id="M249" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.35</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M250" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>, excluding Antarctica. Fluxcom and MOD16 do not provide ET values in Greenland and desert areas.</p></table-wrap-foot></table-wrap>

</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Discussion</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Characteristics of the global terrestrial ET product based on the 3T
model</title>
      <p id="d1e4400">As indicated in Sect. 3, the 3T model-based global terrestrial ET product
agreed well with ground observations and was comparable to other commonly
used ET products. Particularly, the determined global terrestrial (excluding
Antarctica) ET volume (in units of 10<inline-formula><mml:math id="M269" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> km<inline-formula><mml:math id="M270" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M271" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) based on 3T
model-based estimates reached 73.8 from 2003 to 2013, which is not only consistent with that determined based on the other ET products (excluding
MOD16), as indicated in Sect. 3.3, ranging from 73.2 to 74.5 (Table 3),
but also consistent with values reported in other studies, e.g., <inline-formula><mml:math id="M272" display="inline"><mml:mrow><mml:mn mathvariant="normal">72.3</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.9</mml:mn></mml:mrow></mml:math></inline-formula>, as obtained with a complementary relationship-based ET product from
1982 to 2016 (Ma et al., 2021), and 71.1, as determined with a water-balance- and machine-learning-based ET product from 1982 to 2009 (Zeng et al., 2014).</p>
      <p id="d1e4445">It should be noted that the 3T model differed from the methods used to
estimate ET in the adopted ET products, as listed in Table 2. In particular,
the 3T model excludes resistance and requires no parameter calibration.
Resistance terms are unavoidable in PM models, which could lead to high uncertainty in ET estimates (Zhao et al., 2020; Cao et al., 2021). As
described in Sect. 3.3, the MOD16, P-LSH, and PML products, based on the
PM equation with varied resistance parameterization methods, exhibited
obvious differences (e.g., 300 mm yr<inline-formula><mml:math id="M273" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> at a few locations, as shown in
Fig. 7b) and performed differently via a comparison to ground observations.
This occurred because the canopy resistance is difficult to estimate, in
addition to the empirical relationship adopted in the estimation process. These empirical equations are site- and biome-specific equations and normally
require calibration (Mu et al., 2011; Zhang et al., 2015,
2019). Because a large number of EC tower sites are used for calibration in resistance estimation in P-LSH and PML, these two products performed better
than MOD16, using only 46 sites (Figs. 5 and 6). Nonetheless, calibration typically requires observational data, while limited in situ observations
restrict accurate calibration of biome-specific coefficients on a global
scale. A recent study confirmed that models requiring no calibration could
decrease the uncertainty in global ET estimates (Ma et al., 2021). The
obtained results indicate that the 3T model-based ET product achieved a
lower uncertainty than that achieved by MOD16 retrieved from the PM equation
with a complex resistance parameterization scheme and limited calibration
and that the 3T model-based ET product was comparable to P-LSH and PML
developed from the PM equation with adequate calibration during resistance
parameterization.</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="d1e4462">Comparison of the estimated (3T model) and measured ET values in
2011 (daily ET from EC tower and annual ET from the water balance equation). The left column shows ET estimates using Köppen–Geiger climate regimes with 31 subregions at the daily <bold>(a)</bold> and annual <bold>(c)</bold> scales, respectively, whereas the
right column is the same but with ET estimates using 90–110 subregions.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022-f10.png"/>

        </fig>

      <p id="d1e4478">Although the 3T model-based ET estimates suffer from the domain size when
determining the reference site, the uncertainty may be limited. We tested
the difference between the 3T model-based ET values estimated using two
different regimes with different subregions and sizes. Specifically,
Köppen–Geiger climate regimes with 31 subregions and detailed subregions with numbers of 90–110 were used. In general, the two groups of daily ET
estimates in 2011 showed little difference, with mean ET values of 47 and 42 W m<inline-formula><mml:math id="M274" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively, and were close to the EC observation, with RMSE values of 32 and 33 W m<inline-formula><mml:math id="M275" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (Fig. 10a and b, respectively). At a
yearly scale, however, the 3T model-based ET estimates from 90 to 110 subregions (Fig. 10d) were much closer to the water balance ET than those
estimates using 31 subregions (Fig. 10c). The results indicate that the smaller the domain size of a region where the reference parameters were
obtained, the more accurate the 3T model, which is consistent with our previous findings (Xiong et al., 2015, 2019).</p>
      <p id="d1e4505">In addition, the 3T model-based global terrestrial ET product required fewer data in terms of model inputs than those required by the adopted ET
products, as listed in Table 2. Specifically, the 3T model requires net
radiation, soil heat flux, air temperature, LST, and vegetation index (i.e.,
NDVI) data to decompose the radiation (or LST) components of vegetation and
soil. For example, PM-based ET estimation requires wind speed and VPD data in addition to net radiation, soil heat flux, and air temperature data.
However, wind speed and VPD data, especially the former, exhibit high
heterogeneity in space, and current commonly used reanalysis datasets
contain high uncertainty; e.g., the difference in wind speed can exceed 5 m s<inline-formula><mml:math id="M276" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> among several products (Yang et al., 2019), thus increasing bias in global ET products. While a model with a higher complexity may better
describe the ET process, a satisfactory model performance normally depends
on abundant data, not only regarding model inputs, but also regarding model (or parameter) calibration (Medici et al., 2012; Wu et al., 2020).
Otherwise, a relatively simple model with fewer input datasets could be more
reasonable; e.g., the GLEAM product based on the PT method, a simplified version of the PM equation, outperformed the PM-based MOD16 product in this
and other studies (e.g., Cao et al., 2021). Although the performance of the
3T model-based ET product was similar to that of the GLEAM product, an
empirical parameter, namely, the PT coefficient, is required in the PT-based
GLEAM product. In estimation with the GLEAM product, the PT coefficient was
set to 0.8 for tall canopies and 1.26 for short vegetation and bare soil,
respectively (Miralles et al., 2011), but the value varies among the
different biomes (e.g., Komatsu, 2005), especially on a short timescale (daily) (Guo et al., 2015). In fact, the input datasets of the 3T model are
commonly available with an adequate credibility (Bao and Zhang, 2013; Cao
et al., 2022; Fu and Wang, 2014; Ji et al., 2015; Peng et al., 2019; Xu et
al., 2019; X. Zhang et al., 2016; Zhou et al., 2017), resulting in easy model
application.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><?xmltex \currentcnt{11}?><?xmltex \def\figurename{Figure}?><label>Figure 11</label><caption><p id="d1e4522">Monitoring performance of the 3T model-based terrestrial ET
product under extreme heat conditions in the different biomes. The daily ET
is shown in energy units. In the box plot <bold>(a)</bold>, the black point indicates the
mean, while the central line in the box indicates the median value. The edges of the box indicate the 25th and 75th percentiles, and the whiskers indicate
the outlier values. In the violin plot <bold>(b)</bold>, the white point indicates the
median value, and a wider violin plot indicates denser data for the same
RMSE value. <inline-formula><mml:math id="M277" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> denotes the number of data points.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022-f11.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>The 3T model-based terrestrial ET product for extreme weather condition
monitoring</title>
      <p id="d1e4552">Although the 3T model is the most sensitive to the LST among the various
model inputs (Xiong and Qiu, 2011), this characteristic may result in a
suitable model ability in capturing ET variation during extreme-temperature
events such as heat waves and flash droughts. Since both the frequency and damage extent of heat waves and flash droughts are increasing, these extreme
weather conditions have attracted extensive attention worldwide (IPCC,
2022). For instance, Senay et al. (2020) applied a temperature-sensitive
model, i.e., the Operational Simplified Surface Energy Balance (SSEBop)
model, to estimate ET and used its anomalies to successfully detect the
2011/2012 drought in the southern–central United States and the 2005 drought in Australia. However, this study mainly used relatively low ET values to
qualitatively describe droughts, while few studies focused on the accuracy of ET estimates under similar extreme conditions (i.e., heat and drought
conditions). Hence, this section further examines the 3T model-based
terrestrial ET product for extreme weather condition monitoring by
validating its performance against EC flux tower observations under extreme
heat, extreme atmospheric drought, and extreme soil drought conditions.
These three types of extreme hazards were defined according to daily
observations from 2001 to 2020 retrieved from FLUXNET and GLDAS reanalysis data (version 2.1) based on corresponding site locations: (1) extreme heat
conditions occur when the daily <inline-formula><mml:math id="M278" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> at a given EC tower site is higher
than the 95th percentile of the daily <inline-formula><mml:math id="M279" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> in GLDAS data, (2) extreme atmospheric drought conditions occur when the daily VPD at a given EC tower
location is higher than the 95th percentile of the daily VPD in GLDAS data, and (3) extreme soil drought conditions occur when the daily soil moisture
matches the 5th percentile of EC tower data. It should be mentioned that
some data points indicated both extreme heat and extreme atmospheric drought
conditions. These points were designated as extreme heat conditions instead
of extreme atmospheric drought conditions. Finally, there remained 11 213
data points across 80 sites, 19 687 data points across 112 sites, and 12 338
data points across 95 sites representing extreme heat, extreme atmospheric
drought, and extreme soil drought conditions, respectively. GLDAS estimates,
with a high temporal resolution in the monitoring of extreme events (Liu et
al., 2019) and the same spatiotemporal input datasets such as those employed for the 3T model, were also used in the analysis.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12" specific-use="star"><?xmltex \currentcnt{12}?><?xmltex \def\figurename{Figure}?><label>Figure 12</label><caption><p id="d1e4579">Monitoring performance of the 3T model-based terrestrial ET
product under extreme atmospheric drought conditions in the different
biomes. The symbols are the same as those in Fig. 11.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022-f12.png"/>

        </fig>

      <p id="d1e4588">Under extreme heat conditions (Fig. 11), although the 3T model-based ET
product exhibited various performance levels in the different biomes, the
product generally yielded results closely agreeing with observations. In
terms of the mean ET value, extreme heat conditions at the DBF, WET, OSH,
MF, CRO, and ENF sites were best captured with the 3T model-based ET product (Fig. 11a), with a maximum difference of 11.9 W m<inline-formula><mml:math id="M280" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> from EC
observations, followed by the GRA, WSA, SAV, and EBF sites with difference
values ranging from 24.0 to 51.1 W m<inline-formula><mml:math id="M281" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The GLDAS performed similarly
to the 3T model-based ET product but with a notably higher bias than that of EC observations. The RMSE violin plots shown in Fig. 11b further verify
the above statement because the RMSE values obtained with the 3T model-based
ET product, with median values of 23.6, 29.0, 15.3, 31.2, and 24.4 W m<inline-formula><mml:math id="M282" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> at the OSH, ENF, WET, CRO, and MF sites, respectively, were much
smaller than those obtained with the GLDAS (37.9, 37.4, 19.9, 35.2, and 28.2 W m<inline-formula><mml:math id="M283" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively). The maximum RMSE values obtained with the 3T
model-based ET product were also smaller than those obtained with the GLDAS,
48.3, 20.6, 20.2, 15.6, and 14.1 W m<inline-formula><mml:math id="M284" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> lower at the CRO, DBF, OSH, WET,
and MF sites, respectively. These results indicate that the 3T model-based
ET product could accurately capture the low ET values under extreme heat
conditions in most biomes and performed better than did the GLDAS.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F13" specific-use="star"><?xmltex \currentcnt{13}?><?xmltex \def\figurename{Figure}?><label>Figure 13</label><caption><p id="d1e4654">Monitoring performance of the 3T model-based terrestrial ET
product under extreme soil drought conditions in the different biomes. The
symbols are the same as those in Fig. 11.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://essd.copernicus.org/articles/14/3673/2022/essd-14-3673-2022-f13.png"/>

        </fig>

      <p id="d1e4663">Under extreme atmospheric drought conditions (Fig. 12), in terms of the mean ET value, the 3T model-based ET product suitably captured extreme
atmospheric drought conditions at the OSH, ENF, MF, DBF, GRA, WET, CRO, and
WSA sites (Fig. 12a), with a maximum difference of 14.5 W m<inline-formula><mml:math id="M285" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> from EC
observations, followed by the SAV and EBF sites, with difference values ranging from 18.2 to 29.7 W m<inline-formula><mml:math id="M286" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The GLDAS also performed similarly to
the 3T model-based ET product but with a higher bias over EC observations, which was further confirmed by the RMSE violin plots shown in Fig. 12b. The
median RMSE values obtained with the 3T model-based ET product (the white
points in Fig. 12b) reached 30.7, 22.2, 26.2, 21.0, and 12.7 W m<inline-formula><mml:math id="M287" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> at
the CRO, MF, ENF, SAV, and WET sites, respectively, while the values
obtained with the GLDAS reached 38.4, 27.4, 29.0, 22.9, and 14.4,
respectively. The above results indicate that the 3T model-based ET product
could accurately capture the low ET values under extreme atmospheric drought
conditions at the CRO, MF, ENF, and WET sites and performed better than did
the GLDAS.</p>
      <p id="d1e4702">Under extreme soil drought conditions (Fig. 13), in terms of the mean ET value, the 3T model-based ET product suitably captured extreme soil drought
conditions at the GRA, OSH, MF, WSA, WET, CRO, DBF, and ENF sites (Fig. 13a), with a maximum difference of 7.2 W m<inline-formula><mml:math id="M288" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> from EC observations,
followed by the SAV and EBF sites with difference values ranging from 13.2 to 25.5 W m<inline-formula><mml:math id="M289" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The median RMSE values obtained with the 3T model-based
ET product (the white points in Fig. 13b) at the SAV, EBF, CRO, OSH, and ENF
sites reached 18.9, 23.2, 18.2, 5.4, and 15.3 W m<inline-formula><mml:math id="M290" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively,
while the values obtained with the GLDAS reached 23.8, 26.4, 20.0, 6.9, and
15.8, respectively. In addition, compared to the GLDAS, the maximum RMSE
values obtained with the 3T model-based ET product at the ENF, EBF, CRO,
WET, and SAV sites were reduced by 55.6, 18.5, 14.0, 9.3, and 3.0 W m<inline-formula><mml:math id="M291" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively. The acquired results indicate that the 3T model-based ET
product could accurately capture the low ET values under extreme atmospheric
drought conditions at the CRO, EBF, and ENF and performed better than did
the GLDAS.</p>
      <p id="d1e4753">It should be noted that the 3T model-based ET product exhibited a good
performance in crop ET estimation under these three types of extreme
conditions. Compared to the GLDAS, the 3T model-based ET estimates were
closer to the considered EC observations and exhibited smaller errors, as
described in the previous discussion. Considering that CRO areas are
important for human society but highly sensitive to extreme events (Xia et
al., 2021) and crop ET estimation suffers from more challenges than those encountered in the other natural biomes (He et al., 2019; Melton et al.,
2021), the sensitivity of the 3T model to the temperature ensures that the
method could provide very high potential ability for crop ET estimation,
especially under extreme temperature conditions.</p>
</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Data availability</title>
      <p id="d1e4766">The daily and monthly ET dataset presented and analyzed in this article has been released and is available for free download from the Science Data Bank
(<ext-link xlink:href="https://doi.org/10.57760/sciencedb.o00014.00001" ext-link-type="DOI">10.57760/sciencedb.o00014.00001</ext-link>, Xiong et al., 2022). The
dataset is published under the Creative Commons Attribution 4.0
International (CC BY 4.0) license.</p>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Conclusions</title>
      <p id="d1e4780">A global ET product, derived from reanalysis and RS data based on the 3T
model, was provided with daily and 0.25<inline-formula><mml:math id="M292" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> resolutions from 2001 to
2020. The product was thoroughly assessed via direct evaluation against
FLUXNET EC tower data at the daily and monthly scales and water-balance-based catchment ET data at the annual scale, in addition to cross-validation against six commonly used global ET products. The 3T model-based
ET estimates generally agreed well with the above observations. Furthermore,
the 3T model exhibited a very high potential for accurate ET estimation
under extreme weather conditions. Since the 3T model requires only a few
input parameters (i.e., <inline-formula><mml:math id="M293" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, LST, and <inline-formula><mml:math id="M294" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) without the need for
parameter calibration, it could be concluded that the model is easy and
simple to apply, and the proposed ET product could provide reasonable information to support water-cycle-related studies.</p>
</sec>

      
      </body>
    <back><app-group>
        <supplementary-material position="anchor"><p id="d1e4813">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/essd-14-3673-2022-supplement" xlink:title="pdf">https://doi.org/10.5194/essd-14-3673-2022-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e4824">YL was responsible for the writing, original draft preparation, data processing and presentation, and programming and visualization. GYQ contributed to the methodology, supervision, project administration, funding
acquisition, and writing, review, and editing. CY, WZ, ZZ, and LQ were responsible for the writing and review and editing. JD was responsible for the programming and visualization. YX was responsible
for the conceptualization, formal analysis, funding acquisition, writing, review, and editing and supervision.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e4830">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e4836">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="d1e4842">MOD13C2 data were obtained from the NASA Land Processes
Distributed Active Archive Center (<uri>https://lpdaac.usgs.gov/</uri>, last access: 17 January 2022).  The Köppen–Geiger climate classification data were obtained from <uri>http://koeppen-geiger.vu-wien.ac.at/present.htm</uri> (last access: 16 April 2021). The Fluxcom data were obtained from
<uri>http://www.fluxcom.org/</uri> (last access: 3 October 2020). The GLEAM data were obtained from <uri>https://www.gleam.eu/</uri> (last access: 17 June 2021). The MOD16
data were obtained from the Numerical Terradynamic Simulation Group
(<uri>http://files.ntsg.umt.edu/</uri>, last access: 25 November 2020). The P-LSH data
were obtained from the Numerical Terradynamic Simulation Group
(<uri>http://files.ntsg.umt.edu/</uri>, last access: 25 November 2020). The PML data
were obtained from the National Tibetan Plateau Data Center
(<uri>http://data.tpdc.ac.cn/zh-hans/data/48c16a8d-d307-4973-abab-972e9449627c/</uri>,
last access: 24 November 2020). The authors would like to thank the above
organizations for providing datasets.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e4869">This research has been supported by the Shenzhen Science and Technology Innovation Program (grant nos. GXWD20201231165807007–20200827105738001), the National Natural Science Foundation of China (grant nos. 42071395 and 42001022), and the Sichuan Province Science and Technology Support Program (grant nos. 2021YFH0082 and 5132202020000046).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e4875">This paper was edited by David Carlson and reviewed by Yongqiang Zhang and one anonymous referee.</p>
  </notes><ref-list>
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