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  <front>
    <journal-meta>
<journal-id journal-id-type="publisher">ESD</journal-id>
<journal-title-group>
<journal-title>Earth System Dynamics</journal-title>
<abbrev-journal-title abbrev-type="publisher">ESD</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Earth Syst. Dynam.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">2190-4987</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/esd-8-889-2017</article-id><title-group><article-title>A method to preserve trends in quantile mapping bias correction of climate
modeled temperature</article-title>
      </title-group><?xmltex \runningtitle{A method to preserve trends in quantile mapping bias correction}?><?xmltex \runningauthor{M. G. Grillakis et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Grillakis</surname><given-names>Manolis G.</given-names></name>
          <email>manolis@hydromech.gr</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Koutroulis</surname><given-names>Aristeidis G.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2999-7575</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Daliakopoulos</surname><given-names>Ioannis N.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-9333-4963</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Tsanis</surname><given-names>Ioannis K.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4997-9307</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Technical University of Crete, School of Environmental
Engineering, Chania, Greece</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>McMaster University, Department of Civil Engineering,
Hamilton, ON, Canada</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Manolis G. Grillakis (manolis@hydromech.gr)</corresp></author-notes><pub-date><day>28</day><month>September</month><year>2017</year></pub-date>
      
      <volume>8</volume>
      <issue>3</issue>
      <fpage>889</fpage><lpage>900</lpage>
      <history>
        <date date-type="received"><day>30</day><month>May</month><year>2017</year></date>
           <date date-type="rev-request"><day>7</day><month>June</month><year>2017</year></date>
           <date date-type="rev-recd"><day>30</day><month>August</month><year>2017</year></date>
           <date date-type="accepted"><day>15</day><month>September</month><year>2017</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://esd.copernicus.org/articles/8/889/2017/esd-8-889-2017.html">This article is available from https://esd.copernicus.org/articles/8/889/2017/esd-8-889-2017.html</self-uri>
<self-uri xlink:href="https://esd.copernicus.org/articles/8/889/2017/esd-8-889-2017.pdf">The full text article is available as a PDF file from https://esd.copernicus.org/articles/8/889/2017/esd-8-889-2017.pdf</self-uri>


      <abstract>
    <p>Bias correction of climate variables is a standard practice in
climate change impact (CCI) studies. Various methodologies have been
developed within the framework of quantile mapping. However, it is well known
that quantile mapping may significantly modify the long-term statistics due
to the time dependency of the temperature bias. Here, a method to overcome
this issue without compromising the day-to-day correction statistics is
presented. The methodology separates the modeled temperature signal into a
normalized and a residual component relative to the modeled reference
period climatology, in order to adjust the biases only for the former and
preserve the signal of the later. The results show that this method allows
for the preservation of the originally modeled long-term signal in the mean,
the standard deviation and higher and lower percentiles of temperature. To
illustrate the improvements, the methodology is tested on daily time series
obtained from five Euro CORDEX regional climate models (RCMs).</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>Climate model output provides the primary source of information used to
quantify the effect of the foreseen anthropogenic climate change on natural
systems. One of the most common and technically sound practices in climate
change impact (CCI) studies is to calibrate impact models using the most
suitable observational data and then to replace them with the climate model
data in order to assess the effect of potential changes in the climate
regime. Often, raw climate model data cannot be used in CCI models due to the
presence of biases in the representation of regional climate (Christensen et
al., 2008; Haerter et al., 2011). In fact, hydrological CCI studies outcome
have been reported to become unrealistic without a prior adjustment of
climate forcing biases (Hagemann et al., 2013; Hansen et al., 2006; Harding
et al., 2014; Sharma et al., 2007). Papadimitriou et al. (2017) quantified
the effect of the bias in seven forcing parameters on the resulting runoff of
a land surface model, emphasizing the necessity of bias adjustments beyond
the precipitation and temperature parameters. These biases are attributed to
a number of reasons such as the imperfect representation of the physical
processes within the model code and the coarse spatial resolution that does not
permit the accurate representation of small-scale processes. Furthermore, in
some cases, climate model tuning for global projections focuses on the
adequate representation of feedbacks between processes, and hence the
realistic depiction of a variable, such as temperature, against observations
is sidelined (Hawkins et al., 2016).</p>
      <p>A number of statistical bias correction methods have been developed and
successfully applied in CCI studies (e.g., Grillakis et al., 2013; Haerter et
al., 2011; Ines and Hansen, 2006; Teutschbein and Seibert, 2012). Their main
task is to adjust the statistical properties of climate simulations to
resemble those of observations, in a common climatological period. A commonly
used type of procedure to accomplish this is a transfer function (TF)
which minimizes the difference between the cumulative density function (CDF)
of the climate model output and that of the observations, a process also
referred to as quantile mapping. As a result of quantile mapping, the
reference (calibration) period's adjusted data are statistically closer, and
sometimes near-identical to the observations. Hence, the statistical outcome
of an impact model run using observational data is likely to be reproduced by
the adjusted data. The good performance of statistical bias correction
methods in the reference period is well documented  (Grillakis et al., 2011, 2013;
Ines and Hansen, 2006; Papadimitriou et al., 2015).
The procedure, however, overlooks the time dependency of the distribution and
hence the unequal effect of the TF to the varying over time CDF. An
indicative example is presented in Fig. 1, where modeled temperature data
have a mean bias of 2.49 <inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C in the reference period (Fig. 1a)
relative to the observations. This mean bias is expressed by the average
horizontal distance between the TF and the bisector of the central plot. The
left histogram illustrates the reference period modeled data for 1981–2010.
The histogram at the bottom is derived from observational data. The histogram
on the right is derived from a moving 30-year period between 1981 and 2098.
The rightmost histogram shows the difference between the reference period and
the moving 30-year period. The red mark shows the theoretical change in the
average correction applied by the TF, due to the changes in the projected
temperature histogram. Hence, the average correction applied for the period
2068–2097 reaches 3.85 <inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, significantly higher than the reference
period's bias (Fig. 1b). The time-dependency of the correction magnitude
introduces a long-term signal distortion in the corrected data. In the
quantile-mapping-based correction methodologies in which the TF distance from
the bisector is variable, this effect is unavoidable. Nevertheless, in cases
where the TF retains a relatively constant distance to the bisector (i.e.,
parallel to the bisector), the trend of the corrected data remains similar to
the raw model data regardless of the temporal change in the model data
histogram.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p>The transfer function (TF – heavy black line) between observed
(bottom histograms) and modeled (histograms on the left) for the reference
period (1981–2010) is used to adjust bias of a 30-year moving window
from 1981–2010 to 2068–2097. The rightmost plot shows the residual
histogram after bias correction. The change in the average correction (red
mark) on the TF in comparison to the reference period mean correction
(square) is shown. The animated version provided in the Supplement shows the
temporal evolution of the bias as the 30-year time window moves on the
projection data. Data were obtained from ICHEC-EC-EARTH r12i1p1 SMHI-RCA4_v1
RCM of Euro-CORDEX experiment (0.11<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> resolution) simulation
under the representative concentration pathway of RCP85, for the location
Chania International Airport (long <inline-formula><mml:math id="M4" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 24.08, lat <inline-formula><mml:math id="M5" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 35.54).
Observational data were obtained from the E-OBS v14 dataset (Haylock et al.,
2008) of 0.25<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> spatial resolution.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://esd.copernicus.org/articles/8/889/2017/esd-8-889-2017-f01.png"/>

      </fig>

      <p>Based on the previous example, the time extrapolation of the TF is regarded
as a leap of faith that may lead to a false certainty about the robustness of
the adjusted projection. This may significantly change the original
modeled long-term trend or other higher moments of the climate variable
statistics that eventually change the long-term signal of the climate
variable. In their work on distribution-based scaling (DBS) bias correction,
Olsson et al. (2015) showed that their methodology might alter the long-term
temperature trends, attributing the phenomenon in the severity of the biases
in the mean or the standard deviation between the uncorrected temperatures
and the observations. Maraun (2016) discusses whether the change in the
trend is a desired feature of bias correction, concluding that it is case-specific and depends on the skillfulness of the climate model to simulate the
correct long-term signal. In the case of CCI studies, this implies that
climate model data are assessed for their skill to well represent the trend,
which is not a common practice. A possible but indirect solution to this is
described in Maurer and Pierce (2014), who study the change in precipitation
trend over an ensemble of atmospheric general circulation model (AGCM). They
conclude that, while individual quantile-mapping-corrected AGCM data may
significantly modify the signal of change, a relatively large ensemble
estimation diminishes the problem as individual model trend changes were
canceled out. Li et al. (2010) present a quantile mapping method to adjust
temperature biases taking into account the differences of the future and
reference period distributions. A drawback of the method is that the
difference between the two periods' distributions depends on the future
period length. In their work,  Hempel et al. (2013) propose a methodology to
resolve the trend changing issue by preserving the absolute changes in
monthly temperature and relative changes in monthly values of precipitation.
A characteristic of their approach is that it maps anomalies instead of
absolute values, indicating that specific correction values are attached to
each temperature anomaly, while it also has the drawback that the edges of
the distribution are not corrected adequately. A similar approach that is additive for
temperature and multiplicative for precipitation was also followed
by Pierce et al. (2015). Bürger et al. (2013) and Cannon et al. (2015)
test the de-trending of the data prior to their quantile mapping correction,
figuring that the removal of the trends prior to the quantile mapping and their
reintroduction after the correction tends without absolutely maintaining the
long-term trend.</p>
      <p>In this study, we present a methodology to conserve the long-term statistics
such as trend and variability of the climate model data in quantile mapping.
The methodology considers the separation of the temperature signal relative
to the raw data reference period, producing a normalized and a residuals data
stream. The separation is performed on an annual basis. The residuals include
the gradual changes in the signal and the year-to-year fluctuations in the
distribution of the temperature. The quantile mapping bias correction is then
applied to the normalized daily temperature. Finally, the residual components
are merged to the bias-corrected time series to form the corrected time
series. The idea of identifying and using two different timescales in bias
correction of temperature was introduced in Haerter et al. (2011), who
present a method to separate the different timescales and apply a correction
to each one. The methodology presented here is tested along with a
generalized version of the multi-segment statistical bias correction (MSBC)
quantile mapping methodology (Grillakis et al., 2013). The methodology takes
the form of a pre- and post-processing module that can be applied along with
different statistical bias correction methodologies. The two-step procedure
is examined for its ability to remove the daily biases with simultaneous
preservation of the long-term statistics. The procedure is compared to the
simple quantile mapping and a quantile mapping in combination with a simpler
trend preservation procedure.</p>
</sec>
<sec id="Ch1.S2">
  <title>Methods</title>
<sec id="Ch1.S2.SS1">
  <title>Residual separation</title>
      <p>The statistical difference of each individual year's simulated data,
compared to the average reference period simulated data is identified as
residuals. These are estimated between the CDF of each year's modeled
climate data and the CDF of the entire reference period of the model data.
Let <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi mathvariant="normal">R</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> be the reference period model data and <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> the climate data
for year <inline-formula><mml:math id="M9" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>, then the normalized data <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:msubsup><mml:mi>S</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">N</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> for year <inline-formula><mml:math id="M11" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>
are estimated by transferring each year's data onto the average reference
period CDF through a transfer function <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">TF</mml:mi><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> estimated annually.
This can be formulated as Eq. (1).

                <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M13" display="block"><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msubsup><mml:mi>S</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">N</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:msubsup><mml:mi mathvariant="normal">TF</mml:mi><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi mathvariant="normal">R</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:mfenced close=")" open="("><mml:msub><mml:mi mathvariant="normal">TF</mml:mi><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mfenced open="(" close=")"><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mfenced></mml:mfenced></mml:mrow></mml:math></disp-formula>

          The difference between the original model data <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the normalized
data <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:msubsup><mml:mi>S</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">N</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> is the residual components <inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:msubsup><mml:mi>S</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">D</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> of the time series
(Eq. 2).

                <disp-formula id="Ch1.E2" content-type="numbered"><mml:math id="M17" display="block"><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msubsup><mml:mi>S</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">D</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msubsup><mml:mi>S</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">N</mml:mi></mml:msubsup></mml:mrow></mml:math></disp-formula>

          The original model data  <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can be reproduced by adding back the
residuals <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msubsup><mml:mi>S</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">D</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> to the normalized data <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:msubsup><mml:mi>S</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">N</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>. After the
separation, the normalized climate model data are statistically bias-corrected following a suitable methodology. The residuals are preserved in
order to be later added back to the bias-corrected time series. We refer to
the described method as a normalization module (NM) to hereafter lighten the
nomenclature of the paper. The normalization procedure is performed on
annual basis, as this consists of an obvious periodicity to use in the case of
temperature, even if it is not so well defined in the tropics. The
underlying assumption of the NM procedure is that it considers no major
changes in the reference period data, a notion that can hardly fall short
due to the usually short length of the reference period.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p>MSBC methodology on temperature correction using linear functions
(borrowed from Grillakis et al., 2013; modified) in one of the data
segments.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esd.copernicus.org/articles/8/889/2017/esd-8-889-2017-f02.png"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS2">
  <title>Bias correction</title>
      <p>Here, the NM is applied along with a modification of the MSBC algorithm that
is presented in Grillakis et al. (2013). This methodology follows the
principles of quantile mapping correction techniques and was originally
designed and tested for GCM precipitation adjustment. The method partitions
the CDF data into discrete segments and an individual quantile mapping
correction is applied to each segment, achieving a better-fitted transfer
function. Here the methodology is modified to use linear functions instead of
the gamma functions used in the original methodology, in order to facilitate
potential negative temperature values but also as a known technique in
quantile mapping, as it has also been used elsewhere (Themeßl et al.,
2011). An indicative example is shown in Fig. 2, where the CDFs are split
into discrete segments and linear functions are fit to each of them. In
Fig. 2, <inline-formula><mml:math id="M21" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> symbolizes the cumulative probability and <inline-formula><mml:math id="M22" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> is the slope of
the linear function. Then the corrected temperature for each temperature
value of the specific segment is estimated as in Eq. (3).

                <disp-formula id="Ch1.E3" content-type="numbered"><mml:math id="M23" display="block"><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msubsup><mml:mi>T</mml:mi><mml:mi mathvariant="normal">corr</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:msubsup><mml:mi>s</mml:mi><mml:mi mathvariant="normal">obs</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msubsup><mml:mo>⋅</mml:mo><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi>T</mml:mi><mml:mi mathvariant="normal">raw</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi>b</mml:mi><mml:mi mathvariant="normal">raw</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msubsup></mml:mrow><mml:mrow><mml:msubsup><mml:mi>s</mml:mi><mml:mi mathvariant="normal">raw</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>+</mml:mo><mml:msubsup><mml:mi>b</mml:mi><mml:mi mathvariant="normal">obs</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msubsup></mml:mrow></mml:math></disp-formula>

          The optimal number of segments is estimated using the Schwarz Bayesian
information criterion (SBIC) to balance between complexity and performance.
Additionally, the upper and lower edge segments are explicitly corrected
using the average difference between the reference period of the raw model
data and the observations (Fig. 2 <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>. This provides
robustness, avoiding unrealistic temperature values at the edges of the model
CDF. The bias correction methodology modification has been already used in
the Bias Correction Intercomparison Project (BCIP) (Nikulin et al., 2015),
while produced adjusted data have been used in a number of CCI studies
(Daliakopoulos et al., 2016; Grillakis et al., 2016; Koutroulis et al.,
2016; Papadimitriou et al., 2017, 2016). As the MSBC methodology belongs to
the parametric quantile mapping techniques, it shares their advantages and
drawbacks. A comprehensive shakedown of advantages and disadvantages of
quantile mapping in comparison to other methods can be found in Maraun et
al. (2010) and Themeßl et al. (2011). A step-by-step example of the
multisegment correction procedure is provided in Appendix A of Grillakis
et al. (2013).</p>
</sec>
<sec id="Ch1.S2.SS3">
  <title>Validation of the results</title>
      <p>The Klemes (1986) split sample test methodology was adopted for
verification. Split sample is the most common type of test used for the
validation of model efficiency. The methodology considers two periods of
calibration and validation between the observed and modeled data. The first
period is used for the calibration, while the second period is used as a
pseudo-future period in which the adjusted data are assessed against the
observations. A drawback of the split sample test in bias correction
validation operations is that the remaining bias of the validation period is
a function of the bias correction methodology deficiency and the model
deficiency itself to describe the validation period's climate, in aspects
that are not intended to be bias-corrected. That said, a skillful bias
correction method should deal well in that context, as model “democracy”
(Knutti, 2010), i.e., the assumption that all model projections are equally
possible, is common in CCI studies in which little attention is given to the model selection.</p><?xmltex \hack{\newpage}?>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Case study area and data</title>
      <p>To examine the effect of NM on the bias correction on a time series, the
Hadley Centre Central England Temperature (HadCET – Parker et al., 1992)
observational dataset was considered to adjust the simulated output from the
earth system model MIROC-ESM-CHEM (Hasumi and Emori, 2004) historical
emissions run between 1850 and 2005 for central England. This particular case
study was chosen due to the large observational record (the longest
instrumental record of temperature in the world) that is available for
central England, i.e., the triangular area of the United Kingdom enclosed by
Lancashire, London and Bristol. Discussion about dataset-related
uncertainties can be found in Parker et al. (1992) and Parker and Horton (2005).
In the specific application and in order to resemble a typical CCI
study, data between 1850 and 1899 serve as the calibration period, while the rest
of the data between 1900 and 2005 are used as the pseudo-future period for the
validation. Finally, the bias correction results of the two procedures, with
(BC-NM) and without (BC) the normalization module, were compared against the
validation period observations. An additional comparison was also performed
to a less complicated trend preservation procedure, inspired by Bürger et
al. (2013) and Cannon et al. (2015). This procedure considers the detrending
of the raw data using a 5-year moving average temperature. The detrended data
are corrected using the BC methodology, while the trend is additively put
back into the time series after the correction, similarly to the NM. We refer
to this as BC-TREND. This comparison is used to benchmark the BC-NM towards a
simpler quantile mapping that also approaches the trend preservation.</p>
      <p>Furthermore, to expand the methodology assessment on the regional scale, the
split sample test is adopted to assess the efficiency of the two procedures
on a pan-European scale. In order to scale up the split sample test, the
<inline-formula><mml:math id="M25" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-fold cross validation test (Geisser, 1993) is employed. The procedure has
been proposed for evaluating the performance of bias correction procedures in
Maraun (2016). In the <inline-formula><mml:math id="M26" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-fold cross validation test, the data are
partitioned into <inline-formula><mml:math id="M27" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> equal sized folds. Of the <inline-formula><mml:math id="M28" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> folds, one subsample is
retained each time as the validation data for testing the model, and the
remaining <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:mi>k</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> subsamples are used as calibration data. In a final test, the
procedures are applied on a long-term transient climate projection experiment
to assess their effect in the long-term attributes of the temperature in a
European-scale application.</p>
      <p>Temperature data from the European division of the Coordinated Regional
Downscaling Experiment (CORDEX), openly available through the Earth System
Grid Federation (ESGF), are considered. Additional information about the Euro CORDEX domain can be found on the CORDEX web page
(<uri>http://wcrp-cordex.ipsl.jussieu.fr/</uri>). Data from five regional climate models (RCMs) (Table 1)
with 0.44<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> spatial resolution and daily time step between 1951 and 2100 are
used. The projection data are considered under Representative
Concentration Pathway (RCP) 8.5, which projects an 8.5 W m<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> average
increase in the radiative forcing until 2100. The European domain CORDEX
simulations have been evaluated for their performance in previous studies
(Kotlarski et al., 2014; Prein et al., 2015). The EOBSv12 temperature data
were used (Haylock et al., 2008). Discussion about the applicability of EOBS
to compare temperature of RCMs control climate simulations can be found in
Kyselý and Plavcová (2010). Figure 3 shows the 1951–2005 daily
temperature average and standard deviation for the five RCMs of Table 1. The
RCMs' mean bias ranges between about <inline-formula><mml:math id="M32" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2 and 1 <inline-formula><mml:math id="M33" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C relative to
the EOBS dataset (individual models data are included to the ESM). The
positive mean bias in all RCMs is mainly seen in eastern Europe, while the
same areas exhibit negative bias in standard deviation. Some of the bias may,
however, be attributed to the ability of the observational dataset to
represent the true temperature (Hofstra et al., 2010).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><caption><p>Mean temperature (upper) and standard deviation (lower) for EOBS,
RCM ensemble (ENS) and for their difference (model – obs) (DIFF) for
the reference period 1951–2005.</p></caption>
        <?xmltex \igopts{width=213.395669pt}?><graphic xlink:href="https://esd.copernicus.org/articles/8/889/2017/esd-8-889-2017-f03.png"/>

      </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1"><caption><p>RCMs used in this experiment.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">#</oasis:entry>  
         <oasis:entry colname="col2">{GCM}_{realization}_{RCM}</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">1</oasis:entry>  
         <oasis:entry colname="col2">CNRM-CM5_r1i1p1_SMHI-RCA4_v1</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">2</oasis:entry>  
         <oasis:entry colname="col2">EC-EARTH_r12i1p1_SMHI-RCA4_v1</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">3</oasis:entry>  
         <oasis:entry colname="col2">EC-EARTH_r3i1p1_DMI-HIRHAM5_v1</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">4</oasis:entry>  
         <oasis:entry colname="col2">IPSL-CM5A-MR_r1i1p1_SMHI-RCA4_v1</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">RCA4_v1RCA4_v1RCA4_v1</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">5</oasis:entry>  
         <oasis:entry colname="col2">MPI-ESM-LR_r1i1p1_SMHI-RCA4_v1</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p>For the <inline-formula><mml:math id="M34" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-fold cross validation, the RCM data between 1951 and 2010 are split
into six 10-year sections, comprising a 6-fold, five-RCM-ensemble experiment of
Fig. 4. Each section is validated once by using
the remaining five sections for the calibration. A total of 30 tests
are conducted using each procedure.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p>The 6-fold cross validation scheme with the calibration (C) and the
validation (V) periods of each fold. Each experiment (Exp) was replicated for
all five RCMs.</p></caption>
        <?xmltex \igopts{width=128.037402pt}?><graphic xlink:href="https://esd.copernicus.org/articles/8/889/2017/esd-8-889-2017-f04.png"/>

      </fig>

      <p>For the transient experiment, the RCM data between 1951 and 2100 are
considered, using the 1951–2010 as calibration to correct the 1951–2100
data.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><caption><p>Statistical properties of the calibration and the validation
periods for the two bias correction procedures. Variables denoted with <inline-formula><mml:math id="M35" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula> are
estimated on annual aggregates. SD stands for standard deviation, p<inline-formula><mml:math id="M36" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>
for the <inline-formula><mml:math id="M37" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>th  quantile and IQR for the interquartile range.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="9">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"/>

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

         <oasis:entry colname="col3">RAW</oasis:entry>

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

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

         <oasis:entry colname="col6">OBS</oasis:entry>

         <oasis:entry colname="col7">BC</oasis:entry>

         <oasis:entry colname="col8">BC-NM</oasis:entry>

         <oasis:entry colname="col9">BC<inline-formula><mml:math id="M38" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">TREND</mml:mi></mml:msub></mml:math></inline-formula></oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
       <?xmltex \rotentry?>
         <oasis:entry rowsep="1" colname="col1" morerows="6">Calibration</oasis:entry>

         <oasis:entry colname="col2">Mean (<inline-formula><mml:math id="M39" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C)</oasis:entry>

         <oasis:entry colname="col3">11.2</oasis:entry>

         <oasis:entry colname="col4">11.2</oasis:entry>

         <oasis:entry colname="col5">0.0</oasis:entry>

         <oasis:entry colname="col6">9.1</oasis:entry>

         <oasis:entry colname="col7">9.2</oasis:entry>

         <oasis:entry colname="col8">9.2</oasis:entry>

         <oasis:entry colname="col9">9.1</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">SD (<inline-formula><mml:math id="M40" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C)</oasis:entry>

         <oasis:entry colname="col3">4.5</oasis:entry>

         <oasis:entry colname="col4">4.6</oasis:entry>

         <oasis:entry colname="col5">0.9</oasis:entry>

         <oasis:entry colname="col6">5.3</oasis:entry>

         <oasis:entry colname="col7">5.3</oasis:entry>

         <oasis:entry colname="col8">5.3</oasis:entry>

         <oasis:entry colname="col9">5.3</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">p10 (<inline-formula><mml:math id="M41" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C)</oasis:entry>

         <oasis:entry colname="col3">5.7</oasis:entry>

         <oasis:entry colname="col4">5.7</oasis:entry>

         <oasis:entry colname="col5"><inline-formula><mml:math id="M42" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.9</oasis:entry>

         <oasis:entry colname="col6">2.1</oasis:entry>

         <oasis:entry colname="col7">2.2</oasis:entry>

         <oasis:entry colname="col8">2.2</oasis:entry>

         <oasis:entry colname="col9">2.1</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">p90 (<inline-formula><mml:math id="M43" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C)</oasis:entry>

         <oasis:entry colname="col3">17.4</oasis:entry>

         <oasis:entry colname="col4">17.2</oasis:entry>

         <oasis:entry colname="col5">1.0</oasis:entry>

         <oasis:entry colname="col6">16.3</oasis:entry>

         <oasis:entry colname="col7">16.3</oasis:entry>

         <oasis:entry colname="col8">16.2</oasis:entry>

         <oasis:entry colname="col9">16.2</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">Slope (<inline-formula><mml:math id="M44" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C 10 years<inline-formula><mml:math id="M45" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)<inline-formula><mml:math id="M46" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col3"><inline-formula><mml:math id="M47" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.067</oasis:entry>

         <oasis:entry colname="col4">0.000</oasis:entry>

         <oasis:entry colname="col5"><inline-formula><mml:math id="M48" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.067</oasis:entry>

         <oasis:entry colname="col6"><inline-formula><mml:math id="M49" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.026</oasis:entry>

         <oasis:entry colname="col7"><inline-formula><mml:math id="M50" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.086</oasis:entry>

         <oasis:entry colname="col8"><inline-formula><mml:math id="M51" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.065</oasis:entry>

         <oasis:entry colname="col9"><inline-formula><mml:math id="M52" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.061</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">SD (<inline-formula><mml:math id="M53" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C)<inline-formula><mml:math id="M54" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col3">0.46</oasis:entry>

         <oasis:entry colname="col4">0.46</oasis:entry>

         <oasis:entry colname="col5">0.01</oasis:entry>

         <oasis:entry colname="col6">0.61</oasis:entry>

         <oasis:entry colname="col7">0.57</oasis:entry>

         <oasis:entry colname="col8">0.45</oasis:entry>

         <oasis:entry colname="col9">0.53</oasis:entry>

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

         <oasis:entry colname="col2">IQR<inline-formula><mml:math id="M55" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col3">0.76</oasis:entry>

         <oasis:entry colname="col4">0.76</oasis:entry>

         <oasis:entry colname="col5">0.01</oasis:entry>

         <oasis:entry colname="col6">0.86</oasis:entry>

         <oasis:entry colname="col7">0.95</oasis:entry>

         <oasis:entry colname="col8">0.75</oasis:entry>

         <oasis:entry colname="col9">0.94</oasis:entry>

       </oasis:row>
       <oasis:row>
       <?xmltex \rotentry?>
         <oasis:entry colname="col1" morerows="6">Validation</oasis:entry>

         <oasis:entry colname="col2">Mean (<inline-formula><mml:math id="M56" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C)</oasis:entry>

         <oasis:entry colname="col3">11.3</oasis:entry>

         <oasis:entry colname="col4">11.2</oasis:entry>

         <oasis:entry colname="col5">0.1</oasis:entry>

         <oasis:entry colname="col6">9.6</oasis:entry>

         <oasis:entry colname="col7">9.3</oasis:entry>

         <oasis:entry colname="col8">9.3</oasis:entry>

         <oasis:entry colname="col9">9.2</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">SD (<inline-formula><mml:math id="M57" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C)</oasis:entry>

         <oasis:entry colname="col3">4.7</oasis:entry>

         <oasis:entry colname="col4">4.6</oasis:entry>

         <oasis:entry colname="col5">0.9</oasis:entry>

         <oasis:entry colname="col6">5.2</oasis:entry>

         <oasis:entry colname="col7">5.5</oasis:entry>

         <oasis:entry colname="col8">5.4</oasis:entry>

         <oasis:entry colname="col9">5.5</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">p10 (<inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C)</oasis:entry>

         <oasis:entry colname="col3">5.6</oasis:entry>

         <oasis:entry colname="col4">5.7</oasis:entry>

         <oasis:entry colname="col5"><inline-formula><mml:math id="M59" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.9</oasis:entry>

         <oasis:entry colname="col6">2.7</oasis:entry>

         <oasis:entry colname="col7">2.0</oasis:entry>

         <oasis:entry colname="col8">2.0</oasis:entry>

         <oasis:entry colname="col9">1.9</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">p90 (<inline-formula><mml:math id="M60" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C)</oasis:entry>

         <oasis:entry colname="col3">17.4</oasis:entry>

         <oasis:entry colname="col4">17.2</oasis:entry>

         <oasis:entry colname="col5">1.0</oasis:entry>

         <oasis:entry colname="col6">16.3</oasis:entry>

         <oasis:entry colname="col7">16.3</oasis:entry>

         <oasis:entry colname="col8">16.2</oasis:entry>

         <oasis:entry colname="col9">16.2</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">Slope (<inline-formula><mml:math id="M61" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C 10 years<inline-formula><mml:math id="M62" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)<inline-formula><mml:math id="M63" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col3">0.052</oasis:entry>

         <oasis:entry colname="col4">0.000</oasis:entry>

         <oasis:entry colname="col5">0.051</oasis:entry>

         <oasis:entry colname="col6">0.076</oasis:entry>

         <oasis:entry colname="col7">0.062</oasis:entry>

         <oasis:entry colname="col8">0.051</oasis:entry>

         <oasis:entry colname="col9">0.044</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">SD (<inline-formula><mml:math id="M64" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C)<inline-formula><mml:math id="M65" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col3">0.48</oasis:entry>

         <oasis:entry colname="col4">0.47</oasis:entry>

         <oasis:entry colname="col5">0.01</oasis:entry>

         <oasis:entry colname="col6">0.54</oasis:entry>

         <oasis:entry colname="col7">0.57</oasis:entry>

         <oasis:entry colname="col8">0.46</oasis:entry>

         <oasis:entry colname="col9">0.53</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">IQR<inline-formula><mml:math id="M66" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col3">0.63</oasis:entry>

         <oasis:entry colname="col4">0.62</oasis:entry>

         <oasis:entry colname="col5">0.01</oasis:entry>

         <oasis:entry colname="col6">0.76</oasis:entry>

         <oasis:entry colname="col7">0.75</oasis:entry>

         <oasis:entry colname="col8">0.62</oasis:entry>

         <oasis:entry colname="col9">0.68</oasis:entry>

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

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p><bold>(a)</bold> Annual average temperature of raw model, observations
and the bias-corrected with and without the NM data and following the BC-TREND
approach, for the calibration period 1850–1899 (solid lines) and the
validation period 1900–2005 (dashed lines). <bold>(b)</bold> Annual averages of
the normalized and the residuals of the raw temperature. Probability
densities of annual <bold>(c)</bold> and of daily means <bold>(d)</bold>.</p></caption>
        <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://esd.copernicus.org/articles/8/889/2017/esd-8-889-2017-f05.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p>Power spectral density of temperature <bold>(a)</bold> and high-power
regions of annual and half-year periods <bold>(b)</bold>. <bold>(c)</bold> Standard deviation of
temperature aggregates between 1 and 10 957 days (horizontal axis visible
between 1 day and 10 years). <bold>(d)</bold> The
inter-annual and sub-annual periods' average (denoted with red and cyan arrows
respectively) spectral power <bold>(a)</bold> and standard
deviation <bold>(c)</bold>.</p></caption>
        <?xmltex \igopts{width=384.112205pt}?><graphic xlink:href="https://esd.copernicus.org/articles/8/889/2017/esd-8-889-2017-f06.png"/>

      </fig>

</sec>
<sec id="Ch1.S4">
  <title>Results</title>
      <p>The results of the split sample test on the central England example are
presented in Fig. 5. The NM separates of the raw
data into a residuals and a normalized stream (Fig. 5b). In the annual aggregates
the normalized time series do not exhibit any trend or significant
fluctuation, since the normalization is performed on annual basis, while the
long-term trend and variability are contained in the residual time series.
In Fig. 5a, annual aggregates obtained via the
BC, BC-NM, and the BC-TREND procedures are compared to the raw data and the
observations. Results show that all three procedures adjust the raw data to
better fit the observations in the calibration period 1850–1899. In the
validation period, all three procedures produce similar results in terms of
mean and standard deviation, but the BC-NM long-term linear trend is
slightly lower than that of the BC results and slightly higher than the
respective BC-TREND slope. While both BC and BC-TREND slopes are closer to
the observations' linear trend, the BC-NM is closer to the raw data trend
(Table 2). The BC-TREND validation period trend is
found lower relative to the RAW data, but closer to it relative to the
BC. This is attributed to the new trend that was introduced to the detrended
time series by the differential quantile mapping in each year's CDF,
similar to the Fig. 1 example.</p>
      <p>Figure 5c shows that, in the annual aggregated
temperature, the BC-NM resembles the raw data histograms in shape, but
shifted in mean towards the observations. A small decrease in the
variability can also be observed in the BC-NM relative to the raw data but
consists of a substantially smaller disturbance relative to the BC. The
annual variability in BC-TREND is closer to the raw data compared to the BC
approach, but the BC-NM still outperforms in the annual variability
preservation. The transfer of the mean with a simultaneous preservation of
the larger part of the variability of the BC consists of a nearly idealized
behavior for the adjusted data when the long-term statistics preservation is
a desired characteristic, as the distribution of the annual temperature
averages is retained after the correction (trend, standard deviation,
interquartile range – Table 2). The respective
results generated on daily data (Fig. 5d) show
that all three procedures adjust the calibration and validation histograms
to a similar degree towards the observations. This can also be verified by
the mean, the standard deviation, and the 10th and 90th percentile
of the daily data of Table 2. An early concluding
remark about the NM is that it retained the long-term statistics of the
adjusted data towards the climate model signal better than the alternative
approaches, without, however, sacrificing the daily scale quality of the
correction.</p>
      <p>To further inter-compare the effect of each approach in the data variability
beyond the inter-annual and the daily basis, we estimate the power spectral
density (PSD; Huybers and Curry, 2006) over their daily temperature signals
(Fig. 6). The marked spectral peaks associated with the annual and 6-month
periodicity are an expected result. Focusing on those regions (Fig. 6b), it
is shown that the BC-NM is closer to the observational variability relative
to the other two correction techniques, while in the 6 months all techniques
provide similar results. The average power density of the domain beyond the
annual periodic shows that the BC-NM is closer to the raw data, while the
respective sub-annual average is almost equal to the BC and the BC-TREND
averages. Figure 6c shows the standard deviation estimated on temperature
aggregates between 1 and 10 957 days (i.e., 30 years). Figure 6d shows the
average variability and average spectral power of the two scaling regimes,
above and below annual. The sub-annual scales average variability of the BC-NM
resembles the observational variability, outperforming the BC and BC-TREND
approaches that show higher values. More importantly, the NM works well on
the inter-annual scale, where the average variability is found to be closer
to the raw data variability compared to the inflated BC and the deflated
BC-TREND results.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><caption><p>Mean surface temperature of the cross validation test.
Panels <bold>(a)</bold> and <bold>(b)</bold> show the ensemble mean of the five raw
models data and the EOBS respectively, while panel <bold>(c)</bold> shows their
difference. Panels <bold>(d)</bold> and <bold>(e)</bold> show the ensemble mean
remaining bias of the five RCMs after the correction with and without the
NM module respectively, for the calibration periods' data.
Panels <bold>(f)</bold> and <bold>(g)</bold> are the same as <bold>(d)</bold> and <bold>(e)</bold> but for the validation period
data.</p></caption>
        <?xmltex \igopts{width=221.931496pt}?><graphic xlink:href="https://esd.copernicus.org/articles/8/889/2017/esd-8-889-2017-f07.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><caption><p>Ensemble long-term linear trend of the five RCMs' data. The trend
is estimated on the mean temperature (top) and the 10th (middle) and 90th
(bottom) percentiles on an annual basis. The change in the corrected data
trend relative to the raw data trend is provided for the BC (middle panels)
and the BC-NM data (right panels). All values are expressed as degrees per
century (<inline-formula><mml:math id="M67" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C 100 years<inline-formula><mml:math id="M68" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>).</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://esd.copernicus.org/articles/8/889/2017/esd-8-889-2017-f08.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><caption><p>Average of standard deviations for the study domain, for the raw
data <bold>(a)</bold>, the BC <bold>(b)</bold> and the BC-NM <bold>(c)</bold> for the
different models and the observations, on an annual basis. Differences between
the raw and the bias-corrected standard deviations are shown
in <bold>(d)</bold> and <bold>(e)</bold>.
Plots <bold>(f)</bold> and <bold>(g)</bold> correspond to the same data
as <bold>(d)</bold> and <bold>(e)</bold>, but normalized for their 1951–2005 mean.</p></caption>
        <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://esd.copernicus.org/articles/8/889/2017/esd-8-889-2017-f09.png"/>

      </fig>

      <p>In Fig. 7, the results of the cross validation
test of the BC on the Euro CORDEX data with and without the use of NM are
shown, in terms of mean temperature. The means of the raw temperature data
and the observations are respectively equal for their calibration and the
validation periods due to the design of the experiment. The bias correction
results show that both the correction with and without the NM, appropriately
meet the needs in terms of the mean value. The differences between the
calibration and validation averages with the corresponding observations show
consistently low residuals. A significant difference between the two tests
is that the use of the BC-NM increases the residuals due to the exclusion of
some parts of the signal from the correction process. Nonetheless, the scale
of the residuals is considered below significance in the context of CCI
studies, as it ranges only up to 0.035 <inline-formula><mml:math id="M69" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. The increased residuals of
the NM are the trade-off to the preservation of the model long-term climate
change signal, in the transient experiment. Potential drawbacks that arise
from the residuals' existence are discussed later.
Figure 8 shows the long-term change in the signal
of the mean temperature, for the 10th and 90th percentiles
(estimated on annual basis). The trends are estimated by linear least squares
regression and are expressed in degrees Celcius per century. The use of the NM was
superior in preserving the long-term trend relative to the raw model data
in all three cases. Without using the NM module, the distortion in the mean
annual temperature trend lies between <inline-formula><mml:math id="M70" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.5 and 0.5<inline-formula><mml:math id="M71" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C per century,
while the distortion in the 10th and 90th percentiles is
apparently more profound. Additionally, the northeastern Europe 10th
and 90th percentiles reveal a widening of the temperature distribution
when NM is not used. This widening is attributed to the considerable
negative trend in the 10th percentile and
the considerable positive 90th percentile trend in the
same areas. The magnitude of the distortion is considerable and can
potentially lead to CCI overestimation. In contrast, with the use of NM the
change in the trend is reduced in most of the European area.</p>
      <p>The impact of NM on the standard deviation is also significant.
Figure 9 shows the evolution of the standard
deviations of the adjusted daily data for each model, in the cases of raw
data and the bias-corrected data using the BC and the BC-NM. The
standard deviation is estimated for each grid point and calendar year, and
is averaged across the study domain. The results show that the standard
deviation of the adjusted data differs from the respective standard
deviations of the raw data, in both adjustment approaches. This is an
expected outcome, as raw model data standard deviations differ from the
respective observed data standard deviation (Fig. 9d, e).
However, the standard deviation differences between BC-NM and
the raw data (Fig. 9f) are significantly more
stable than the respective differences from BC
(Fig. 9g), meaning that the signal of standard
deviation is better preserved and does not inflate significantly with time
in the former case. Additionally, the variation of the standard deviations
time series exhibits lower fluctuations.</p>
</sec>
<sec id="Ch1.S5">
  <title>Discussion</title>
      <p>This study focuses on known issues of bias correction that have been well
discussed in the literature. Whether the long-term signal of temperature
should be preserved or not has been discussed on a more theoretical level in
Maraun (2016), while Haerter et al. (2011) mention that a credible bias
correction methodology should involve the consequences of greenhouse gas
concentration changes. This is somehow consistent with the temperature trend
preservation as the model sensitivity is retained in the corrected
time series. As pointed in Fischer et al. (2012), models tend to
underestimate the inter-annual variability due to deficiencies between
land–atmosphere interactions, which urges for its correction. Nevertheless,
the long-term statistics' preservation may be necessitated in cases that
temperature is used in biophysical impact modeling (Rubino et al., 2016), or
may be preferred as a safer option than the unintentional alteration,
especially in cases where the observational data record is not long enough.</p>
      <p>The methodology shares similarities to other correction methods found in the
literature. Furthermore it exhibits a number of advancements that overpass
drawbacks of other trend preserving methodologies. The fundamental idea of
the presented method is also identified in the method of Haerter et
al. (2011) method that considers two different timescales and performs a
cascade correction of temperature. In the present study, a discrimination of
annual and daily scales is used for the separation of the temperature signal
in two parts. While in the former methodology, the cascade correction
benefits the results in both timescales, here the separation offers a
correction on the daily scale and an intentional preservation of the raw
model statistics on the annual scale. Comparisons can also be performed with
the methodology of Li et al. (2010), who use the differences in the raw data
between the reference period and the projection period. In the present study
the differences are defined between the reference period and each year of
correction separately. This can be considered as an evolution of the
technique that overcomes the subjectivity of the future period selection.
Additionally, the quantile mapping correction ensures the skillful correction
in the higher and lower quantiles, relative to simpler additive approaches
such as that of Hempel et al. (2013), which, while preserving the trend and
year-to-year variability, marginally improves the tails of the temperature
distribution (Sippel et al., 2016). Regarding the simpler BC-TREND version
that was used for the central England example, it was found that it tends to
preserve the long-term statistics as also noted by Cannon et al. (2015), but the 5-year average that was used for the trend preservation still cannot
encompass the changes in each year's CDF, as the NM can.</p>
      <p>Beyond these advancements, a critical drawback of the presented methodology
is that it uses a large number of parameters to approximate the transfer
functions in the two stages of the correction. The methodology can be
described as of “varying complexity” as the number of the estimated
parameters (number of segments) and the added value of the complexity is
weighted by an information criterion. Nonetheless, it is highly invasive,
which means that in the case that high-noise observations were used, it
would lead to transfer of that noise to the corrected data variability. This
was marginally detected in the analysis of the standard deviations in Fig. 9,
even if the effect of the BC-NM mitigated the effect compared to the BC.
Another weakness stems from the residuals' exclusion from the correction. In
the theoretical case where the future projected temperature variability
changes radically relative to the reference period, the correction would
result in larger remaining biases as it was shown earlier, which could impair
the physical continuity of the time series. This limitation should be taken
into consideration for the case that the BC-NM is used to correct other types of
variables, without forbidding its use on them.</p>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <title>Conclusions</title>
      <p>This study elaborates the issue of the distortion of the long-term statistics
in quantile mapping statistical bias correction relative to the raw model
data. An extra processing step is presented that can be applied along with
quantile mapping statistical bias correction techniques. This step, namely
NM, splits the original data into two parts – a normalized one that is bias
adjusted using quantile mapping, and a residuals part that is added to the
former after the bias correction. The methodology is tested and validated
from several points of view, leading to some key remarks about its added
value. First, it is shown that the use of the NM module results in the
long-term temperature trend preservation of the mean temperature change, as well as of the trend in the higher and lower percentiles. Furthermore, the
examination of the standard deviation temporal evolution shows that it is
better retained relative to the raw data, as the exclusion of the residuals
from the correction minimizes the inflation of the variance. Additionally,
the inter-annual variability of the raw data is preserved relative to the
compared simpler quantile mapping methods, which is an important
feature for climate impact studies that involve carbon cycle simulations
(Rubino et al., 2016). Another noteworthy feature of the proposed method is
that the normalization is performed on an annual basis; hence, the projection
period results are not affected by the length of the projection period.
Nevertheless, it has to be stressed that a range of issues – such as the
disruption of the physical consistency of climate variables, the mass/energy
balance and the omission of correction feedback mechanisms to other climate
variables (Ehret et al., 2012) – were not examined in this work, despite the
existence of methods that preserve consistency between specific variables
(Sippel et al., 2016). As an epilogue, bias correction cannot add further
accuracy to the data but rather add usefulness to it, depending on the needs
of each application. Nevertheless, it should not be underestimated that this
added usefulness may obscure a deterioration of the climate change signal
owing to the bias correction.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability">

      <p>All the underlying research data are freely accessible. The
RCM data were obtained from the Earth System Grid Federation (ESGF –
<uri>https://esg-dn1.nsc.liu.se/search/cordex/</uri>, Jacob et al., 2014). The
E-OBS data were obtained from the European Climate Assessment &amp; Dataset
project website (<uri>http://www.ecad.eu</uri>, Haylock et al., 2008). The HadCET
temperature data were obtained from the Met Office website
(<uri>https://www.metoffice.gov.uk/hadobs/hadcet/</uri>, Parker et al., 1992).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p><bold>The Supplement related to this article is available online at <inline-supplementary-material xlink:href="https://doi.org/10.5194/esd-8-889-2017-supplement" xlink:title="zip">https://doi.org/10.5194/esd-8-889-2017-supplement</inline-supplementary-material>.</bold></p></supplementary-material>
        </app-group><notes notes-type="competinginterests">

      <p>The authors declare that they have no conflict of
interest.</p>
  </notes><ack><title>Acknowledgements</title><p>The authors would like to thank  Stefan Hagemann and the anonymous
reviewer for their valuable comments and suggestions which improved the quality
of the paper. The research leading to these results has received funding from
the HELIX project of the European Union's Seventh Framework Programme for
research, technological development and demonstration under grant agreement
no. 603864. We acknowledge the World Climate Research Programme's Working
Group on Regional Climate, and the Working Group on Coupled Modeling, former
coordinating body of CORDEX and responsible panel for CMIP5. We also thank
the climate modeling groups (listed in Table 1 of this paper) for producing
and making available their model output. Finally, we acknowledge the E-OBS
dataset from the ENSEMBLES EU-FP6 project
(<uri>http://ensembles-eu.metoffice.com</uri>) and the data providers in the ECA&amp;D
project (<uri>http://www.ecad.eu</uri>).<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: Axel Kleidon<?xmltex \hack{\newline}?>
Reviewed by: Stefan Hagemann and one anonymous referee</p></ack><ref-list>
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  </ref-list><app-group content-type="float"><app><title/>

    </app></app-group></back>
    <!--<article-title-html>A method to preserve trends in quantile mapping bias correction of climate modeled temperature</article-title-html>
<abstract-html><p class="p">Bias correction of climate variables is a standard practice in
climate change impact (CCI) studies. Various methodologies have been
developed within the framework of quantile mapping. However, it is well known
that quantile mapping may significantly modify the long-term statistics due
to the time dependency of the temperature bias. Here, a method to overcome
this issue without compromising the day-to-day correction statistics is
presented. The methodology separates the modeled temperature signal into a
normalized and a residual component relative to the modeled reference
period climatology, in order to adjust the biases only for the former and
preserve the signal of the later. The results show that this method allows
for the preservation of the originally modeled long-term signal in the mean,
the standard deviation and higher and lower percentiles of temperature. To
illustrate the improvements, the methodology is tested on daily time series
obtained from five Euro CORDEX regional climate models (RCMs).</p></abstract-html>
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