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  <front>
    <journal-meta><journal-id journal-id-type="publisher">HESS</journal-id><journal-title-group>
    <journal-title>Hydrology and Earth System Sciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">HESS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Hydrol. Earth Syst. Sci.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1607-7938</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/hess-27-4187-2023</article-id><title-group><article-title>A statistical–dynamical approach for probabilistic <?xmltex \hack{\break}?> prediction of sub-seasonal precipitation anomalies <?xmltex \hack{\break}?> over 17 hydroclimatic regions in China</article-title><alt-title>A statistical–dynamical approach for sub-seasonal precipitation prediction</alt-title>
      </title-group><?xmltex \runningtitle{A statistical--dynamical approach for sub-seasonal precipitation prediction}?><?xmltex \runningauthor{Y.~Li et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Li</surname><given-names>Yuan</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Xü</surname><given-names>Kangning</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Wu</surname><given-names>Zhiyong</given-names></name>
          <email>wzyhhu@gmail.com</email>
        <ext-link>https://orcid.org/0000-0001-7186-3776</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Zhu</surname><given-names>Zhiwei</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Wang</surname><given-names>Quan J.</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>College of Hydrology and Water Resources, Hohai University, Nanjing 210098, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Key Laboratory of Meteorological Disaster, Ministry of Education (KLME)/Collaborative Innovation Center on Forecast and Evaluation of Meteorological Disasters (CIC-FEMD)/Joint International Research Laboratory of Climate and Environment Change (ILCEC), Nanjing University of Information Science and Technology, Nanjing 210044, China</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Infrastructure Engineering, The University of Melbourne, Parkville 3010, Australia</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Zhiyong Wu (wzyhhu@gmail.com)</corresp></author-notes><pub-date><day>21</day><month>November</month><year>2023</year></pub-date>
      
      <volume>27</volume>
      <issue>22</issue>
      <fpage>4187</fpage><lpage>4203</lpage>
      <history>
        <date date-type="received"><day>26</day><month>April</month><year>2023</year></date>
           <date date-type="rev-request"><day>25</day><month>July</month><year>2023</year></date>
           <date date-type="rev-recd"><day>9</day><month>November</month><year>2023</year></date>
           <date date-type="accepted"><day>14</day><month>November</month><year>2023</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2023 </copyright-statement>
        <copyright-year>2023</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://hess.copernicus.org/articles/.html">This article is available from https://hess.copernicus.org/articles/.html</self-uri><self-uri xlink:href="https://hess.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://hess.copernicus.org/articles/.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e134">In this study, we develop a spatial–temporal projection-based calibration, bridging, and merging (STP-CBaM) method to improve probabilistic sub-seasonal precipitation forecast skill over 17 hydroclimatic regions in China. The calibration model is established by post-processing ECMWF raw forecasts using the Bayesian joint probability (BJP) approach. The bridging models are built using large-scale atmospheric intraseasonal predictors, including zonal wind at 200 hPa (U200) and 850 hPa (U850); an outgoing longwave radiation anomaly (OLRA); and geopotential height at 200 hPa (H200), 500 hPa (H500), and 850 hPa (H850) defined by the STP method. The calibration model and the bridging models are then merged through the Bayesian modelling averaging (BMA) method. Our results indicate that the forecast skill of the calibration model is higher compared to bridging models when the lead time is within 5–10 d. The U200- and OLRA-based bridging models outperform the calibration model in certain months and certain regions. The BMA-merged forecasts take advantage of both calibration models and bridging models. Meanwhile, the BMA-merged forecasts also show high reliability at longer lead times. However, some improvements to reliability are still needed at shorter lead times. These findings demonstrate the great potential to combine dynamical models and statistical models in improving sub-seasonal precipitation forecasts.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>National Natural Science Foundation of China</funding-source>
<award-id>52009027</award-id>
<award-id>U2240225</award-id>
<award-id>42088101</award-id>
</award-group>
</funding-group>
</article-meta>
  </front>
<body>
      

      <?xmltex \hack{\newpage}?>
<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e148">Sub-seasonal forecasting (defined as the time range between 2 weeks and 2 months) bridges the gap between short- to medium-range weather forecasts and seasonal climate prediction (Vitart and Robertson, 2018; Liu et al., 2023). Skilful and reliable sub-seasonal precipitation forecasts are highly valuable for water resource management, flood disaster preparedness, and many other climate-sensitive sectors (White et al., 2022; Yan et al., 2023; Zhu et al., 2022). However, it is considered a difficult time range to generate skilful forecasts. The memory of atmospheric initial conditions is lost compared to short- to medium-range forecasts, while the variability of lower-boundary conditions, such as sea surface temperature, is too slow to take effect (Vitart and Robertson, 2018). Statistical models, which use observational relationships between sub-seasonal precipitation and atmospheric intraseasonal oscillations, have been developed in recent years. The spatial–temporal projection model (STPM), which extracts the coupled patterns of preceding atmospheric intraseasonal oscillations and precipitation, has shown skill in predicting sub-seasonal precipitation. Zhu and Li (2017) constructed STPMs over different climatic regions during the boreal summer monsoon season, and their results indicated that the STPMs could generate skilful forecasts for intraseasonal precipitation patterns with lead times of up to 20 d. Our previous study developed a spatial–temporal projection-based Bayesian hierarchical model (STP-BHM) to take the<?pagebreak page4188?> uncertainties in the relationships between atmospheric intraseasonal oscillations and sub-seasonal precipitation into account (Li et al., 2022). However, statistical models are highly reliant on stationary relationships between predictors and predictands. Seasonal changes in climatological conditions may lead to different relationships between atmospheric intraseasonal oscillations and precipitation. Liu and Lu (2022) suggested that the impacts of boreal summer intraseasonal oscillation (BSISO) on precipitation are different between early and late summers. W. Li et al. (2023) found that the long-period BSISO event-affected region and the associated precipitation anomalies are different compared to short-period BSISO events.</p>
      <p id="d1e151">With a more comprehensive understanding and better representation of potential sources of predictability, there has been much improvement in dynamical models in recent years. The Subseasonal-to-Seasonal (S2S) prediction project and the Subseasonal Experiment (SubX) project have been established to provide S2S forecasts from dynamical models. However, the sub-seasonal precipitation forecasts of global climate models (GCMs) are always of low accuracy (de Andrade et al., 2019; Li et al., 2022). The physical equations are simplified, while the small-scale processes, such as convections, cannot be well represented in most GCMs. In addition, insufficient data assimilation schemes, low capacity in capturing dynamic sources, and misrepresentation of atmosphere–ocean interactions and atmosphere–ocean interactions also contribute to the limited forecast skill (Wu et al., 2023; Zhang et al., 2021). Although post-processing methods have been proposed in recent years, the forecast skill after post-processing was still limited for lead times beyond 10–14 d (Li et al., 2021).</p>
      <p id="d1e154">Despite the low forecast skill of sub-seasonal precipitation, the GCMs show much higher performance in predicting large-scale circulation patterns. Cui et al. (2021) evaluated the potential of GCMs to predict intraseasonal surface air temperature over mid- to high-latitude Eurasia. Their results indicated that the upper limit of the useful forecast skill ranged from <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> d. The BSISO is the predominant variability of the Asian summer monsoon, and most GCMs exhibit predictability on timescales of above 3 weeks for BSISO events (Chen and Zhai, 2017; Hsu et al., 2016; Ren et al., 2018). Lee et al. (2015) evaluated the prediction skill of BSISO indices using six coupled models in the Intraseasonal Variability Hindcast Experiment (ISVHE) project, and their results suggested that skilful BSISO prediction was about 22 d under strong initial conditions. Shibuya et al. (2021) suggested that the overall useful prediction skill of the BSISO was approximately 24 d in a global non-hydrostatic icosahedral atmospheric model (NICAM) with explicit cloud microphysics. Similar results were also found by Wu et al. (2023), i.e. that the ECMWF model showed skilful prediction of the BSISO index at a 24 d lead time.</p>
      <p id="d1e177">Given the strengths and weaknesses of both statistical models and dynamical models, there has been growing interest in developing hybrid prediction models that combine forecasts from both statistical and dynamical models (Slater et al., 2023). Schepen et al. (2014) used POAMA (Predictive Ocean Atmosphere Model for Australia) forecasts of seasonal climate indices as predictors to predict seasonal precipitation over Australia. Strazzo et al. (2019b) developed a hybrid statistical–dynamical system to predict seasonal temperature and precipitation over North America. Most previous statistical–dynamical models focus on seasonal predictions. Far fewer attempts have been made on sub-seasonal timescales. Specq and Batté (2020) proposed a statistical–dynamical post-processing scheme to improve the quality of sub-seasonal forecasts of weekly precipitation using Madden–Julian Oscillation (MJO) and El Niño–Southern Oscillation (ENSO) indices as predictors. Wu et al. (2022) established a dynamical–statistical prediction model (DSPM) to improve sub-seasonal precipitation forecasts. Deep-learning models were also proposed to predict sub-seasonal extreme rainfall events, with the GCM-predicted large-scale circulation patterns used as predictors (Xie et al., 2023). Zhu et al. (2023) developed a dynamical–statistical hybrid model using the novel indices of the zonal displacements of the South Asia high and the western Pacific sub-tropical high to predict the Meiyu intraseasonal variation. Nevertheless, the relationships between large-scale circulation patterns and sub-seasonal precipitation have high uncertainty. More sophisticated hybrid models are required to further improve the probabilistic sub-seasonal precipitation forecast skill.</p>
      <p id="d1e181">The calibration, bridging, and merging (CBaM) method, which employed Bayesian-theorem-based approaches to take advantage of both dynamical models and statistical models, has proven able to generate skilful and reliable seasonal precipitation and temperature forecasts over different regions (Peng et al., 2014; Schepen et al., 2014, 2016;  Strazzo et al., 2019a). In calibration, the Bayesian joint probability (BJP) approach was used to post-process raw precipitation forecasts derived from GCMs. The BJP approach was also used to generate probabilistic forecasts using large-scale circulation patterns as predictors. This was also referred to as bridging. The calibrated forecasts and bridged forecasts were then merged through the Bayesian modelling averaging (BMA) method (Wang et al., 2012). Most previous studies used the CBaM method to generate seasonal forecasts. However, much less work has been done on sub-seasonal timescales for several reasons. Compared to seasonal forecasts, there are far fewer climate indices that can be used as predictors on sub-seasonal timescales. Moreover, the atmospheric intraseasonal oscillations may have different effects on precipitation anomalies in different months. As a consequence, it is much more difficult to establish bridging models for sub-seasonal precipitation forecasts. In addition, the evolution of the intraseasonal variability of precipitation varies in different stages with different periods in different regions (Liu et al., 2020; Zhu and Li, 2017). The effectiveness of the<?pagebreak page4189?> calibration models will be greatly affected if seasonality is not considered.</p>
      <p id="d1e184">In this study, we develop a spatial–temporal projection-based calibration, bridging, and merging (STP-CBaM) method to improve probabilistic sub-seasonal precipitation forecast skill by combining the strengths of both dynamical models and statistical models. The ECMWF sub-seasonal precipitation forecasts are calibrated using the BJP approach for each month. The bridging models are then built using large-scale atmospheric intraseasonal predictors defined by the STPM. The calibration model and bridging models are merged through the BMA method to generate skilful and reliable sub-seasonal precipitation forecasts. The STP-CBaM method will be applied to predict sub-seasonal precipitation anomalies over each hydroclimatic region during the boreal summer monsoon from May to October. The accuracy and reliability will be evaluated through a leave-one-year-out cross-validation strategy.</p>
      <p id="d1e187">In the following two sections, the data and methodology are introduced. The prediction skill and reliability of the STP-CBaM method are provided in Sect. 4. Section 5 discusses the forecast skill, limitations, and future work. Key findings are summarized in Sect. 6.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Precipitation dataset</title>
      <p id="d1e205">In this study, China is divided into 17 hydroclimatic regions on the basis of both climate classifications and watershed division standards (Fig. 1). The precipitation data are derived from the latest Multi-Source Weighted-Ensemble Precipitation, version 2.8 (MSWEP V2.8) dataset. This dataset is developed by optimally merging precipitation data derived from gauge, satellite, and reanalysis datasets. It covers the period from 1979 to the near past with a spatial resolution of <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">0.1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>. Many studies have found that the MSWEP dataset is of a high quality over China (Y. Li et al., 2023; Liu et al., 2019; Guo et al., 2023).</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="d1e230">The 17 hydroclimatic regions over China. Publisher's remark: please note that the above figure contains disputed territories.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://hess.copernicus.org/articles/27/4187/2023/hess-27-4187-2023-f01.png"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Reanalysis dataset and outgoing long-wave radiation (OLR) dataset</title>
      <p id="d1e247">The daily mean geopotential height at 200, 500, and 850 hPa (H200, H500, H850) and zonal wind at 200 hPa (U200) and 850 hPa (U850) are derived from the ERA5 (Hersbach et al., 2020) reanalysis dataset at <uri>https://cds.climate.copernicus.eu/</uri> (last access: 10 December 2022). The daily mean OLR data are provided by the National Oceanic and Atmospheric Administration (NOAA) Physical Sciences Laboratory (PSL), Boulder, Colorado, USA, from their website at <uri>https://psl.noaa.gov</uri> (last access: 17 December 2022). The OLR data are developed from high-resolution infrared radiation sounder instruments and have been widely used over the globe. All daily mean data including U200, U850, OLR, H200, H500, and H850 are bilinearly interpolated onto a horizontal resolution of <inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.5</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> over the period of 2001–2020.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Hindcast dataset</title>
      <p id="d1e284">The ECMWF hindcast data of precipitation, U850, U200, OLR, H200, H500, and H850 are retrieved from the S2S database at <uri>http://apps.ecmwf.int/datasets/data/s2s/</uri> (last access: 31 December 2022). Compared to other GCMs, the ECMWF model shows the highest forecast skill in various aspects (Jie et al., 2017; Wu et al., 2023; Zhang et al., 2021). In this study, we choose hindcasts when the ECMWF model version dates are in the year 2021 from May to October. Thus, the hindcasts cover the period of 2001–2020. The gridded precipitation hindcasts are area-weighted averages through 17 hydroclimatic regions as the observational data. In addition, all atmospheric hindcast fields including U200, U850, OLRA, H200, H500, and H850 are bilinearly interpolated onto a horizontal resolution of <inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.5</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> as the reanalysis dataset.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Methodology</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Intraseasonal signal extraction</title>
      <p id="d1e326">In this study, a non-filtering method is used to extract 10–60 d signals for both atmospheric variables (U200, U850, OLRA, H200, H500, and H850) and precipitation (Hsu et al., 2015; Zhu et al., 2015). The climatological annual cycle of observational data is first removed by subtracting a 90 d low-pass filtered climatological component. Lower-frequency signals are then removed by subtracting the last 30 d running mean. The higher-frequency signals are then removed by taking a pentad mean. The variable derived in this way represents the observational 10–60 d signals of a daily atmospheric field or precipitation. The daily intraseasonal signals are then averaged to pentad data to further reduce the noise and improve the predictability. The pentad mean 10–60 d intraseasonal precipitation is also referred to as pentad mean precipitation anomalies in the following sections.</p>
      <p id="d1e329">As for the hindcast fields of the ECMWF model, the model climatology of the atmospheric variables (U200, U850, OLRA, H200, H500, and H850) and precipitation is removed as a function of the initial date and lead time. Lower-frequency signals longer than 60 d are then removed in the same way as the observations by subtracting the running mean of the last 30 d. In this process, the observed anomalies before the forecast initial date are used to make enough data for the running mean. The higher-frequency signals of the predicted variables are then removed by taking a pentad mean. The variable derived in this way represents the ECMWF model-forecasted 10–60 d signals of the daily atmospheric field or precipitation.</p><?xmltex \hack{\newpage}?>
</sec>
<?pagebreak page4190?><sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Model formulation</title>
<sec id="Ch1.S3.SS2.SSS1">
  <label>3.2.1</label><title>Predictor definition for bridging models</title>
      <p id="d1e348">In this study, we establish the calibration model and bridging models for each hydroclimatic region, month, and lead time. For the calibration model, the ensemble means of ECMWF-forecasted pentad mean precipitation anomalies are used as predictors. For the bridging models, we define potential predictors using the STPM. Relevant areas of atmospheric fields that could affect 10–60 d precipitation variability are found by cell-wise correlation analysis. The effective degree of freedom is estimated following Livezey and Chen (1983).</p>
      <p id="d1e351">The spatial–temporal coupled covariance patterns are constructed for grid points where the correlation is statistically significant at the 5 % level. The predictor is then defined by summing the product of the covariance field derived from the observational data and the ECMWF model-forecasted atmospheric intraseasonal signals:

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M6" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E1"><mml:mtd><mml:mtext>1</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="normal">cov</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mi>Y</mml:mi></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mi>T</mml:mi></mml:mfrac></mml:mstyle><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>T</mml:mi></mml:munderover><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi>E</mml:mi><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfenced><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mi>E</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E2"><mml:mtd><mml:mtext>2</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msubsup><mml:mi>X</mml:mi><mml:mi>p</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>=</mml:mo><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:mi mathvariant="normal">cov</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mi>Y</mml:mi></mml:mrow></mml:mfenced><mml:mo>⋅</mml:mo><mml:msubsup><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi></mml:mrow><mml:mo>*</mml:mo></mml:msubsup><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              where <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> denotes the pentad mean 10–60 d signal of the <inline-formula><mml:math id="M8" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>th observational atmospheric field (U200, U850, OLRA, U200, H500, H850) where the correlation is statistically significant at the 5 % level for grid <inline-formula><mml:math id="M9" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> during the training period, <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, 2, …, 6. <inline-formula><mml:math id="M11" display="inline"><mml:mi>Y</mml:mi></mml:math></inline-formula> denotes the corresponding pentad mean precipitation anomalies. <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msubsup><mml:mi>X</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi></mml:mrow><mml:mo>*</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> denotes the pentad mean 10–60 d signal of the <inline-formula><mml:math id="M13" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>th hindcast atmospheric field derived from the ECMWF model for grid <inline-formula><mml:math id="M14" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>. <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:msubsup><mml:mi>X</mml:mi><mml:mi>p</mml:mi><mml:mo>*</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> denotes the <inline-formula><mml:math id="M16" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>th predictor defined by the STPM.</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <label>3.2.2</label><title>Calibration and bridging models</title>
      <p id="d1e633">The calibration model and bridging models are established independently of each other, and each model has only one predictor and one predictand. Therefore, there is one calibration model and there are six bridging models for each hydroclimatic region, month, and lead time.</p>
      <p id="d1e636">Each calibration model or bridging model is established using the BJP approach. The predictor <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M18" 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>, …, <inline-formula><mml:math id="M19" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> and the corresponding predictand <inline-formula><mml:math id="M20" display="inline"><mml:mi>Y</mml:mi></mml:math></inline-formula> (pentad mean precipitation anomalies) are normalized to <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M22" display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula> using the Yeo–John transformation method.

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M23" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E3"><mml:mtd><mml:mtext>3</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>u</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mfenced open="{" close=""><mml:mtable class="array" columnalign="left left"><mml:mtr><mml:mtd><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mfenced open="{" close="}"><mml:mrow><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:msup><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mtd><mml:mtd><mml:mrow><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>≠</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mi>log⁡</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mfenced close="}" open="{"><mml:mrow><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:mo>-</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:msup><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>≠</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mi>log⁡</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mo>-</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E4"><mml:mtd><mml:mtext>4</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi>v</mml:mi><mml:mo>=</mml:mo><mml:mfenced close="" open="{"><mml:mtable class="array" columnalign="left left"><mml:mtr><mml:mtd><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mfenced close="}" open="{"><mml:mrow><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>y</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>y</mml:mi></mml:msub></mml:mrow></mml:msup><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>y</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mtd><mml:mtd><mml:mrow><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>y</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:mo>≠</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mi>log⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>y</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mfenced close="}" open="{"><mml:mrow><mml:mo>(</mml:mo><mml:mo>-</mml:mo><mml:mi>y</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>y</mml:mi></mml:msub></mml:mrow></mml:msup><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>y</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mfenced close=")" open="("><mml:mrow><mml:mi>y</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:mo>≠</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mi>log⁡</mml:mi><mml:mo>(</mml:mo><mml:mo>-</mml:mo><mml:mi>y</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>y</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>y</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the unknown transformation parameters for predictor <inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and predictand <inline-formula><mml:math id="M27" display="inline"><mml:mi>Y</mml:mi></mml:math></inline-formula>.</p>
      <?pagebreak page4191?><p id="d1e1218">The matrix <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold">Z</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:mo>=</mml:mo><mml:mo>[</mml:mo><mml:msub><mml:mi>U</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mi>V</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> is then assumed to follow a bivariate normal distribution,
              <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M29" display="block"><mml:mrow><mml:mi mathvariant="bold">Z</mml:mi><mml:mo>∼</mml:mo><mml:mi mathvariant="bold">N</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">μ</mml:mi><mml:mi mathvariant="bold">Σ</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M30" display="inline"><mml:mi mathvariant="bold-italic">μ</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M31" display="inline"><mml:mi mathvariant="bold">Σ</mml:mi></mml:math></inline-formula> are the mean vector and covariance matrices to be estimated: <?xmltex \hack{\newpage}?><?xmltex \hack{\vspace*{-6mm}}?>

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M32" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E6"><mml:mtd><mml:mtext>6</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msup><mml:mi mathvariant="bold-italic">μ</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:mo>=</mml:mo><mml:mfenced close="]" open="["><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>V</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E7"><mml:mtd><mml:mtext>7</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi mathvariant="normal">Σ</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="bold">Σ</mml:mi><mml:mi mathvariant="bold">R</mml:mi><mml:msup><mml:mi mathvariant="bold-italic">σ</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              where <inline-formula><mml:math id="M33" display="inline"><mml:mi mathvariant="bold-italic">σ</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M34" display="inline"><mml:mi mathvariant="bold">R</mml:mi></mml:math></inline-formula> are the standard deviation vector and correlation coefficient matrix, respectively:

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M35" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E8"><mml:mtd><mml:mtext>8</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msup><mml:mi mathvariant="bold-italic">σ</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:mo>=</mml:mo><mml:mfenced close="]" open="["><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>V</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E9"><mml:mtd><mml:mtext>9</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi mathvariant="bold">R</mml:mi><mml:mo>=</mml:mo><mml:mfenced close="]" open="["><mml:mtable class="array" columnalign="left left"><mml:mtr><mml:mtd><mml:mn mathvariant="normal">1</mml:mn></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mi>V</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mrow><mml:mi>V</mml:mi><mml:msub><mml:mi>U</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mn mathvariant="normal">1</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:mfenced><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              Note that the correlation coefficient matrix <inline-formula><mml:math id="M36" display="inline"><mml:mi mathvariant="bold">R</mml:mi></mml:math></inline-formula> is symmetric. Thus, there are only five unknown parameters. Here, we denote the five unknown parameters of the joint distribution as <inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mo>=</mml:mo><mml:mo mathvariant="italic">{</mml:mo><mml:mi mathvariant="bold-italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="bold">Σ</mml:mi><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e1481">Given a data series of <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">D</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi>y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, …, <inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula>, we apply the SCE-UA (shuffled complex evolution method developed at the University of Arizona) method to estimate transformation parameters that maximize the log-likelihood function (Duan et al., 1994). The data series <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">D</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is then normalized to <inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:mi mathvariant="bold">D</mml:mi><mml:mo>=</mml:mo><mml:mo mathvariant="italic">{</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>u</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi>v</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, …, <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula>. The posterior distribution of <inline-formula><mml:math id="M45" display="inline"><mml:mi mathvariant="bold-italic">θ</mml:mi></mml:math></inline-formula> is estimated using a Bayesian framework:
              <disp-formula id="Ch1.E10" content-type="numbered"><label>10</label><mml:math id="M46" display="block"><mml:mrow><mml:mi>p</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mi mathvariant="normal">|</mml:mi><mml:mi mathvariant="bold">D</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mi>V</mml:mi></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mo>∝</mml:mo><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>)</mml:mo><mml:mi>p</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mi mathvariant="bold">D</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mi>V</mml:mi></mml:mrow></mml:mfenced><mml:mi mathvariant="normal">|</mml:mi><mml:mi mathvariant="bold-italic">θ</mml:mi></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the prior distribution of the parameters, and <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold">D</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>U</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mi>V</mml:mi><mml:mo>)</mml:mo><mml:mi mathvariant="normal">|</mml:mi><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the likelihood. As the posterior distributions of parameters <inline-formula><mml:math id="M49" display="inline"><mml:mi mathvariant="bold-italic">θ</mml:mi></mml:math></inline-formula> are not standard distributions, analytical integration is difficult. To overcome this problem, we use the new Gibbs sampling algorithm proposed by Wang et al. (2019) to draw a sample of 1000 sets of parameter values. A more detailed description of the sampling strategy can be found in Li et al. (2021).</p>
      <p id="d1e1718">The posterior predictive distribution of <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msup><mml:mi>t</mml:mi><mml:mo>*</mml:mo></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is given by
              <disp-formula id="Ch1.E11" content-type="numbered"><label>11</label><mml:math id="M51" display="block"><mml:mtable rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:msup><mml:mi>t</mml:mi><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mo>=</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo movablelimits="false">∫</mml:mo><mml:mi>p</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:msup><mml:mi>t</mml:mi><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:mfenced><mml:mi mathvariant="normal">|</mml:mi><mml:msub><mml:mi>u</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msup><mml:mi>t</mml:mi><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:mfenced><mml:mo>,</mml:mo><mml:mi mathvariant="bold-italic">θ</mml:mi></mml:mrow></mml:mfenced><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mi>p</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mi mathvariant="bold">D</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>V</mml:mi></mml:mrow></mml:mfenced><mml:mi mathvariant="normal">|</mml:mi><mml:mi mathvariant="bold-italic">θ</mml:mi></mml:mrow></mml:mfenced><mml:mi mathvariant="normal">d</mml:mi><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
            where <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msup><mml:mi>t</mml:mi><mml:mo>*</mml:mo></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the new forecast value.</p>
      <p id="d1e1872">Again, the Gibbs sampling algorithm is used to obtain 1000 samples of <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>v</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msup><mml:mi>t</mml:mi><mml:mo>*</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>. The samples are then back-transformed to produce the calibrated or bridged predictive density <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mi mathvariant="normal">|</mml:mi><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> using parameter <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>y</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS3">
  <label>3.2.3</label><title>Combining models</title>
      <p id="d1e1951">The merging forecasts are carried out by the BMA method proposed by Wang et al. (2012). Given all the candidate models, <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mi mathvariant="normal">|</mml:mi><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M57" 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>, …, <inline-formula><mml:math id="M58" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>, and the corresponding model weights, <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M60" 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>, …, <inline-formula><mml:math id="M61" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>, the predictive density of the BMA probabilistic forecasts can be represented as
              <disp-formula id="Ch1.E12" content-type="numbered"><label>12</label><mml:math id="M62" display="block"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">BMA</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:mi>y</mml:mi><mml:mi mathvariant="normal">|</mml:mi><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msub><mml:mi>x</mml:mi><mml:mi>K</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><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>K</mml:mi></mml:munderover><mml:msub><mml:mi>w</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:msub><mml:mi>f</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:mi>y</mml:mi><mml:mi mathvariant="normal">|</mml:mi><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the predictor and <inline-formula><mml:math id="M64" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> is the corresponding predictand.</p>
      <p id="d1e2118">To encourage even weights among the models, the prior of the model weights is assumed to follow a symmetric Dirichlet distribution, given as
              <disp-formula id="Ch1.E13" content-type="numbered"><label>13</label><mml:math id="M65" display="block"><mml:mrow><mml:mi>p</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi>K</mml:mi></mml:mrow></mml:mfenced><mml:mo>∝</mml:mo><mml:munderover><mml:mo movablelimits="false">∏</mml:mo><mml:mrow><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>K</mml:mi></mml:munderover><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M66" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> is the concentration parameter slightly over 1 and, more specifically, <inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>/</mml:mo><mml:mi>K</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula>. The posterior distribution of model weights given <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, …, <inline-formula><mml:math id="M70" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> events is as follows:
              <disp-formula id="Ch1.E14" content-type="numbered"><label>14</label><mml:math id="M71" display="block"><mml:mtable class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mi>p</mml:mi><mml:mfenced close="" open="("><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>k</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:mfenced></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mfenced open="" close=")"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi>K</mml:mi><mml:mfenced open="|" close=""><mml:mrow><mml:msubsup><mml:mi>x</mml:mi><mml:mi>k</mml:mi><mml:mi>T</mml:mi></mml:msubsup><mml:mo>,</mml:mo><mml:msup><mml:mi>y</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:mfenced><mml:msub><mml:mi>f</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:mi>y</mml:mi><mml:mi mathvariant="normal">|</mml:mi><mml:msub><mml:mi>x</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi>K</mml:mi></mml:mrow></mml:mfenced></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>k</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>K</mml:mi></mml:munderover><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:munderover><mml:mo movablelimits="false">∏</mml:mo><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>T</mml:mi></mml:munderover><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>K</mml:mi></mml:munderover><mml:msub><mml:mi>w</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:msubsup><mml:mi>f</mml:mi><mml:mi>k</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mfenced open="(" close=")"><mml:mrow><mml:msup><mml:mi>y</mml:mi><mml:mi>t</mml:mi></mml:msup><mml:mi mathvariant="normal">|</mml:mi><mml:msubsup><mml:mi>x</mml:mi><mml:mi>k</mml:mi><mml:mi>t</mml:mi></mml:msubsup></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="M72" display="inline"><mml:mrow><mml:msubsup><mml:mi>f</mml:mi><mml:mi>k</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>(</mml:mo><mml:msup><mml:mi>y</mml:mi><mml:mi>t</mml:mi></mml:msup><mml:mi mathvariant="normal">|</mml:mi><mml:msubsup><mml:mi>x</mml:mi><mml:mi>k</mml:mi><mml:mi>t</mml:mi></mml:msubsup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the cross-validated predictive density. This indicates that the weights are assigned by the model's predictive ability rather than the fitting ability. An expectation–maximization (EM) algorithm is then used to estimate the weights by maximizing the likelihood function. Initially, all the weights are equal. The EM algorithm is then iterated until the likelihood function converges.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Evaluation</title>
      <p id="d1e2478">In this study, a leave-one-year-out cross-validation strategy is used to avoid any bias in skill, including predictor selection, data normalization, model building, parameter inference, and verification.</p>
      <p id="d1e2481">The temporal correlation coefficient (TCC) is used to evaluate the performance of the ECMWF model in predicting atmospheric intraseasonal oscillations. We should note that the ECMWF model has an initial frequency of twice a week on Tuesday and Thursday. Therefore, 160 or 180 initial dates are found for each month during the period of 2001–2020. As the atmospheric variables are auto-correlated, the effective degree of freedom is estimated following Livezey and Chen (1983).</p>
      <?pagebreak page4192?><p id="d1e2484">The continuous ranked probability score (Matheson and Winkler, 1976) is used to evaluate the accuracy of probabilistic forecasts for a given lead time <inline-formula><mml:math id="M73" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>:
            <disp-formula id="Ch1.E15" content-type="numbered"><label>15</label><mml:math id="M74" display="block"><mml:mrow><mml:mi mathvariant="normal">CRPS</mml:mi><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 movablelimits="false">∫</mml:mo><mml:msup><mml:mfenced close="]" open="["><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi>H</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>y</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>o</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mi mathvariant="normal">d</mml:mi><mml:mi>y</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:msup><mml:mi>F</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msup><mml:mo>(</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the cumulative distribution function of the probabilistic forecasts for case <inline-formula><mml:math id="M76" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> at lead time <inline-formula><mml:math id="M77" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:mi>H</mml:mi><mml:mo>(</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the Heaviside step function defined as
            <disp-formula id="Ch1.E16" content-type="numbered"><label>16</label><mml:math id="M79" display="block"><mml:mrow><mml:mi>H</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:mi>y</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>o</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mfenced open="{" close=""><mml:mtable class="array" columnalign="center left"><mml:mtr><mml:mtd><mml:mn mathvariant="normal">0</mml:mn></mml:mtd><mml:mtd><mml:mrow><mml:mi>y</mml:mi><mml:mo>&lt;</mml:mo><mml:msub><mml:mi>o</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mn mathvariant="normal">1</mml:mn></mml:mtd><mml:mtd><mml:mrow><mml:mi>y</mml:mi><mml:mo>≥</mml:mo><mml:msub><mml:mi>o</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:msub><mml:mi>o</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the corresponding observation.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e2711">Correlation coefficient between pentad mean 10–60 d signals of U200 and precipitation over Region 1 (Inland rivers in Xinjiang) in different months. Correlation coefficients that are statistically significant at the 5 % level are shaded.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://hess.copernicus.org/articles/27/4187/2023/hess-27-4187-2023-f02.jpg"/>

        </fig>

      <p id="d1e2720">A CRPS skill score is then calculated by comparing the CRPS of STP-CBaM forecasts to the CRPS of reference forecasts:
            <disp-formula id="Ch1.E17" content-type="numbered"><label>17</label><mml:math id="M81" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">SS</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">REF</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi mathvariant="normal">CRPS</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">REF</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          The reference forecasts are generated using the BJP approach to fit the observations used in the training dataset. When the CRPS skill score is 100 %, the probabilistic forecasts are the same as the observations, whereas a skill score of 0 % indicates that the probabilistic forecasts show similar accuracies compared to the cross-validated climatology. A negative skill score means that the probabilistic forecasts are inferior to the cross-validated climatology.</p>
      <p id="d1e2763">The forecast reliability is evaluated using the <inline-formula><mml:math id="M82" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> index (Renard et al., 2010). The probability integral transform (PIT) values of probabilistic forecasts for each case <inline-formula><mml:math id="M83" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> at lead time <inline-formula><mml:math id="M84" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> are given as
            <disp-formula id="Ch1.E18" content-type="numbered"><label>18</label><mml:math id="M85" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">π</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msup><mml:mi>F</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>o</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:msup><mml:mi>F</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msup><mml:mo>(</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the cumulative distribution function of probabilistic forecasts and <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi>o</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> are the corresponding observations. If the ensemble forecasts are reliable, <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">π</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> should be uniformly distributed. The <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">π</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values are then summarized into an <inline-formula><mml:math id="M90" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> index: <?xmltex \hack{\newpage}?><?xmltex \hack{\vspace*{-6mm}}?>
            <disp-formula id="Ch1.E19" content-type="numbered"><label>19</label><mml:math id="M91" display="block"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">2</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:mfenced open="|" close="|"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">π</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow><mml:mo>*</mml:mo></mml:msubsup><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi>i</mml:mi><mml:mrow><mml:mi>N</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">π</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow><mml:mo>*</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> is the sorted <inline-formula><mml:math id="M93" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">π</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> in increasing order. The <inline-formula><mml:math id="M94" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> index ranges from 0 to 1, and a higher <inline-formula><mml:math id="M95" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> index indicates higher reliability.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e3016">Same as Fig. 2 but for OLRA.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://hess.copernicus.org/articles/27/4187/2023/hess-27-4187-2023-f03.jpg"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Results</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Correlation analysis between atmospheric intraseasonal oscillation and precipitation anomalies</title>
      <p id="d1e3042">Figure 2 presents the correlation between pentad mean 10–60 d signals of U200 and precipitation over Region 1 (Inland rivers in Xinjiang) from May to October. The U200 signals near the Mongolian Plateau have a positive impact on precipitation anomalies over Region 1 in May, while the impact of U200 signals near the eastern Tibetan Plateau is negative. In June and July, the U200 signals in the West Siberian Plain and the Mongolian Plateau show positive correlations with precipitation anomalies. The spatial patterns of correlations between U200 signals and precipitation anomalies are similar in August, September, and October. The U200<?pagebreak page4193?> signals near the Barents Sea and the Iranian Plateau have positive impacts on precipitation anomalies over Region 1. In comparison, U200 signals over the West Siberian Plain show strong negative correlations with precipitation anomalies in these months. The OLRA signals show similar wave patterns to other atmospheric variables (Fig. 3). The spatial patterns of correlations between U850, U200, OLRA, H200, H500, H850, and precipitation anomalies are different for each month as well (Figs. S1–S4 in the Supplement).</p>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Skill of the ECMWF model in forecasting atmospheric intraseasonal oscillations</title>
      <p id="d1e3053">The forecast skill of bridging models is reliant on the forecast skill of atmospheric intraseasonal oscillations derived from dynamical models. The TCC between the ensemble mean of ECMWF-forecasted U200 intraseasonal signals and the observations in May is shown in Fig. 4. The ECMWF model shows high forecast skill in predicting U200 intraseasonal signals when the lead time is within 10 d, and the correlation coefficients are mostly over 0.7 over the globe. Although the forecast skill decreases as the lead time increases, there are still regions where the forecasted U200 signals are significantly correlated with the observations. The forecast skill of the OLRA intraseasonal oscillations is lower than that of the U200 signals (Fig. 5). High forecast skill is mostly observed near the Equator from 30 to 30<inline-formula><mml:math id="M96" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E when the lead time is beyond 10 d. Similar results are also found for U850, H200, H500, and H850, where significant correlations are found mostly near the Equator at longer lead times (Figs. S5 to S8). This suggests that the forecast skill of sub-seasonal precipitation can potentially be improved by taking advantage of both skilful prediction of atmospheric intraseasonal oscillations and stable relationships between precipitation and large-scale circulations, especially for tropical regions.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e3067">Temporal correlation coefficient (TCC) of the ensemble mean of U200 intraseasonal signals derived from the ECMWF model compared to the ERA5 reanalysis data in May. Correlation coefficients that are statistically significant at the 5 % level are shaded.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://hess.copernicus.org/articles/27/4187/2023/hess-27-4187-2023-f04.jpg"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e3078">Same as Fig. 4 but for OLRA.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://hess.copernicus.org/articles/27/4187/2023/hess-27-4187-2023-f05.jpg"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e3090">Spatial distribution of the CRPS skill score of the calibration model, bridging models (U200, U850, OLRA, H200, H500, H850), and merged forecasts (BMA) at different lead times in May. Publisher's remark: please note that the above figure contains disputed territories.</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://hess.copernicus.org/articles/27/4187/2023/hess-27-4187-2023-f06.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS3">
  <label>4.3</label><title>Skill of the calibration model, bridging models, and merged forecasts</title>
      <?pagebreak page4195?><p id="d1e3107">Figure 6 presents the spatial distribution of the CRPS skill score of the calibration model, bridging models, and merged forecasts at different lead times in May. The calibration model shows the highest forecast skill compared to the bridging models at short lead times. The forecast skill of the calibrated forecasts decreases rapidly, and the CRPS skill scores are mostly below 10 % when the lead time is beyond 10 d. The forecast skill of the bridging models is higher than the calibration model in Region 10 (Huai River), Region 14 (Middle Yangtze River), and Region 17 (Southeast rivers) at a lead time of 15 d when OLRA is used as a predictor. The forecast skill of the bridging models is higher in Region 6 (Hai River) and Region 7 (Songhua River) when the OLRA and U200 signals are used separately as predictors at a lead time of 20 d. The merged forecasts take advantage of both the calibration model and the bridging models. Figure 7 shows the boxplots of the CRPS skill scores of the calibration model, bridging models (U200, U850, OLRA, H200, H500, H850), and merged forecasts (BMA) at different lead times in May. The distribution of the CRPS skill score of the merged forecasts is similar to the calibration model at a lead time of 0 d. The minimum CRPS skill score of the merged forecasts is over 20 % in Region 13 (Yangtze River) at a lead time of 5 d, higher than both the calibration model and the bridging models. The bridging models, which use the U200 and OLRA as predictors, show a higher minimum CRPS skill score compared to the calibration model and other bridging models at a lead time of 10–15 d. The distributions of the CRPS skill score of the calibration model, bridging models, and BMA-merged forecasts are similar at longer lead times.</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="d1e3112">Boxplots of the CRPS skill score of the calibration model, bridging models (U200, U850, OLRA, H200, H500, H850), and merged forecasts (BMA) at different lead times in May. The red lines are the 50th percentiles, the top and bottom of each box are the 75th and 25th percentiles, and the whiskers are the maximum and minimum skill scores.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://hess.copernicus.org/articles/27/4187/2023/hess-27-4187-2023-f07.png"/>

        </fig>

      <p id="d1e3121">Figure 8 shows the distribution of model weights at different lead times for Region 1 (Inland rivers in Xinjiang) in May. The weights are rather stable at short lead times, when more than 90 % of the total weights are assigned to the calibration model. Similar results are also found in other regions and months (not shown). The weights of the calibration model decrease rapidly when the lead time is beyond 10 d. More weights are assigned to U200 and OLRA at longer lead times. This is mostly consistent with the distribution of CRPS skill scores shown in Fig. 7. The CRPS skill scores of the U200- and OLRA-based bridging models are higher than the calibration model and other bridging models, especially when the lead time is between 10 and 20 d. This indicates that the U200 and OLRA signals are more useful in predicting sub-seasonal precipitation anomalies compared to other large-scale atmospheric circulation variables.</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="d1e3127">Boxplots showing the distribution of model weights at different lead times in cross-validation for Region 1 (Inland rivers in Xinjiang) in May.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://hess.copernicus.org/articles/27/4187/2023/hess-27-4187-2023-f08.png"/>

        </fig>

      <p id="d1e3136">Figure 9 presents the CRPS skill score of merged forecasts at different lead times from May to October. In general, the forecast skill shows regional, monthly, and lead-time-dependent patterns. The merged forecasts show higher skill in predicting sub-seasonal precipitation anomalies over Region 16 (Pearl River) than other regions. The CRPS skill scores are positive for all months at lead times of 0–20 d. This is mainly due to the higher prediction skill of OLRA in these regions, as shown in Fig. 5. In addition, the merged forecasts show the highest skill in October, when positive skill scores are found over 14 hydroclimatic regions for all lead times except in Region 1 (Inland rivers in Xinjiang), Region 7 (Songhua River), and Region 8 (Liao River). In comparison,<?pagebreak page4196?> positive skill scores are found only over three hydroclimatic regions for all lead times (Region 1, Inland rivers in Xinjiang, Region 13, Yangtze River, and Region 14, Middle Yangtze River) in July.</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="d1e3141">CRPS skill score of merged forecasts at different lead times from May to October.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/27/4187/2023/hess-27-4187-2023-f09.png"/>

        </fig>

      <p id="d1e3150">The <inline-formula><mml:math id="M97" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> indices of merged forecasts at different lead times are shown in Fig. 10. The <inline-formula><mml:math id="M98" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> index is around 0.7 at short lead times, suggesting that the forecasts have a relatively low reliability. The <inline-formula><mml:math id="M99" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> index is over 0.85 when the lead time is beyond 10 d for all hydroclimatic regions and lead times. This indicates that the merged forecasts have a higher reliability at longer lead times. To figure out the relatively low reliability at short lead times, we analyse the merged forecasts over Region 3 (Inland rivers in Inner Mongolia) in May at a lead time of 0 d. The <inline-formula><mml:math id="M100" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> index of the merged forecasts is around 0.6, suggesting that the merged forecasts have a low reliability. We also investigate the model weights of calibrated forecasts and bridging forecasts. The results suggest that the calibrated forecasts are more important than the bridging forecasts, while the cross-validated model weights are over 0.95. This suggests that the low reliability of merged forecasts is mostly caused by the low reliability of calibrated forecasts. Figure S9 presents the quantile ranges of calibrated forecasts and merged forecasts against time. The quantile ranges of both the calibrated forecasts and merged forecasts are small, suggesting that the forecasts are too narrow (too confident).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><?xmltex \currentcnt{10}?><?xmltex \def\figurename{Figure}?><label>Figure 10</label><caption><p id="d1e3183">Same as Fig. 9 but for the <inline-formula><mml:math id="M101" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> index.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/27/4187/2023/hess-27-4187-2023-f10.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Discussion</title>
<sec id="Ch1.S5.SS1">
  <label>5.1</label><title>Discussion of forecast skill</title>
      <p id="d1e3215">Though the STP-CBaM model displays a good ability to generate skilful and reliable sub-seasonal precipitation forecasts over China, the forecast skill shows great diversity in different regions, months, and lead times. The calibration model shows the highest forecast skill compared to the bridging models for all regions and all months when the lead time is within 5 d (Figs. S10–S14). The U200- and OLRA-based bridging models outperform the calibration model and the other bridging models when the lead time is beyond 10 d in certain months and in certain regions. This may be explained by the strong relationship between U200, OLRA, and<?pagebreak page4197?> precipitation anomalies and the forecast skill of U200 and OLRA in the ECMWF model in these regions (Figs. S5–S8).</p>
      <p id="d1e3218">However, we also note that there are several regions where the forecast skill of the calibration model is higher than the bridging models at longer lead times. This may be caused by the auto-correlations of the sub-seasonal precipitation anomalies defined in this study. In our data processing section, the observed anomalies before the forecast initial date are used to make enough data for the running mean. Thus, the predictand is not purely based on the ECMWF raw forecasts. The observational data are also introduced. The preceding observed precipitation anomalies may provide useful forecast information when the auto-correlations are high.</p>
      <p id="d1e3221">In addition, the limited forecast skill of large-scale circulations at mid to high latitudes in dynamical models may contribute to the limited forecast skill of bridging models as well. To figure out the potential skill of the STP-CBaM method in predicting sub-seasonal precipitation anomalies, we use the <inline-formula><mml:math id="M102" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>th 10–60 d signal of the atmospheric field derived from the ERA5 reanalysis dataset as a predictor for the bridging model instead of the atmospheric field derived from the ECMWF model. Thus, the potential forecast skill is based on ERA5 reanalysis data, while the practical forecast skill is based on the ECMWF model. Figure 11 compares the potential CRPS skill score (based on the ERA5 reanalysis) and the practical CRPS skill score (based on the ECMWF model) of merged forecasts over China. The potential CRPS skill scores are similar to the practical CRPS skill scores as the precipitation forecasts derived from the ECMWF model have a high accuracy at short lead times. The potential CRPS skill scores are much higher than the practical CRPS skill scores at longer lead times. This indicates that the forecast skill will be greatly improved when the atmospheric field is well predicted in the GCMs.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><?xmltex \currentcnt{11}?><?xmltex \def\figurename{Figure}?><label>Figure 11</label><caption><p id="d1e3234">Practical CRPS skill score of merged forecasts based on the ECMWF model (solid) and potential CRPS skill score based on ERA5 reanalysis (hatched). The red lines are the 50th percentiles, the top and bottom of each box are the 75th and 25th percentiles, and the whiskers are the maximum and minimum skill scores.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://hess.copernicus.org/articles/27/4187/2023/hess-27-4187-2023-f11.png"/>

        </fig>

      <p id="d1e3243">We also note that the weights do not always match the skill patterns. In this study, the posterior distributions of model weights are assigned by a model's predictive ability rather than fitting ability. Indeed, there is much literature in support of using predictive performance measures for model choice and combination based on the idea that a model is only as good as its predictions (Stock and Watson, 2006; Eklund and Karlsson, 2007). Thus, the CRPS skill score is not used when inferring model weights. This may lead to the discrepancy<?pagebreak page4198?> between the model weights and the forecast skill score, especially when none of the models shows high predictive skill.</p>
</sec>
<sec id="Ch1.S5.SS2">
  <label>5.2</label><title>Limitations and future work</title>
      <p id="d1e3254">In this study, we aim at investigating the capability of dynamical models to improve the forecast skill of sub-seasonal precipitation anomalies using large-scale circulations as predictors. The bridging models are built based on the concurrent relationships between atmospheric intraseasonal oscillations and precipitation anomalies. Thus, the forecast skill of bridging models is highly reliant on the forecast skill of atmospheric intraseasonal oscillations derived from dynamical<?pagebreak page4199?> models. In the future, the lagged relationships between atmospheric intraseasonal oscillations and precipitation anomalies will be considered to further improve sub-seasonal precipitation forecast skill. Although the forecast skill of the calibration model is high at short lead times, the results also suggest that the calibrated forecasts are too narrow (too confident). We would like to focus on improving the forecast reliability, especially at short lead times, in the future.</p>
      <p id="d1e3257">Meanwhile, we define the predictors using the STPM for each month and each hydroclimatic region. Intraseasonal climate indices, such as the MJO index and the BSISO index, have not been considered yet. Recently, Zhu et al. (2023)<?pagebreak page4200?> proposed two sets of novel indices based on the compound zonal displacements of the South Asia high (SAH) and the western Pacific sub-tropical high (WPH) to monitor and predict the intraseasonal variation of Meiyu. These climate indices will be introduced in the bridging models to investigate the potential improvement of the forecast skill.</p>
      <p id="d1e3260">In addition, we mainly focus on the prediction of intraseasonal (10–60 d) precipitation anomalies in this study. However, previous studies suggested that the intraseasonal component may only account for 7 % of the total variability in north-eastern China, while the seasonal component accounted for nearly 70 %. Thus, the relationships between seasonal precipitation anomalies and large-scale circulation patterns should also be investigated in these regions in the future.</p>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Conclusions</title>
      <p id="d1e3272">In this study, we develop a STP-CBaM method to improve probabilistic sub-seasonal precipitation forecast skill over 17 hydroclimatic regions in China. The STP-CBaM method takes advantage of both dynamical models and statistical models. The calibration model is built by calibrating pentad mean precipitation anomalies derived from the ECMWF model. Bridging models are built by defining potential predictors using the spatial–temporal projection method (STPM). The calibration model and bridging models are merged through the Bayesian modelling averaging (BMA) method. Our results suggest that the forecast skill of the calibration model is higher compared to the bridging models when the lead time is within 5–10 d. The U200- and OLRA-based bridging models outperform the calibration model when the lead time is beyond 10 d in certain months and certain regions. The BMA-merged forecasts take advantage of both the calibration model and the bridging models. The BMA weights are rather stable at short lead times, where over 90 % of the total weights are assigned to the calibration model. More weights are assigned to the U200- and OLRA-based bridging models when the lead time is beyond 10 d. The results of the <inline-formula><mml:math id="M103" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> index suggest that BMA-merged forecasts are reliable at longer lead times. Some improvements to reliability are still needed at shorter lead times.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e3286">The ERA5 dataset can be sourced from <uri>https://cds.climate.copernicus.eu/</uri> (Copernicus Climate Change Service, 2022), and the precipitation dataset is derived from<?pagebreak page4201?> <uri>http://www.gloh2o.org/mswep/</uri> (GloH20, 2023). The OLR dataset can be sourced from <uri>https://psl.noaa.gov/thredds/catalog/Datasets/olrcdr/catalog.html</uri> (NOAA, 2023). The ECMWF hindcast data can be retrieved from the S2S database at <uri>http://apps.ecmwf.int/datasets/data/s2s/</uri> (ECMWF, 2023).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e3301">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/hess-27-4187-2023-supplement" xlink:title="pdf">https://doi.org/10.5194/hess-27-4187-2023-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e3310">YL: conceptualization, methodology, writing (original draft preparation, review and editing). KX: methodology, writing (review and editing). ZW: conceptualization, funding acquisition, supervision, writing (review and editing). ZZ: conceptualization, review and editing. QJW: conceptualization, supervision, writing (review and editing).</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e3316">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e3322">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims made in the text, published maps, institutional affiliations, or any other geographical representation in this paper. While Copernicus Publications makes every effort to include appropriate place names, the final responsibility lies with the authors.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e3329">We would like to thank the two anonymous reviewers for their reviews of early versions of this paper.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e3334">This research has been supported by the National Natural Science Foundation of China (grant nos. 52009027, U2240225, and 42088101).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e3340">This paper was edited by Louise Slater and reviewed by two anonymous referees.</p>
  </notes><ref-list>
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