<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing with OASIS Tables v3.0 20080202//EN" "journalpub-oasis3.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0" article-type="research-article">
  <front>
    <journal-meta><journal-id journal-id-type="publisher">GMD</journal-id><journal-title-group>
    <journal-title>Geoscientific Model Development</journal-title>
    <abbrev-journal-title abbrev-type="publisher">GMD</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Geosci. Model Dev.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1991-9603</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/gmd-15-251-2022</article-id><title-group><article-title>Convolutional conditional neural processes for <?xmltex \hack{\break}?> local climate downscaling</article-title><alt-title>Convolutional conditional neural processes for local climate downscaling</alt-title>
      </title-group><?xmltex \runningtitle{Convolutional conditional neural processes for local climate downscaling}?><?xmltex \runningauthor{A.~Vaughan~et~al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Vaughan</surname><given-names>Anna</given-names></name>
          <email>av555@cam.ac.uk</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Tebbutt</surname><given-names>Will</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff3">
          <name><surname>Hosking</surname><given-names>J. Scott</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3646-3504</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Turner</surname><given-names>Richard E.</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Department of Engineering, University of Cambridge, Cambridge, UK</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>British Antarctic Survey, Cambridge, UK</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>The Alan Turing Institute, London, UK</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Anna Vaughan (av555@cam.ac.uk)</corresp></author-notes><pub-date><day>13</day><month>January</month><year>2022</year></pub-date>
      
      <volume>15</volume>
      <issue>1</issue>
      <fpage>251</fpage><lpage>268</lpage>
      <history>
        <date date-type="received"><day>12</day><month>December</month><year>2020</year></date>
           <date date-type="accepted"><day>3</day><month>September</month><year>2021</year></date>
           <date date-type="rev-recd"><day>3</day><month>September</month><year>2021</year></date>
           <date date-type="rev-request"><day>15</day><month>March</month><year>2021</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 Anna Vaughan 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://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022.html">This article is available from https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022.html</self-uri><self-uri xlink:href="https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022.pdf">The full text article is available as a PDF file from https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e124">A new model is presented for multisite statistical downscaling of temperature and precipitation using convolutional conditional neural processes
(convCNPs). ConvCNPs are a recently developed class of models that allow deep-learning techniques to be applied to off-the-grid spatio-temporal
data. In contrast to existing methods that map from low-resolution model output to high-resolution predictions at a discrete set of locations, this
model outputs a stochastic process that can be queried at an arbitrary latitude–longitude coordinate. The convCNP model is shown to outperform an
ensemble of existing downscaling techniques over Europe for both temperature and precipitation taken from the VALUE intercomparison project. The
model also outperforms an approach that uses Gaussian processes to interpolate single-site downscaling models at unseen locations. Importantly,
substantial improvement is seen in the representation of extreme precipitation events. These results indicate that the convCNP is a robust
downscaling model suitable for generating localised projections for use in climate impact studies.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e136">Statistical downscaling methods are vital tools in translating global and regional climate model output to actionable guidance for climate impact
studies. General circulation models (GCMs) and regional climate models (RCMs) are used to provide projections of future climate scenarios; however,
coarse resolution and systematic biases result in unrealistic behaviour, particularly for extreme events
<xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx44" id="paren.1"/>. In recognition of these limitations, downscaling is routinely performed to correct raw GCM and RCM
outputs. This is achieved either by dynamical downscaling, running a nested high-resolution simulation or via statistical methods. Comparisons of
statistical and dynamical downscaling suggest that neither group of methods is clearly superior <xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx11" id="paren.2"/>;
however, in practice computationally cheaper statistical methods are widely used.</p>
      <p id="d1e145">Major classes of statistical downscaling methods are model output statistics (MOS) and perfect prognosis (PP; <xref ref-type="bibr" rid="bib1.bibx42" id="altparen.3"/>). MOS methods explicitly adjust the simulated distribution of a given variable to the observed distribution
using variations of quantile mapping <xref ref-type="bibr" rid="bib1.bibx57 bib1.bibx49 bib1.bibx10" id="paren.4"/>. Though these methods are widely applied in
impact studies, they struggle to downscale extreme values and artificially alter trends <xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx44" id="paren.5"/>. In contrast, in PP
downscaling, the aim is to learn a transfer function <inline-formula><mml:math id="M1" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> such that
          <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M2" display="block"><mml:mrow><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
        where <inline-formula><mml:math id="M3" display="inline"><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover></mml:math></inline-formula> is the downscaled prediction of a given climate variable whose true value is <inline-formula><mml:math id="M4" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> at location <inline-formula><mml:math id="M5" display="inline"><mml:mi mathvariant="bold-italic">x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M6" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> is a set of predictors from
the climate model <xref ref-type="bibr" rid="bib1.bibx41" id="paren.6"/>. This is based on the assumption that while sub-grid-scale and parameterised processes are poorly
represented in GCMs, the large-scale flow is generally better resolved <xref ref-type="bibr" rid="bib1.bibx41" id="paren.7"/>.</p>
      <?pagebreak page252?><p id="d1e229">Multiple different models have been trialled for parameterising <inline-formula><mml:math id="M7" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula>. Traditional statistical methods used for this purpose include multiple linear
regression <xref ref-type="bibr" rid="bib1.bibx22 bib1.bibx27" id="paren.8"/>, generalised linear models <xref ref-type="bibr" rid="bib1.bibx55" id="paren.9"/> and analogue techniques
<xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx2" id="paren.10"/>. More recently, there has been considerable interest in applying advances in machine learning
to this problem, including relevance vector machines <xref ref-type="bibr" rid="bib1.bibx18" id="paren.11"/>, artificial neural networks <xref ref-type="bibr" rid="bib1.bibx54" id="paren.12"/>,
auto-encoders <xref ref-type="bibr" rid="bib1.bibx61" id="paren.13"/>, recurrent neural networks <xref ref-type="bibr" rid="bib1.bibx8 bib1.bibx47" id="paren.14"/>, generative adversarial
networks <xref ref-type="bibr" rid="bib1.bibx66" id="paren.15"/> and convolutional neural networks
<xref ref-type="bibr" rid="bib1.bibx59 bib1.bibx60 bib1.bibx48 bib1.bibx3 bib1.bibx29 bib1.bibx38" id="paren.16"/>. These models are trained
in a supervised framework by learning a mapping from low-resolution predictors to downscaled values at a particular set of locations for which
observations are available. Unsupervised downscaling using normalising flows has also been proposed <xref ref-type="bibr" rid="bib1.bibx21" id="paren.17"/>.</p>
      <p id="d1e270">Limitations remain in these models. In many climate applications it is desirable to make projections that are both (i) consistent over multiple
locations and (ii) specific to an arbitrary locality. The problem of multi-site downscaling has been widely studied, with two classes of approaches
emerging. Traditional methods take analogues or principal components of the coarse-resolution field as predictors. The spatial dependence is then
explicitly modelled for a given set of sites, using observations at those locations to train the model
<xref ref-type="bibr" rid="bib1.bibx41 bib1.bibx9 bib1.bibx7 bib1.bibx46" id="paren.18"/>. More recent work has sought to leverage
advances in machine learning, for example convolutional neural networks (CNNs), for feature extraction
<xref ref-type="bibr" rid="bib1.bibx59 bib1.bibx8 bib1.bibx47 bib1.bibx3 bib1.bibx29" id="paren.19"/>. These methods take in a grid of
low-resolution predictors and output downscaled predictions either on a fixed grid or at a pre-determined list of sites. The question naturally arises
as to how we can generate predictions at new locations at test time. Models trained in one location can be applied in another using transfer learning
<xref ref-type="bibr" rid="bib1.bibx65" id="paren.20"/>. In this case, however, the output predictions are still at the resolution or list of sites determined at training time (i.e. a
CNN model trained on 0.1<inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> resolution will output 0.1<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> resolution predictions, regardless of where it is applied). To make predictions on a
grid with a different resolution or at a new set of locations requires interpolation of model predictions or taking the closest location.</p>
      <p id="d1e301">In this study we propose a new approach to statistical downscaling using a convolutional conditional neural process model (convCNP; <xref ref-type="bibr" rid="bib1.bibx20" id="altparen.21"/>), a state-of-the-art probabilistic machine learning method combining ideas from Gaussian processes (GPs) and deep neural networks. This model
learns a mapping between a gridded set of low-resolution predictors and a continuous stochastic process over longitude and latitude representing the
downscaled prediction of the required variable. In contrast to previous work where discrete predictions are made at a list of locations determined at
training time, the stochastic process output from the convCNP can be queried at any location where a prediction is required. Although to our knowledge
this is the first application of such a model in downscaling, similar work has demonstrated the advantages of learning a mapping from discrete input
data to continuous prediction fields in modelling idealised fluid flow <xref ref-type="bibr" rid="bib1.bibx37 bib1.bibx36 bib1.bibx39" id="paren.22"/>.</p>
      <p id="d1e310">The specific aims of this study are as follows.
<list list-type="order"><list-item>
      <p id="d1e315">Develop a new statistical model for downscaling GCM output capable of generating a stochastic process as a prediction that can be queried at an
arbitrary site.</p></list-item><list-item>
      <p id="d1e319">Compare the performance of the statistical model to existing strong baselines.</p></list-item><list-item>
      <p id="d1e323">Compare the performance of the statistical model at locations outside of the training set to existing interpolation methods.</p></list-item><list-item>
      <p id="d1e327">Quantify the impact of including sub-grid-scale topography on model predictions.</p></list-item></list></p>
      <p id="d1e330">Section 2 outlines the development of the downscaling model and presents the experimental setup used to address aims 2–4. Section 3 compares the
performance of the statistical model to an ensemble of baselines. Sections 4 and 5 explore model performance at unseen locations and the impact of
including local topographic data. Finally, Sect. 6 presents a discussion of these results and suggestions for further applications.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Datasets and methodology</title>
      <p id="d1e341">We first outline the development of the statistical downscaling model, followed by a description of three validation experiments.</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="d1e346">Schematic of the convCNP model for downscaling precipitation demonstrating the flow of data in predicting precipitation for a given day at target locations <inline-formula><mml:math id="M10" display="inline"><mml:mi mathvariant="bold-italic">x</mml:mi></mml:math></inline-formula>. Gridded coarse-resolution data for each predictor are fed into the CNN, producing predictions of <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">β</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> at each grid point. These gridded predictions are then transformed to a prediction at the target location using an exponentiated-quadratic kernel. Finally, these elevation agnostic predictions are fed into a multi-layer perceptron together with topographic data <inline-formula><mml:math id="M12" display="inline"><mml:mi mathvariant="bold-italic">e</mml:mi></mml:math></inline-formula> to produce a final prediction of the parameters.</p></caption>
        <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022-f01.png"/>

      </fig>

<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>The downscaling model</title>
      <p id="d1e400">Our aim is to approximate the function <inline-formula><mml:math id="M13" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> in Eq. (1) to
predict the value of a downscaled climate variable <inline-formula><mml:math id="M14" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> at locations <inline-formula><mml:math id="M15" display="inline"><mml:mi mathvariant="bold-italic">x</mml:mi></mml:math></inline-formula> given a set of coarse-scale predictors <inline-formula><mml:math id="M16" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula>. In order to take the local
topography into account, we assume that this function also depends on the local topography at each target point, denoted <inline-formula><mml:math id="M17" display="inline"><mml:mi mathvariant="bold-italic">e</mml:mi></mml:math></inline-formula>, i.e.
            <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M18" display="block"><mml:mrow><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e469">In this study, <inline-formula><mml:math id="M19" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> is modelled as a convCNP <xref ref-type="bibr" rid="bib1.bibx20" id="paren.23"/>, a member of the conditional neural process family
<xref ref-type="bibr" rid="bib1.bibx17" id="paren.24"/>. A neural process model is a deep-learning model that parameterises a mapping from a discrete input set to a posterior
stochastic process as a neural network. This is implemented as an encoder that maps the input set to<?pagebreak page253?> a latent representation, followed by a decoder
that takes the latent representation and a target location as input and outputs the predictive distribution at that location
<xref ref-type="bibr" rid="bib1.bibx15" id="paren.25"/>. In the context of this downscaling problem, the input set is the low-resolution predictors, the mapping of a neural network, and
the output a stochastic process over temperature or precipitation that can be queried at an arbitrary spatial location to generate the downscaled
predictions. For spatial problems such as downscaling, a desirable inductive bias in a model is that it is translation equivariant, i.e. the model
makes identical predictions if the input data are spatially translated. The convCNP model applied here builds this equivariance into the conditional
neural process.</p>
      <p id="d1e488">Using the convCNP model, we take a probabilistic approach to specifying <inline-formula><mml:math id="M20" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> where we include a noise model, and thus
            <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M21" display="block"><mml:mrow><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>|</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>|</mml:mo><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          <?xmltex \hack{\newpage}?>Deterministic predictions are made from this by using, for example, the predictive mean
            <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M22" display="block"><mml:mrow><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mo movablelimits="false">∫</mml:mo><mml:mi>y</mml:mi><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>|</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mo>)</mml:mo><mml:mi mathvariant="normal">d</mml:mi><mml:mi>y</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e601">In this model <inline-formula><mml:math id="M23" display="inline"><mml:mi mathvariant="bold-italic">θ</mml:mi></mml:math></inline-formula> is parameterised as
            <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M24" display="block"><mml:mrow><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">ψ</mml:mi><mml:mtext>MLP</mml:mtext></mml:msub><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="italic">ϕ</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">h</mml:mi><mml:mo>=</mml:mo><mml:mtext>CNN</mml:mtext><mml:mo>(</mml:mo><mml:mi>Z</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mo>]</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e679">Examples of convCNP model predictions compared to observations for <bold>(a–c)</bold> maximum temperature in Heligoland, Germany, and <bold>(d–f)</bold> precipitation in Madrid, Spain.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022-f02.png"/>

        </fig>

      <?xmltex \floatpos{p}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e696">Locations of ECA&amp;D <bold>(a)</bold> and VALUE <bold>(b)</bold> stations, with altitude shaded.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022-f03.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e713">Comparison of the convCNP model to VALUE ensemble baselines for mean metrics, with the convCNP model shaded in blue. Each box summarises the performance for one model in the ensemble over the 86 training stations on the held-out validation data.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022-f04.png"/>

        </fig>

      <p id="d1e722">Here <inline-formula><mml:math id="M25" display="inline"><mml:mi mathvariant="bold-italic">θ</mml:mi></mml:math></inline-formula> is a vector  of
parameters of a distribution for the climate variable at prediction locations <inline-formula><mml:math id="M26" display="inline"><mml:mi mathvariant="bold-italic">x</mml:mi></mml:math></inline-formula>. Consistent with previous stochastic downscaling studies
<xref ref-type="bibr" rid="bib1.bibx9 bib1.bibx69" id="paren.26"/>, this is assumed to be Gaussian for maximum temperature and a Gamma–Bernoulli mixture for
precipitation. We note that this is an extension of existing conditional and convolutional conditional neural process models where the predictive
distribution is assumed to be Gaussian <xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx20" id="paren.27"/>. <inline-formula><mml:math id="M27" display="inline"><mml:mi mathvariant="bold-italic">e</mml:mi></mml:math></inline-formula> is a vector of sub-grid-scale topographic
information at each of the prediction locations, <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ψ</mml:mi><mml:mtext>MLP</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is a multi-layer perceptron, <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϕ</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is a kernel function with learnable
length scale and CNN is a convolutional neural network. Each component of this is described below, with a schematic of the model shown in Fig. 1.
<list list-type="order"><list-item>
      <?pagebreak page256?><p id="d1e777"><italic>Convolutional neural network.</italic><?xmltex \hack{\newline}?> In the first step, daily gridded reanalysis predictor data <inline-formula><mml:math id="M30" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> for a single time step are
fed into the model. These grids are used as input to a convolutional neural network to extract relevant features. This is implemented as a six-block
Resnet architecture <xref ref-type="bibr" rid="bib1.bibx26" id="paren.28"/> with depth-wise separable convolutions <xref ref-type="bibr" rid="bib1.bibx12" id="paren.29"/>. The output from this step is a prediction
of the relevant parameters for each variable at each grid point in the predictor set, i.e.<disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M31" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">h</mml:mi><mml:mtext>nm</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mtext>CNN</mml:mtext><mml:mo>(</mml:mo><mml:mi>Z</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>where <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">h</mml:mi><mml:mtext>nm</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is the vector-valued output at latitude <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and longitude <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi><mml:mo>∈</mml:mo><mml:msup><mml:mi mathvariant="double-struck">Z</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> with
<inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> indicating the grid spacing where the grid consists of <inline-formula><mml:math id="M37" display="inline"><mml:mi>M</mml:mi></mml:math></inline-formula> points in the longitude direction and <inline-formula><mml:math id="M38" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> points in the latitude direction.</p></list-item><list-item>
      <p id="d1e909"><italic>Translation to off-the-grid predictions.</italic><?xmltex \hack{\newline}?> These gridded predictions are translated to the off-the-grid target
locations <inline-formula><mml:math id="M39" display="inline"><mml:mi mathvariant="bold-italic">x</mml:mi></mml:math></inline-formula> using outputs from step 1 as weights for an exponentiated-quadratic (EQ) kernel <inline-formula><mml:math id="M40" display="inline"><mml:mi mathvariant="italic">ϕ</mml:mi></mml:math></inline-formula>, i.e.<disp-formula id="Ch1.E7" content-type="numbered"><label>7</label><mml:math id="M41" display="block"><mml:mtable class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϕ</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">h</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>M</mml:mi></mml:munderover><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:munderover><mml:msub><mml:mi mathvariant="bold-italic">h</mml:mi><mml:mtext>nm</mml:mtext></mml:msub><mml:mi mathvariant="italic">ϕ</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:mi>m</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:mi>n</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>M</mml:mi></mml:munderover><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:munderover><mml:msub><mml:mi mathvariant="bold-italic">h</mml:mi><mml:mtext>nm</mml:mtext></mml:msub><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mstyle scriptlevel="+1"><mml:mfrac><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:msubsup><mml:mi>l</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:mi>m</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>-</mml:mo><mml:mstyle scriptlevel="+1"><mml:mfrac><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:msubsup><mml:mi>l</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:mi>n</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msup><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p>
      <p id="d1e1146">This outputs predictions of the relevant distributional parameters, <inline-formula><mml:math id="M42" display="inline"><mml:mi mathvariant="bold-italic">θ</mml:mi></mml:math></inline-formula>, at each target location. An EQ kernel is chosen here as it ensures
that the predictions are approximately translation equivariant.</p></list-item><list-item>
      <p id="d1e1157"><italic>Inclusion of sub-grid-scale topography</italic><?xmltex \hack{\newline}?> By design, the predictions from the previous step only model variation on the
scale of the context grid spacing. This elevation agnostic output is post-processed using a multi-layer perceptron (MLP). This takes the parameter
predictions from the EQ kernel as input together with a vector of topographic data <inline-formula><mml:math id="M43" display="inline"><mml:mi mathvariant="bold-italic">e</mml:mi></mml:math></inline-formula> at each target location.<disp-formula id="Ch1.E8" content-type="numbered"><label>8</label><mml:math id="M44" display="block"><mml:mrow><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">ψ</mml:mi><mml:mtext>MLP</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">ϕ</mml:mi><mml:mi>c</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">h</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e1222">The vector <inline-formula><mml:math id="M45" display="inline"><mml:mi mathvariant="bold-italic">e</mml:mi></mml:math></inline-formula> consists of the following three measurements at each target point:
<list list-type="alpha-lower"><list-item>
      <p id="d1e1234">true elevation,</p></list-item><list-item>
      <p id="d1e1238">difference between the true and grid-scale elevation,</p></list-item><list-item>
      <p id="d1e1242">multi-scale topographic position index (mTPI; measuring the topographic prominence of the location, i.e. quantifying whether the point is in a
valley or on a ridge).</p></list-item></list></p>
      <p id="d1e1245">This MLP outputs the final prediction of the distributional parameters <inline-formula><mml:math id="M46" display="inline"><mml:mi mathvariant="bold-italic">θ</mml:mi></mml:math></inline-formula> at each target location.</p></list-item></list></p>
      <p id="d1e1255">Figure 2 shows a concrete example of temperature and precipitation time series produced using this model by sampling from the output
distributions. Maximum temperature is shown for Heligoland, Germany, and precipitation is shown for Madrid, Spain. For both variables the model produces
qualitatively realistic time series.</p>
<sec id="Ch1.S2.SS1.SSS1">
  <label>2.1.1</label><title>Training</title>
      <p id="d1e1266">The convCNP models are trained by minimising the average negative log likelihood. For temperature, this is given by
              <disp-formula id="Ch1.E9" content-type="numbered"><label>9</label><mml:math id="M47" display="block"><mml:mtable rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:msub><mml:mtext>NLL</mml:mtext><mml:mtext>temp</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mi>N</mml:mi></mml:mfrac></mml:mstyle><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:munderover></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mspace width="1em" linebreak="nobreak"/><mml:mi>ln⁡</mml:mi><mml:mfenced close="]" open="["><mml:mrow><mml:mi mathvariant="script">N</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>|</mml:mo><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
            where <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the observed value and <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:mi mathvariant="script">N</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>;</mml:mo><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> denotes a Gaussian distribution over <inline-formula><mml:math id="M50" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> with mean <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and
variance <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>. These parameters <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mo mathvariant="italic">{</mml:mo><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula> are
generated by the model at each location <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and use topography <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. N is the total number of target locations. For precipitation, the
negative log likelihood is given by
              <disp-formula id="Ch1.E10" content-type="numbered"><label>10</label><mml:math id="M56" display="block"><mml:mtable class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:msub><mml:mtext>NLL</mml:mtext><mml:mtext>precip</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mi>N</mml:mi></mml:mfrac></mml:mstyle><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:munderover><mml:mo>[</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mfenced open="(" close=""><mml:mrow><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mfenced close=")" open=""><mml:mrow><mml:mo>+</mml:mo><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Γ</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>|</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>)</mml:mo><mml:mo>]</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
            where <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is a Bernoulli random variable describing whether precipitation was observed at the <inline-formula><mml:math id="M58" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>th target location, <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the observed
precipitation, <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> parameterises the predicted Bernoulli distribution, and <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:mi mathvariant="normal">Γ</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>;</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is a Gamma distribution with shape
parameter <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and scale parameter <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. Here <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mo mathvariant="italic">{</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e1999">Weights are optimised using Adam <xref ref-type="bibr" rid="bib1.bibx34" id="paren.30"/>, with the learning rate set to 5 <inline-formula><mml:math id="M65" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M66" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Each model is trained for 100 epochs on
456 batches of 16 <inline-formula><mml:math id="M67" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">d</mml:mi></mml:mrow></mml:math></inline-formula> each, using early stopping with a patience of 10 epochs.</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="d1e2034">The same as Fig. 4 but for extreme metrics.</p></caption>
            <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022-f05.png"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Experiments and datasets</title>
      <p id="d1e2053">Having addressed the first aim in developing the convCNP model, we next evaluate model performance via three experiments. The first experiment
compares the convCNP model to an ensemble of existing downscaling methods following a standardised experimental protocol. In contrast to the convCNP
model, these methods are unable to make predictions at locations where training data are not available. In the second experiment, we assess the
performance of the convCNP model at these unseen locations compared to a baseline constructed by interpolating single-site models. Finally, ablation
experiments are performed to quantify the impact of including sub-grid-scale topographic information on performance.</p>
<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>Experiment 1 – baseline comparison</title>
      <p id="d1e2063">ConvCNP model performance is first compared to strong baseline methods taken from the VALUE experimental protocol. VALUE <xref ref-type="bibr" rid="bib1.bibx43" id="paren.31"/>
provides a standardised suite of experiments to evaluate new downscaling methods, together with data benchmarking the performance of<?pagebreak page257?> existing
methods. In the VALUE 1a experiment, each downscaling method predicts the maximum temperature and daily precipitation at 86 stations across Europe
(Fig. 2), given gridded data from the ERA-Interim reanalysis <xref ref-type="bibr" rid="bib1.bibx14" id="paren.32"/>. These stations are chosen as they offer continuous, high-fidelity
data over the training and held-out test periods and represent multiple different climate regimes <xref ref-type="bibr" rid="bib1.bibx23" id="paren.33"/>. Data are taken
from 1979–2008, with 5-fold cross-validation used over 6-year intervals to produce a 30-year time series.</p>
      <p id="d1e2075">The convCNPs are trained to predict maximum temperature and precipitation at these 86 VALUE stations given the ERA Interim grids over Europe. Station
data are taken from the European Climate Assessment Dataset <xref ref-type="bibr" rid="bib1.bibx35" id="paren.34"/>. These grids are restricted to points between 35 and 72<inline-formula><mml:math id="M68" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
latitude and <inline-formula><mml:math id="M69" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>15 to 40<inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> longitude. The VALUE experiment protocol does not specify which predictors are used in each downscaling model (i.e.
which gridded variables are included in <inline-formula><mml:math id="M71" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula>), with different predictors chosen for each member of the baseline ensemble, as detailed in
<xref ref-type="bibr" rid="bib1.bibx23" id="text.35"/>. It is emphasised that in the VALUE baselines a separate model is trained for every location; hence, topographic
predictors are not required.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e2120">Gridded predictors from ERA-Interim reanalysis included in <inline-formula><mml:math id="M72" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula>.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Predictor</oasis:entry>
         <oasis:entry colname="col2">Level</oasis:entry>
         <oasis:entry colname="col3">Description</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col3">Surface </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">TMAX</oasis:entry>
         <oasis:entry colname="col2">surface</oasis:entry>
         <oasis:entry colname="col3">Maximum temperature</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">TMEAN</oasis:entry>
         <oasis:entry colname="col2">surface</oasis:entry>
         <oasis:entry colname="col3">Mean temperature</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">U10</oasis:entry>
         <oasis:entry colname="col2">surface</oasis:entry>
         <oasis:entry colname="col3">Northward wind</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">V10</oasis:entry>
         <oasis:entry colname="col2">surface</oasis:entry>
         <oasis:entry colname="col3">Eastward wind</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Pr</oasis:entry>
         <oasis:entry colname="col2">surface</oasis:entry>
         <oasis:entry colname="col3">Accumulated precipitation</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col3">Upper level </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Q</oasis:entry>
         <oasis:entry colname="col2">850, 700, 500 <inline-formula><mml:math id="M73" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">hPa</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">Specific humidity</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">TA</oasis:entry>
         <oasis:entry colname="col2">850, 700, 500 <inline-formula><mml:math id="M74" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">hPa</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">Temperature</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">UA</oasis:entry>
         <oasis:entry colname="col2">850, 700, 500 <inline-formula><mml:math id="M75" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">hPa</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">Northward wind</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">VA</oasis:entry>
         <oasis:entry colname="col2">850, 700, 500 <inline-formula><mml:math id="M76" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">hPa</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">Eastward wind</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col3">Invariant </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ASO</oasis:entry>
         <oasis:entry colname="col2">surface</oasis:entry>
         <oasis:entry colname="col3">Angle of sub-grid-scale orography</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ANSO</oasis:entry>
         <oasis:entry colname="col2">surface</oasis:entry>
         <oasis:entry colname="col3">Anisotropy of sub-grid-scale orography</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">FSO</oasis:entry>
         <oasis:entry colname="col2">surface</oasis:entry>
         <oasis:entry colname="col3">Standard deviation of filtered subgrid orography</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SDO</oasis:entry>
         <oasis:entry colname="col2">surface</oasis:entry>
         <oasis:entry colname="col3">Standard deviation of orography</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GSFC</oasis:entry>
         <oasis:entry colname="col2">surface</oasis:entry>
         <oasis:entry colname="col3">Geopotential</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">LAT</oasis:entry>
         <oasis:entry colname="col2">surface</oasis:entry>
         <oasis:entry colname="col3">Latitude</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">LON</oasis:entry>
         <oasis:entry colname="col2">surface</oasis:entry>
         <oasis:entry colname="col3">Longitude</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col3">Temporal </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Time</oasis:entry>
         <oasis:entry colname="col2">–</oasis:entry>
         <oasis:entry colname="col3">Day of year, transformed as <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:mi>cos⁡</mml:mi><mml:mo>(</mml:mo><mml:mtext>time</mml:mtext><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:mi>sin⁡</mml:mi><mml:mo>(</mml:mo><mml:mtext>time</mml:mtext><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e2449">Evaluation metrics.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col3">Means </oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Metric</oasis:entry>
         <oasis:entry colname="col2">Variables</oasis:entry>
         <oasis:entry colname="col3">Description</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">mb</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Mean bias</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">sp</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Spearman correlation between observed and predicted timeseries</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MAE</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Mean absolute error</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">R01</oasis:entry>
         <oasis:entry colname="col2">Precip</oasis:entry>
         <oasis:entry colname="col3">Relative wet day frequency (predicted precipitation days: observed precipitation days.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">SDII</oasis:entry>
         <oasis:entry colname="col2">Precip</oasis:entry>
         <oasis:entry colname="col3">Mean wet day precipitation</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col3">Extremes </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Metric</oasis:entry>
         <oasis:entry colname="col2">Variables</oasis:entry>
         <oasis:entry colname="col3">Description</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">98P</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Bias in the 98th percentile.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">R10</oasis:entry>
         <oasis:entry colname="col2">Precip</oasis:entry>
         <oasis:entry colname="col3">Relative frequency of days with precipitation greater than 10 <inline-formula><mml:math id="M82" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e2637">Based on the predictors used by methods in the baseline ensemble, winds, humidity and temperature are included at multiple levels together with time,
latitude, longitude and invariant fields. Predictors are summarised in Table 1.</p>
      <p id="d1e2640">For the sub-grid-scale information for input into the final MLP, the point measurement of three products is provided at each station. True station
elevation is taken from the Global Multi-resolution Terrain Elevation Dataset <xref ref-type="bibr" rid="bib1.bibx13" id="paren.36"/>. This is provided to the model together with the difference
between the ERA-Interim grid-scale resolution elevation and true elevation. Finally, topographic prominence is quantified using the ALOS Global mTPI
<xref ref-type="bibr" rid="bib1.bibx58" id="paren.37"/>.</p>
      <p id="d1e2649">Results of the convCNP model are compared to all available PP models in the VALUE ensemble, a total of 16 statistical models for precipitation and
23 for maximum temperature. These models comprise a range of techniques<?pagebreak page258?> including analogues, multiple linear regression, generalised multiple linear
regression and genetic programming. For a complete description of all models included in the comparison, see Appendix A.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e2654">Comparison of the convCNP model to the GP-baseline. Boxes summarise model performance over the 86 held-out VALUE stations for maximum temperature <bold>(a–c)</bold> and precipitation <bold>(d–f)</bold> for each of the mean metrics.</p></caption>
            <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022-f06.png"/>

          </fig>

</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <label>2.2.2</label><title>Experiment 2 – performance at unseen locations</title>
      <p id="d1e2677">We next quantify model performance at unseen locations compared to an interpolation baseline. The convCNP models are retrained using station data from
the European Climate Assessment Dataset (ECA&amp;D), comprising 3010 stations for precipitation and 3047 stations for maximum temperature (Fig. 2). The
86 VALUE stations are held out as the validation set, testing the model performance at both unseen times and locations.</p>
      <p id="d1e2680">As existing downscaling models are unable to handle unseen locations, it is necessary to construct a new baseline. A natural baseline for this problem
is to construct individual models for each station using the training set, use these to make predictions at future times and then interpolate to<?pagebreak page259?> get
predictions at the held-out locations. For the single-station models, predictors are taken from ERA-Interim data at the closest grid box, similar to
<xref ref-type="bibr" rid="bib1.bibx22" id="text.38"/>. Multiple linear regression is used for maximum temperature. For precipitation, occurrence is modelled using logistic
regression, and accumulation is modelled using a generalised linear model with gamma error distribution, similar to <xref ref-type="bibr" rid="bib1.bibx55" id="text.39"/>. These methods are
chosen as they are amongst the best-performing methods of the VALUE ensemble for each variable <xref ref-type="bibr" rid="bib1.bibx23" id="paren.40"/>.</p>
      <p id="d1e2692">Following techniques used to convert station observations to gridded datasets <xref ref-type="bibr" rid="bib1.bibx25" id="paren.41"/>, predictions at these known stations in the
future time period are made by first interpolating monthly means (totals) for temperature (precipitation) using a thin-plate spline and then using a GP
to interpolate the anomalies (fraction of the total value). All interpolation is three-dimensional over longitude, latitude and elevation. Throughout
the results section, this model is referred to as the GP-baseline.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS3">
  <label>2.2.3</label><title>Experiment 3 – topography ablation</title>
      <p id="d1e2706">Finally, the impact of topography on predictions is quantified. Experiment 2 is repeated three times with different combinations of topographic data
fed into the final MLP (step 3 in Fig. 1): no topographic data, elevation and elevation difference only, and mTPI only.</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="d1e2711">Spatial distribution of mean absolute error for convCNP <bold>(a, d)</bold>, GP-baseline <bold>(b, e)</bold> and convCNP–GP-baseline <bold>(c, f)</bold>. Maximum temperature (precipitation) is shown on the top (bottom) row. All panels show results for each of the 86 held-out VALUE stations.</p></caption>
            <?xmltex \igopts{width=412.564961pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022-f07.png"/>

          </fig>

<?xmltex \hack{\newpage}?>
</sec>
</sec>
<?pagebreak page260?><sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Evaluation metrics</title>
      <p id="d1e2740">A selection of standard climate metrics are chosen to assess model performance over the evaluation period, quantifying the representation of mean
properties and extreme events (Table 2). Metrics are chosen based on those reported for the VALUE baseline ensemble
<xref ref-type="bibr" rid="bib1.bibx23 bib1.bibx67 bib1.bibx45 bib1.bibx28" id="paren.42"/>.</p>
      <p id="d1e2746">Comparison to these metrics requires generating a time series of values from the distributions predicted by the convCNP model. For temperature, this is
generated by taking the mean of the predicted distribution for mean metrics, and sampling is used to complete the extreme metrics. For precipitation,
a day is first classified as wet if <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> or dry if <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula>. For wet days, accumulations are generated by taking the mean of the gamma
distribution for mean metrics or sampling for extreme metrics.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results: baseline comparison (experiment 1)</title>
      <p id="d1e2782">The convCNP model outperforms all VALUE baselines on median mean absolute error (MAE) and Spearman correlation for both maximum temperature and
precipitation. Comparisons of convCNP model performance at the 86 VALUE stations to each model in the VALUE baseline ensemble are shown in Fig. 4. The
low MAE and high Spearman correlation indicate that the model performs well at capturing day-to-day variability.</p>
      <p id="d1e2785">For maximum temperature, the mean bias is larger than baseline models at many stations, with interquartile range <inline-formula><mml:math id="M85" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.02 to
0.08 <inline-formula><mml:math id="M86" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>. This is a direct consequence of training a global model as opposed to individual models to each station which will trivially
correct the mean <xref ref-type="bibr" rid="bib1.bibx41" id="paren.43"/>. Though larger than baseline models, this error is still small for a majority of stations. Similarly
for precipitation, though mean biases are larger than many of the VALUE models, the interquartile range is just <inline-formula><mml:math id="M87" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.07 to 0.12 <inline-formula><mml:math id="M88" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula>. For
precipitation, the bias in convCNP relative wet day frequency<?pagebreak page261?> (R01) and mean wet day precipitation (SDII) are comparable to the best models in the
VALUE ensemble (not shown).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e2827">The same as for Fig. 6 but for P98 and R10 biases.</p></caption>
        <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022-f08.png"/>

      </fig>

      <p id="d1e2837">When downscaling GCM output for impact studies, it is of particular importance to accurately reproduce extreme events <xref ref-type="bibr" rid="bib1.bibx33" id="paren.44"/>. In line
with previous work comparing the VALUE baselines <xref ref-type="bibr" rid="bib1.bibx28" id="paren.45"/>, an extreme event is defined to be a value greater than the 98th
percentile of observations. Comparisons of biases in the 98th percentile of maximum temperature and precipitation are shown in Fig. 5. The convCNP
performs similarly to the best baselines, with a median bias of <inline-formula><mml:math id="M89" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.02 <inline-formula><mml:math id="M90" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> for temperature and <inline-formula><mml:math id="M91" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.04 <inline-formula><mml:math id="M92" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> for precipitation
across the VALUE stations. R10 biases are comparable to baselines, with a median bias of just <inline-formula><mml:math id="M93" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.003 <inline-formula><mml:math id="M94" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula>.</p>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Results: performance at unseen locations (experiment 2)</title>
      <p id="d1e2904">The convCNP model outperforms the GP-baseline at unseen stations. Results for MAE, Spearman correlation and mean bias are shown in Fig. 6. For maximum
temperature, the convCNP model gives small improvements over the baseline model, with Spearman correlations of 0.99 (0.98) and MAE of
1.19 <inline-formula><mml:math id="M95" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> (1.35 <inline-formula><mml:math id="M96" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>) for the convCNP (GP baseline). Importantly, large outliers (<inline-formula><mml:math id="M97" display="inline"><mml:mo lspace="0mm">&gt;</mml:mo></mml:math></inline-formula> 10 <inline-formula><mml:math id="M98" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>) in the
baseline MAE are not observed in the convCNP predictions. Figure 7 shows the spatial distribution of MAE for the convCNP and GP-baseline together with
the difference in MAE between the two models. This demonstrates that stations with high MAE in the convCNP model are primarily concentrated in the
complex topography of the European Alps. The GP-baseline model displays large MAE not only in the Alps but also at other locations, for example in
Spain and France. The convCNP improves predictions at 82 out of the 86 stations.</p>
      <p id="d1e2950">Repeating this analysis for precipitation, the convCNP model gives substantial improvement over the baseline for MAE and Spearman
correlation. Spearman correlations are 0.57 (0.20) and MAE 2.10 <inline-formula><mml:math id="M99" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> (2.71 <inline-formula><mml:math id="M100" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula>) for convCNP (GP-baseline). In contrast to maximum
temperature, there is no clear link between topography and MAE, though again convCNP predictions have large MAE for multiple stations located in the
Alps. The convCNP model improves on baseline predictions at 80 out of 86 stations.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><?xmltex \currentcnt{9}?><?xmltex \def\figurename{Figure}?><label>Figure 9</label><caption><p id="d1e2971">The same as for Fig. 7 but for P98 biases. Here, the “difference” panels quantify the difference in absolute bias <inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:mi>P</mml:mi><mml:msub><mml:mn mathvariant="normal">98</mml:mn><mml:mtext>convCNP</mml:mtext></mml:msub><mml:mo>|</mml:mo><mml:mo>-</mml:mo><mml:mo>|</mml:mo><mml:mi>P</mml:mi><mml:msub><mml:mn mathvariant="normal">98</mml:mn><mml:mtext>GP-baseline</mml:mtext></mml:msub><mml:mo>|</mml:mo></mml:mrow></mml:math></inline-formula>. Negative (positive) values indicate that the convCNP (GP-baseline) has better performance.</p></caption>
        <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022-f09.png"/>

      </fig>

      <p id="d1e3011">Comparisons between models for extreme metrics are shown in Fig. 8. For maximum temperature, the convCNP has slightly lower absolute 98th percentile
bias than the baseline. For precipitation, errors are substantially lower, with median absolute 98th percentile bias of 4.90 <inline-formula><mml:math id="M102" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> for convCNP
compared to 22.92 <inline-formula><mml:math id="M103" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> for GP-baseline. The spatial distributions of 98th percentile bias for maximum temperature and precipitation
predictions together with the difference in absolute bias are shown in Fig. 9. For maximum temperature, the convCNP does not improve on the baseline
at all stations. The GP-baseline exhibits uniformly positive biases, while the convCNP model has both positive and negative biases. Improvements are
seen through central and eastern Europe, while the convCNP performs comparatively poorly in southern Europe and the British Isles. For precipitation,
predictions have low biases across much of Europe for the convCNP, with the exception of in the complex terrain of the Alps. GP-baseline biases are
negative throughout the domain. For this case, convCNP predictions have lower bias at 84 of the 86 validation stations.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F10" specific-use="star"><?xmltex \currentcnt{10}?><?xmltex \def\figurename{Figure}?><label>Figure 10</label><caption><p id="d1e3032">Histograms showing probability integral transforms for model predictions compared to a uniform distribution to assess calibration for temperature <bold>(a–c)</bold> and precipitation <bold>(d–f)</bold>. For temperature PIT plots are shown for all values <bold>(a)</bold>, a station where the model is well calibrated (Bragança, Portugal; <bold>b</bold>) and a station where the model is poorly calibrated (Gospić, Croatia; <bold>c</bold>). Similarly for precipitation, PIT plots are shown for all values <bold>(d)</bold>, a station where the model is well calibrated (Stornoway, UK; <bold>e</bold>) and a station where the model is poorly calibrated (Sodankylä, Finland; <bold>f</bold>).</p></caption>
        <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022-f10.png"/>

      </fig>

      <p id="d1e3066">A limitation to the analysis of the standard climate metrics in Table 2 is that these only assess certain aspects of the predicted distribution. To
assess the calibration of the models, we next examine the probability integral transform (PIT) values. The PIT value for a given prediction is defined
as the cumulative density function (CDF) of the distribution predicted by the convCNP model evaluated at the true observed value. These values can be used to determine whether the
model is calibrated by evaluating the PIT for every model prediction at the true observation, and plotting their distribution. If the model is
properly calibrated, it is both necessary and sufficient for this distribution to be uniform <xref ref-type="bibr" rid="bib1.bibx19" id="paren.46"/>. PIT distributions for
maximum temperature and wet-day precipitation are shown in Fig. 10. For temperature, the model is well calibrated overall, although the predicted
distributions are often too narrow, as demonstrated by the peaks around zero and one indicating that the observed value falls outside the predicted
normal distribution. Calibration of the precipitation model is poorer overall. The peak in PIT mass around zero indicates that this model often over-predicts rainfall accumulation. Performance varies between individual stations for both temperature and precipitation, with examples of PIT
distributions for both well-calibrated and poorly calibrated stations shown in Fig. 10.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F11" specific-use="star"><?xmltex \currentcnt{11}?><?xmltex \def\figurename{Figure}?><label>Figure 11</label><caption><p id="d1e3074">Comparison of model performance in the topography ablation experiment. The complete model (All) is compared to models with no topographic data (None), elevation and elevation difference only (Elevation) and mTPI only (mTPI). Boxes summarise model performance over the 86 held-out VALUE stations for maximum temperature <bold>(a–c)</bold> and precipitation <bold>(d–f)</bold> for each of the mean metrics.</p></caption>
        <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022-f11.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12" specific-use="star"><?xmltex \currentcnt{12}?><?xmltex \def\figurename{Figure}?><label>Figure 12</label><caption><p id="d1e3092">The same as Fig. 11 but for extreme metrics.</p></caption>
        <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/251/2022/gmd-15-251-2022-f12.png"/>

      </fig>

</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Results: topography ablation (experiment 3)</title>
      <p id="d1e3110">Results of the topography ablation experiment are shown in Fig. 11 (mean metrics) and Fig. 12 (extreme metrics). These figures compare the performance
on each metric between the convCNP model with all topographic predictors and convCNP models trained with no topography, elevation and elevation
difference only, and mTPI only.</p>
      <p id="d1e3113">For maximum temperature, inclusion of topographic information improves MAE, mean bias and Spearman correlation. Models including only mTPI or no
topographic predictors have a number of stations with very large MAE, exceeding 10 <inline-formula><mml:math id="M104" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> at several stations. Unsurprisingly, these
stations are found to be located in areas of complex topography in the Alps (not shown). Including elevation both decreases the median MAE and
corrects errors at these outliers, with further improvement observed with mTPI added. A similar pattern is seen for mean bias. More modest
improvements are seen for precipitation, though inclusion of topographic data does result in slightly improved performance.</p>
      <?pagebreak page264?><p id="d1e3128">For maximum temperature, inclusion of topographic data results in reduced 98th percentile bias. This is primarily as a result of including elevation
and elevation difference data, with limited benefit derived from the inclusion of mTPI. In contrast, for precipitation, models with topographic
correction perform worse than the elevation agnostic model for both 98th percentile and R10 biases. This reduced performance for precipitation may
result from overfitting.</p>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Discussion and conclusion</title>
      <p id="d1e3139">This study demonstrated the successful application of convCNPs to statistical downscaling of temperature and precipitation. The convCNP model performs
well compared to strong baselines from the VALUE ensemble on both mean and extreme metrics. For both variables the convCNP model outperforms an
interpolation-based baseline. Inclusion of sub-grid-scale topographic information is shown to improve model performance for mean and extreme metrics
for maximum temperature and mean metrics for precipitation. The convCNP model has a significant advantage over these baselines in that the output
prediction is a continuous function, allowing predictions to be made at an arbitrary (longitude, latitude, elevation) location. Although only
temperature and precipitation are considered in this study, the model is easily applied to any climate variable with available station observations,
for example wind speed.</p>
      <p id="d1e3142"><?xmltex \hack{\newpage}?>Several areas remain for future work, both within the convCNP model and in comparison to other downscaling methods. In the convCNP predictions,
representation of certain metrics, notably precipitation extremes requires further improvement, particularly in areas with complex topography. The
topography ablation experiments demonstrate that the convCNP P98 bias increases in regions with complex topography. Dynamically, this is likely due to
local flow effects such as Föhn winds <xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx4" id="paren.47"/>, which depend on the incident angle of the background flow. A
possible explanation for this is that the MLP is insufficient to model these effects. Further experimentation with adding a second CNN to
capture the sub-grid-scale processes and possibly conditioning predictions of this model on local flow is left as a topic for future
research. Another avenue for improving model performance would be to change the distribution predicted by the convCNP. Model calibration results
presented in Sect. 4 indicate that the temperature downscaling model could be improved using a distribution with heavier tails. Precipitation model
calibration requires improvement, with the model frequently under-predicting wet-day accumulations. A possible explanation for this is that the left-hand tail of the gamma distribution decays rapidly. For cases where the mode of the predicted distribution is greater than zero, small observed
accumulations are heavily penalised. Previous work has acknowledged that the Bernoulli–gamma distribution used in this study is not
realistic for all sites <xref ref-type="bibr" rid="bib1.bibx63" id="paren.48"/> and suggested that representation of precipitation extremes can be improved using a
Bernoulli–gamma–generalised Pareto distribution <xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx64" id="paren.49"/>. Future work will explore improving the
calibration of the downscaling models using mixture distributions and normalising flows <xref ref-type="bibr" rid="bib1.bibx52" id="paren.50"/> to improve the calibration <?pagebreak page265?>of
the model. A further possibility for extending the convCNP model would be to explicitly incorporate time by building recurrence into the model
<xref ref-type="bibr" rid="bib1.bibx50 bib1.bibx56" id="paren.51"/>.</p>
      <p id="d1e3161">Future work will also focus on developing a standardised framework to compare the convCNP model to a variety of deep-learning baselines, building on
the work of <xref ref-type="bibr" rid="bib1.bibx61" id="paren.52"/>. Although some studies have indicated that in certain cases deep-learning models offer little advantage
over widely used statistical methods such as those included in the VALUE ensemble <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx61" id="paren.53"/>, others
suggest that deep-learning methods offer improved performance
<xref ref-type="bibr" rid="bib1.bibx66 bib1.bibx59 bib1.bibx29 bib1.bibx38 bib1.bibx54 bib1.bibx47" id="paren.54"/>. Further work is
required both to rigorously compare the convCNP model to other machine learning models for downscaling and to generate a standardised intercomparison
of models more broadly. Examination of a larger set of metrics, particularly for precipitation, would also be beneficial.</p>
      <p id="d1e3173">The final aspect to consider is extending these promising results downscaling reanalysis data to apply to future climate simulations from GCMs. An in
depth analysis of the convCNP model performance on seasonal and annual metrics would be beneficial in informing application to impact scenarios. A
limitation in all PP downscaling techniques is that applying a transfer function trained on reanalysis data to a GCM makes the assumption that the
predictors included in the context set are realistically simulated in the GCM <xref ref-type="bibr" rid="bib1.bibx41" id="paren.55"/>. Future work will aim to address this
issue through training a convCNP model directly on RCM or GCM hindcasts available through projects such as EURO-CORDEX <xref ref-type="bibr" rid="bib1.bibx31" id="paren.56"/>.</p><?xmltex \hack{\clearpage}?>
</sec>

      
      </body>
    <back><app-group>

<?pagebreak page266?><app id="App1.Ch1.S1">
  <?xmltex \currentcnt{A}?><label>Appendix A</label><title>VALUE ensemble methods</title>
      <p id="d1e3194">Table A1 summarises the baseline methods in the VALUE ensemble. This information is adapted from <xref ref-type="bibr" rid="bib1.bibx23" id="text.57"/>.</p>

<?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.S1.T3"><?xmltex \hack{\hsize\textwidth}?><?xmltex \currentcnt{A1}?><label>Table A1</label><caption><p id="d1e3204">Summary of models included in the VALUE ensemble.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="120mm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Model</oasis:entry>
         <oasis:entry colname="col2">Variables</oasis:entry>
         <oasis:entry colname="col3">Description</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">ANALOGUE</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Standard analogue, no seasonal component <xref ref-type="bibr" rid="bib1.bibx22" id="paren.58"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ANALOGUE-ANOM</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">Analogue with seasonal component <xref ref-type="bibr" rid="bib1.bibx2" id="paren.59"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ANALOGUE-MP</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Analogue method with seasonal component <xref ref-type="bibr" rid="bib1.bibx51" id="paren.60"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ANALOGUE-SP</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Analogue method with seasonal component <xref ref-type="bibr" rid="bib1.bibx51" id="paren.61"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ESD-EOFSLP</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">Multiple linear regression <xref ref-type="bibr" rid="bib1.bibx6" id="paren.62"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ESD-SLP</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">Multiple linear regression <xref ref-type="bibr" rid="bib1.bibx6" id="paren.63"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ESD-T2</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">Multiple linear regression <xref ref-type="bibr" rid="bib1.bibx6" id="paren.64"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">FIC01P</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Two-step analogue method <xref ref-type="bibr" rid="bib1.bibx53" id="paren.65"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">FIC03P</oasis:entry>
         <oasis:entry colname="col2">precip</oasis:entry>
         <oasis:entry colname="col3">Two-step analogue method <xref ref-type="bibr" rid="bib1.bibx53" id="paren.66"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GLM</oasis:entry>
         <oasis:entry colname="col2">precip</oasis:entry>
         <oasis:entry colname="col3">Generalised linear model with log-canonical link function <xref ref-type="bibr" rid="bib1.bibx55" id="paren.67"/>, Bernoulli error distribution for occurrence and gamma error distribution for accumulation; predictions sampled from output distribution</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GLM-det</oasis:entry>
         <oasis:entry colname="col2">precip</oasis:entry>
         <oasis:entry colname="col3">As for GLM, predictions given as mean of output distribution <xref ref-type="bibr" rid="bib1.bibx55" id="paren.68"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GLM-WT</oasis:entry>
         <oasis:entry colname="col2">precip</oasis:entry>
         <oasis:entry colname="col3">As for GLM, conditioned on 12 weather types identified by <inline-formula><mml:math id="M113" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-means clustering <xref ref-type="bibr" rid="bib1.bibx55" id="paren.69"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MLR</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">Multiple linear regression using principal component analysis (PCA) for predictors <xref ref-type="bibr" rid="bib1.bibx22" id="paren.70"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MLR-AAI</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Multiple linear regression, annual training, anomaly data, inflation variance correction <xref ref-type="bibr" rid="bib1.bibx30" id="paren.71"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MLR-AAN</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Multiple linear regression, annual training, anomaly data, white-noise variance correction <xref ref-type="bibr" rid="bib1.bibx30" id="paren.72"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MLR-AAW</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Multiple linear regression, annual training, anomaly data, white-noise variance correction <xref ref-type="bibr" rid="bib1.bibx30" id="paren.73"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MLR-ASI</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Multiple linear regression, seasonal training, anomaly data, inflation variance correction <xref ref-type="bibr" rid="bib1.bibx30" id="paren.74"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MLR-ASW</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Multiple linear regression, seasonal training, anomaly data, white-noise variance correction <xref ref-type="bibr" rid="bib1.bibx30" id="paren.75"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MLR-PCA-ZTR</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">Multiple linear regression with s-mode principal component predictors <xref ref-type="bibr" rid="bib1.bibx32" id="paren.76"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MLR-RAN</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Multiple linear regression, seasonal training, raw data, no variance correction <xref ref-type="bibr" rid="bib1.bibx30" id="paren.77"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MLR-RSN</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Multiple linear regression, seasonal training, raw data, no variance correction <xref ref-type="bibr" rid="bib1.bibx30" id="paren.78"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MLR-SDSM</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Single-site multiple linear regression using the statistical downscaling method <xref ref-type="bibr" rid="bib1.bibx68" id="paren.79"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MLR-WT</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">As for MLR but conditioned on weather types defined using <inline-formula><mml:math id="M125" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-means clustering <xref ref-type="bibr" rid="bib1.bibx22" id="paren.80"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MO-GP</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Multi-objective genetic programming <xref ref-type="bibr" rid="bib1.bibx70" id="paren.81"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SWG</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Two-step vectorised generalised linear models <xref ref-type="bibr" rid="bib1.bibx2" id="paren.82"/>.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">WT-WG</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula>, precip</oasis:entry>
         <oasis:entry colname="col3">Distributional fitting based on weather types selected using <inline-formula><mml:math id="M129" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-means clustering <xref ref-type="bibr" rid="bib1.bibx22" id="paren.83"/>.</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \hack{\clearpage}?>
</app>
  </app-group><notes notes-type="codeavailability"><title>Code availability</title>

      <p id="d1e3861">Model code is available at <uri>https://github.com/anna-184702/convCNPClimate</uri> (last access: 14 December 2020) and <ext-link xlink:href="https://doi.org/10.5281/zenodo.4554603" ext-link-type="DOI">10.5281/zenodo.4554603</ext-link> <xref ref-type="bibr" rid="bib1.bibx62" id="paren.84"/>.</p>
  </notes><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e3876">ERA-Interim reanalysis data are publicly available at
<uri>https://apps.ecmwf.int/datasets/data/interim-full-daily/levtype=sfc/</uri> <xref ref-type="bibr" rid="bib1.bibx14" id="paren.85"/>. Elevation data are available through the Google Earth engine at <uri>https://developers.google.com/earth-engine/datasets/catalog/USGS_GMTED2010</uri> <xref ref-type="bibr" rid="bib1.bibx13" id="paren.86"/> and ALOS mTPI
<uri>https://developers.google.com/earth-engine/datasets/catalog/CSP_ERGo_1_0_Global_ALOS_mTPI</uri> <xref ref-type="bibr" rid="bib1.bibx58" id="paren.87"/>. ECA&amp;D observations are available at <uri>https://www.ecad.eu/dailydata/index.php</uri> <xref ref-type="bibr" rid="bib1.bibx35" id="paren.88"/>.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e3907">AV implemented the code, conducted the experiments and wrote the first draft. All authors designed the study and contributed to the analysis of results and final version of the paper.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e3913">The authors declare that they have no conflict of interest.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e3919">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="d1e3925">Anna Vaughan acknowledges the UKRI Centre for Doctoral Training in the Application of Artificial Intelligence to the study of Environmental Risks (AI4ER), led by the University of Cambridge and British Antarctic Survey, and studentship funding from Google DeepMind. Will Tebbutt is supported by Google DeepMind.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e3931">This research has been supported by the UKRI Centre for Doctoral Training in the Application of Artificial Intelligence to the study of Environmental Risks (AI4ER), led by the University of Cambridge and British Antarctic Survey, and by Google DeepMind.</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e3937">This paper was edited by Simone Marras and reviewed by two anonymous referees.</p>
  </notes><ref-list>
    <title>References</title>

      <ref id="bib1.bibx1"><?xmltex \def\ref@label{{Allen et~al.(2016)Allen, Boschung, Nauels, Xia, Bex, and Midgley}}?><label>Allen et al.(2016)Allen, Boschung, Nauels, Xia, Bex, and Midgley</label><?label allen2016climate?><mixed-citation>
Allen, S., Boschung, J., Nauels, A., Xia, Y., Bex, V., and Midgley, P.:
Climate change 2013: the physical science basis. Contribution of working group I to the fifth assessment report of the Intergovernmental Panel on Climate Change, Cambridge University Press, Cambridge, UK, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx2"><?xmltex \def\ref@label{{Ayar et~al.(2016)Ayar, Vrac, Bastin, Carreau, D{\'{e}}qu{\'{e}}, and Gallardo}}?><label>Ayar et al.(2016)Ayar, Vrac, Bastin, Carreau, Déqué, and Gallardo</label><?label ayar2016intercomparison?><mixed-citation>
Ayar, P. V., Vrac, M., Bastin, S., Carreau, J., Déqué, M., and Gallardo, C.:
Intercomparison of statistical and dynamical downscaling models under the EURO-and MED-CORDEX initiative framework: present climate evaluations,
Clim. Dynam.,
46, 1301–1329, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx3"><?xmltex \def\ref@label{{Ba{\~{n}}o-Medina et~al.(2020)Ba{\~{n}}o-Medina, Garc{\'{\i}}a~Manzanas, Guti{\'{e}}rrez~Llorente et~al.}}?><label>Baño-Medina et al.(2020)Baño-Medina, García Manzanas, Gutiérrez Llorente et al.</label><?label bano2020configuration?><mixed-citation>Baño-Medina, J., Manzanas, R., and Gutiérrez, J. M.: Configuration and intercomparison of deep learning neural models for statistical downscaling, Geosci. Model Dev., 13, 2109–2124, <ext-link xlink:href="https://doi.org/10.5194/gmd-13-2109-2020" ext-link-type="DOI">10.5194/gmd-13-2109-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx4"><?xmltex \def\ref@label{{Basist et~al.(1994)Basist, Bell, and Meentemeyer}}?><label>Basist et al.(1994)Basist, Bell, and Meentemeyer</label><?label basist1994statistical?><mixed-citation>
Basist, A., Bell, G. D., and Meentemeyer, V.:
Statistical relationships between topography and precipitation patterns,
J. Climate,
7, 1305–1315, 1994.</mixed-citation></ref>
      <ref id="bib1.bibx5"><?xmltex \def\ref@label{{Ben~Alaya et~al.(2015)Ben~Alaya, Chebana, and Ouarda}}?><label>Ben Alaya et al.(2015)Ben Alaya, Chebana, and Ouarda</label><?label ben2015probabilistic?><mixed-citation>
Ben Alaya, M. A., Chebana, F., and Ouarda, T. B.:
Probabilistic multisite statistical downscaling for daily precipitation using a Bernoulli–generalized pareto multivariate autoregressive model,
J. Climate,
28, 2349–2364, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx6"><?xmltex \def\ref@label{{Benestad et~al.(2015)Benestad, Chen, Mezghani, Fan, and Parding}}?><label>Benestad et al.(2015)Benestad, Chen, Mezghani, Fan, and Parding</label><?label benestad2015using?><mixed-citation>Benestad, R. E., Chen, D., Mezghani, A., Fan, L., and Parding, K.:
On using principal components to represent stations in empirical–statistical downscaling, Tellus A, 67, 28326, <ext-link xlink:href="https://doi.org/10.3402/tellusa.v67.28326" ext-link-type="DOI">10.3402/tellusa.v67.28326</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx7"><?xmltex \def\ref@label{{Bevacqua et~al.(2017)Bevacqua, Maraun, Hob{\ae}k~Haff, Widmann, and Vrac}}?><label>Bevacqua et al.(2017)Bevacqua, Maraun, Hobæk Haff, Widmann, and Vrac</label><?label bevacqua2017multivariate?><mixed-citation>Bevacqua, E., Maraun, D., Hobæk Haff, I., Widmann, M., and Vrac, M.: Multivariate statistical modelling of compound events via pair-copula constructions: analysis of floods in Ravenna (Italy), Hydrol. Earth Syst. Sci., 21, 2701–2723, <ext-link xlink:href="https://doi.org/10.5194/hess-21-2701-2017" ext-link-type="DOI">10.5194/hess-21-2701-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx8"><?xmltex \def\ref@label{{Bhardwaj et~al.(2018)Bhardwaj, Misra, Mishra, Wootten, Boyles, Bowden, and Terando}}?><label>Bhardwaj et al.(2018)Bhardwaj, Misra, Mishra, Wootten, Boyles, Bowden, and Terando</label><?label bhardwaj2018downscaling?><mixed-citation>
Bhardwaj, A., Misra, V., Mishra, A., Wootten, A., Boyles, R., Bowden, J., and Terando, A. J.:
Downscaling future climate change projections over Puerto Rico using a non-hydrostatic atmospheric model, Climatic Change, 147, 133–147, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx9"><?xmltex \def\ref@label{{Cannon(2008)}}?><label>Cannon(2008)</label><?label cannon2008probabilistic?><mixed-citation>
Cannon, A. J.:
Probabilistic multisite precipitation downscaling by an expanded Bernoulli–Gamma density network,
J. Hydrometeorol.,
9, 1284–1300, 2008.</mixed-citation></ref>
      <ref id="bib1.bibx10"><?xmltex \def\ref@label{{Cannon et~al.(2020)Cannon, Piani, and Sippel}}?><label>Cannon et al.(2020)Cannon, Piani, and Sippel</label><?label cannon2020bias?><mixed-citation>Cannon, A. J., Piani, C., and Sippel, S.: Bias correction of climate model output for impact models, chap. 5, in: Climate Extremes and Their Implications for Impact and Risk Assessment, edited by: Sillmann, J., Sippel, S., and Russo, S., Elsevier, 77–104, <ext-link xlink:href="https://doi.org/10.1016/B978-0-12-814895-2.00005-7" ext-link-type="DOI">10.1016/B978-0-12-814895-2.00005-7</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx11"><?xmltex \def\ref@label{{Casanueva et~al.(2016)Casanueva, Herrera, Fern{\'{a}}ndez, and Guti{\'{e}}rrez}}?><label>Casanueva et al.(2016)Casanueva, Herrera, Fernández, and Gutiérrez</label><?label casanueva2016towards?><mixed-citation>
Casanueva, A., Herrera, S., Fernández, J., and Gutiérrez, J. M.:
Towards a fair comparison of statistical and dynamical downscaling in the framework of the EURO-CORDEX initiative,
Climatic Change,
137, 411–426, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx12"><?xmltex \def\ref@label{{Chollet(2017)}}?><label>Chollet(2017)</label><?label chollet2017xception?><mixed-citation>
Chollet, F.:
Xception: Deep learning with depthwise separable convolutions,
in: Proceedings of the IEEE conference on computer vision and pattern recognition, 1251–1258, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx13"><?xmltex \def\ref@label{{Danielson and Gesch(2011)}}?><label>Danielson and Gesch(2011)</label><?label gmtr?><mixed-citation>Danielson, J. J. and Gesch, D. B.: Global multi-resolution terrain elevation data 2010 (GMTED2010), U.S. Geological Survey Open-File Report 2011-1073, 26 pp., available at: <uri>https://developers.google.com/earth-engine/datasets/catalog/USGS_GMTED2010</uri> (last access: 8 December 2020), 2011.</mixed-citation></ref>
      <ref id="bib1.bibx14"><?xmltex \def\ref@label{{Dee et~al.(2011)}}?><label>Dee et al.(2011)</label><?label dee2011era?><mixed-citation>Dee, D. P., Uppala, S. M., Simmons, A. J., Berrisford, P., Poli, P., Kobayashi, S., Andrae, U., Balmaseda, M. A., Balsamo, G., Bauer, P., Bechtold, P., Beljaars, A. C. M., van de Berg, L., Bidlot, J., Bormann, N., Delsol, C., Dragani, R., Fuentes, M., Geer, A. J., Haimberger, L., Healy,
S. B., Hersbach, H., Hólm, E. V., Isaksen, L., Kållberg, P., Köhler, M., Matricardi, M., McNally, A. P., Monge-Sanz, B. M., Morcrette, J.-J., Park, B.-K., Peubey, C., de R<?pagebreak page268?>osnay, P., Tavolato, C., Thépaut, J.-N., and Vitart, F.: The ERA-Interim reanalysis: Configuration and performance of the data assimilation system, Q. J. Roy. Meteor. Soc.,
137, 553–597, <ext-link xlink:href="https://doi.org/10.1002/qj.828" ext-link-type="DOI">10.1002/qj.828</ext-link>, 2011 (data available at: <uri>https://apps.ecmwf.int/datasets/data/interim-full-daily/levtype=sfc/</uri>, last access: 7 December 2020).</mixed-citation></ref>
      <ref id="bib1.bibx15"><?xmltex \def\ref@label{{Dubois et~al.(2020)Dubois, Gordon, and Foong}}?><label>Dubois et al.(2020)Dubois, Gordon, and Foong</label><?label dubois2020npf?><mixed-citation>Dubois, Y., Gordon, J., and Foong, A. Y.:
Neural Process Family,
available at: <uri>http://yanndubs.github.io/Neural-Process-Family/</uri>, last access: 10 December 2020.</mixed-citation></ref>
      <ref id="bib1.bibx16"><?xmltex \def\ref@label{{Gaffin(2007)}}?><label>Gaffin(2007)</label><?label gaffin2007foehn?><mixed-citation>
Gaffin, D. M.:
Foehn winds that produced large temperature differences near the southern Appalachian Mountains,
Weather Forecast.,
22, 145–159, 2007.</mixed-citation></ref>
      <ref id="bib1.bibx17"><?xmltex \def\ref@label{{Garnelo et~al.(2018)Garnelo, Rosenbaum, Maddison, Ramalho, Saxton, Shanahan, Teh, Rezende, and Eslami}}?><label>Garnelo et al.(2018)Garnelo, Rosenbaum, Maddison, Ramalho, Saxton, Shanahan, Teh, Rezende, and Eslami</label><?label garnelo2018conditional?><mixed-citation>Garnelo, M., Rosenbaum, D., Maddison, C. J., Ramalho, T., Saxton, D., Shanahan, M., Teh, Y. W., Rezende, D. J., and Eslami, S.:
Conditional neural processes,
arXiv [preprint], <ext-link xlink:href="https://arxiv.org/abs/1807.01613">arXiv:1807.01613</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx18"><?xmltex \def\ref@label{{Ghosh and Mujumdar(2008)}}?><label>Ghosh and Mujumdar(2008)</label><?label ghosh2008statistical?><mixed-citation>
Ghosh, S. and Mujumdar, P. P.:
Statistical downscaling of GCM simulations to streamflow using relevance vector machine,
Adv. Water Resour.,
31, 132–146, 2008.</mixed-citation></ref>
      <ref id="bib1.bibx19"><?xmltex \def\ref@label{{Gneiting et~al.(2007)Gneiting, Balabdaoui, and Raftery}}?><label>Gneiting et al.(2007)Gneiting, Balabdaoui, and Raftery</label><?label gneiting2007probabilistic?><mixed-citation>
Gneiting, T., Balabdaoui, F., and Raftery, A. E.:
Probabilistic forecasts, calibration and sharpness,
J. R. Stat. Soc. B,
69, 243–268, 2007.</mixed-citation></ref>
      <ref id="bib1.bibx20"><?xmltex \def\ref@label{{Gordon et~al.(2019)Gordon, Bruinsma, Foong, Requeima, Dubois, and Turner}}?><label>Gordon et al.(2019)Gordon, Bruinsma, Foong, Requeima, Dubois, and Turner</label><?label gordon2019convolutional?><mixed-citation>Gordon, J., Bruinsma, W. P., Foong, A. Y., Requeima, J., Dubois, Y., and Turner, R. E.:
Convolutional conditional neural processes,
arXiv [preprint], <ext-link xlink:href="https://arxiv.org/abs/1910.13556">arXiv:1910.13556</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx21"><?xmltex \def\ref@label{{Groenke et~al.(2020)Groenke, Madaus, and Monteleoni}}?><label>Groenke et al.(2020)Groenke, Madaus, and Monteleoni</label><?label groenke2020climalign?><mixed-citation>
Groenke, B., Madaus, L., and Monteleoni, C.:
ClimAlign: Unsupervised statistical downscaling of climate variables via normalizing flows,
in: Proceedings of the 10th International Conference on Climate Informatics, 60–66, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx22"><?xmltex \def\ref@label{{Guti{\'{e}}rrez et~al.(2013)Guti{\'{e}}rrez, San-Mart{\'{\i}}n, Brands, Manzanas, and Herrera}}?><label>Gutiérrez et al.(2013)Gutiérrez, San-Martín, Brands, Manzanas, and Herrera</label><?label gutierrez2013reassessing?><mixed-citation>
Gutiérrez, J. M., San-Martín, D., Brands, S., Manzanas, R., and Herrera, S.:
Reassessing statistical downscaling techniques for their robust application under climate change conditions,
J. Climate,
26, 171–188, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx23"><?xmltex \def\ref@label{{Guti{\'{e}}rrez et~al.(2019)Guti{\'{e}}rrez, Maraun, Widmann, Huth, Hertig, Benestad, R{\"{o}}ssler, Wibig, Wilcke, Kotlarski et~al.}}?><label>Gutiérrez et al.(2019)Gutiérrez, Maraun, Widmann, Huth, Hertig, Benestad, Rössler, Wibig, Wilcke, Kotlarski et al.</label><?label gutierrez2019intercomparison?><mixed-citation>
Gutiérrez, J. M., Maraun, D., Widmann, M., Huth, R., Hertig, E., Benestad, R., Rössler, O., Wibig, J., Wilcke, R., Kotlarski, S., and San Martin, D.:
An intercomparison of a large ensemble of statistical downscaling methods over Europe: Results from the VALUE perfect predictor cross-validation experiment,
Int. J. Climatol.,
39, 3750–3785, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx24"><?xmltex \def\ref@label{{Hatfield and Prueger(2015)}}?><label>Hatfield and Prueger(2015)</label><?label hatfield2015temperature?><mixed-citation>
Hatfield, J. L. and Prueger, J. H.:
Temperature extremes: Effect on plant growth and development,
Weather and Climate Extremes,
10, 4–10, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx25"><?xmltex \def\ref@label{{Haylock et~al.(2008)Haylock, Hofstra, Klein~Tank, Klok, Jones, and New}}?><label>Haylock et al.(2008)Haylock, Hofstra, Klein Tank, Klok, Jones, and New</label><?label haylock2008european?><mixed-citation>Haylock, M., Hofstra, N., Klein Tank, A., Klok, E., Jones, P., and New, M.:
A European daily high-resolution gridded data set of surface temperature and precipitation for 1950–2006,
J. Geophys. Res.-Atmos.,
113, D20119, <ext-link xlink:href="https://doi.org/10.1029/2008JD010201" ext-link-type="DOI">10.1029/2008JD010201</ext-link>, 2008.</mixed-citation></ref>
      <ref id="bib1.bibx26"><?xmltex \def\ref@label{{He et~al.(2016)He, Zhang, Ren, and Sun}}?><label>He et al.(2016)He, Zhang, Ren, and Sun</label><?label he2016deep?><mixed-citation>
He, K., Zhang, X., Ren, S., and Sun, J.:
Deep residual learning for image recognition,
in: Proceedings of the IEEE conference on computer vision and pattern recognition, 770–778, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx27"><?xmltex \def\ref@label{{Hertig and Jacobeit(2013)}}?><label>Hertig and Jacobeit(2013)</label><?label hertig2013novel?><mixed-citation>
Hertig, E. and Jacobeit, J.:
A novel approach to statistical downscaling considering nonstationarities: application to daily precipitation in the Mediterranean area,
J. Geophys. Res.-Atmos.,
118, 520–533, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx28"><?xmltex \def\ref@label{{Hertig et~al.(2019)Hertig, Maraun, Bartholy, Pongracz, Vrac, Mares, Guti{\'{e}}rrez, Wibig, Casanueva, and Soares}}?><label>Hertig et al.(2019)Hertig, Maraun, Bartholy, Pongracz, Vrac, Mares, Gutiérrez, Wibig, Casanueva, and Soares</label><?label hertig2019comparison?><mixed-citation>
Hertig, E., Maraun, D., Bartholy, J., Pongracz, R., Vrac, M., Mares, I., Gutiérrez, J. M., Wibig, J., Casanueva, A., and Soares, P. M.:
Comparison of statistical downscaling methods with respect to extreme events over Europe: Validation results from the perfect predictor experiment of the COST Action VALUE,
Int. J. Climatol.,
39, 3846–3867, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx29"><?xmltex \def\ref@label{{H{\"{o}}hlein et~al.(2020)H{\"{o}}hlein, Kern, Hewson, and Westermann}}?><label>Höhlein et al.(2020)Höhlein, Kern, Hewson, and Westermann</label><?label hohlein2020comparative?><mixed-citation>Höhlein, K., Kern, M., Hewson, T., and Westermann, R.:
A Comparative Study of Convolutional Neural Network Models for Wind Field Downscaling,
arXiv [preprint], <ext-link xlink:href="https://arxiv.org/abs/2008.12257">arXiv:2008.12257</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx30"><?xmltex \def\ref@label{{Huth et~al.(2015)Huth, Mik{\v{s}}ovsk{\`{y}}, {\v{S}}t{\v{e}}p{\'{a}}nek, Belda, Farda, Chl{\'{a}}dov{\'{a}}, and Pi{\v{s}}oft}}?><label>Huth et al.(2015)Huth, Mikšovskỳ, Štěpánek, Belda, Farda, Chládová, and Pišoft</label><?label huth2015comparative?><mixed-citation>
Huth, R., Mikšovskỳ, J., Štěpánek, P., Belda, M., Farda, A., Chládová, Z., and Pišoft, P.:
Comparative validation of statistical and dynamical downscaling models on a dense grid in central Europe: temperature,
Theor. Appl. Climatol.,
120, 533–553, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx31"><?xmltex \def\ref@label{{Jacob et~al.(2014)Jacob, Petersen, Eggert, Alias, Christensen, Bouwer, Braun, Colette, D{\'{e}}qu{\'{e}}, Georgievski et~al.}}?><label>Jacob et al.(2014)Jacob, Petersen, Eggert, Alias, Christensen, Bouwer, Braun, Colette, Déqué, Georgievski et al.</label><?label jacob2014euro?><mixed-citation>
Jacob, D., Petersen, J., Eggert, B., Alias, A., Christensen, O. B., Bouwer, L. M., Braun, A., Colette, A., Déqué, M., Georgievski, G., and Georgopoulou, E.:
EURO-CORDEX: new high-resolution climate change projections for European impact research,
Reg. Environ. Change,
14, 563–578, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx32"><?xmltex \def\ref@label{{Jacobeit et~al.(2014)Jacobeit, Hertig, Seubert, and Lutz}}?><label>Jacobeit et al.(2014)Jacobeit, Hertig, Seubert, and Lutz</label><?label jacobeit2014statistical?><mixed-citation>
Jacobeit, J., Hertig, E., Seubert, S., and Lutz, K.:
Statistical downscaling for climate change projections in the Mediterranean region: methods and results,
Reg. Environ. Change,
14, 1891–1906, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx33"><?xmltex \def\ref@label{{Katz and Brown(1992)}}?><label>Katz and Brown(1992)</label><?label katz1992extreme?><mixed-citation>
Katz, R. W. and Brown, B. G.:
Extreme events in a changing climate: variability is more important than averages,
Climatic Change,
21, 289–302, 1992.</mixed-citation></ref>
      <ref id="bib1.bibx34"><?xmltex \def\ref@label{{Kingma and Ba(2014)}}?><label>Kingma and Ba(2014)</label><?label kingma2014adam?><mixed-citation>Kingma, D. P. and Ba, J.:
Adam: A method for stochastic optimization,
arXiv [preprint], <ext-link xlink:href="https://arxiv.org/abs/1412.6980">arXiv:1412.6980</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx35"><?xmltex \def\ref@label{{Klein~Tank et~al.(2002)}}?><label>Klein Tank et al.(2002)</label><?label klein2002daily?><mixed-citation>Klein Tank, A. M. G., Wijngaard, J. B., Können, G. P., Böhm, R., Demarée, G., Gocheva, A., Mileta, M., Pashiardis, S., Hejkrlik, L., Kern‐Hansen, C., and Heino, R.: Daily dataset of 20th-century surface air temperature and precipitation series for the European Climate Assessment, Int. J. Climatol.,
22, 1441–1453, <ext-link xlink:href="https://doi.org/10.1002/joc.773" ext-link-type="DOI">10.1002/joc.773</ext-link>, 2002 (data available at: <uri>https://www.ecad.eu/dailydata/index.php</uri>, last access: 8 December 2020).</mixed-citation></ref>
      <ref id="bib1.bibx36"><?xmltex \def\ref@label{{Li et~al.(2020{\natexlab{a}})Li, Kovachki, Azizzadenesheli, Liu, Bhattacharya, Stuart, and Anandkumar}}?><label>Li et al.(2020a)Li, Kovachki, Azizzadenesheli, Liu, Bhattacharya, Stuart, and Anandkumar</label><?label li2020fourier?><mixed-citation>Li, Z., Kovachki, N., Azizzadenesheli, K., Liu, B., Bhattacharya, K., Stuart, A., and Anandkumar, A.:
Fourier neural operator for parametric partial differential equations,
arXiv [preprint], <ext-link xlink:href="https://arxiv.org/abs/2010.08895">arXiv:2010.08895</ext-link>, 2020a.</mixed-citation></ref>
      <ref id="bib1.bibx37"><?xmltex \def\ref@label{{Li et~al.(2020{\natexlab{b}})Li, Kovachki, Azizzadenesheli, Liu, Bhattacharya, Stuart, and Anandkumar}}?><label>Li et al.(2020b)Li, Kovachki, Azizzadenesheli, Liu, Bhattacharya, Stuart, and Anandkumar</label><?label li2020neural?><mixed-citation>Li, Z., Kovachki, N., Azizzadenesheli, K., Liu, B., Bhattacharya, K., Stuart, A., and Anandkumar, A.:
Neural operator: Graph kernel network for partial differential equations,
arXiv [preprint], <ext-link xlink:href="https://arxiv.org/abs/2003.03485">arXiv:2003.03485</ext-link>, 2020b.</mixed-citation></ref>
      <ref id="bib1.bibx38"><?xmltex \def\ref@label{{Liu et~al.(2020)Liu, Ganguly, and Dy}}?><label>Liu et al.(2020)Liu, Ganguly, and Dy</label><?label liu2020climate?><mixed-citation>
Liu, Y., Ganguly, A. R., and Dy, J.:
Climate Downscaling Using YNet: A Deep Convolutional Network with Skip Connections and Fusion,
in: Proceedings of the 26th ACM SIGKDD International Conference on Knowledge Discovery &amp; Data Mining, 3145–3153, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx39"><?xmltex \def\ref@label{{Lu et~al.(2019)Lu, Jin, and Karniadakis}}?><label>Lu et al.(2019)Lu, Jin, and Karniadakis</label><?label lu2019deeponet?><mixed-citation>Lu, L., Jin, P., and Karniadakis, G. E.:
Deeponet: Learning nonlinear operators for identifying differential equations based on the universal approximation theorem of operators,
arXiv [preprint], <ext-link xlink:href="https://arxiv.org/abs/1910.03193">arXiv:1910.03193</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx40"><?xmltex \def\ref@label{{Maraun(2013)}}?><label>Maraun(2013)</label><?label maraun2013bias?><mixed-citation>
Maraun, D.:
Bias correction, quantile mapping, and downscaling: Revisiting the inflation issue,
J. Climate,
26, 2137–2143, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx41"><?xmltex \def\ref@label{{Maraun and Widmann(2018)}}?><label>Maraun and Widmann(2018)</label><?label maraun2018statistical?><mixed-citation>
Maraun, D. and Widmann, M.:
Statistical downscaling and bias correction for climate research,
Cambridge University Press, Cambridge, UK, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx42"><?xmltex \def\ref@label{{Maraun et~al.(2010)Maraun, Wetterhall, Ireson, Chandler, Kendon, Widmann, Brienen, Rust, Sauter, Theme{\ss}l et~al.}}?><label>Maraun et al.(2010)Maraun, Wetterhall, Ireson, Chandler, Kendon, Widmann, Brienen, Rust, Sauter, Themeßl et al.</label><?label maraun2010precipitation?><mixed-citation>Maraun, D., Wetterhall, F., Ireson, A. M., Chandler, R. E., Kendon, E. J., Widmann, M., Brienen, S., Rust, H. W., Sauter, T., Themeßl, M., and Venema, V. K. C.:
Precipitation downscaling under climate change: Recent developments to bridge the gap between dynamical models and the end user,
Rev. Geophys., 48, RG3003, <ext-link xlink:href="https://doi.org/10.1029/2009RG000314" ext-link-type="DOI">10.1029/2009RG000314</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bibx43"><?xmltex \def\ref@label{{Maraun et~al.(2015)Maraun, Widmann, Guti{\'{e}}rrez, Kotlarski, Chandler, Hertig, Wibig, Huth, and Wilcke}}?><label>Maraun et al.(2015)Maraun, Widmann, Gutiérrez, Kotlarski, Chandler, Hertig, Wibig, Huth, and Wilcke<?pagebreak page269?></label><?label maraun2015value?><mixed-citation>
Maraun, D., Widmann, M., Gutiérrez, J. M., Kotlarski, S., Chandler, R. E., Hertig, E., Wibig, J., Huth, R., and Wilcke, R. A.:
VALUE: A framework to validate downscaling approaches for climate change studies,
Earths Future,
3, 1–14, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx44"><?xmltex \def\ref@label{{Maraun et~al.(2017)Maraun, Shepherd, Widmann, Zappa, Walton, Guti{\'{e}}rrez, Hagemann, Richter, Soares, Hall et~al.}}?><label>Maraun et al.(2017)Maraun, Shepherd, Widmann, Zappa, Walton, Gutiérrez, Hagemann, Richter, Soares, Hall et al.</label><?label maraun2017towards?><mixed-citation>
Maraun, D., Shepherd, T. G., Widmann, M., Zappa, G., Walton, D., Gutiérrez, J. M., Hagemann, S., Richter, I., Soares, P. M., Hall, A., and Mearns, L. O.:
Towards process-informed bias correction of climate change simulations,
Nat. Clim. Change,
7, 764–773, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx45"><?xmltex \def\ref@label{{Maraun et~al.(2019)Maraun, Huth, Guti{\'{e}}rrez, Mart{\'{\i}}n, Dubrovsky, Fischer, Hertig, Soares, Bartholy, Pongr{\'{a}}cz et~al.}}?><label>Maraun et al.(2019)Maraun, Huth, Gutiérrez, Martín, Dubrovsky, Fischer, Hertig, Soares, Bartholy, Pongrácz et al.</label><?label maraun2019value?><mixed-citation>
Maraun, D., Huth, R., Gutiérrez, J. M., Martín, D. S., Dubrovsky, M., Fischer, A., Hertig, E., Soares, P. M., Bartholy, J., Pongrácz, R., and Widmann, M.:
The VALUE perfect predictor experiment: evaluation of temporal variability,
Int. J. Climatol.,
39, 3786–3818, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx46"><?xmltex \def\ref@label{{Mehrotra and Sharma(2005)}}?><label>Mehrotra and Sharma(2005)</label><?label mehrotra2005nonparametric?><mixed-citation>Mehrotra, R. and Sharma, A.:
A nonparametric nonhomogeneous hidden Markov model for downscaling of multisite daily rainfall occurrences,
J. Geophys. Res.-Atmos., 110, D16108, <ext-link xlink:href="https://doi.org/10.1029/2004JD005677" ext-link-type="DOI">10.1029/2004JD005677</ext-link>, 2005.</mixed-citation></ref>
      <ref id="bib1.bibx47"><?xmltex \def\ref@label{{Misra et~al.(2018)Misra, Sarkar, and Mitra}}?><label>Misra et al.(2018)Misra, Sarkar, and Mitra</label><?label misra2018statistical?><mixed-citation>
Misra, S., Sarkar, S., and Mitra, P.:
Statistical downscaling of precipitation using long short-term memory recurrent neural networks,
Theor. Appl. Climatol.,
134, 1179–1196, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx48"><?xmltex \def\ref@label{{Pan et~al.(2019)Pan, Hsu, AghaKouchak, and Sorooshian}}?><label>Pan et al.(2019)Pan, Hsu, AghaKouchak, and Sorooshian</label><?label pan2019improving?><mixed-citation>
Pan, B., Hsu, K., AghaKouchak, A., and Sorooshian, S.:
Improving precipitation estimation using convolutional neural network,
Water Resour. Res.,
55, 2301–2321, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx49"><?xmltex \def\ref@label{{Piani et~al.(2010)Piani, Haerter, and Coppola}}?><label>Piani et al.(2010)Piani, Haerter, and Coppola</label><?label piani2010statistical?><mixed-citation>
Piani, C., Haerter, J., and Coppola, E.:
Statistical bias correction for daily precipitation in regional climate models over Europe,
Theor. Appl. Climatol.,
99, 187–192, 2010.</mixed-citation></ref>
      <ref id="bib1.bibx50"><?xmltex \def\ref@label{{Qin et~al.(2019)Qin, Zhu, Qin, Wang, and Zhao}}?><label>Qin et al.(2019)Qin, Zhu, Qin, Wang, and Zhao</label><?label qin2019recurrent?><mixed-citation>Qin, S., Zhu, J., Qin, J., Wang, W., and Zhao, D.:
Recurrent attentive neural process for sequential data,
arXiv [preprint], <ext-link xlink:href="https://arxiv.org/abs/1910.09323">arXiv:1910.09323</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx51"><?xmltex \def\ref@label{{Raynaud et~al.(2017)Raynaud, Hingray, Zin, Anquetin, Debionne, and Vautard}}?><label>Raynaud et al.(2017)Raynaud, Hingray, Zin, Anquetin, Debionne, and Vautard</label><?label raynaud2017atmospheric?><mixed-citation>
Raynaud, D., Hingray, B., Zin, I., Anquetin, S., Debionne, S., and Vautard, R.:
Atmospheric analogues for physically consistent scenarios of surface weather in Europe and Maghreb,
Int. J. Climatol.,
37, 2160–2176, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx52"><?xmltex \def\ref@label{{Rezende and Mohamed(2015)}}?><label>Rezende and Mohamed(2015)</label><?label rezende2015variational?><mixed-citation>Rezende, D. J. and Mohamed, S.:
Variational inference with normalizing flows,
arXiv [preprint], <ext-link xlink:href="https://arxiv.org/abs/1505.05770">arXiv:1505.05770</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx53"><?xmltex \def\ref@label{{Ribalaygua et~al.(2013)Ribalaygua, Torres, P{\'{o}}rtoles, Monjo, Gait{\'{a}}n, and Pino}}?><label>Ribalaygua et al.(2013)Ribalaygua, Torres, Pórtoles, Monjo, Gaitán, and Pino</label><?label ribalaygua2013description?><mixed-citation>
Ribalaygua, J., Torres, L., Pórtoles, J., Monjo, R., Gaitán, E., and Pino, M.:
Description and validation of a two-step analogue/regression downscaling method,
Theor. Appl. Climatol.,
114, 253–269, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx54"><?xmltex \def\ref@label{{Sachindra et~al.(2018)Sachindra, Ahmed, Rashid, Shahid, and Perera}}?><label>Sachindra et al.(2018)Sachindra, Ahmed, Rashid, Shahid, and Perera</label><?label sachindra2018statistical?><mixed-citation>
Sachindra, D., Ahmed, K., Rashid, M. M., Shahid, S., and Perera, B.:
Statistical downscaling of precipitation using machine learning techniques,
Atmos. Res.,
212, 240–258, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx55"><?xmltex \def\ref@label{{San-Mart{\'{\i}}n et~al.(2017)San-Mart{\'{\i}}n, Manzanas, Brands, Herrera, and Guti{\'{e}}rrez}}?><label>San-Martín et al.(2017)San-Martín, Manzanas, Brands, Herrera, and Gutiérrez</label><?label san2017reassessing?><mixed-citation>
San-Martín, D., Manzanas, R., Brands, S., Herrera, S., and Gutiérrez, J. M.:
Reassessing model uncertainty for regional projections of precipitation with an ensemble of statistical downscaling methods,
J. Climate,
30, 203–223, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx56"><?xmltex \def\ref@label{{Singh et~al.(2019)Singh, Yoon, Son, and Ahn}}?><label>Singh et al.(2019)Singh, Yoon, Son, and Ahn</label><?label singh2019sequential?><mixed-citation>Singh, G., Yoon, J., Son, Y., and Ahn, S.:
Sequential Neural Processes, arXiv [preprint], <ext-link xlink:href="https://arxiv.org/abs/1906.10264">arXiv:1906.10264</ext-link>, 27 October 2019.</mixed-citation></ref>
      <ref id="bib1.bibx57"><?xmltex \def\ref@label{{Teutschbein and Seibert(2012)}}?><label>Teutschbein and Seibert(2012)</label><?label teutschbein2012bias?><mixed-citation>Teutschbein, C. and Seibert, J.:
Bias correction of regional climate model simulations for hydrological climate-change impact studies: Review and evaluation of different methods,
J. Hydrol.,
456, 12–29, 2012.
 </mixed-citation></ref><?xmltex \hack{\newpage}?>
      <ref id="bib1.bibx58"><?xmltex \def\ref@label{{Theobald et~al.(2015)}}?><label>Theobald et al.(2015)</label><?label theobald2015ecologically?><mixed-citation>Theobald, D. M., Harrison-Atlas, D., Monahan, W. B., and Albano, C. M.:
Ecologically-relevant maps of landforms and physiographic diversity for climate adaptation planning, PLoS One,
10, e0143619, <ext-link xlink:href="https://doi.org/10.1371/journal.pone.0143619" ext-link-type="DOI">10.1371/journal.pone.0143619</ext-link>, 2015 (data available at: <uri>https://developers.google.com/earth-engine/datasets/catalog/CSP_ERGo_1_0_Global_ALOS_mTPI</uri>, last access: 9 December 2020).</mixed-citation></ref>
      <ref id="bib1.bibx59"><?xmltex \def\ref@label{{Vandal et~al.(2017)Vandal, Kodra, Ganguly, Michaelis, Nemani, and Ganguly}}?><label>Vandal et al.(2017)Vandal, Kodra, Ganguly, Michaelis, Nemani, and Ganguly</label><?label vandal2017deepsd?><mixed-citation>
Vandal, T., Kodra, E., Ganguly, S., Michaelis, A., Nemani, R., and Ganguly, A. R.:
Deepsd: Generating high resolution climate change projections through single image super-resolution,
in: Proceedings of the 23rd acm sigkdd international conference on knowledge discovery and data mining, 1663–1672, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx60"><?xmltex \def\ref@label{{Vandal et~al.(2018)Vandal, Kodra, Dy, Ganguly, Nemani, and Ganguly}}?><label>Vandal et al.(2018)Vandal, Kodra, Dy, Ganguly, Nemani, and Ganguly</label><?label vandal2018quantifying?><mixed-citation>
Vandal, T., Kodra, E., Dy, J., Ganguly, S., Nemani, R., and Ganguly, A. R.:
Quantifying uncertainty in discrete-continuous and skewed data with Bayesian deep learning,
in: Proceedings of the 24th ACM SIGKDD International Conference on Knowledge Discovery &amp; Data Mining, 2377–2386, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx61"><?xmltex \def\ref@label{{Vandal et~al.(2019)Vandal, Kodra, and Ganguly}}?><label>Vandal et al.(2019)Vandal, Kodra, and Ganguly</label><?label vandal2019intercomparison?><mixed-citation>
Vandal, T., Kodra, E., and Ganguly, A. R.:
Intercomparison of machine learning methods for statistical downscaling: the case of daily and extreme precipitation,
Theor. Appl. Climatol.,
137, 557–570, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx62"><?xmltex \def\ref@label{Vaughan(2021)}?><label>Vaughan(2021)</label><?label Vaughan?><mixed-citation>Vaughan, A.:  annavaughan/convCNPClimate: First release (v1.0.0), Zenodo [code], <ext-link xlink:href="https://doi.org/10.5281/zenodo.4554603" ext-link-type="DOI">10.5281/zenodo.4554603</ext-link>, 2021.</mixed-citation></ref>
      <ref id="bib1.bibx63"><?xmltex \def\ref@label{{Vl{\v{c}}ek and Huth(2009)}}?><label>Vlček and Huth(2009)</label><?label vlvcek2009daily?><mixed-citation>
Vlček, O. and Huth, R.:
Is daily precipitation Gamma-distributed?: Adverse effects of an incorrect use of the Kolmogorov–Smirnov test,
Atmos. Res.,
93, 759–766, 2009.</mixed-citation></ref>
      <ref id="bib1.bibx64"><?xmltex \def\ref@label{{Volosciuk et~al.(2017)Volosciuk, Maraun, Vrac, and Widmann}}?><label>Volosciuk et al.(2017)Volosciuk, Maraun, Vrac, and Widmann</label><?label volosciuk2017combined?><mixed-citation>Volosciuk, C., Maraun, D., Vrac, M., and Widmann, M.: A combined statistical bias correction and stochastic downscaling method for precipitation, Hydrol. Earth Syst. Sci., 21, 1693–1719, <ext-link xlink:href="https://doi.org/10.5194/hess-21-1693-2017" ext-link-type="DOI">10.5194/hess-21-1693-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx65"><?xmltex \def\ref@label{{Wang et~al.(2021)Wang, Tian, Lowe, Kalin, and Lehrter}}?><label>Wang et al.(2021)Wang, Tian, Lowe, Kalin, and Lehrter</label><?label wang2021deep?><mixed-citation>Wang, F., Tian, D., Lowe, L., Kalin, L., and Lehrter, J.:
Deep Learning for Daily Precipitation and Temperature Downscaling,
Water Resour. Res.,
57, e2020WR029308, <ext-link xlink:href="https://doi.org/10.1029/2020WR029308" ext-link-type="DOI">10.1029/2020WR029308</ext-link>, 2021.</mixed-citation></ref>
      <ref id="bib1.bibx66"><?xmltex \def\ref@label{{White et~al.(2019)White, Singh, and Albert}}?><label>White et al.(2019)White, Singh, and Albert</label><?label white2019downscaling?><mixed-citation>
White, B., Singh, A., and Albert, A.:
Downscaling Numerical Weather Models with GANs,
in: AGU Fall Meeting Abstracts, vol. 2019,
GC43D–1357, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx67"><?xmltex \def\ref@label{{Widmann et~al.(2019)Widmann, Bedia, Guti{\'{e}}rrez, Bosshard, Hertig, Maraun, Casado, Ramos, Cardoso, Soares et~al.}}?><label>Widmann et al.(2019)Widmann, Bedia, Gutiérrez, Bosshard, Hertig, Maraun, Casado, Ramos, Cardoso, Soares et al.</label><?label widmann2019validation?><mixed-citation>
Widmann, M., Bedia, J., Gutiérrez, J. M., Bosshard, T., Hertig, E., Maraun, D., Casado, M. J., Ramos, P., Cardoso, R. M., Soares, P. M., and Ribalaygua, J.:
Validation of spatial variability in downscaling results from the VALUE perfect predictor experiment,
Int. J. Climatol.,
39, 3819–3845, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx68"><?xmltex \def\ref@label{{Wilby et~al.(2002)Wilby, Dawson, and Barrow}}?><label>Wilby et al.(2002)Wilby, Dawson, and Barrow</label><?label wilby2002sdsm?><mixed-citation>
Wilby, R. L., Dawson, C. W., and Barrow, E. M.:
SDSM?a decision support tool for the assessment of regional climate change impacts,
Environ. Modell. Softw.,
17, 145–157, 2002.</mixed-citation></ref>
      <ref id="bib1.bibx69"><?xmltex \def\ref@label{{Wilks(2012)}}?><label>Wilks(2012)</label><?label wilks2012stochastic?><mixed-citation>
Wilks, D. S.:
Stochastic weather generators for climate-change downscaling, part II: multivariable and spatially coherent multisite downscaling,
WIREs Clim. Change,
3, 267–278, 2012.</mixed-citation></ref>
      <ref id="bib1.bibx70"><?xmltex \def\ref@label{{Zerenner et~al.(2016)Zerenner, Venema, Friederichs, and Simmer}}?><label>Zerenner et al.(2016)Zerenner, Venema, Friederichs, and Simmer</label><?label zerenner2016downscaling?><mixed-citation>
Zerenner, T., Venema, V., Friederichs, P., and Simmer, C.:
Downscaling near-surface atmospheric fields with multi-objective Genetic Programming,
Environ. Modell. Softw.,
84, 85–98, 2016.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>Convolutional conditional neural processes for  local climate downscaling</article-title-html>
<abstract-html/>
<ref-html id="bib1.bib1"><label>Allen et al.(2016)Allen, Boschung, Nauels, Xia, Bex, and Midgley</label><mixed-citation>
Allen, S., Boschung, J., Nauels, A., Xia, Y., Bex, V., and Midgley, P.:
Climate change 2013: the physical science basis. Contribution of working group I to the fifth assessment report of the Intergovernmental Panel on Climate Change, Cambridge University Press, Cambridge, UK, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>Ayar et al.(2016)Ayar, Vrac, Bastin, Carreau, Déqué, and Gallardo</label><mixed-citation>
Ayar, P. V., Vrac, M., Bastin, S., Carreau, J., Déqué, M., and Gallardo, C.:
Intercomparison of statistical and dynamical downscaling models under the EURO-and MED-CORDEX initiative framework: present climate evaluations,
Clim. Dynam.,
46, 1301–1329, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>Baño-Medina et al.(2020)Baño-Medina, García Manzanas, Gutiérrez Llorente et al.</label><mixed-citation>
Baño-Medina, J., Manzanas, R., and Gutiérrez, J. M.: Configuration and intercomparison of deep learning neural models for statistical downscaling, Geosci. Model Dev., 13, 2109–2124, <a href="https://doi.org/10.5194/gmd-13-2109-2020" target="_blank">https://doi.org/10.5194/gmd-13-2109-2020</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>Basist et al.(1994)Basist, Bell, and Meentemeyer</label><mixed-citation>
Basist, A., Bell, G. D., and Meentemeyer, V.:
Statistical relationships between topography and precipitation patterns,
J. Climate,
7, 1305–1315, 1994.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>Ben Alaya et al.(2015)Ben Alaya, Chebana, and Ouarda</label><mixed-citation>
Ben Alaya, M. A., Chebana, F., and Ouarda, T. B.:
Probabilistic multisite statistical downscaling for daily precipitation using a Bernoulli–generalized pareto multivariate autoregressive model,
J. Climate,
28, 2349–2364, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>Benestad et al.(2015)Benestad, Chen, Mezghani, Fan, and Parding</label><mixed-citation>
Benestad, R. E., Chen, D., Mezghani, A., Fan, L., and Parding, K.:
On using principal components to represent stations in empirical–statistical downscaling, Tellus A, 67, 28326, <a href="https://doi.org/10.3402/tellusa.v67.28326" target="_blank">https://doi.org/10.3402/tellusa.v67.28326</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>Bevacqua et al.(2017)Bevacqua, Maraun, Hobæk Haff, Widmann, and Vrac</label><mixed-citation>
Bevacqua, E., Maraun, D., Hobæk Haff, I., Widmann, M., and Vrac, M.: Multivariate statistical modelling of compound events via pair-copula constructions: analysis of floods in Ravenna (Italy), Hydrol. Earth Syst. Sci., 21, 2701–2723, <a href="https://doi.org/10.5194/hess-21-2701-2017" target="_blank">https://doi.org/10.5194/hess-21-2701-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>Bhardwaj et al.(2018)Bhardwaj, Misra, Mishra, Wootten, Boyles, Bowden, and Terando</label><mixed-citation>
Bhardwaj, A., Misra, V., Mishra, A., Wootten, A., Boyles, R., Bowden, J., and Terando, A. J.:
Downscaling future climate change projections over Puerto Rico using a non-hydrostatic atmospheric model, Climatic Change, 147, 133–147, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>Cannon(2008)</label><mixed-citation>
Cannon, A. J.:
Probabilistic multisite precipitation downscaling by an expanded Bernoulli–Gamma density network,
J. Hydrometeorol.,
9, 1284–1300, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>Cannon et al.(2020)Cannon, Piani, and Sippel</label><mixed-citation>
Cannon, A. J., Piani, C., and Sippel, S.: Bias correction of climate model output for impact models, chap. 5, in: Climate Extremes and Their Implications for Impact and Risk Assessment, edited by: Sillmann, J., Sippel, S., and Russo, S., Elsevier, 77–104, <a href="https://doi.org/10.1016/B978-0-12-814895-2.00005-7" target="_blank">https://doi.org/10.1016/B978-0-12-814895-2.00005-7</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>Casanueva et al.(2016)Casanueva, Herrera, Fernández, and Gutiérrez</label><mixed-citation>
Casanueva, A., Herrera, S., Fernández, J., and Gutiérrez, J. M.:
Towards a fair comparison of statistical and dynamical downscaling in the framework of the EURO-CORDEX initiative,
Climatic Change,
137, 411–426, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>Chollet(2017)</label><mixed-citation>
Chollet, F.:
Xception: Deep learning with depthwise separable convolutions,
in: Proceedings of the IEEE conference on computer vision and pattern recognition, 1251–1258, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>Danielson and Gesch(2011)</label><mixed-citation>
Danielson, J. J. and Gesch, D. B.: Global multi-resolution terrain elevation data 2010 (GMTED2010), U.S. Geological Survey Open-File Report 2011-1073, 26 pp., available at: <a href="https://developers.google.com/earth-engine/datasets/catalog/USGS_GMTED2010" target="_blank"/> (last access: 8 December 2020), 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>Dee et al.(2011)</label><mixed-citation>
Dee, D. P., Uppala, S. M., Simmons, A. J., Berrisford, P., Poli, P., Kobayashi, S., Andrae, U., Balmaseda, M. A., Balsamo, G., Bauer, P., Bechtold, P., Beljaars, A. C. M., van de Berg, L., Bidlot, J., Bormann, N., Delsol, C., Dragani, R., Fuentes, M., Geer, A. J., Haimberger, L., Healy,
S. B., Hersbach, H., Hólm, E. V., Isaksen, L., Kållberg, P., Köhler, M., Matricardi, M., McNally, A. P., Monge-Sanz, B. M., Morcrette, J.-J., Park, B.-K., Peubey, C., de Rosnay, P., Tavolato, C., Thépaut, J.-N., and Vitart, F.: The ERA-Interim reanalysis: Configuration and performance of the data assimilation system, Q. J. Roy. Meteor. Soc.,
137, 553–597, <a href="https://doi.org/10.1002/qj.828" target="_blank">https://doi.org/10.1002/qj.828</a>, 2011 (data available at: <a href="https://apps.ecmwf.int/datasets/data/interim-full-daily/levtype=sfc/" target="_blank"/>, last access: 7 December 2020).
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>Dubois et al.(2020)Dubois, Gordon, and Foong</label><mixed-citation>
Dubois, Y., Gordon, J., and Foong, A. Y.:
Neural Process Family,
available at: <a href="http://yanndubs.github.io/Neural-Process-Family/" target="_blank"/>, last access: 10 December 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>Gaffin(2007)</label><mixed-citation>
Gaffin, D. M.:
Foehn winds that produced large temperature differences near the southern Appalachian Mountains,
Weather Forecast.,
22, 145–159, 2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>Garnelo et al.(2018)Garnelo, Rosenbaum, Maddison, Ramalho, Saxton, Shanahan, Teh, Rezende, and Eslami</label><mixed-citation>
Garnelo, M., Rosenbaum, D., Maddison, C. J., Ramalho, T., Saxton, D., Shanahan, M., Teh, Y. W., Rezende, D. J., and Eslami, S.:
Conditional neural processes,
arXiv [preprint], <a href="https://arxiv.org/abs/1807.01613" target="_blank">arXiv:1807.01613</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>Ghosh and Mujumdar(2008)</label><mixed-citation>
Ghosh, S. and Mujumdar, P. P.:
Statistical downscaling of GCM simulations to streamflow using relevance vector machine,
Adv. Water Resour.,
31, 132–146, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>Gneiting et al.(2007)Gneiting, Balabdaoui, and Raftery</label><mixed-citation>
Gneiting, T., Balabdaoui, F., and Raftery, A. E.:
Probabilistic forecasts, calibration and sharpness,
J. R. Stat. Soc. B,
69, 243–268, 2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>Gordon et al.(2019)Gordon, Bruinsma, Foong, Requeima, Dubois, and Turner</label><mixed-citation>
Gordon, J., Bruinsma, W. P., Foong, A. Y., Requeima, J., Dubois, Y., and Turner, R. E.:
Convolutional conditional neural processes,
arXiv [preprint], <a href="https://arxiv.org/abs/1910.13556" target="_blank">arXiv:1910.13556</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>Groenke et al.(2020)Groenke, Madaus, and Monteleoni</label><mixed-citation>
Groenke, B., Madaus, L., and Monteleoni, C.:
ClimAlign: Unsupervised statistical downscaling of climate variables via normalizing flows,
in: Proceedings of the 10th International Conference on Climate Informatics, 60–66, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>Gutiérrez et al.(2013)Gutiérrez, San-Martín, Brands, Manzanas, and Herrera</label><mixed-citation>
Gutiérrez, J. M., San-Martín, D., Brands, S., Manzanas, R., and Herrera, S.:
Reassessing statistical downscaling techniques for their robust application under climate change conditions,
J. Climate,
26, 171–188, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>Gutiérrez et al.(2019)Gutiérrez, Maraun, Widmann, Huth, Hertig, Benestad, Rössler, Wibig, Wilcke, Kotlarski et al.</label><mixed-citation>
Gutiérrez, J. M., Maraun, D., Widmann, M., Huth, R., Hertig, E., Benestad, R., Rössler, O., Wibig, J., Wilcke, R., Kotlarski, S., and San Martin, D.:
An intercomparison of a large ensemble of statistical downscaling methods over Europe: Results from the VALUE perfect predictor cross-validation experiment,
Int. J. Climatol.,
39, 3750–3785, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>Hatfield and Prueger(2015)</label><mixed-citation>
Hatfield, J. L. and Prueger, J. H.:
Temperature extremes: Effect on plant growth and development,
Weather and Climate Extremes,
10, 4–10, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>Haylock et al.(2008)Haylock, Hofstra, Klein Tank, Klok, Jones, and New</label><mixed-citation>
Haylock, M., Hofstra, N., Klein Tank, A., Klok, E., Jones, P., and New, M.:
A European daily high-resolution gridded data set of surface temperature and precipitation for 1950–2006,
J. Geophys. Res.-Atmos.,
113, D20119, <a href="https://doi.org/10.1029/2008JD010201" target="_blank">https://doi.org/10.1029/2008JD010201</a>, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>He et al.(2016)He, Zhang, Ren, and Sun</label><mixed-citation>
He, K., Zhang, X., Ren, S., and Sun, J.:
Deep residual learning for image recognition,
in: Proceedings of the IEEE conference on computer vision and pattern recognition, 770–778, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>Hertig and Jacobeit(2013)</label><mixed-citation>
Hertig, E. and Jacobeit, J.:
A novel approach to statistical downscaling considering nonstationarities: application to daily precipitation in the Mediterranean area,
J. Geophys. Res.-Atmos.,
118, 520–533, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>Hertig et al.(2019)Hertig, Maraun, Bartholy, Pongracz, Vrac, Mares, Gutiérrez, Wibig, Casanueva, and Soares</label><mixed-citation>
Hertig, E., Maraun, D., Bartholy, J., Pongracz, R., Vrac, M., Mares, I., Gutiérrez, J. M., Wibig, J., Casanueva, A., and Soares, P. M.:
Comparison of statistical downscaling methods with respect to extreme events over Europe: Validation results from the perfect predictor experiment of the COST Action VALUE,
Int. J. Climatol.,
39, 3846–3867, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>Höhlein et al.(2020)Höhlein, Kern, Hewson, and Westermann</label><mixed-citation>
Höhlein, K., Kern, M., Hewson, T., and Westermann, R.:
A Comparative Study of Convolutional Neural Network Models for Wind Field Downscaling,
arXiv [preprint], <a href="https://arxiv.org/abs/2008.12257" target="_blank">arXiv:2008.12257</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>Huth et al.(2015)Huth, Mikšovskỳ, Štěpánek, Belda, Farda, Chládová, and Pišoft</label><mixed-citation>
Huth, R., Mikšovskỳ, J., Štěpánek, P., Belda, M., Farda, A., Chládová, Z., and Pišoft, P.:
Comparative validation of statistical and dynamical downscaling models on a dense grid in central Europe: temperature,
Theor. Appl. Climatol.,
120, 533–553, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>Jacob et al.(2014)Jacob, Petersen, Eggert, Alias, Christensen, Bouwer, Braun, Colette, Déqué, Georgievski et al.</label><mixed-citation>
Jacob, D., Petersen, J., Eggert, B., Alias, A., Christensen, O. B., Bouwer, L. M., Braun, A., Colette, A., Déqué, M., Georgievski, G., and Georgopoulou, E.:
EURO-CORDEX: new high-resolution climate change projections for European impact research,
Reg. Environ. Change,
14, 563–578, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>Jacobeit et al.(2014)Jacobeit, Hertig, Seubert, and Lutz</label><mixed-citation>
Jacobeit, J., Hertig, E., Seubert, S., and Lutz, K.:
Statistical downscaling for climate change projections in the Mediterranean region: methods and results,
Reg. Environ. Change,
14, 1891–1906, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>Katz and Brown(1992)</label><mixed-citation>
Katz, R. W. and Brown, B. G.:
Extreme events in a changing climate: variability is more important than averages,
Climatic Change,
21, 289–302, 1992.
</mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>Kingma and Ba(2014)</label><mixed-citation>
Kingma, D. P. and Ba, J.:
Adam: A method for stochastic optimization,
arXiv [preprint], <a href="https://arxiv.org/abs/1412.6980" target="_blank">arXiv:1412.6980</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>Klein Tank et al.(2002)</label><mixed-citation>
Klein Tank, A. M. G., Wijngaard, J. B., Können, G. P., Böhm, R., Demarée, G., Gocheva, A., Mileta, M., Pashiardis, S., Hejkrlik, L., Kern‐Hansen, C., and Heino, R.: Daily dataset of 20th-century surface air temperature and precipitation series for the European Climate Assessment, Int. J. Climatol.,
22, 1441–1453, <a href="https://doi.org/10.1002/joc.773" target="_blank">https://doi.org/10.1002/joc.773</a>, 2002 (data available at: <a href="https://www.ecad.eu/dailydata/index.php" target="_blank"/>, last access: 8 December 2020).
</mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>Li et al.(2020a)Li, Kovachki, Azizzadenesheli, Liu, Bhattacharya, Stuart, and Anandkumar</label><mixed-citation>
Li, Z., Kovachki, N., Azizzadenesheli, K., Liu, B., Bhattacharya, K., Stuart, A., and Anandkumar, A.:
Fourier neural operator for parametric partial differential equations,
arXiv [preprint], <a href="https://arxiv.org/abs/2010.08895" target="_blank">arXiv:2010.08895</a>, 2020a.
</mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>Li et al.(2020b)Li, Kovachki, Azizzadenesheli, Liu, Bhattacharya, Stuart, and Anandkumar</label><mixed-citation>
Li, Z., Kovachki, N., Azizzadenesheli, K., Liu, B., Bhattacharya, K., Stuart, A., and Anandkumar, A.:
Neural operator: Graph kernel network for partial differential equations,
arXiv [preprint], <a href="https://arxiv.org/abs/2003.03485" target="_blank">arXiv:2003.03485</a>, 2020b.
</mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>Liu et al.(2020)Liu, Ganguly, and Dy</label><mixed-citation>
Liu, Y., Ganguly, A. R., and Dy, J.:
Climate Downscaling Using YNet: A Deep Convolutional Network with Skip Connections and Fusion,
in: Proceedings of the 26th ACM SIGKDD International Conference on Knowledge Discovery &amp; Data Mining, 3145–3153, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>Lu et al.(2019)Lu, Jin, and Karniadakis</label><mixed-citation>
Lu, L., Jin, P., and Karniadakis, G. E.:
Deeponet: Learning nonlinear operators for identifying differential equations based on the universal approximation theorem of operators,
arXiv [preprint], <a href="https://arxiv.org/abs/1910.03193" target="_blank">arXiv:1910.03193</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib40"><label>Maraun(2013)</label><mixed-citation>
Maraun, D.:
Bias correction, quantile mapping, and downscaling: Revisiting the inflation issue,
J. Climate,
26, 2137–2143, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib41"><label>Maraun and Widmann(2018)</label><mixed-citation>
Maraun, D. and Widmann, M.:
Statistical downscaling and bias correction for climate research,
Cambridge University Press, Cambridge, UK, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib42"><label>Maraun et al.(2010)Maraun, Wetterhall, Ireson, Chandler, Kendon, Widmann, Brienen, Rust, Sauter, Themeßl et al.</label><mixed-citation>
Maraun, D., Wetterhall, F., Ireson, A. M., Chandler, R. E., Kendon, E. J., Widmann, M., Brienen, S., Rust, H. W., Sauter, T., Themeßl, M., and Venema, V. K. C.:
Precipitation downscaling under climate change: Recent developments to bridge the gap between dynamical models and the end user,
Rev. Geophys., 48, RG3003, <a href="https://doi.org/10.1029/2009RG000314" target="_blank">https://doi.org/10.1029/2009RG000314</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib43"><label>Maraun et al.(2015)Maraun, Widmann, Gutiérrez, Kotlarski, Chandler, Hertig, Wibig, Huth, and Wilcke</label><mixed-citation>
Maraun, D., Widmann, M., Gutiérrez, J. M., Kotlarski, S., Chandler, R. E., Hertig, E., Wibig, J., Huth, R., and Wilcke, R. A.:
VALUE: A framework to validate downscaling approaches for climate change studies,
Earths Future,
3, 1–14, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib44"><label>Maraun et al.(2017)Maraun, Shepherd, Widmann, Zappa, Walton, Gutiérrez, Hagemann, Richter, Soares, Hall et al.</label><mixed-citation>
Maraun, D., Shepherd, T. G., Widmann, M., Zappa, G., Walton, D., Gutiérrez, J. M., Hagemann, S., Richter, I., Soares, P. M., Hall, A., and Mearns, L. O.:
Towards process-informed bias correction of climate change simulations,
Nat. Clim. Change,
7, 764–773, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib45"><label>Maraun et al.(2019)Maraun, Huth, Gutiérrez, Martín, Dubrovsky, Fischer, Hertig, Soares, Bartholy, Pongrácz et al.</label><mixed-citation>
Maraun, D., Huth, R., Gutiérrez, J. M., Martín, D. S., Dubrovsky, M., Fischer, A., Hertig, E., Soares, P. M., Bartholy, J., Pongrácz, R., and Widmann, M.:
The VALUE perfect predictor experiment: evaluation of temporal variability,
Int. J. Climatol.,
39, 3786–3818, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib46"><label>Mehrotra and Sharma(2005)</label><mixed-citation>
Mehrotra, R. and Sharma, A.:
A nonparametric nonhomogeneous hidden Markov model for downscaling of multisite daily rainfall occurrences,
J. Geophys. Res.-Atmos., 110, D16108, <a href="https://doi.org/10.1029/2004JD005677" target="_blank">https://doi.org/10.1029/2004JD005677</a>, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib47"><label>Misra et al.(2018)Misra, Sarkar, and Mitra</label><mixed-citation>
Misra, S., Sarkar, S., and Mitra, P.:
Statistical downscaling of precipitation using long short-term memory recurrent neural networks,
Theor. Appl. Climatol.,
134, 1179–1196, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib48"><label>Pan et al.(2019)Pan, Hsu, AghaKouchak, and Sorooshian</label><mixed-citation>
Pan, B., Hsu, K., AghaKouchak, A., and Sorooshian, S.:
Improving precipitation estimation using convolutional neural network,
Water Resour. Res.,
55, 2301–2321, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib49"><label>Piani et al.(2010)Piani, Haerter, and Coppola</label><mixed-citation>
Piani, C., Haerter, J., and Coppola, E.:
Statistical bias correction for daily precipitation in regional climate models over Europe,
Theor. Appl. Climatol.,
99, 187–192, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib50"><label>Qin et al.(2019)Qin, Zhu, Qin, Wang, and Zhao</label><mixed-citation>
Qin, S., Zhu, J., Qin, J., Wang, W., and Zhao, D.:
Recurrent attentive neural process for sequential data,
arXiv [preprint], <a href="https://arxiv.org/abs/1910.09323" target="_blank">arXiv:1910.09323</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib51"><label>Raynaud et al.(2017)Raynaud, Hingray, Zin, Anquetin, Debionne, and Vautard</label><mixed-citation>
Raynaud, D., Hingray, B., Zin, I., Anquetin, S., Debionne, S., and Vautard, R.:
Atmospheric analogues for physically consistent scenarios of surface weather in Europe and Maghreb,
Int. J. Climatol.,
37, 2160–2176, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib52"><label>Rezende and Mohamed(2015)</label><mixed-citation>
Rezende, D. J. and Mohamed, S.:
Variational inference with normalizing flows,
arXiv [preprint], <a href="https://arxiv.org/abs/1505.05770" target="_blank">arXiv:1505.05770</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib53"><label>Ribalaygua et al.(2013)Ribalaygua, Torres, Pórtoles, Monjo, Gaitán, and Pino</label><mixed-citation>
Ribalaygua, J., Torres, L., Pórtoles, J., Monjo, R., Gaitán, E., and Pino, M.:
Description and validation of a two-step analogue/regression downscaling method,
Theor. Appl. Climatol.,
114, 253–269, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib54"><label>Sachindra et al.(2018)Sachindra, Ahmed, Rashid, Shahid, and Perera</label><mixed-citation>
Sachindra, D., Ahmed, K., Rashid, M. M., Shahid, S., and Perera, B.:
Statistical downscaling of precipitation using machine learning techniques,
Atmos. Res.,
212, 240–258, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib55"><label>San-Martín et al.(2017)San-Martín, Manzanas, Brands, Herrera, and Gutiérrez</label><mixed-citation>
San-Martín, D., Manzanas, R., Brands, S., Herrera, S., and Gutiérrez, J. M.:
Reassessing model uncertainty for regional projections of precipitation with an ensemble of statistical downscaling methods,
J. Climate,
30, 203–223, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib56"><label>Singh et al.(2019)Singh, Yoon, Son, and Ahn</label><mixed-citation>
Singh, G., Yoon, J., Son, Y., and Ahn, S.:
Sequential Neural Processes, arXiv [preprint], <a href="https://arxiv.org/abs/1906.10264" target="_blank">arXiv:1906.10264</a>, 27 October 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib57"><label>Teutschbein and Seibert(2012)</label><mixed-citation>
Teutschbein, C. and Seibert, J.:
Bias correction of regional climate model simulations for hydrological climate-change impact studies: Review and evaluation of different methods,
J. Hydrol.,
456, 12–29, 2012.

</mixed-citation></ref-html>
<ref-html id="bib1.bib58"><label>Theobald et al.(2015)</label><mixed-citation>
Theobald, D. M., Harrison-Atlas, D., Monahan, W. B., and Albano, C. M.:
Ecologically-relevant maps of landforms and physiographic diversity for climate adaptation planning, PLoS One,
10, e0143619, <a href="https://doi.org/10.1371/journal.pone.0143619" target="_blank">https://doi.org/10.1371/journal.pone.0143619</a>, 2015 (data available at: <a href="https://developers.google.com/earth-engine/datasets/catalog/CSP_ERGo_1_0_Global_ALOS_mTPI" target="_blank"/>, last access: 9 December 2020).
</mixed-citation></ref-html>
<ref-html id="bib1.bib59"><label>Vandal et al.(2017)Vandal, Kodra, Ganguly, Michaelis, Nemani, and Ganguly</label><mixed-citation>
Vandal, T., Kodra, E., Ganguly, S., Michaelis, A., Nemani, R., and Ganguly, A. R.:
Deepsd: Generating high resolution climate change projections through single image super-resolution,
in: Proceedings of the 23rd acm sigkdd international conference on knowledge discovery and data mining, 1663–1672, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib60"><label>Vandal et al.(2018)Vandal, Kodra, Dy, Ganguly, Nemani, and Ganguly</label><mixed-citation>
Vandal, T., Kodra, E., Dy, J., Ganguly, S., Nemani, R., and Ganguly, A. R.:
Quantifying uncertainty in discrete-continuous and skewed data with Bayesian deep learning,
in: Proceedings of the 24th ACM SIGKDD International Conference on Knowledge Discovery &amp; Data Mining, 2377–2386, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib61"><label>Vandal et al.(2019)Vandal, Kodra, and Ganguly</label><mixed-citation>
Vandal, T., Kodra, E., and Ganguly, A. R.:
Intercomparison of machine learning methods for statistical downscaling: the case of daily and extreme precipitation,
Theor. Appl. Climatol.,
137, 557–570, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib62"><label>Vaughan(2021)</label><mixed-citation>
Vaughan, A.:  annavaughan/convCNPClimate: First release (v1.0.0), Zenodo [code], <a href="https://doi.org/10.5281/zenodo.4554603" target="_blank">https://doi.org/10.5281/zenodo.4554603</a>, 2021.
</mixed-citation></ref-html>
<ref-html id="bib1.bib63"><label>Vlček and Huth(2009)</label><mixed-citation>
Vlček, O. and Huth, R.:
Is daily precipitation Gamma-distributed?: Adverse effects of an incorrect use of the Kolmogorov–Smirnov test,
Atmos. Res.,
93, 759–766, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib64"><label>Volosciuk et al.(2017)Volosciuk, Maraun, Vrac, and Widmann</label><mixed-citation>
Volosciuk, C., Maraun, D., Vrac, M., and Widmann, M.: A combined statistical bias correction and stochastic downscaling method for precipitation, Hydrol. Earth Syst. Sci., 21, 1693–1719, <a href="https://doi.org/10.5194/hess-21-1693-2017" target="_blank">https://doi.org/10.5194/hess-21-1693-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib65"><label>Wang et al.(2021)Wang, Tian, Lowe, Kalin, and Lehrter</label><mixed-citation>
Wang, F., Tian, D., Lowe, L., Kalin, L., and Lehrter, J.:
Deep Learning for Daily Precipitation and Temperature Downscaling,
Water Resour. Res.,
57, e2020WR029308, <a href="https://doi.org/10.1029/2020WR029308" target="_blank">https://doi.org/10.1029/2020WR029308</a>, 2021.
</mixed-citation></ref-html>
<ref-html id="bib1.bib66"><label>White et al.(2019)White, Singh, and Albert</label><mixed-citation>
White, B., Singh, A., and Albert, A.:
Downscaling Numerical Weather Models with GANs,
in: AGU Fall Meeting Abstracts, vol. 2019,
GC43D–1357, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib67"><label>Widmann et al.(2019)Widmann, Bedia, Gutiérrez, Bosshard, Hertig, Maraun, Casado, Ramos, Cardoso, Soares et al.</label><mixed-citation>
Widmann, M., Bedia, J., Gutiérrez, J. M., Bosshard, T., Hertig, E., Maraun, D., Casado, M. J., Ramos, P., Cardoso, R. M., Soares, P. M., and Ribalaygua, J.:
Validation of spatial variability in downscaling results from the VALUE perfect predictor experiment,
Int. J. Climatol.,
39, 3819–3845, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib68"><label>Wilby et al.(2002)Wilby, Dawson, and Barrow</label><mixed-citation>
Wilby, R. L., Dawson, C. W., and Barrow, E. M.:
SDSM?a decision support tool for the assessment of regional climate change impacts,
Environ. Modell. Softw.,
17, 145–157, 2002.
</mixed-citation></ref-html>
<ref-html id="bib1.bib69"><label>Wilks(2012)</label><mixed-citation>
Wilks, D. S.:
Stochastic weather generators for climate-change downscaling, part II: multivariable and spatially coherent multisite downscaling,
WIREs Clim. Change,
3, 267–278, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib70"><label>Zerenner et al.(2016)Zerenner, Venema, Friederichs, and Simmer</label><mixed-citation>
Zerenner, T., Venema, V., Friederichs, P., and Simmer, C.:
Downscaling near-surface atmospheric fields with multi-objective Genetic Programming,
Environ. Modell. Softw.,
84, 85–98, 2016.
</mixed-citation></ref-html>--></article>
