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  <front>
    <journal-meta><journal-id journal-id-type="publisher">NHESS</journal-id><journal-title-group>
    <journal-title>Natural Hazards and Earth System Sciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">NHESS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Nat. Hazards Earth Syst. Sci.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1684-9981</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/nhess-22-3461-2022</article-id><title-group><article-title>Interactions between precipitation, evapotranspiration and soil-moisture-based indices to characterize drought with high-resolution remote sensing and land-surface model data</article-title><alt-title>Interactions between precipitation, evapotranspiration and soil-moisture-based indices</alt-title>
      </title-group><?xmltex \runningtitle{Interactions between precipitation, evapotranspiration and soil-moisture-based indices}?><?xmltex \runningauthor{J. Gaona et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Gaona</surname><given-names>Jaime</given-names></name>
          <email>jaimegaona@usal.es</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Quintana-Seguí</surname><given-names>Pere</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7107-9671</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Escorihuela</surname><given-names>María José</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7780-7334</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Boone</surname><given-names>Aaron</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Llasat</surname><given-names>María Carmen</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8720-4193</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Instituto de Investigación en Agrobiotecnología, CIALE,
Universidad de Salamanca, Villamayor, Salamanca, 37185, Spain</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Hydrology and climate change, Observatori de l'Ebre (Universitat Ramon Llull – CSIC), Roquetes, 43520, Catalonia, Spain</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>IsardSAT, Parc Tecnològic – Barcelona Activa, Barcelona, 08042,
Catalonia, Spain</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Groupe de Météorologie de Moyenne Echelle, MOdélisation de l'Atmosphère Nuageuse et Analyse, GMME-MOANA, CNRM-GAME (URA CNRS &amp; Météo-France), 42, Av. G. Coriolis, 31057, Toulouse CEDEX 1, France</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Department of Applied Physics, Faculty of Physics, University of
Barcelona, Barcelona, 08028, Catalonia, Spain</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Jaime Gaona (jaimegaona@usal.es)</corresp></author-notes><pub-date><day>21</day><month>October</month><year>2022</year></pub-date>
      
      <volume>22</volume>
      <issue>10</issue>
      <fpage>3461</fpage><lpage>3485</lpage>
      <history>
        <date date-type="received"><day>21</day><month>February</month><year>2022</year></date>
           <date date-type="rev-request"><day>9</day><month>March</month><year>2022</year></date>
           <date date-type="rev-recd"><day>12</day><month>August</month><year>2022</year></date>
           <date date-type="accepted"><day>29</day><month>September</month><year>2022</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 Jaime Gaona 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://nhess.copernicus.org/articles/22/3461/2022/nhess-22-3461-2022.html">This article is available from https://nhess.copernicus.org/articles/22/3461/2022/nhess-22-3461-2022.html</self-uri><self-uri xlink:href="https://nhess.copernicus.org/articles/22/3461/2022/nhess-22-3461-2022.pdf">The full text article is available as a PDF file from https://nhess.copernicus.org/articles/22/3461/2022/nhess-22-3461-2022.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e145">The Iberian Peninsula is prone to drought due to the high variability in the Mediterranean climate with severe consequences for drinking water supply, agriculture, hydropower and ecosystem functioning. Because of the
complexity and relevance of droughts in this region, it is necessary to
increase our understanding of the temporal interactions of precipitation,
evapotranspiration and soil moisture that originate from drought within the
Ebro basin, in northeastern Spain, as the study region. Remote sensing and
land-surface models provide high-spatial-resolution and high-temporal-resolution data to characterize evapotranspiration and soil moisture anomalies in detail. The increasing availability of these datasets has the potential to overcome the lack of in situ observations of evapotranspiration and soil moisture. In this study, remote sensing data of evapotranspiration from MOD16A2 and soil moisture data from SMOS1km as well as SURFEX-ISBA land-surface model data are used to calculate the evapotranspiration deficit index (ETDI) and the soil moisture deficit index (SMDI) for the period 2010–2017. The study compares the remote sensing time series of the ETDI and SMDI with the ones estimated using the land-surface model SURFEX-ISBA, including the standardized precipitation index (SPI) computed at a weekly scale. The study focuses on the analysis of the time lags between the indices to identify the synchronicity and memory of the anomalies between precipitation, evapotranspiration and soil moisture. Lag analysis results demonstrate the capabilities of the SPI, ETDI and SMDI drought indices computed at a weekly scale to give information about the mechanisms of drought propagation at distinct levels of the land–atmosphere system. Relevant feedback for both antecedent and subsequent conditions is identified, with a preeminent role of evapotranspiration in the link between rainfall and soil moisture. Both
remote sensing and the land-surface model show capability to characterize
drought events, with specific advantages and drawbacks of the remote sensing and land-surface model datasets. Results underline the value of analyzing drought with dedicated indices, preferably at a weekly scale, to better identify the quick self-intensifying and mitigating mechanisms governing drought, which are relevant for drought monitoring in semi-arid areas.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e157">Drought is a major natural hazard for societies in semi-arid climates (Van Loon, 2015) and demands increasing levels of adaptation and resilience
measures to guarantee water supply (Watts et al., 2012), particularly in
water-stressed environments. Rainfed agriculture (Tigkas and Tsakiris,
2015) and even the enduring natural vegetation are very exposed to drought,
especially under climate change, which has long-lasting implications for the
local environment (Gudmundsson et al., 2014). Knowing that complex
interactions take place in the land–atmosphere system under drought, the
traditional meteorological or hydrologic approach may overlook
drought-relevant interactions between evapotranspiration and soil moisture
(Teuling et al., 2013).</p>
      <p id="d1e160">To track drought status and to analyze the interactions of the
land–atmosphere system, modern drought monitoring combines evapotranspiration, soil moisture and even vegetation anomalies in composite drought indices, such as the Objective Blends of Drought Indicators (OBDI) integrated in the U.S. Drought Monitor (USDM; Svoboda et al., 2002) or the Combined Drought Indicator (CDI) of the European Drought Observatory (Sepulcre-Canto et al., 2012). The use of this combined approach to monitoring drought is on an upward trend because even parsimonious composite drought indices like the probabilistic precipitation vegetation index (PPVI) (Monteleone et al., 2020) outperform the capabilities of common indices to characterize drought. One of the major advantages of composite indices is that they facilitate the characterization of drought from multiple perspectives (e.g., meteorological, hydrological or agricultural). Conversely, composite indices can be impractical to explore the mechanisms of drought, whose understanding may require focusing on key variables of the system. Unfortunately, evapotranspiration and soil moisture are still challenging to monitor compared to the meteorological, hydrological or vegetation variables currently regularly recorded. Despite the relevance of these two variables in the recurrence of drought and heat waves (Zampieri et al., 2009; Dasari et al., 2014), even at short timescales (Teuling, 2018), relatively few studies have evaluated their anomalies due to the limited availability of data of sufficient spatial and temporal resolution.</p>
      <p id="d1e163">Well-known drought indices such as the standardized precipitation index
(SPI) (McKee et al., 1993) and the Palmer drought severity
index (PDSI) (Palmer, 1965), primarily defined on the monthly scale, can
lack detail to identify short-term anomalies of temperature, wind or
radiation-originating “flash droughts” (Otkin et al., 2013). Rainfed
agriculture and natural vegetation are particularly sensitive to quickly
evolving droughts in specific moments of the growing season (Saini and
Westgate, 1999), which subsequently generate evapotranspiration and soil
moisture anomalies of short- and long-term impact (Jiménez et al., 2011).
Recently, there has been more interest in using drought indices with high temporal
resolution for short-term drought monitoring, such as the SPI and other
indices at the weekly scale (Otkin et al., 2015). Indices with this
short-term timescale include the weekly-scale evapotranspiration deficit
index (ETDI) and the soil moisture deficit index (SMDI) (Narasimhan and
Srinivasan, 2005). The ETDI and SMDI are variable-specific, enabling
full characterization of anomalies at specific levels of the land–atmosphere
system. This is especially useful in the Mediterranean climates where drought originates from not
only rainfall anomalies (Vicente-Serrano et al., 2004).</p>
      <p id="d1e166">This study focuses on the Ebro basin, which is an important Mediterranean
river basin of the Iberian Peninsula (IP). In view of the increase in the
frequency of drought events (Sousa et al., 2011) and the number of
consecutive dry spells (Turco and Llasat, 2011) identified in the area, we
can expect consequences in the long-term environmental state and the balance
between water availability and demands. Furthermore, being placed in a
semi-arid climate where most of the rainfall evaporates (68 %, Table 15
of <italic>Libro blanco del agua</italic>; MMA, 2000), the Ebro basin represents an
example of how important natural water demands are, particularly in the
headwaters where reforestation decreases runoff (López-Moreno et al., 2014). Rainfed agriculture dominates the rest of the un-forested areas and represents the other big consumer of water in the basin. However, despite
the relevance of rainfed agriculture, its analysis is often overshadowed by
irrigation, the biggest anthropogenic demand in the basin (Hoerling et al., 2012). Due to the importance of these water demands and others such as
hydropower and energy, the Ebro Hydrographic Confederation operates a dense hydrologic monitoring network, but the lack of dedicated soil moisture and evapotranspiration monitoring jeopardizes drought characterization
(Seneviratne et al., 2010). Fortunately, the increasing availability of
remote sensing (RS) products enables distributed, precise and frequent
monitoring of these coarsely observed variables (Martínez-Fernández
et al., 2016).</p>
      <p id="d1e173">Space agencies have released multiple RS products in the last decade
facilitating the distributed analysis of drought (AghaKouchak et al., 2015).
Optical spectrometry of the atmospheric (rainfall, temperature, water vapor)
and surface (vegetation reflectance) variables has often been the basis for
distributed characterization of drought indicators. Surface vegetation
indices such as the widespread normalized difference vegetation index (NDVI; Liu and Kogan, 1996) pioneered the application of RS data to assess the impacts of drought, but thereafter the increasing availability of RS data for multiple meteorological variables has increased their usage in drought indices (West et al., 2019). Currently, common indices like the SPI can rely on RS data (Sahoo et al., 2015) because integrating the increasing resolution of RS data into drought indicators enables short-term drought monitoring at least at the weekly scale (USDM – Svoboda et al., 2002; CDI – Sepulcre-Canto et al., 2012; Monteleone et al., 2020). However, unlike precipitation, temperature, and other directly observable and densely monitored meteorological variables, the measurement of evapotranspiration and soil moisture on the ground is still challenging and often costly or impractical at sufficient spatial resolution. Overcoming this gap is possible now thanks to the increasing availability of RS-based
evapotranspiration databases such as the global dataset included in GLEAM
(Miralles et al., 2011; Martens et al., 2017) or the soil moisture global
database CCI (Dorigo et al., 2017). Despite the coarse spatial resolution of
these global datasets, the recent developments in RS processing and downscaling improve their applicability at regional spatial scales and
short timescales (Wagner et al., 2007). Aiming to gain insight into drought
mechanisms, the availability of high-resolution datasets focused on such relevant variables of the land–atmosphere facilitates the use of single-variable drought indices such as the SPI, ETDI and SMDI, which is
advantageous to analyze the interactions between variables during droughts.</p>
      <p id="d1e176">On this basis, there are soil moisture datasets of increasingly high
resolution available from a combination of passive microwave sensors such
as those from SMOS and Soil Moisture Active Passive (SMAP) missions (Kerr et al., 2010, and Entekhabi et al., 2010, respectively) and active microwave sensors such as ASCAT or Sentinel-1
(Bartalis et al., 2007, and Hornacek et al., 2012, respectively). This is the
case of the high-resolution soil moisture product SMOS1km (Merlin et al., 2013; Molero et al., 2016; Escorihuela and Quintana-Seguí, 2016;
Escorihuela et al., 2018), which has been tested in the area and has been shown to
outperform ASCAT and AMSR-E due to its lack of roughness and vegetation
effects. SMAP and Sentinel-1 options are of similar resolution to SMOS1km and
accurate in the study area (Dari et al., 2021), but they are of much shorter series
length and are consequently not selected. Similarly, high-resolution RS
evapotranspiration products such as MOD16A2 (Mu et al., 2013) used in
this study are currently available. Therefore, it is worth exploring the
capabilities and limitations of high-resolution RS evapotranspiration data
for drought monitoring at the regional scale. High-resolution RS data are
most suitable for analysis at the basin scale where the resolution of
alternative reanalysis or modeled datasets such as ERA5-Land
(Muñoz-Sabater et al., 2021), LISFLOOD (Van Der Knijff et al., 2008) or
GLEAM v3 (Miralles et al., 2011; Martens et al., 2017) lack detail. To date,
relatively few works have used high-resolution satellite data for drought
analysis in the IP (Vicente-Serrano, 2006; Scaini et al., 2015;
Martínez-Fernández et al., 2016; Sánchez et al., 2016; Ribeiro
et al., 2019), especially at the spatial and temporal resolution of this
study (Pablos et al., 2017).</p>
      <p id="d1e179">Another source of high-temporal-resolution and high-spatial-resolution data is land-surface
models (LSMs). Used in atmospheric models to simulate the interactions
between soil, vegetation and the atmosphere, LSMs represent a suitable
alternative to RS to evaluate the surface water and energy balances at
regional to local scales. The development of LSMs was initiated with one-layer
models such as TOPUP (Schultz et al., 1998) or PROMET (Mauser and
Schadlich, 1998). Avissar and Pielke (1989) inaugurated the mosaic approach,
applying just one-layer models to the different fractions of land-use type.
One of the mosaic models able to distinguish between soil evaporation and
transpiration is the Météo-France-developed model SURFEX (Masson et
al., 2013), which, fed by the atmospheric analysis SAFRAN (Durand et al., 1999), uses the ISBA scheme for natural surfaces (Noilhan and Mahfouf, 1996).
SURFEX has been improved to study the continental water cycle in
applications such as SIM and SIM2 (Habets et al., 2008; Le Moigne et al., 2020), often in combination with the hydrologic model MODCOU (Ledoux et al., 1989). The modeling chain called SASER (SAFRAN–SURFEX–Eaudyssée–RAPID)
used in this study has been applied to Spain before (Barella-Ortiz and
Quintana-Seguí, 2019; Quintana-Seguí et al., 2020). This LSM
provides the precipitation required for the SPI and the evapotranspiration and
soil moisture necessary to generate LSM-based ETDI and SMDI series
comparable to the ones generated using RS data. Despite the limitations of
this LSM when applied as an offline model, it has been validated and
shown to provide useful evaluations of water resources in the study area
(Escorihuela and Quitana-Seguí, 2016; Barella-Ortiz and
Quintana-Seguí, 2019) and nearby Portugal and France (Nogueira et al., 2020; Le Moigne et al., 2020).</p>
      <p id="d1e182">This study aims at evaluating the suitability of high-resolution RS (SMOS1km
and MOD16A2) and LSM (SURFEX-ISBA) data for generating rainfall (SPI), soil
moisture (SMDI) and evapotranspiration (ETDI) drought (single-variable)
indices to better understand the mechanisms behind the temporal evolution of
drought in semi-arid climates. The comparison of RS and LSM data results is a
main aim of the study to detect the factors impacting drought indices based
on RS and LSM data. The study further evaluates the advantage of the barely
explored weekly temporal scale to capture the short-term anomalies of
evaporation and soil moisture decisive for drought in semi-arid areas. The
study has an agricultural scope focused on drought in rainfed environments
given its importance to land–atmosphere feedbacks (Herrera-Estrada et
al., 2017) and regional socioeconomic sustainability.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Study area</title>
      <p id="d1e193">The study area is the Ebro basin, located in the northeast of the Iberian
Peninsula (IP). Placed in between Atlantic and Mediterranean climatic
influences, the vast area (85 534 km<inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>) of the basin (Fig. 1a) has a complex topography (Fig. 1c) which defines a wide range of climatic conditions (Fig. 1d) of distinct spatial and temporal patterns of precipitation, evapotranspiration and soil moisture. The northern border has humid cool climates typical of the Atlantic-exposed Cantabrian coastline, while the
southeastern border enjoys a warm Mediterranean climate. The southwestern and
northeastern borders are dominated by the Iberian and Pyrenees mountains
which together with the Cantabrian and Mediterranean ranges restrict the
oceanic influence on the central part of the basin. Soil types (e.g., gypsum,
limestones) intensify the aridity of certain areas of the basin (Fig. 1b).
The combination of semi-arid climatic conditions and unfavorable soil types
to vegetation development determines extreme regimes of rainfall, soil
moisture and evapotranspiration, prone to drought. The basin is densely
populated and supplies a wide range of water demands, especially for
agriculture and energy. The vast network of irrigated areas, located mostly
in the arid central depression, is vulnerable to hydrological drought risks.</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="d1e207"><bold>(a)</bold> Ebro basin location in the Iberian Peninsula (OSM
OpenTopoMap). <bold>(b)</bold> Land cover of the basin depicting a contrasting basin between the forested areas of the mountains and the steppes of the central depression (© Esri satellite online maps, World Imagery, 2022). <bold>(c)</bold> Altitudinal range of the basin (IGN ES/FR MDT25, CC-BY 4.0). <bold>(d)</bold> Climatic classes present in the basin according to the climatic classification of Köppen–Geiger (data from Beck et al., 2018).</p></caption>
        <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3461/2022/nhess-22-3461-2022-f01.png"/>

      </fig>

</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Data</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Land-surface model data</title>
      <p id="d1e242">SURFEX, the land-surface modeling platform originally developed and
currently maintained by Météo-France (Masson et al., 2013; Le Moigne et al., 2020), has been chosen to perform the LSM simulation used in this
study. Simulations for the IP and Balearic Islands developed within the
HUMID project have <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mn mathvariant="normal">5</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> km spatial resolution and use the forcing provided by the Iberian application (Quintana-Seguí et al., 2008, 2016, 2017) of the SAFRAN meteorological analysis system (Durand et al., 1999). This is a modeling chain whose offline mode operates using the atmospheric forcing of SAFRAN to feed the LSM SURFEX-ISBA and simulate even the hydrology with Eaudyssée–RAPID (David et al., 2011).</p>
      <p id="d1e257">ISBA (Noilhan and Mahouf, 1996) is the SURFEX module in charge of simulating
natural surfaces. There are different versions of ISBA. In this study, we
have used the diffusion version (ISBA-DIF; Boone, 1999; Decharme et al., 2011), which performs better in the study area than the simpler three-layer force restore version (Quintana-Seguí et al., 2020). In this version of ISBA, the leaf area index (LAI) has a prescribed annual cycle (constant every year), which may limit the ability of the model to reproduce the long-term effects of drought on vegetation. The model simulates the soil column, but it is unable to simulate groundwater, which despite its impact on soil moisture memory, is not very relevant in the Ebro basin. SURFEX-ISBA requires additional physiographic information that is incorporated from the ECOCLIMAP-II land cover database (Faroux et al., 2013), which includes topographic, soil and land cover information at high resolution.</p>
      <p id="d1e260">The available SAFRAN forcing data allow us to simulate the period
1979–2017, but the period used for this study is restricted by the
relatively short length of the RS SMOS data coverage (2010–present) compared to the
model. To ensure the comparability of RS-based and LSM-based drought
indices, the study period is 2010–2017, for which both RS and LSM data are
available. To ensure that the RS soil moisture and the LSM soil moisture are comparable,
we have averaged the first three soil layers of the model according to their
discretization in the first 5 cm of the soil (1, 3 and 10 cm of depth,
respectively). The simulation is performed using a regular <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mn mathvariant="normal">5</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> km
resolution grid based on a custom Lambert conformal conic projection.</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Remote sensing data</title>
<sec id="Ch1.S3.SS2.SSS1">
  <label>3.2.1</label><title>Evapotranspiration</title>
      <p id="d1e291">To evaluate evapotranspiration, barely measured on the ground and not
directly measurable from space, we adopt a product based on multiple
evaporation-related variables observed by MODIS (Moderate Resolution Imaging
Spectroradiometer on NASA's Terra satellite): the MOD16A2 dataset. This is a
level-4 product providing 8 d evapotranspiration (ET) and potential
evapotranspiration (PET) based on daily meteorological forcing and 8 d RS
data of vegetation dynamics from MODIS (Mu et al., 2013). The datasets of
MOD16A2 are published in a sinusoidal projection at a resolution of 500 m
(Running et al., 2017). In this study, we have reprojected and interpolated
all RS products to the same <inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mn mathvariant="normal">5</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> km grid that the LSM simulations use. After the re-gridding step, the temporal step of the datasets is rearranged from the original 8 d accumulation period to a 7 d accumulation period,
which is more suitable for weekly analysis. Values are linearly weighted
depending on their contribution to each week for the 52 weeks of a
year. We also calculate the monthly means of the evapotranspiration product
to evaluate the impact of the time resolution on drought recognition. The
formatting of MOD16A2 datasets requires the evaluation of the quality
control flags (ET_QC), given that areas of the Pyrenees show missing data. Only the classes classified as good and optimal in the ET_QC flags are accepted as data for our study.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <label>3.2.2</label><title>Surface soil moisture</title>
      <p id="d1e314">Because of the relatively few years of data currently available from the
Soil Moisture Active Passive (SMAP) mission (Entekhabi et al., 2010), the
study adopts SMOS data (Kerr et al., 2010), in particular, the high-resolution SMOS1km dataset (Merlin et al., 2013). This dataset
downscales the original coarse-resolution SMOS data using the Disaggregation
based on Physical And Theoretical scale Change (DisPATCh) algorithm (Merlin et al., 2012) and the C4DIS algorithm (Molero et al., 2016). The algorithm enables the downscaling of the 40 km resolution of the SMOS soil moisture data available from 2010 into 1 km resolution using two products at 1 km
resolution from MODIS, the NDVI and land surface temperature (LST), and an elevation map at the same resolution. Precisely because the scale of interest to study relevant interactions to droughts is the weekly scale, the data are primarily used on a weekly scale. The spatial scale of interest for the study is that of a regular <inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:mn mathvariant="normal">5</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> km resolution grid, which takes advantage of the high resolution of SMOS1km. The 2010–2017 dataset presents frequent gaps in the mountainous areas of the Pyrenees. In order to fill the gaps, we apply temporal interpolation pixel by pixel considering a maximum period for temporal interpolation of 2 weeks. These data are also spatially aggregated and reprojected onto the same grid as the LSM.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Methods</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Drought indices</title>
      <p id="d1e346">Drought indices allow quantifying several aspects of drought, like the
magnitude and duration, and may also focus on particular variables depending
on the scope of interest (i.e., precipitation, soil moisture,
aridity, etc.). In view of the convenience to combine several
single-variable indicators to describe most of the drought mechanisms and
our focus on rainfed environments, we adopt the use of the standardized
precipitation index (SPI) (McKee et al., 1993), the evapotranspiration
deficit index (ETDI) and the soil moisture deficit index (SMDI) (Narasimhan
and Srinivasan, 2005). Using these three indices, the study aims to
investigate the interaction between the two main water fluxes (rainfall and
evapotranspiration) and the main storage (soil moisture) involved in the
water balance of the land–atmosphere system. The aggregation periods of the
SPI inform us about the different responding times of rainfall, soil
moisture, streamflow and groundwater anomalies. By evaluating the evolution
of these indices along with their interactions, this study aims to
characterize drought mechanisms in the Ebro basin. In this study, the
indices have been computed using gridded datasets, thus generating a time
series for each grid point.</p>
<sec id="Ch1.S4.SS1.SSS1">
  <label>4.1.1</label><title>SPI</title>
      <p id="d1e356">The standardized precipitation index (SPI) (McKee et al., 1993) is an index
of precipitation anomalies, which is calculated by transforming the
accumulated precipitation from its original distribution (usually gamma or
Pearson type III) to the normal distribution with zero mean and unit
standard deviation. As a result, we obtain a time series that shows, for
each time step, the departure from the expected value in terms of standard
deviations. The calculation of the index is usually made based on monthly
time series of rainfall, aggregated over multiple accumulation periods,
typically at 3, 6 and 12 months. However, the SPI can also be calculated on a
weekly basis, provided that the accumulation periods are at least 4 weeks (1 month). In this way, this study uses the notation SPIm-<inline-formula><mml:math id="M6" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> to denote the SPI at a monthly scale with an accumulation period of <inline-formula><mml:math id="M7" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> months and SPIw-<inline-formula><mml:math id="M8" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> to denote the weekly SPI with an accumulation period of <inline-formula><mml:math id="M9" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> weeks. Using SAFRAN data, we adopt the non-parametric methodology proposed by Farahmand and Aghakouchak (2015) to calculate the SPI on a monthly and weekly basis using the multi-month accumulation of 1, 3, 6 and 12 months suitable for rainfall, soil moisture, streamflow and groundwater evaluation.</p>
</sec>
<sec id="Ch1.S4.SS1.SSS2">
  <label>4.1.2</label><title>ETDI</title>
      <p id="d1e395">The second index incorporated into the analysis is the evapotranspiration
deficit index (ETDI) defined by Narasimhan and Srinivasan (2005). The first
step for calculating this index implies defining the water stress (WS) ratio
for each week, which is the difference between potential evapotranspiration
(PET) and actual evapotranspiration (AET) divided by PET. Then the water
stress anomaly (WSA) is computed as follows:
              <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M10" display="block"><mml:mtable class="split" rowspacing="4.267913pt" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{9}{9}\selectfont$\displaystyle}?><mml:msub><mml:mtext mathvariant="normal">WSA</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mtext>MWS</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mtext>WS</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mtext>MWS</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mo>min⁡</mml:mo><mml:msub><mml:mtext>WS</mml:mtext><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mtext>if</mml:mtext><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msub><mml:mtext>WS</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>≤</mml:mo><mml:msub><mml:mtext>MWS</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mo>,</mml:mo><?xmltex \hack{$\egroup}?></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{9}{9}\selectfont$\displaystyle}?><mml:msub><mml:mtext mathvariant="normal">WSA</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mtext>MWS</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mtext>WS</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mo>max⁡</mml:mo><mml:msub><mml:mtext>WS</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mtext>MWS</mml:mtext><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mtext>if</mml:mtext><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msub><mml:mtext>WS</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>&gt;</mml:mo><mml:msub><mml:mtext>MWS</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mo>,</mml:mo><?xmltex \hack{$\egroup}?></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
            where <inline-formula><mml:math id="M11" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula> denotes the week of the year (<inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>⇐</mml:mo><mml:mi>j</mml:mi><mml:mo>⇐</mml:mo><mml:mn mathvariant="normal">52</mml:mn></mml:mrow></mml:math></inline-formula>) and
<inline-formula><mml:math id="M13" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> denotes the year. <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:msub><mml:mtext>WS</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the water stress of the week <inline-formula><mml:math id="M15" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula> of the year <inline-formula><mml:math id="M16" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>. <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:msub><mml:mtext>MWS</mml:mtext><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the median WS for the week <inline-formula><mml:math id="M18" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula> of the year; <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:mo>min⁡</mml:mo><mml:msub><mml:mtext>WS</mml:mtext><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> corresponds to the minimum and <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:mo>max⁡</mml:mo><mml:msub><mml:mtext>WS</mml:mtext><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> to the maximum. This process removes the seasonality of the time series. WSA ranges from <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> (maximum water stress) to 100 (minimum water stress). The WSA accumulates over time to define the ETDI as in the following equation:
              <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M22" display="block"><mml:mrow><mml:msub><mml:mtext>ETDI</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn><mml:msub><mml:mtext>ETDI</mml:mtext><mml:mrow><mml:mi>j</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mtext>WSA</mml:mtext><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:mn mathvariant="normal">50</mml:mn></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            To define a range between <inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> and 4 for the index, the ETDI of value <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> must
correspond to a WSA of value <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> and the ETDI of value 4 to a WSA of value 100.
This range adjustment determines the coefficients 0.5 and the divisor 50 of
Eq. (2). In this way, the ETDI becomes a non-seasonal index suitable for comparing time series of diverse climatic characteristics. Monthly values of
the ETDI are calculated by computing the average of the weekly values of the
corresponding month. In this study, we calculate the ETDI using potential
and actual evapotranspiration provided by MOD16A2. We have also calculated
it using the SURFEX-ISBA-simulated AET and PET. By default, SURFEX-ISBA does
not calculate potential evapotranspiration. In order to do so, we have
modified the source code to set soil moisture permanently at field capacity
and have run a simulation with this modification. The resulting
evapotranspiration corresponds to the potential one.</p>
</sec>
<sec id="Ch1.S4.SS1.SSS3">
  <label>4.1.3</label><title>SMDI</title>
      <p id="d1e765">The third index incorporated into the analysis is the soil moisture deficit
index (SMDI) also defined by Narasimhan and Srinivasan (2005). The sequence
to calculate this index follows the same procedure as the ETDI. We first
calculate a weekly soil moisture deficit (SD) as follows:
              <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M26" display="block"><mml:mtable rowspacing="4.267913pt" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{9}{9}\selectfont$\displaystyle}?><mml:msub><mml:mtext mathvariant="normal">SD</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mtext>SW</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mtext>MSW</mml:mtext><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mtext>MSW</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mtext>minSW</mml:mtext><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mtext>if</mml:mtext><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msub><mml:mtext>SW</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>≤</mml:mo><mml:msub><mml:mtext>MSW</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mo>,</mml:mo><?xmltex \hack{$\egroup}?></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{9}{9}\selectfont$\displaystyle}?><mml:msub><mml:mtext mathvariant="normal">SD</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mtext>SW</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mtext>MSW</mml:mtext><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mtext>maxSW</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mtext>MSW</mml:mtext><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mtext>if</mml:mtext><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msub><mml:mtext>SW</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>&gt;</mml:mo><mml:msub><mml:mtext>MSW</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mo>.</mml:mo><?xmltex \hack{$\egroup}?></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
            Then, the time series of the SMDI is generated accumulating the <inline-formula><mml:math id="M27" display="inline"><mml:mi mathvariant="normal">SD</mml:mi></mml:math></inline-formula>:
              <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M28" display="block"><mml:mrow><mml:msub><mml:mtext>SMDI</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn><mml:msub><mml:mtext>SMDI</mml:mtext><mml:mrow><mml:mi>j</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mtext>SD</mml:mtext><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:mn mathvariant="normal">50</mml:mn></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            The SMDI also ranges between <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M30" display="inline"><mml:mn mathvariant="normal">4</mml:mn></mml:math></inline-formula>, corresponding to extremely
dry and very wet soil moisture conditions, respectively. The SMDI, similarly to the ETDI,
becomes a non-seasonal index able to compare time series of diverse climatic
characteristics at different soil depths. In this study, we have calculated
the SMDI using SMOS1km surface soil moisture data and SURFEX-ISBA-simulated
surface soil moisture data. In the case of SURFEX-ISBA, we have calculated
the weighted averages of the first two layers of the soil, which correspond
to the first 5 cm of the soil.</p>
</sec>
<sec id="Ch1.S4.SS1.SSS4">
  <label>4.1.4</label><title>Temporal consistency of drought indices calculated based on relatively short RS and LSM data series</title>
      <p id="d1e1010">Given the relatively short availability of data for the calculation of ETDI
and SMDI series, which depend on the maximum, minimum and median values of the available series, we conducted a sensitivity analysis of the indices in
reference to the length of the series and the subset of spatial data.
Results shown in Table S1 illustrate the relatively low impact of the length
of the series thanks to the high spatial resolution of the dataset. The
shortening of the series by half or a quarter barely alters the ETDI series
compared to the case of using the full temporal length. The subset of the
dataset to a fraction of its spatial resolution increasingly impacts the
robustness of ETDI and SMDI series. Therefore, the high-resolution spatial
and temporal datasets such as the RS and LSM used for this study support the
consistency of drought indices even when data availability remains under a
decade long.</p><?xmltex \hack{\newpage}?>
</sec>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Analysis of interaction between the indices</title>
<sec id="Ch1.S4.SS2.SSS1">
  <label>4.2.1</label><title>Correlation between the indices</title>
      <p id="d1e1030">To evaluate the similarity between the series of the drought indices (SPI,
ETDI and SMDI), we use a variant of the procedure applied by Barella-Ortiz
and Quintana-Seguí (2019) and Quintana-Seguí et al. (2020), based
on Barker et al. (2016). The method consists of computing the <inline-formula><mml:math id="M31" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> Pearson
correlation between each pair of series of these three drought indices (e.g., SPIw-<inline-formula><mml:math id="M32" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> and ETDIw and SMDIw), where <inline-formula><mml:math id="M33" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> is the accumulation period, which varies from 4 weeks (1 month) to 52 weeks (1 year). For this evaluation and the following lag analysis, we adopt the <inline-formula><mml:math id="M34" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> Pearson coefficient because the time it consumes to process our RS and LSM datasets is an order of magnitude
lower (e.g., weeks) than the time required using <inline-formula><mml:math id="M35" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> Spearman (e.g., months). To further support the use of <inline-formula><mml:math id="M36" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> Pearson despite the concerns about the
non-normality of SMDI and ETDI distributions, we conducted a similarity test
of the series of lags between indices obtained with <inline-formula><mml:math id="M37" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> Pearson and <inline-formula><mml:math id="M38" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> Spearman. Similarity tests indicate <inline-formula><mml:math id="M39" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> Pearson and <inline-formula><mml:math id="M40" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> Spearman correlate
generally over <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.9</mml:mn></mml:mrow></mml:math></inline-formula> for RS data and at a moderately lower level for LSM data, while they
do not differ significantly in the timing characteristics of the series
(Fig. S1 in the Supplement). Therefore, we can consider <inline-formula><mml:math id="M42" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> Pearson suitable and sufficiently accurate for the approach and focus of the study.</p>
</sec>
<sec id="Ch1.S4.SS2.SSS2">
  <label>4.2.2</label><title>Temporal lag analysis of the indices</title>
      <p id="d1e1132">Following the correlation analysis between the series, we perform a lag
analysis of the correlation of the pairs of drought indices at a weekly
scale, introducing lags from <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> weeks to <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> weeks. We compare ETDIw and SMDIw with SPIw-<inline-formula><mml:math id="M45" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> (being the period of accumulation for
SPIw-<inline-formula><mml:math id="M46" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>, where <inline-formula><mml:math id="M47" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> is 4, 13, 26 and 52 weeks, equivalent to SPIm-1, SPIm-3, SPIm-6 and
SPIm-12), as well as ETDIw with SMDIw. The purpose of this
analysis is to diagnose the reciprocity and memory in the interaction
between rainfall and evapotranspiration and between rainfall and surface soil
moisture. The relative abundance of positive over negative lags (and vice
versa) provides information about the asymmetry of the interaction between
the indices (precedence and delay). Negative lags refer to leading times of
ETDIw and SMDIw with respect to SPIw-<inline-formula><mml:math id="M48" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> (e.g., lag <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula>, left side of the time bar), while positive ones (e.g., lag <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula>) represent lag times when SPIw-<inline-formula><mml:math id="M51" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> precedes ETDIw and SMDIw (e.g., lag <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula>, right side of the time bar). The number of consecutive weeks of positive or negative lags of SPIw-<inline-formula><mml:math id="M53" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> can inform us about the memory of the interactions. For each time lag, the percentage of the basin affected by non-significant/significant correlations is indicated (grey/colored scales of bars in Figs. 3–7). Positive/negative correlations indicate a direct/indirect relationship (red/blue bars in Figs. 3–7).</p><?xmltex \hack{\newpage}?>
</sec>
</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Results</title>
<sec id="Ch1.S5.SS1">
  <label>5.1</label><title>Correlation between indices: monthly scale in comparison to the weekly scale</title>
      <p id="d1e1247">The first two aims of the study are to evaluate the suitability of the SPI, ETDI and SMDI to characterize the main anomalies in water exchanges of
the land–atmosphere system and to evaluate the suitability of adopting the
weekly scale for the analysis of drought indices compared to the use of the
monthly scale. Regarding the first, results shown in Fig. 2 indicate a
general agreement of the SPI, ETDI and SMDI (computed at either a
monthly or a weekly scale) on the major events of dry and wet anomalies of the period 2010–2017. The dry period of 2011–2012 and the wet period from the end of 2012 to 2015 were properly depicted. However, we identified
differences, especially in the case of the SMDI. This index tends to show a
generally lower variability than other indices when calculated with the LSM.
RS results of the SMDI differ from the other indices during the start of 2010
due to the uncertainties during the test period of the SMOS mission. The
left column of Fig. 2 shows the monthly SPIm-<inline-formula><mml:math id="M54" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> and the monthly averaged
ETDIm and SMDIm. Correlations between the SPI and the ETDI and SMDI are calculated on the monthly scale (Table 1, top row) and on the weekly scale (bottom row) for both RS and LSM data (where <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 4, 13, 26 and 52 weeks of aggregation, equivalent to 1, 3, 6 and 12 months). We test the significance of the correlations (<inline-formula><mml:math id="M56" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> value <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) between indices for two subsets: the entire period (2010–2017) and a subset of dry periods (i.e., when SPI <inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>, ETDI <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>, SMDI <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>). Then, we compare the observed (RS) and simulated (LSM) estimates of the indices to explore differences between data sources. RS and LSM ETDIm and SMDIm indices are moderately correlated (barely over 0.5, significant). Table 1 reports a value of <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.58</mml:mn></mml:mrow></mml:math></inline-formula> (significant) between ETDIm RS and SMDIm RS, which is significantly higher than the <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.32</mml:mn></mml:mrow></mml:math></inline-formula> between the ETDIm LSM and SMDIm LSM. In general, despite the resemblance of RS and LSM series of the ETDI and SMDI shown in Fig. 2, these two series differ. There is a higher agreement between the RS and the LSM estimates of ETDIm (<inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.77</mml:mn></mml:mrow></mml:math></inline-formula>, significant) than between the RS and LSM ones of SMDIm (<inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.27</mml:mn></mml:mrow></mml:math></inline-formula>).</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="d1e1365">Time series of the SPI, ETDI and SMDI at the monthly scale (left
column of subplots identified with sub-index 1) and weekly scale (right
column of subplots identified with sub-index 2). Panels <bold>(a)</bold> to <bold>(d)</bold> correspond to SPIm-1, SPIm-3, SPIm-6 and SPIm-12; panels <bold>(e)</bold> and <bold>(f)</bold> display the temporal evolution of the ETDI and SMDI. These ones show two rows corresponding to the series based on RS and LSM data. Red/blue color represents dry/wet periods. Periods of drought occur when SPI <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>, ETDI <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> and SMDI <inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3461/2022/nhess-22-3461-2022-f02.png"/>

        </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e1420">Matrices of significant (in bold) correlation coefficients
considering a <inline-formula><mml:math id="M68" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> values of <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula> for pairs of indices at the monthly and
weekly scale for the period 2010–2017 of the SPI, ETDI and SMDI series
and the corresponding dry-period subsets. Higher correlation values show a
more intense red color. Since the correlations of interest refer to
comparing the same type of data source for different indices, dark grey
cells identify unsuitable combinations for the analysis such as comparing RS
results from one index with LSM results from another index.</p></caption>
  <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3461/2022/nhess-22-3461-2022-t01.png"/>
</table-wrap>

      <p id="d1e1446">Table 1 also reveals differences in the moderate correlation of SPIm-<inline-formula><mml:math id="M70" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>
with the ETDI and the SMDI of different temporal aggregations (<inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 1, 3, 6, 12 months of SPIm-<inline-formula><mml:math id="M72" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> accumulation) as well as between their RS and LSM versions. Correlation between SPIm and ETDIm RS increases with the aggregation period of SPIm (<inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 0.39, 0.62, 0.72 and 0.81 for SPIm-1, SPIm-3, SPIm-6 and SPIm-12, respectively) while correlations of SPIm with the ETDI LSM peak at SPIm-3 (<inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula>) and remain high for SPIm-6 (<inline-formula><mml:math id="M75" 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 SPIm-12 (<inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.71</mml:mn></mml:mrow></mml:math></inline-formula>). The correlations between SPIm-<inline-formula><mml:math id="M77" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> and SMDI RS show moderate correlation ranging from SPIm-1 (<inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.42</mml:mn></mml:mrow></mml:math></inline-formula>) to the maximum value of SPIm-12 (<inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.63</mml:mn></mml:mrow></mml:math></inline-formula>). The SMDIm LSM exhibits a decreasing correlation pattern with the increasing aggregation of SPIm from SPIm-3 to SPIm-12 (<inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 0.45, 0.31, 0.3 and 0.24 for SPIm-1, SPIm-3, SPIm-6 and SPIm-12, respectively). Remarkably, correlations of the LSM SPIm–SMDIm are lower than their RS pairs, which suggests data uncertainties in RS and the LSM, as reported by Barella-Ortiz and Quintana-Seguí (2019) and by Quintana-Seguí et al. (2020).</p>
      <p id="d1e1561">The monthly correlation analysis is additionally conducted for the subsets
of dry periods (those with negative signs of SPIm, ETDIm and SMDIm).
Using the dry subset instead of the entire period primarily decreases all
correlations. Compared to the correlations of the entire period, the RS
ETDIm–SMDIm values decrease a little while the LSM ones increase a little. Also the SPIm-<inline-formula><mml:math id="M81" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>–ETDIm and the SPIm-<inline-formula><mml:math id="M82" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>–SMDIm correlations decline noticeably. Despite the loss of correlation and significance with the dry subset, the increase in the period of aggregation causes an increase in correlations, equal to the case of the entire period series.</p>
      <p id="d1e1578">Figure 2 provides an overview of the effect of adopting the weekly scale
(right column) instead of the monthly scale (left column). The weekly scale
substantially improves the temporal resolution of the plots. Subplots of
SPI-<inline-formula><mml:math id="M83" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> (a–d), the ETDI (e) and the SMDI (f) show how the weekly scale accurately
reproduces the magnitude, tendency and duration of the monthly-scale
anomalies, while the increase in temporal resolution additionally captures
quick changes. Graphically, we noticed that the aggregation period applied
to the SPI counteracts the gain in the resolution of the weekly scale, which
often prevents users from adopting the weekly scale instead of the monthly
scale. Conversely, Fig. 2e2 and f2 illustrate the strong increase
in the resolution of the ETDI and SMDI resolution on the weekly scale.</p>
      <p id="d1e1588">The right columns of Table 1 indicate the correlations between indices on a
weekly scale compared to those on a monthly scale (the “w” sub-index of
ETDIw, SMDIw and SPIw denotes the weekly scale). There is an overall decrease
in correlations at the weekly scale compared to the monthly scale, accentuated by the increasing period of aggregation (from SPIw-3 to
SPIw-12). Correlations increase compared to the monthly scale at the lowest period of aggregation of SPIw-<inline-formula><mml:math id="M84" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>, especially for SPIw-1–ETDIw (from <inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.39</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.57</mml:mn></mml:mrow></mml:math></inline-formula>) compared to SPIw-1–SMDIw (from <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.51</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.68</mml:mn></mml:mrow></mml:math></inline-formula>). For both RS and LSM data, the weekly scale lowers the correlation values of SPIw-<inline-formula><mml:math id="M89" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> with SMDIw more than those with ETDIw. Within the dry-period subset, all the correlations decrease too. The weekly scale lowers correlations due to the increase in variability in the weekly time series compared to the monthly ones but enables capturing the increasing complexity of interactions at shorter timescales. Therefore, since quick shifts (Fig. 2e1 and f1) are of great interest for drought analysis, we consider the weekly scale the most convenient for the lag analysis of the next section. This decision benefits comparing drought indices at their highest temporal definition, which for the ETDI and SMDI is natively the weekly scale and for the SPI can be easily adopted.</p>
</sec>
<sec id="Ch1.S5.SS2">
  <label>5.2</label><title>Temporal lag analysis</title>
      <p id="d1e1662">The analysis of correlations between pairs of temporally lagged time series
of drought indices provides valuable insights into the interactions between
indices (e.g., in terms of reciprocity) as indicators of synchronicity of
one variable with respect to the other. The analysis addresses the
characterization of the interactions between rainfall, evapotranspiration
and soil moisture while also aiming to examine whether the land–atmosphere
exchange of semi-arid areas under drought events is a quickly evolving or
rather inertial system. Plots of the fraction of the area affected by each
correlation level (from <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M91" display="inline"><mml:mn mathvariant="normal">1</mml:mn></mml:math></inline-formula> in steps of <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula>) for each lag period are shown in Figs. 3–7. It is anticipated that the three evaluated indices agree the most in a narrow range around lag <inline-formula><mml:math id="M93" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> (no lag) and that their correlation fades away progressively for the increasing lag periods beyond the scale of the propagation of drought. Figures 3 to 6 in which SPIw-<inline-formula><mml:math id="M94" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> interacts with the ETDI and SMDI illustrate the range of aggregation periods of SPIw (i.e., from 4 weeks of aggregation SPIw-4 to 52 weeks SPIw-52) along which the interpretation of the interactions between drought indices becomes most altered. The range of aggregation periods aims to open discussion about the optimal timescale to analyze the interacting drought processes. In general, the upper two subplots of Figs. 3 to 6 identify the admissible aggregation periods to interpret the clusters of interaction (SPIw-4 and SPIw-13, equivalent to SPI-1 and SPI-3 on a monthly scale), while the bottom two subplots (SPIw-26 and SPIw-52, equivalent to SPI-6 and SPI-12 at the monthly
scale) depict the increasingly merged clusters of interaction due to
excessively long aggregation periods of the SPI.</p>
<sec id="Ch1.S5.SS2.SSS1">
  <label>5.2.1</label><title>Lag analysis SPI–ETDI</title>
</sec>
<sec id="Ch1.S5.SS2.SSSx1" specific-use="unnumbered">
  <title>RS</title>
      <p id="d1e1724">The lag analysis of SPIw–ETDIw and SPIw–SMDIw shown in Figs. 3–6
aims at diagnosing the reciprocity, synchronicity and memory in the interaction between rainfall and evapotranspiration and between rainfall and
surface soil moisture. Each subplot of Figs. 3–6 shows the correlation
between the ETDIw and SMDIw indices with SPIw-<inline-formula><mml:math id="M95" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> calculated for
different aggregation periods (<inline-formula><mml:math id="M96" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>) at the weekly scale: SPIw-4, SPIw-13, SPIw-26 and SPIw-52. Negative lags refer to leading times of ETDIw and SMDIw with respect to SPIw-<inline-formula><mml:math id="M97" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> (e.g., lag <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula>, left side of the time bar) while positive ones (e.g., lag <inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula>) represent lag times when SPIw-<inline-formula><mml:math id="M100" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> precedes ETDIw and SMDIw (e.g., lag <inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula>, right side of the time bar).</p>
      <p id="d1e1786">In the case of the ETDIw–SPIw-<inline-formula><mml:math id="M102" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> analysis based on the RS data, there is a
remarkable cluster of positive correlations in the short term (indicated
with the tag ST<inline-formula><mml:math id="M103" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> (short-term) over the subplots of Fig. 3). This
ST<inline-formula><mml:math id="M104" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> cluster shows relevant fractions of the basin affected by
significant moderate (0.4–0.6) values of correlation, particularly in the
first weeks of the positive range of lags (from lag 0 to <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula>) (Fig. 3). The
cluster lasts more with the increasing period of aggregation (Fig. 3a to d), eventually becoming merged with the mid-term clusters. In view of
subplots Fig. 3a to d, the ST<inline-formula><mml:math id="M106" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> cluster extends from lag <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">13</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M108" display="inline"><mml:mn mathvariant="normal">4</mml:mn></mml:math></inline-formula>
in the case of SPIw-4; from lag <inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">13</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">13</mml:mn></mml:mrow></mml:math></inline-formula> in the case of SPIw-13; and
once merged with MT<inline-formula><mml:math id="M111" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> (mid-term), from <inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">26</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">26</mml:mn></mml:mrow></mml:math></inline-formula> in the case of SPIw-26 and from <inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">26</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">39</mml:mn></mml:mrow></mml:math></inline-formula> for SPIw-52. The mid-term cluster MT<inline-formula><mml:math id="M116" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>,
originally indicating a period of correlation of ETDIw preceding SPIw-<inline-formula><mml:math id="M117" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> from 4 to 13 weeks of aggregation, displays moderate to low but significant
values of correlation (from 0.2 to 0.4) from lag <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">36</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">13</mml:mn></mml:mrow></mml:math></inline-formula>. The merging of the cluster ST<inline-formula><mml:math id="M120" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> and MT<inline-formula><mml:math id="M121" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> decreases the asymmetry defining the leading role of ETDIw over SPIw-<inline-formula><mml:math id="M122" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>. The initially asymmetric interaction of ETDIw–SPIw-<inline-formula><mml:math id="M123" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> that is mostly located in the negative range of lags
(ST<inline-formula><mml:math id="M124" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> and MT<inline-formula><mml:math id="M125" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> shown between lag <inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> for the SPIw-4 and SPI-13 cases) propagates and dampens towards the positive range of lags with increasing aggregation. The dampening eventually shifts the interaction of ETDIw to SPIw-<inline-formula><mml:math id="M128" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> from preceding to delayed (at 26 and 52 weeks of aggregation, the clusters of significant positive correlations are mostly within the positive range of lags, especially in Fig. 3d). The loss of asymmetry due to the increasing aggregation translates into an increase in the duration of the cluster as well as of the fraction of the basin significantly affected by correlations. Both effects may indicate the
inconvenience of adopting long aggregation periods that alter the interaction magnitude and timing. There is an additional cluster of positive correlations, LT<inline-formula><mml:math id="M129" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> (long-term), past 1.5 years (lags <inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">78</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula>), particularly noticeable at SPIw-13 and SPIw-26. Blue bars in Fig. 3 indicate
negative correlations for the relationship ETDIw–SPIw-<inline-formula><mml:math id="M132" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> dominating the
long-term between evapotranspiration and rainfall anomalies. There is a
couple of clusters around lag <inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">42</mml:mn></mml:mrow></mml:math></inline-formula> (tagged LT<inline-formula><mml:math id="M134" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>) and around lag
<inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> (LT<inline-formula><mml:math id="M136" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>), slightly significant, that similarly to the positive
correlations, increased in duration and magnitude with the increase in the
aggregation period of the SPI, particularly for SPIw-26 and SPIw-52 (Fig. 3c–d).</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="d1e2113">Lag plots of SPI-1, SPI-3, SPI-6 and SPI-12 (expressed as SPIw-4, SPIw-13, SPIw-26 and SPIw-52, respectively) with remote sensing (RS) ETDIw at the weekly scale for the period 2010–2017. Lags are calculated for the <inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> leading and <inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> lagged time steps of ETDIw in reference to SPIw-<inline-formula><mml:math id="M139" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>. The height of the bars of the plot indicates the area of the basin affected by non-significant (grey scale) or significant (colored scale) correlations. The saturation of the colored scale indicates the magnitude of the significant positive (red) or negative (blue) Pearson correlation coefficient of SPIw-<inline-formula><mml:math id="M140" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> and ETDIw.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3461/2022/nhess-22-3461-2022-f03.png"/>

          </fig>

</sec>
<sec id="Ch1.S5.SS2.SSSx2" specific-use="unnumbered">
  <title>LSM</title>
      <p id="d1e2162">Results from the LSM SURFEX-ISBA (Fig. 4) show a less lasting and more
concentrated cluster of significant positive correlations around lag 0
(ST<inline-formula><mml:math id="M141" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> tagged in Fig. 4) than those observed in the RS results (Fig. 3). This result implies there is more synchronicity between the SPI and ETDI in the LSM data than in the RS data. Furthermore, the LSM provides higher
magnitudes of the significant positive correlations of ETDIw–SPIw-<inline-formula><mml:math id="M142" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> of
ST<inline-formula><mml:math id="M143" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> than RS results. Similarly to RS data, the duration of the highly
correlated period ST<inline-formula><mml:math id="M144" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> extends with the increasing aggregation of
SPIw-<inline-formula><mml:math id="M145" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> (Fig. 4a to d), eventually causing the merging of clusters ST<inline-formula><mml:math id="M146" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> and MT<inline-formula><mml:math id="M147" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>. The initial asymmetry of the positive correlations towards the negative range of lags is due to the cluster MT<inline-formula><mml:math id="M148" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> placed around lag <inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">26</mml:mn></mml:mrow></mml:math></inline-formula> and cluster LT<inline-formula><mml:math id="M150" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> (Fig. 4a and b). In the SPIw-26 and SPIw-52 cases (Fig. 4c and d) LT<inline-formula><mml:math id="M151" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> disappears and ST<inline-formula><mml:math id="M152" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> merges with MT<inline-formula><mml:math id="M153" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>, artificially shifting the initial asymmetry dominating the negative range of lags towards the positive range. Thus, the precedence of ETDIw with SPIw-<inline-formula><mml:math id="M154" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> prevalent in the period of aggregation of 4 and 13 weeks may look like the precedence of SPIw-<inline-formula><mml:math id="M155" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> with ETDIw when long aggregation periods such as the ones in SPIw-26 and SPIw-52 are applied. The initial asymmetry of the cluster ST<inline-formula><mml:math id="M156" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>–MT<inline-formula><mml:math id="M157" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> is lower in LSM results (Fig. 4) than in RS results (Fig. 3) due to the lower magnitude of MT<inline-formula><mml:math id="M158" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>. The additional cluster of positive correlations, LT<inline-formula><mml:math id="M159" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, past the 1.5-year range of positive lags (lags <inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">78</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula>) in LSM results (Fig. 4a to c) concurs with that of RS results (Fig. 3a to c). LSM results (Fig. 4) show a few more clusters of negative correlations for ETDIw–SPIw-<inline-formula><mml:math id="M162" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>, but these are of lower magnitude than those of RS ones (Fig. 3). These significant clusters merge with the increasing aggregation period LT<inline-formula><mml:math id="M163" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>–LT<inline-formula><mml:math id="M164" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">5</mml:mn></mml:msub></mml:math></inline-formula>, which agrees with LT<inline-formula><mml:math id="M165" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> shown in RS at the 26- and 52-week period of aggregation of SPIw-<inline-formula><mml:math id="M166" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>. LSM results further include a cluster of significant negative correlation values in the lead time range (cluster LT<inline-formula><mml:math id="M167" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>) that is absent in RS results (Fig. 4 vs. Fig. 3). The agreement between LSM and RS results confirms the asymmetrical interaction between ETDIw and SPIw-<inline-formula><mml:math id="M168" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>. The asymmetry suggests a prevalence of the precedence of positive correlations of ETDIw with SPIw-<inline-formula><mml:math id="M169" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> in the short term (from the monthly to the seasonal scale) while pointing to some delayed response of ETDIw to SPIw-<inline-formula><mml:math id="M170" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> in the negative correlations in the middle to long term (from a seasonal to interannual scale). The LSM results tend to amplify the magnitude and the area affected by positive correlations compared to the RS dataset.</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="d1e2427">Lag plots of SPI-1, SPI-3, SPI-6 and SPI-12 (expressed as SPIw-4, SPIw-13, SPIw-26 and SPIw-52, respectively) with the land-surface model (LSM) ETDIw index at the weekly scale for the period 2010–2017. Lags are
calculated for the <inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> leading and <inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> lagged time steps of
ETDIw in reference to SPIw-<inline-formula><mml:math id="M173" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>. The height of the bars of the plot
indicates the area of the basin affected by non-significant (greyscale) or
significant (colored scale) correlations. The saturation of the colored
scale indicates the magnitude of the significant positive (red) or negative
(blue) Pearson correlation coefficient of SPIw-<inline-formula><mml:math id="M174" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> and ETDIw.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3461/2022/nhess-22-3461-2022-f04.png"/>

          </fig>

</sec>
<sec id="Ch1.S5.SS2.SSS2">
  <label>5.2.2</label><title>Lag analysis SPI–SMDI</title>
</sec>
<sec id="Ch1.S5.SS2.SSSx3" specific-use="unnumbered">
  <title>RS</title>
      <p id="d1e2485">The interaction of SPIw-<inline-formula><mml:math id="M175" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> with SMDIw for the RS dataset is not as strong as
it was with ETDIw (Figs. 5 and 6 vs. Figs. 3 and 4). Both the correlation
values and the significant fraction of the basin affected by them are lower
than in the case of ETDIw. Similarly to ETDIw, the significant
positive correlations around lag 0 (ST<inline-formula><mml:math id="M176" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>) are asymmetrical. Because of this, SMDIw tends to experience the effect of the preceding conditions
of SPIw-<inline-formula><mml:math id="M177" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> less than influencing those of SPIw-<inline-formula><mml:math id="M178" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>. The increasing
period of aggregation of SPIw-13, SPIw-26 and SPIw-52 widens and lags the
short-term influence of SPIw-<inline-formula><mml:math id="M179" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> on SMDIw (ST<inline-formula><mml:math id="M180" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>) into a short-term to mid-term influence (ST<inline-formula><mml:math id="M181" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>–MT<inline-formula><mml:math id="M182" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>). This widened cluster of positive correlations stays almost entirely in the positive range of lags, which differs from that of ETDIw where the ST<inline-formula><mml:math id="M183" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>–MT<inline-formula><mml:math id="M184" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> cluster
extends in both positive and negative ranges of the lags (Fig. 5 compared
to Figs. 3 to 4). The leading range of lags (from lag <inline-formula><mml:math id="M185" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> to lag 0) does not show relevant clusters of significant correlation at all, neither in the middle nor in the long term. Negative correlations of the SMDIw–SPIw-<inline-formula><mml:math id="M186" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>
interaction only occasionally stand up at a small cluster (LT<inline-formula><mml:math id="M187" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>, Fig. 5b–d) in the positive range of lags (when SPIw-<inline-formula><mml:math id="M188" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> precedes SMDIw). The
smoothing effect of the aggregation period of SPIw-<inline-formula><mml:math id="M189" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> increasingly alters the initial bias of interactions towards the leading influence of the SMDI on SPIw, as well as delays most clusters similarly to the case with ETDIw.</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="d1e2614">Lag plots of SPI-1, SPI-3, SPI-6 and SPI-12 (expressed as SPIw-4, SPIw-13, SPIw-26 and SPIw-52, respectively) with the remote sensing (RS) SMDIw index at the weekly scale for the period 2010–2017. Lags are calculated for the <inline-formula><mml:math id="M190" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> leading and <inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> lagged time steps of SMDIw in reference to SPIw-<inline-formula><mml:math id="M192" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>. The height of the bars of the plot indicates the area of the basin affected by non-significant (greyscale) or significant (colored scale) correlations. The saturation of the colored scale indicates the magnitude of the significant positive (red) or negative (blue) Pearson correlation coefficient of SPIw-<inline-formula><mml:math id="M193" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> and SMDIw.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3461/2022/nhess-22-3461-2022-f05.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e2659">Lag plots of SPI-1, SPI-3, SPI-6 and SPI-12 (expressed as SPIw-4, SPIw-13, SPIw-26 and SPIw-52, respectively) with the land-surface model (LSM) SMDIw index
at the weekly scale for the period 2010–2017. Lags are calculated for the
<inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> leading and <inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> lagged time steps of SMDIw in reference to
SPIw-<inline-formula><mml:math id="M196" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>. The height of the bars of the plot indicates the area of the basin
affected by non-significant (greyscale) or significant (colored scale)
correlations. The saturation of the colored scale indicates the magnitude of
the significant positive (red) or negative (blue) Pearson correlation
coefficient of SPIw-<inline-formula><mml:math id="M197" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> and SMDIw.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3461/2022/nhess-22-3461-2022-f06.png"/>

          </fig>

</sec>
<sec id="Ch1.S5.SS2.SSSx4" specific-use="unnumbered">
  <title>LSM</title>
      <p id="d1e2708">The LSM results for the SMDIw–SPIw-<inline-formula><mml:math id="M198" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> relationship depict strongly
dampened patterns of significant correlation between SMDIw and SPIw-<inline-formula><mml:math id="M199" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>
compared to those of RS SMDIw–SPIw-<inline-formula><mml:math id="M200" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> or ETDIw–SPIw-<inline-formula><mml:math id="M201" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>. Only the
ST<inline-formula><mml:math id="M202" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> cluster is noticeable around lag 0. The increase in the
aggregation period does not favor its permanence as a relevant cluster
beyond SPIw-4. The cause can be the generalized low values of both
non-significant and significant correlations obtained for these estimates of the
LSM SURFEX-ISBA, which may indicate the difficulties the LSM has to describe
the response of the surface soil moisture (the SMDI) to the
atmospheric forcing (the SPI) that we saw in the RS dataset. The
periods identified of short-term, mid-term and long-term influence of one
SPIw-<inline-formula><mml:math id="M203" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> in SMDIw such as ST<inline-formula><mml:math id="M204" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>, MT<inline-formula><mml:math id="M205" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> or LT<inline-formula><mml:math id="M206" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> cannot be recognized in Fig. 6 compared to Fig. 5. Therefore, the LSM results of the
SPIw-<inline-formula><mml:math id="M207" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>–SMDIw relationship strongly differ from the ones obtained from RS
data and are a matter of debate in the Discussion section.</p>
</sec>
<sec id="Ch1.S5.SS2.SSS3">
  <label>5.2.3</label><title>Lag analysis ETDI–SMDI</title>
</sec>
<sec id="Ch1.S5.SS2.SSSx5" specific-use="unnumbered">
  <title>RS</title>
      <p id="d1e2804">The remaining interaction in this analysis is the ETDI–SMDI. The results
show a less asymmetric relationship between the ETDI and the SMDI compared
to the ones of SPIw with the ETDI and SMDI. The significant moderate positive correlation values (red bars in Fig. 7a) between lag <inline-formula><mml:math id="M208" display="inline"><mml:mn mathvariant="normal">0</mml:mn></mml:math></inline-formula> and <inline-formula><mml:math id="M209" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">13</mml:mn></mml:mrow></mml:math></inline-formula>
and from lag <inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M211" display="inline"><mml:mn mathvariant="normal">0</mml:mn></mml:math></inline-formula> indicate that the influence of the ETDI on the SMDI
lasts longer than the one of the SMDI on the ETDI. The magnitude, though, expresses that the SMDI moderately impacts the short-term conditions of the ETDI for about a month in comparison to the sole week the ETDI affects moderately those of the SMDI. However, the highest correlations occur for the lag <inline-formula><mml:math id="M212" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> when the SMDI precedes the ETDI by 1 week. Negative clusters (MT<inline-formula><mml:math id="M213" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>, MT<inline-formula><mml:math id="M214" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>) at <inline-formula><mml:math id="M215" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">39</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M216" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">39</mml:mn></mml:mrow></mml:math></inline-formula> weeks suggest that the interaction between the indices goes beyond the seasonal scale commented on above. However, the significance of all these mid-term to long-term clusters remains low.</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="d1e2892">Lag plots of ETDIw–SMDIw at the weekly timescale in the period 2010–2017 for <bold>(a)</bold> RS data and <bold>(b)</bold> LSM data. Lags are calculated for the <inline-formula><mml:math id="M217" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> leading and for the <inline-formula><mml:math id="M218" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">104</mml:mn></mml:mrow></mml:math></inline-formula> lagged time steps of SMDIw in reference to ETDIw. The five levels of red and blue indicate the positive (red) or negative (blue) Pearson correlation coefficient between ETDIw and SMDIw for each time step (lead or lag time step). The height of the bars of the plot indicates the area of the basin affected by that level of <inline-formula><mml:math id="M219" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> Pearson values.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3461/2022/nhess-22-3461-2022-f07.png"/>

          </fig>

</sec>
<sec id="Ch1.S5.SS2.SSSx6" specific-use="unnumbered">
  <title>LSM</title>
      <p id="d1e2940">The results of ETDI–SMDI interaction based on LSM data show less evident
periods of interaction between the indices compared to the RS results. The
expected strong correlation around lag 0 is largely diminished. The
strongest cluster appears from lag <inline-formula><mml:math id="M220" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">21</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M221" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">39</mml:mn></mml:mrow></mml:math></inline-formula>, MT<inline-formula><mml:math id="M222" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> (Fig. 7b), when the SMDI precedes the ETDI. No notable negative clusters can be identified. Apart from the lack of agreement on the symmetry of the interaction between LSM and RS results (Fig. 7b vs. a), the notable cluster ST<inline-formula><mml:math id="M223" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> in RS results is less relevant in LSM results. Given the disparity between LSM and RS
results, we raise concerns about the accuracy of offline LSM simulations
compared to the RS results, addressing them in the next
section.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S6">
  <label>6</label><title>Discussion</title>
      <p id="d1e2991">Results require careful discussion regarding three main aspects: firstly,
the effect of adopting the weekly scale for drought indices and analyses,
secondly the meaning behind the complex interactions between drought indices,
and thirdly the comparison of RS and LSMs as tools for high-resolution
monitoring of drought. All comments refer to the results on a weekly scale.</p>
<sec id="Ch1.S6.SS1">
  <label>6.1</label><title>Scales for drought monitoring in semi-arid environments</title>
      <p id="d1e3001">Analyzing the differences in correlations between indices at monthly and
weekly scales (Fig. 2), we support the necessity of adopting the weekly
scale to study lags. The monthly scale preferred for drought assessment from
a hydrological perspective may overlook the quick response of the land–atmosphere interactions. The clusters of moderate to high correlation
between indices mostly occur within the first month preceding or following
an anomaly (Figs. 3–7), particularly in the short to very short term. High
correlations tend to peak and plunge in an interval of a few weeks. This
short-term response recommends the use of the weekly scale and aggregation
periods below the seasonal scale, such as SPIw-13 (equivalent to SPI3), to
evaluate the delay or precedence between indices.</p>
      <p id="d1e3004">Our results showing soil moisture response to rainfall (<inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> to 5 weeks) and
evapotranspiration (<inline-formula><mml:math id="M225" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> to 5 weeks) anomalies in a matter of weeks are
consistent with previous works showing soil moisture echoes rainfall anomalies in a range from days to weeks (Scaini et al., 2015;
Martínez-Fernández et al., 2016) and also when driven by
evapotranspiration (Otkin et al., 2013). Therefore, in a basin exposed to
the high-energy characteristics of semi-arid climates, the weekly scale
allows us to diagnose disregarded short-term interactions, such as the ones of the
ETDI and SMDI on the SPI, without losing resolution in the identification of mid-term
to long-term interactions. The need to apply a weekly scale to the SPI, which is barely used below the monthly scale, is recommended not only
for the analysis of rainfall–evapotranspiration interactions but also for
soil moisture ones, which are often assessed over the monthly scale. Using
the weekly scale for drought assessment demands an increase in spatial
resolution. This is the reason why LSMs using coarse inputs, such as the
semi-aggregated physical characteristics of the basin, may generate results
with scale effects. In fact, scale effects due to the coarse resolution of
the spatial characteristics can increase the temporal scale at which the
processes are effectively correlated (Rodriguez-Iturbe et al., 2001).
Therefore, lag analysis needs to compile datasets of appropriate spatial and
temporal scales for their aims, like the high-resolution RS datasets
evaluated in this study or LSM ones based on completely distributed data.</p>
</sec>
<sec id="Ch1.S6.SS2">
  <label>6.2</label><title>Interpretation of the interactions between drought indices</title>
      <p id="d1e3035">Adopting specific drought indices for rainfall, evapotranspiration and soil
moisture allows exploring the interactions between variables of different
levels of the land–atmosphere system. The pertinence of using the SPI, ETDI
and SMDI to evaluate the interactions between the variables' anomalies can
be the subject of discussion depending on the specific advantages,
drawbacks and applicability of each index. There can be alternative drought
indices even for soil moisture and evapotranspiration of better stability
and statistical characteristics worth exploring. Furthermore, assessing the
interactions of anomalies may be possible without using drought indices.
However, since the commonplace in the analysis of the anomalies behind
drought has been widely based on drought indices for comparable
interpretation, we consider the SPI, ETDI and SMDI to represent a set of
comprehensive indices to flexibly evaluate interactions at different timescales.</p>
      <p id="d1e3038">Figure 8a and graphically Fig. 8b summarize the annual mode of interactions
between the SPI, ETDI and SMDI. In the short to middle term, both the ETDI and the
SMDI interactions with the SPI concur on having moderate significance, with only
a few negative and positive low interactions in the middle to long term.
Positive correlations around lag 0 of the ETDI and SMDI with the SPI indicate
direct precedent dependence of the indices, which means changes on the ETDI and
SMDI correlate positively (negatively) to positive (negative) changes on the
SPI. The short-term correlations after rainfall for both the ETDI and the SMDI
(lagged response of these indices to the SPI) are straightforward and have been
reported before in similar Iberian regions (Martínez-Fernandez et al., 2016). Sustained dry or wet anomalies in both variables favored by a
positive correlation between indices are primarily restricted to a length of
three seasons. Correlations beyond the year may represent the multi-annual
persistence of anomalies common in Mediterranean climates.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e3043"><bold>(a)</bold> Interpretation of the correlations between the SMDI–SPI, ETDI–SPI and SMDI–ETDI. The <inline-formula><mml:math id="M226" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> box exemplifies positive
correlations between the indices (positive correlations of red arrows in panel <bold>b</bold>), while the <inline-formula><mml:math id="M227" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> box defines the negative ones (negative correlations of blue arrows in panel <bold>b</bold>). The abbreviation “vv” denotes vice versa. <bold>(b)</bold> Summary of the annual magnitude and timing of the interactions. Red arrows represent positive correlations and blue arrows the negative ones. Arrow width represents the magnitude of the correlation. Arrow direction determines the direction of the interaction. The timeline at the bottom indicates the scale of the interactions ranging from short-term to long-term. <bold>(c)</bold> Sequences of prevalent reinforcing (upper) and inhibiting
(lower) conditions alternating during the annual cycle based on the scheme
of interactions described in panels <bold>(a)</bold> and <bold>(b)</bold>. The upper sequence is the self-intensifying loop driven by evapotranspiration under high-energy conditions. The lower sequence displays the inhibiting role of rainfall and soil moisture under low-energy conditions.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3461/2022/nhess-22-3461-2022-f08.png"/>

        </fig>

      <p id="d1e3098">The strong aggregation impact occurring when adopting SPIw-26 and
SPIw-52 indicates the analysis of interactions may be uncertain when indices
are aggregated beyond the seasonal scale. It is evaluated if the magnifying
effect of clusters with long aggregation periods (SPIw-26 and SPIw-52) is
the autocorrelation of the indices. Significant autocorrelated values always extend for less than the period of aggregation of SPIw-<inline-formula><mml:math id="M228" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> (2 weeks on SPIw-1, 3 weeks on SPIw-4, 10 weeks on SPIw-13, 18 weeks on SPIw-26, 35 weeks on SPIw-52, 40 weeks on SPI-78, 45 weeks on SPIw-104). Hence, we presume autocorrelation values of the SPI series are only partly caused by the period of aggregation. The partial autocorrelation of both the ETDI and the SMDI shows mostly two significant lags, which indicate the existence of an autoregressive model of type AR(2) (Fig. S2). An AR(2) model may articulate the combination of growing and decaying factors behind the shifting balance of positive and negative correlations between indices. In this way, the clusters of interactions identified in Figs. 3 to 7 can be attributed to interactions between rainfall, evapotranspiration and soil moisture anomalies. Conversely, clusters identified in series with a period of aggregation over the seasonal scale may be misleading for the analysis of drought interactions in Mediterranean environments. Thus, drought evolution in semi-arid environments can be considered an expression of quick exchanges between land–atmosphere variables which develop within the seasonal scale. This implies the temporal resolution of drought indices must adopt short timescales (i.e., weekly scale) to capture the onset of drought.</p>
      <p id="d1e3108">The existence of the precedent influence of the ETDI and SMDI on the SPI (clusters of the negative range of lags) implies some unequal reciprocity (feedback) between evapotranspiration and soil moisture with rainfall. This precedent influence is weaker than the influence of the SPI on subsequent ETDI and SMDI anomalies (lagged response) but still remarkable. It is reasonable that the lagged response of evapotranspiration and soil moisture to rainfall is stronger and longer-lasting than the precedent influence (Fig. 8a). Furthermore, the precedent influence period between the ETDI and SPI is stronger and of longer duration than the one of the SMDI on the SPI. This asymmetry suggests that the ETDI, more than the SMDI, has a weekly to seasonal precedent influence on rainfall (Fig. 8b). We expected a longer period of positive correlations of the SMDI influencing rainfall, given the multiple reports of soil moisture inducing memory at the near-surface atmosphere (Manning et al., 2018).</p>
      <p id="d1e3111">One reason why the ETDI shows a longer influence on the SPI than the SMDI may be
that the ETDI from MOD16A2 is fed by the whole depth of soil moisture, while the
SMDI based on SMOS1km is limited to the top 5 cm of soil moisture, a very exposed soil level in semi-arid climates. The complexity of soil moisture dynamics, which barely follow a cyclic interaction (Rodriguez-Iturbe et al., 1991), can also explain a weaker relationship
between the SMDI and SPI compared to the ETDI. Other reasons for this may lie
in the prevalence of maritime advection as the main contributor to
evapotranspiration in the IP (Gimeno et al., 2010) compared to the
prevalence of local soil moisture recycling common in more continental areas
of Europe (Bisselink and Dolman, 2008). The advective explanation is
supported by the contrast between the few weeks of precedent influence of
soil moisture on rainfall we observe in the Ebro basin and the up to 250 d of precedent influence of continental areas prone to soil moisture
recycling (Rowntree and Bolton, 1983; Bisselink and Dolman, 2008). Some
studies focused on continental climates of relevant summer rainfall have
described the implications of the alteration of the recycling due to soil
moisture depletion during heat waves and drought which can eventually alter
the atmosphere (Rasmijn et al., 2018; Miralles et al., 2019). In the
Mediterranean climate of the Iberian Peninsula characterized by a lack of
summer rainfall, soil moisture annually reaches such low levels that we can
expect annual summer alterations in the near atmosphere. Differences between
areas where soil moisture plays a role, like central Europe, and areas where
soil moisture is unable to control the evolution of the system under
high-energy conditions, like the Iberian Peninsula, have been reported
before in Mediterranean-like Western Australia (Herold et al., 2016).</p>
      <p id="d1e3114">In consequence, our results at the Ebro basin seem compatible with the
frequent activation of a reinforcing or self-intensification loop (Brubaker
and Entekhabi, 1996), by which the precedent influence of negative
(eventually positive) anomalies of evapotranspiration reducing (increasing)
rainfall cascades into a depletion (rise) in soil moisture that further
limits (enhances) the response of evapotranspiration and restarts the cycle
(Fig. 8c, right column). The weak precedence of soil moisture on rainfall
compared to that of evapotranspiration expresses the limited duration of the
control capacity of the soil moisture over evapotranspiration in semi-arid
climates of the Mediterranean type (left column of Fig. 8c). Negative
correlations when indices differ in sign (<inline-formula><mml:math id="M229" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> conditions, Fig. 8a)
can be indicative of transitional periods of mid-seasons. The sharp shift
from the cluster of short-term positive correlations to the cluster of mid-term
to long-term negative correlations suggests a limit in the persistence of
the self-intensification mechanism. A physical interpretation of the shift
may be related to the change in the dominance of the sequence from the one
under high-energy conditions (Fig. 8c, right column) to the one under
low-energy conditions (Fig. 8c, left column). A low-energy inhibiting
mechanism of negative
correlations between soil moisture and surface temperature under low
temperatures has already been described by Brubaker and Entekhabi (1996). Given the direct link between evapotranspiration and
temperature, the shift from positive to negative interactions happening at
timescales over the semester but below the yearly scale suggests that the
arrival of winter low-energy conditions terminates the dominance of the
self-intensifying loop of evapotranspiration.</p>
      <p id="d1e3129">In this way, the annual cycle can be modeled as the seasonal succession of
two sequences: one under the low-energy conditions of winter when
evapotranspiration no longer outweighs the inhibiting of soil moisture due
to rainfall (left column of Fig. 8c) and the other under high-energy
conditions driven by evapotranspiration (right column of Fig. 8c). The shift
between the long period of interactions dominated by evapotranspiration
(right column of Fig. 8c) and a short period of interactions controlled by
rainfall and soil moisture (lower sequence of Fig. 8c) is generally driven
by an energy threshold. However, certain levels of rainfall and soil moisture anomalies may temporally advance or delay the shift. This reason explains why under high-energy conditions drought may terminate due to heavy rainfall, while soil moisture deficits under low-energy conditions may cause
an anticipated onset of the self-intensification loop of evapotranspiration.</p>
      <p id="d1e3132">The conceptualization of the interactions illustrated in Fig. 8 aims to
raise awareness about the power of evapotranspiration anomalies to alter the
land–atmosphere system, year-round, beyond hydrometeorological extremes
(Seneviratne et al., 2006; Otkin et al., 2013; Teuling, 2018; Miralles et
al., 2019). Another reason for supporting the year-round implications of the
dominance of evapotranspiration over soil moisture is that rainfall mostly
transfers to evapotranspiration in semi-arid climates (Rodriguez-Iturbe et
al., 2001), where the often underestimated interception (Savenije et al., 2004) further increases evaporation at the expense of soil moisture.
Additionally, as the semi-arid Mediterranean climate likely presents
thresholds of rainfall, evapotranspiration and soil moisture anomalies
different from those triggering hydrometeorological extremes in other areas
(Tramblay et al., 2021), the evapotranspiration-dominated sequence may
initiate not only more often but also more abruptly than in regions of lower-energy
inputs. All these aspects, together with the increasing chance of extremes
in the Mediterranean area due to climate change (Samaniego et al., 2018),
recommend assessing changes in the balance of land–atmosphere interactions
from the basis of this study.</p>
      <p id="d1e3136">However, we bear in mind that our results may oversimplify the causality,
since processes not analyzed in this study may also play a role. The
multiple periods showing neither prevalently positive nor prevalently negative correlations between indices indicate a loss of linear interaction. A source of non-linearity is vegetation due to its mediating role in water exchanges of the land–atmosphere system. Plants can control evapotranspiration and soil moisture in adaptation to water stress in non-linear manners that depend more on the type of vegetation (Katul et al., 2012), particularly within the Mediterranean floras (Boulet et al., 2020), than on the evapotranspiration or soil moisture status. Vegetation can also modulate the partitioning of energy governing evapotranspiration (Lansu et al., 2020) but similar processes are reported with soil moisture (Barbeta et al., 2015). In consequence, the quick response to drought of rainfed crops and sclerophyllous vegetation (Vicente-Serrano et al., 2019) may obscure the interpretation of the links between rainfall, evapotranspiration and soil moisture. This is of concern regarding the ETDI and SMDI results because interactions of vegetation integrate the status of the atmospheric and the land-surface variables (Peters et al., 1991). Nonetheless, additional factors of uncertainty may arise from teleconnections such as the well-known North Atlantic Oscillation (NAO) or Western Mediterranean Oscillation (WeMO; Barnston and Livezey, 1987; Conte et al., 1989) or the oceanic ones like the Atlantic Multidecadal Oscillation (AMO; Kerr, 2000) altering the land–atmosphere system at large scales.</p>
</sec>
<sec id="Ch1.S6.SS3">
  <label>6.3</label><title>The value of remote sensing and land-surface model estimates</title>
      <p id="d1e3147">The RS and LSM results of the lag analysis of the ETDI–SPI interactions
show consistently comparable results in contrast to the remarkable
disagreement between RS and LSM results for the SMDI–SPI interaction. Results of the
SMDI obtained with the LSM show substantially lower correlations than the
ones of RS while also differing in the timing of the clusters of
correlation. We expected the opposite, i.e., that the LSM, being simpler than
reality, has stronger SPI–ETDI–SMDI correlations than the RS dataset.
We assume the implicit accumulation of uncertainties in modeling
(Rodriguez-Iturbe et al., 1991), partly inherited from inputs but also from the
LSM structure, is the cause of the decrease in correlations. This is
particularly true for soil moisture, a variable integrating exchanges
between climate, soil and vegetation (Rodriguez-Iturbe et al., 2001).
Secondly, this is an offline simulation, where the atmosphere (SAFRAN) is
forcing the land surface (SURFEX-ISBA) without explicit feedback of
SURFEX-ISBA influencing SAFRAN back. SAFRAN estimates real conditions by
ingesting observations, so the feedback is implicit in results, which may be
insufficient to represent reality. Thirdly, the model itself does not
consider important processes like the interactive response of vegetation.
ISBA has an interactive vegetation module (ISBA-A-gs), but Mediterranean
vegetation can be particularly challenging for it. We expect to test the
capabilities of interactive modeling vegetation in a follow-up study.
Uncertainties in ISBA with vegetation also have roots in the use of the
ECOCLIMAP-II database, which shows inaccuracies in cover type and the LAI.
ECOCLIMAP assumes the maximum/minimum LAI occurs in June/February in contrast
with the early spring and autumn LAI maximums characteristic of the
Mediterranean environment (Queguiner et al., 2011). All in all, the
differences between the LSM and RS datasets are already an important result to improve the LSM and comprise a useful insight into the use of offline LSM drought simulations.</p>
      <p id="d1e3150">Our results positively verify that RS represents an effective tool to
overcome the problem of sparsely observed soil moisture or evapotranspiration, whose crucial role in drought evolution requires
high-resolution data similarly to precipitation (AghaKouchak and Nakhjiri,
2012). Including high-resolution evapotranspiration products from MODIS (MOD16A2) and soil moisture from SMOS missions (SMOS1km) together with the distributed rainfall reanalysis data allows dedicated interpretation of the interactions between these two drought-relevant variables and rainfall and their role in the water balance of the land–atmosphere interface (Dai, 2011). Especially for evapotranspiration, the maps and series of the LSM SURFEX-ISBA are comparable to those of RS, which supports the reliability of LSMs despite their limited capability in arid regions (De Kauwe et al., 2015).</p>
      <p id="d1e3153">The temporal and spatial patterns of the anomalies are overly identified by both RS and the LSM. The RS data seem able to capture a more complex scheme of interactions than the LSM, despite the intrinsic data issues of the RS sensors and the performance of the algorithms used to generate the products. Conversely, the LSM seems sensitive to uncertainties from input data, especially surface properties, and the offline forcing. The parametrization of the model assumes a semi-distributed approach by sub-basins of the catchment on which each sub-basin is defined based on average values of land cover and soil characteristics of the ECOCLIMAP
database, which may induce some patchiness of LSM results compared to the RS
results. The offline run means that the meteorological data force the LSM,
but the feedbacks are lost beyond the meteorological observations included
as observation in the model. Additional aspects can be, for instance, the
impact of groundwater redistributing soil moisture depending on topography,
which is underrepresented in the LSM. Limitations of LSMs have been reported
in multiple works before and are the subject of improvement efforts (Teuling et al., 2006; Samaniego et al., 2018). Either way, uncertainties are causes of major concern in the lag analysis where they can alter the correlations between indices and obscure the interpretation of the interactions.</p>
      <p id="d1e3156">These aspects together can be critical to improving evapotranspiration and
soil moisture estimates (Ukkola et al., 2016). Solving these inaccuracies
would increase the value of RS and LSM estimates. This study exemplifies the
potential of high-resolution RS and LSM products for a wide range of
applications, such as drought analysis.</p>
</sec>
</sec>
<sec id="Ch1.S7" sec-type="conclusions">
  <label>7</label><title>Conclusions and perspectives</title>
      <p id="d1e3168">The analysis of droughts in the Ebro basin using dedicated
evapotranspiration and soil moisture drought indices based on
high-resolution data from MOD16A2, SMOS1km and the LSM SURFEX-ISBA provides
the following insights.</p>
      <p id="d1e3171">The monthly scale commonly adopted for drought evaluation (e.g., SPI-3) may
overlook the quick evolution of drought from an agricultural and
environmental perspective, especially in the high-energy climates of the
Mediterranean basin where the anomalies of rainfall, evapotranspiration and
soil moisture can vary in a matter of days. The ETDI shows the strongest
response at a weekly scale while it also remains influential in the
mid-term. The SMDI can also quickly evolve with anomalies of evapotranspiration
and particularly with lasting anomalies of rainfall. The weekly scale is
advantageous to describe trends and shifts in the evolution of the indices
and to identify disregarded interactions such as the preceding influence of the
ETDI on the SPI.</p>
      <p id="d1e3174">The ETDI and SMDI, together with the SPI adapted to the weekly
scale, allow tracking of the evolution of the anomalies of
evapotranspiration, soil moisture and rainfall, as well as their
interactions driving water anomalies in the region. There is great
consistency between the time series of the ETDI, SMDI and SPI. Lag analysis
between these indices clarifies the interactions between anomalies on
different levels of the surface–atmosphere system, information that is
neglected when using multivariable indices or indices aggregated beyond the
seasonal scale. The lag analysis also identifies sequences of interactions
defining reinforcing or inhibiting feedbacks. Evapotranspiration dominates
the water balance of the Iberian semi-arid climate, especially during
high-energy periods. This dominance frequently exceeds the controlling
action of rainfall and soil moisture, inducing the reinforcing dry loop.
Because of the relevance of evapotranspiration, heat waves further fueling
dry events deserve further attention. The weak influence of soil moisture on
subsequent evapotranspiration and rainfall limits its capability to control
the propagation of anomalies.</p>
      <p id="d1e3177">RS datasets of MOD16A2 and SMOS-1km accurately estimate the temporal and
spatial anomalies in the basin. Evapotranspiration from the LSM SURFEX-ISBA
closely resembles the RS one of MOD16A2. Results differ substantially
between SMOS1km and SURFEX-ISBA estimates of soil moisture. RS uncertainties
arise mainly from data gaps. Land-surface model's estimates can extend the
evaluation of soil moisture beyond the surface towards the root zone but
face notable challenges from offline simulation neglecting feedback, as well
as from the quality of input data that define surface characteristics. RS
outcompetes the LSM in its ability to integrate information about
challenging processes, such as vegetation dynamics. Assimilation seems the
way forward to integrate the best aspects of both kinds of data. For as long
as ground-based observations remain sparse, RS and LSMs represent effective
tools to assess the water anomalies of the land–atmosphere system and their
interaction mechanisms.</p>
</sec>

      
      </body>
    <back><notes notes-type="codeavailability"><title>Code availability</title>

      <p id="d1e3184">Codes (as Python scripts) used to analyze the data are available upon request.</p>
  </notes><?xmltex \hack{\newpage}?><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e3191">Several datasets were used for this article.
<list list-type="bullet"><list-item>
      <p id="d1e3196">The satellite-derived evapotranspiration data of MOD16A2 are available at the Land Processes Distributed Active Archive Center (LP-DAAC) of NASA USGS at <uri>https://lpdaac.usgs.gov/products/mod16a2v006/</uri> (USGS 2022).</p></list-item><list-item>
      <p id="d1e3203">The satellite-derived soil moisture data of SMOS1km will be available soon in repositories but are currently available upon request. The authors refer interested readers to the following publications for a detailed description of the data: Escorihuela and Quintana-Seguí (2016) and Merlin et al. (2013).</p></list-item><list-item>
      <p id="d1e3207">The SAFRAN dataset forcing the SURFEX LSM simulations for Spain is being updated for ongoing studies related to this article but can be made available upon request. The last version of the SAFRAN dataset in repositories is available at the MISTRALS HyMeX database: <ext-link xlink:href="https://doi.org/10.14768/MISTRALS-HYMEX.1388" ext-link-type="DOI">10.14768/MISTRALS-HYMEX.1388</ext-link> (Quintana-Segui, 2015). The SURFEX LSM simulations were produced for this study but can be reproduced using the corresponding release of the models: <uri>https://www.umr-cnrm.fr/surfex/spip.php?rubrique</uri> (CNRM, 2022).</p></list-item></list>
The study followed standard statistical routines that can be easily reproduced by the methodological explanations in the text.</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e3217">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/nhess-22-3461-2022-supplement" xlink:title="pdf">https://doi.org/10.5194/nhess-22-3461-2022-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e3226">PQS defined the research aim and together with JG collected, curated and analysed the data. MJE provided the SMOS1km dataset and supervised its integration in the study. JG and PQS analyzed the interactions between indices and the lag analysis. JG, PQS and MJE evaluated and discussed the results. JG and PQS prepared the manuscript. MJE, AB and MCLL provided feedback and improvements to the text and to the interpretation and discussion of results.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e3233">At least one of the (co-)authors is a member of the editorial board of <italic>Natural Hazards and Earth System Sciences</italic>. The peer-review process was guided by an independent editor, and the authors also have no other competing interests to declare.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e3242">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="d1e3248">The authors acknowledge support from the Spanish State Research Agency (AEI) to the Hydrology and Climate Change lab of Pere Quintana-Seguí at Ebro Observatory.</p></ack><?xmltex \hack{\newpage}?><?xmltex \hack{\newpage}?><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e3254">This research has been supported by the Spanish State Research Agency (Agencia Estatal de Investigación, AEI) within the HUMID project  (AEI/FEDER EU grant no. CGL2017-85687-R).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e3260">This paper was edited by David J. Peres and reviewed by Emanuele Romano and one anonymous referee.</p>
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