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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-21-5415-2017</article-id><title-group><article-title>Impact of ENSO regimes on developing- and decaying-phase precipitation during rainy season in China</article-title>
      </title-group><?xmltex \runningtitle{Impact of ENSO regimes on developing- and decaying-phase precipitation}?><?xmltex \runningauthor{Q.~Cao et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Cao</surname><given-names>Qing</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Hao</surname><given-names>Zhenchun</given-names></name>
          <email>zhenchunhao@163.com</email>
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Yuan</surname><given-names>Feifei</given-names></name>
          <email>ffei.yuan@gmail.com</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Su</surname><given-names>Zhenkuan</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-4426-8992</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Berndtsson</surname><given-names>Ronny</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Hao</surname><given-names>Jie</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Nyima</surname><given-names>Tsring</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>State Key Laboratory of Hydrology Water Resources and Hydraulic Engineering, Hohai University, Nanjing, 210098, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>National Cooperative Innovation Center for Water Safety &amp; Hydro-Science, Hohai University, Nanjing, 210098, China</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Water Resources Engineering and Center for Middle Eastern Studies, Lund University, P.O. Box 118, <?xmltex \hack{\newline}?> Lund, 22100, Sweden</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Nanjing Hydraulic Research Institute, Nanjing, 210098, China</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Investigation Bureau of Hydrology and Water Resources, Ali, Tibet Autonomous Region, 859000, China</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Zhenchun Hao (zhenchunhao@163.com) and Feifei Yuan (ffei.yuan@gmail.com)</corresp></author-notes><pub-date><day>6</day><month>November</month><year>2017</year></pub-date>
      
      <volume>21</volume>
      <issue>11</issue>
      <fpage>5415</fpage><lpage>5426</lpage>
      <history>
        <date date-type="received"><day>6</day><month>March</month><year>2017</year></date>
           <date date-type="rev-request"><day>4</day><month>April</month><year>2017</year></date>
           <date date-type="rev-recd"><day>20</day><month>September</month><year>2017</year></date>
           <date date-type="accepted"><day>25</day><month>September</month><year>2017</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://hess.copernicus.org/articles/21/5415/2017/hess-21-5415-2017.html">This article is available from https://hess.copernicus.org/articles/21/5415/2017/hess-21-5415-2017.html</self-uri>
<self-uri xlink:href="https://hess.copernicus.org/articles/21/5415/2017/hess-21-5415-2017.pdf">The full text article is available as a PDF file from https://hess.copernicus.org/articles/21/5415/2017/hess-21-5415-2017.pdf</self-uri>


      <abstract>
    <p>This study investigated the influence of five El Niño–Southern
Oscillation (ENSO) types on rainy-season precipitation in China: central Pacific warming (CPW), eastern
Pacific cooling (EPC), eastern Pacific warming (EPW), conventional ENSO and
ENSO Modoki. The multi-scale moving
<inline-formula><mml:math id="M1" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> test was applied to determine the onset and withdrawal of rainy season.
Results showed that the precipitation anomaly can reach up to 30 <inline-formula><mml:math id="M2" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula> above
average precipitation during decaying CPW and EPW phases. Developing EPW
could cause decreasing precipitation over large areas in China with 10–30 <inline-formula><mml:math id="M3" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula>
lower than average precipitation in most areas. Conventional El Niño in
the developing phase had the largest influence on ENSO-related precipitation
among developing ENSO and ENSO Modoki regimes. Decaying ENSO also showed a
larger effect on precipitation anomalies, compared to decaying ENSO Modoki.
The difference between rainy-season precipitation under various ENSO regimes
may be attributed to the combined influence of anti-cyclone in the western
North Pacific and the Indian monsoon. Stronger monsoon and anti-cyclone are
associated with enhanced rainy-season precipitation. The results suggest a
certain predictability of rainy-season precipitation related to ENSO regimes.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

      <?xmltex \hack{\newpage}?>
<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>El Niño–Southern Oscillation (ENSO) is one of the most important factors
affecting precipitation, which has been achieved urgent attention worldwide
(Li et al., 2016; Wang et al., 2006; Preethi et al., 2015; Yuan et al.,
2016a, b; Zaroug et al., 2014; Brigode et al., 2013). Many
researchers have studied various aspects of precipitation, such as seasonal
precipitation and extreme precipitation (Jiang et al.,
2016, 2013). Rainy season characteristics (e.g., onset,
withdrawal and precipitation of rainy season), however, are less considered,
which are of immense significance to rain-fed agriculture in many countries
like China. Reliable prediction of onset and withdrawal of rainy season will
assist on-time preparation of farmlands and is significant to ecosystems
(Omotosho et al., 2000; Marteau et al., 2011). In addition, rainy season
is a period when it is easier for flooding, and rainy-season precipitation
could provide certain predictability of flood occurrence. China is an
ENSO-sensitive country and prone to flood and drought occurrence (Q. Zhang
et al., 2016; W. Zhang et al., 2014; Feng et al., 2011, 2010; Wang and Wang, 2013; Feng and Li, 2011). Thus, it is significant to investigate
rainy-season precipitation under ENSO regimes. Cai (2003) observed
similar inter-decadal oscillation and abrupt variations between rainfall of
rainy season in Fujian and Niño 3 SST. Lu (2005) pointed out that
rainfall in the rainy season in northern China is related to sea surface
temperature anomalies (SSTA) in the equatorial eastern Pacific and negative
(positive) SSTA could trigger heavier (lighter) rainy-season precipitation.
However, such studies mainly concentrated on regional scales and single ENSO
mode, rather than on continental scale and various ENSO regimes, which is
important for overall understanding of relationship between ENSO and Chinese
rainy-season precipitation. In order to decipher this, it is necessary to
explore the spatial pattern of precipitation during the rainy season under
various ENSO regimes at the continental scale in China.</p>
      <p>Different types of ENSO regimes have been demonstrated based on the Pacific
spatial pattern SSTA (Kao and Yu, 2009; Larkin and Harrison, 2005; Ashok et
al., 2007; Trenberth, 1997; Tedeschi et al., 2013; Kim et al., 2009).
Conventional ENSO episodes, including El Niño (EN) and La Niña (LN),
are defined based on SST anomalies in the Niño 3.4 region, and El
Niño is mainly characterized by eastern Pacific warming in the cold tongue
of the eastern Pacific Ocean (Kim et al., 2009). Several researchers have
identified different episodes of SST in the Pacific, such as the central
Pacific warming and eastern Pacific cooling (Larkin and Harrison, 2005; Weng
et al., 2007; Kao and Yu, 2009). Kim et al. (2009) divided ENSO into
three types, i.e., central Pacific warming (CPW), eastern Pacific cooling
(EPC) and eastern Pacific warming (EPW). The division of ENSO is also based
on SSTA in Niño 3, Niño 3.4 and Niño 4 regions. Ashok
et al. (2007) introduced a new type of ENSO event, ENSO Modoki, which is
different from conventional ENSO. ENSO Modoki is characterized by positive
SSTA in the central Pacific, bounded by negative SSTA in the western and
eastern Pacific.</p>
      <p>ENSO and ENSO Modoki have different influences on precipitation (Ashok et
al., 2007, 2009; Weng et al., 2007; Taschetto and England, 2009).
Q. Zhang et al. (2016) pointed out that CPW, EPC and EPW regimes
showed various performance on seasonal precipitation over the Huaihe
River
basin. Precipitation below average usually occurs in southern China in ENSO
Modoki years, whereas the conventional ENSO tends to imply precipitation
above average (W. Zhang et al., 2014). In contrast, enhanced
precipitation over the Huaihe River basin often occurs during decaying El Niño
Modoki events in summer, whilst reduced precipitation signals are
found in the corresponding season in the decaying year of El Niño
(Feng et al., 2011). It can be seen that the influence of ENSO
regimes on precipitation varies among locations in China. The National
Climate Center (NCC) succeeded in predicting the severe flood over the
Yangtze River basin in the typical El Niño year of 1997–1998.
Nonetheless, NCC failed to predict the enhanced precipitation in the Huaihe River basin in 2002–2003, since it was an El Niño Modoki year rather
than a conventional El Niño. This highlights the significance of correct
distinguishing between ENSO and ENSO Modoki.</p>
      <p>Different performance of precipitation under various ENSO regimes is
associated with atmospheric circulation and monsoon (Tedeschi et al.,
2013; Feng et al., 2010; Cai et al., 2010; Black et al., 2003; Chang et al.,
2001; R. Zhang et al., 2014; Onyutha and Willems, 2015). Wu et al. (2003)
explained the physical mechanism of links between precipitation and
SSTs through features of atmospheric circulation. Wang et al. (2004)
pointed out that the local onset of rainy season in the South China Sea is
related to mean summer monsoon onset. Cai et al. (2010) argued that a
rainfall reduction in South East Queensland in Australia is related to an
eastward shift in the Walker circulation. Feng et al. (2011)
pointed out that China rainfall anomalies were mainly due to anomalous
anti-cyclonic flow in the western North Pacific associated with El Niño
Modoki and El Niño events. Gerlitz et al. (2016) argued that
ENSO-induced precipitation variability in tropical regions is directly
associated with the atmospheric circulation. The atmospheric circulation and
monsoon have different influences on two types of ENSO (Feng and Li,
2013; Zhang et al., 2011; Zhou and Chan, 2007). As a consequence, the
investigation of atmospheric circulation and monsoon is used to explain
different performance of rainy-season precipitation anomalies under various
ENSO regimes in this study.</p>
      <p>850 <inline-formula><mml:math id="M4" display="inline"><mml:mi mathvariant="normal">mbar</mml:mi></mml:math></inline-formula>
wind variability is associated with SSTA in the equatorial Pacific
and precipitation anomalies in China (Zhang et al., 1999; Zhou and Chan,
2007; Wang et al., 2004; W. Zhang et al., 2016). Fan et al. (2013)
pointed out that 850 <inline-formula><mml:math id="M5" display="inline"><mml:mi mathvariant="normal">mbar</mml:mi></mml:math></inline-formula> vector winds are related to the moisture
transportation from western tropical Pacific to the subtropical region,
which determines the precipitation over the Yangtze–Huai river valley
region. Huang et al. (2004) and R. Zhang et al. (2014) presented
the atmospheric circulation and monsoon variability by the composite
distribution of wind anomalies at 850 <inline-formula><mml:math id="M6" display="inline"><mml:mi mathvariant="normal">mbar</mml:mi></mml:math></inline-formula> in different phases of El Niño
and La Niña to explain precipitation variation in China. Feng
et al. (2011) compared the difference of 850 <inline-formula><mml:math id="M7" display="inline"><mml:mi mathvariant="normal">mbar</mml:mi></mml:math></inline-formula> wind anomalies in decaying
ENSO and ENSO Modoki phases to explain the physical mechanism of seasonal
precipitation variation in China. Hence, 850 <inline-formula><mml:math id="M8" display="inline"><mml:mi mathvariant="normal">mbar</mml:mi></mml:math></inline-formula> vector winds reflecting
atmospheric circulation and monsoon variability are used to explore the
underlying causes of precipitation anomalies in this study.</p>
      <p>The influence of ENSO and ENSO Modoki regimes on Chinese precipitation has
been studied intensively. However, research has been limited to the
comparison of impacts of developing (decaying) ENSO and ENSO Modoki on
precipitation at the regional scale in China. Therefore, this study aims to
improve our understanding of ENSO-induced precipitation during rainy season
and to explore the effect of five important ENSO types (i.e., CPW, EPC, EPW,
ENSO and ENSO Modoki) in the developing and decaying phase on the
continental-scale precipitation. The multi-scale moving <inline-formula><mml:math id="M9" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> test method was
applied to determine the onset and withdrawal of the rainy season. The
underlying causes of the spatial patterns of rainy-season precipitation were
analyzed by the variability of atmospheric circulation in the western North
Pacific (WNP) together with monsoon.</p>
</sec>
<sec id="Ch1.S2">
  <title>Study area and data</title>
      <p>China, located in middle latitude in eastern Asia (18–54<inline-formula><mml:math id="M10" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 73–135<inline-formula><mml:math id="M11" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E), is the most
populous country in the world (Fig. 1), with a population of
over 1.381 billion and an area of approximately 9.6 million <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>. China
is mainly dominated by monsoon climate and mountain plateau climate, which
lead to pronounced rainfall differences among different seasons and regions.</p>
      <p>Daily precipitation data from 1960 to 2015 at 536 observation stations in
China were selected for this study  (Ren et al., 2012). The data were obtained from China
Meteorological Data Sharing Service System, and the data quality has been
regularly checked. The locations of the observation stations are shown in
Fig. 1. The stations are distributed unevenly, with fewer stations in the
northwestern part of China. Hence, we applied Kriging interpolation to
induce a resolution of <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">0.2</mml:mn><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">0.2</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>.</p>
      <p>The dataset of National Oceanic and Atmospheric Administration (NOAA)
extended reconstructed SST was used to identify different types of
conventional ENSO (Huang et al., 2015). ENSO Modoki index (EMI) was obtained from the Japan
Agency for Marine Science and Technology. In addition, the National Centers
for Environmental Prediction (NCEP)/National Centers for Atmospheric
Research (NCAR) reanalysis data were used to investigate underlying causes
of the spatial pattern of precipitation under different ENSO regimes
(Kalnay et al., 1996).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p>The spatial distribution of precipitation
stations used in this study.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://hess.copernicus.org/articles/21/5415/2017/hess-21-5415-2017-f01.png"/>

      </fig>

</sec>
<sec id="Ch1.S3">
  <title>Methodology</title>
<sec id="Ch1.S3.SS1">
  <title>Determination of rainy season</title>
      <p>The onset and withdrawal of rainy season was determined by the multi-scale
moving <inline-formula><mml:math id="M14" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> test method. This method is characterized by the detection of
mutation points between two subsamples with equal size <inline-formula><mml:math id="M15" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>, where <inline-formula><mml:math id="M16" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> is the
length of the subsample (<inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula>, 31, …, 182/183; 182/183
corresponds to half the value of length of 1 year 365/366). Theoretically,
the length of subsamples in this study ranged between 1 and 182/183.
However, as the onset or withdrawal of the rainy season, it will not be
considered if the length of the subsample is one day or just several days
when the abruption point is prominent. As a result, the length of the
subsample is limited between 30 and 182/183. The determination of the
mutation point can be described as (Fraedrich et al., 1997)
            <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M18" display="block"><mml:mrow><mml:mi>t</mml:mi><mml:mfenced open="(" close=")"><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mfenced><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo><mml:msup><mml:mi>n</mml:mi><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mo>(</mml:mo><mml:msubsup><mml:mi>s</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>s</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> defined as

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M21" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E2"><mml:mtd/><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mi>i</mml:mi><mml:mo>-</mml:mo><mml:mi>n</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:munderover><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:mi>n</mml:mi></mml:mfrac></mml:mstyle><mml:mo>;</mml:mo><mml:msubsup><mml:mi>s</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mi>i</mml:mi><mml:mo>-</mml:mo><mml:mi>n</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:munderover><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>/</mml:mo><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E3"><mml:mtd/><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mo>+</mml:mo><mml:mi>n</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:munderover><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:mi>n</mml:mi></mml:mfrac></mml:mstyle><mml:mo>;</mml:mo><mml:msubsup><mml:mi>s</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mo>+</mml:mo><mml:mi>n</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:munderover><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msub><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>/</mml:mo><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            and <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is daily precipitation for Julian day <inline-formula><mml:math id="M23" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> within 1 year and for
one station. <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mrow><mml:mi>i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> are the mean values of the
subsamples before and after the Julian day <inline-formula><mml:math id="M26" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>, respectively.</p>
      <p>The <inline-formula><mml:math id="M27" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> value calculated above was normalized by the 0.01 test value shown
in Eq. (4), which is equal to the result of Mann–Kendall test at 0.05
significance level.
            <disp-formula id="Ch1.E4" content-type="numbered"><mml:math id="M28" display="block"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mfenced><mml:mo>=</mml:mo><mml:mi>t</mml:mi><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mi>i</mml:mi><mml:mo>)</mml:mo><mml:mo>/</mml:mo><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0.01</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mfenced></mml:mrow></mml:math></inline-formula> can be taken as the
threshold to detect mutations. <inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mfenced><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula> represents an increasing trend while <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mfenced><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula> is a decreasing trend. The onset of
rainy season in this study was defined as the mutation point corresponding
to a maximum <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mfenced></mml:mrow></mml:math></inline-formula> value. For this case,
precipitation changes from a smaller to a higher value. Likewise, the
withdrawal is defined as the changing point corresponding to a minimum
<inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mfenced></mml:mrow></mml:math></inline-formula> value.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Classification of ENSO and ENSO Modoki regimes</title>
      <p>Three types of ENSO were classified based on the definition proposed by
Kim et al. (2009). The years dominated by CPW, EPC and EPW are listed
in Table 1.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p>Years dominated by CPW, EPC and EPW regimes
during 1960–2015.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="150pt"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">EPW</oasis:entry>  
         <oasis:entry colname="col2">EPC</oasis:entry>  
         <oasis:entry colname="col3">CPW</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">1965, 1972, 1976, 1982, 1987, 1997, 2015</oasis:entry>  
         <oasis:entry colname="col2">1964, 1970, 1973, 1975, 1988, 1998, 1999, 2007, 2010, 2011</oasis:entry>  
         <oasis:entry colname="col3">1963, 1969, 1991, 1994, 2002, 2004, 2009</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p>Spatial pattern for rainy-season precipitation
anomaly (PARS) during the CPW (first row), EPC (second row) and EPW (third
row) episodes in the phase of ENSO developing year (0) and decaying year
(1). The sign “0” in the parentheses denotes ENSO developing year and
“1” denotes decaying year.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/21/5415/2017/hess-21-5415-2017-f02.png"/>

        </fig>

      <p>The definition of ENSO Modoki and conventional ENSO was demonstrated.
Specifically, warm (cold) episodes of ENSO Modoki, abbreviated as MEN (MLN),
were defined as EMI above (below) 0.7 SD (<inline-formula><mml:math id="M34" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.7 SD), where SD is the standard
deviation (Ashok et al., 2007). <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mtext>EMI</mml:mtext><mml:mo>=</mml:mo><mml:mfenced close="]" open="["><mml:mtext>SSTA</mml:mtext></mml:mfenced><mml:mtext>A</mml:mtext><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn><mml:mo>×</mml:mo><mml:mfenced open="[" close="]"><mml:mtext>SSTA</mml:mtext></mml:mfenced><mml:mtext>B</mml:mtext><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn><mml:mo>×</mml:mo><mml:mfenced open="[" close="]"><mml:mtext>SSTA</mml:mtext></mml:mfenced><mml:mtext>C</mml:mtext></mml:mrow></mml:math></inline-formula>, where [SSTA]A, [SSTA]B, [SSTA]C
represents the SSTA in region A (10<inline-formula><mml:math id="M36" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S–10<inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 165<inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E–140<inline-formula><mml:math id="M39" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W),
region B (15<inline-formula><mml:math id="M40" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S–5<inline-formula><mml:math id="M41" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 110<inline-formula><mml:math id="M42" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–70<inline-formula><mml:math id="M43" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W) and
region C (10<inline-formula><mml:math id="M44" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S–20<inline-formula><mml:math id="M45" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 125<inline-formula><mml:math id="M46" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E–145<inline-formula><mml:math id="M47" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E), respectively.
Likewise, the conventional EN (LN), abbreviated as CEN (CLN), was defined as
SSTA above (below) 0.7 SD (<inline-formula><mml:math id="M48" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.7 SD) in the area of
5<inline-formula><mml:math id="M49" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N–5<inline-formula><mml:math id="M50" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, 90<inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–140<inline-formula><mml:math id="M52" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W
(Tedeschi et al., 2013). This definition gives an opportunity
to judge the ENSO type of the rainy season rather than the whole year, which
is greater than definition proposed by Trenberth (1997).</p>
</sec>
<sec id="Ch1.S3.SS3">
  <title>Precipitation anomaly index during rainy season (PARS)</title>
      <p>Precipitation anomaly can present the difference of precipitation between
ENSO years and normal years and demonstrate the influence of ENSO regimes on
precipitation more directly. Q. Zhang et al. (2013) used precipitation
anomaly index to explore the effect of ENSO on precipitation in the East
River basin, southern China. Q. Zhang et al. (2016) investigated the
influence of ENSO and ENSO Modoki on seasonal precipitation over the Huaihe River basin by using precipitation anomaly index. Precipitation anomaly
index is defined as
            <disp-formula id="Ch1.E5" content-type="numbered"><mml:math id="M53" display="block"><mml:mrow><mml:msub><mml:mtext>PARS</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mtext>PRS</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mover accent="true"><mml:mrow><mml:msub><mml:mtext>PRSN</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mfenced><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">%</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msub><mml:mtext>PARS</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> denotes precipitation anomaly during rainy season at <inline-formula><mml:math id="M55" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>th
station in <inline-formula><mml:math id="M56" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>th year; <inline-formula><mml:math id="M57" display="inline"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mtext>PRS</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> denotes mean daily precipitation
during rainy season at <inline-formula><mml:math id="M58" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>th station in <inline-formula><mml:math id="M59" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>th year, and
<inline-formula><mml:math id="M60" display="inline"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mtext>PRSN</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> denotes mean daily precipitation during rainy season at <inline-formula><mml:math id="M61" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>th
station in <inline-formula><mml:math id="M62" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>th normal year. The normal year refers to a year without ENSO
event occurring.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p>Spatial pattern of precipitation anomalies during
rainy season (PARS) during developing (0) conventional ENSO and ENSO Modoki
events.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/21/5415/2017/hess-21-5415-2017-f03.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4">
  <title>Results and discussion</title>
<sec id="Ch1.S4.SS1">
  <title>Precipitation anomaly during rainy season (PARS) influenced by CPW,
EPC and EPW regimes</title>
      <p>The spatial variability of PARS under CPW, EPC and EPW regimes in the phase
of developing and decaying years is presented in Fig. 2. The distribution of
precipitation anomaly is irregular over the whole area in the developing
phase of CPW. The coastal regions in southeastern China that had the largest
amount of rainy-season precipitation presented the largest decreasing trend,
with the precipitation anomaly reaching 30 <inline-formula><mml:math id="M63" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula> below average precipitation.
The upper and middle reaches of the Yangtze River and the Yellow River
showed decreasing precipitation, whereas the lower reaches had the opposite
trend. The decaying CPW regime had a relatively regular spatial pattern. More
specifically, most parts of China presented increasing precipitation during
rainy season, with the largest PARS being 20 <inline-formula><mml:math id="M64" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula> above average
precipitation. The distribution of PARS influenced by the decaying CPW is
similar to that by the developing EPC, with shrinking extent of enhanced
precipitation in central China for developing EPC. The distribution of PARS
is similar as well in the two phases of EPC (Fig. 2, second row), with
precipitation above average in northwestern China and precipitation below
average in northeastern China. The difference between the two phases lies in
the increasing (decreasing) precipitation in southeastern China in the
developing (decaying) phase. Nonetheless, developing and decaying EPW
(Fig. 2, third row) showed opposite spatial precipitation pattern. Most parts
of China presented dry signals in the phase of developing EPW, which became
stronger northwards, and more than 30 <inline-formula><mml:math id="M65" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula> below average precipitation can be
identified in northern China. However, there is above average precipitation in
most regions of China in the case of decaying EPW, with PARS values ranging
between 0 and 30 <inline-formula><mml:math id="M66" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula>. In summary, the CPW decaying phase (EPC developing
phase) deserves more attention than the developing (decaying) phase, since
it shows more prominent wet signals. Both phases are significant for the EPW
regimes, due to the obvious dry (wet) signals shown in the developing
(decaying) phase.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><caption><p>Spatial pattern of precipitation anomalies during
rainy season (PARS) for decaying (1) conventional ENSO and ENSO Modoki
events.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/21/5415/2017/hess-21-5415-2017-f04.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS2">
  <title>Precipitation anomaly during rainy season (PARS) impacted by ENSO
and ENSO Modoki regime </title>
      <p>Figures 3 and 4 present precipitation anomalies during rainy season (PARS)
for warm and cold episodes of conventional ENSO and ENSO Modoki in a
developing phase and a decaying phase, respectively. Precipitation
increased in a band stretching from northwestern China to the coastal region
in the southeast, with the largest precipitation anomaly (40 <inline-formula><mml:math id="M67" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula>) occurring
in southeastern China under a developing CEN regime (Fig. 3a). The dry condition
is more severe northwards in central China, with PARS equal to about <inline-formula><mml:math id="M68" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>30 <inline-formula><mml:math id="M69" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula>
in the northern parts of central China. W. Zhang et al. (2016)
concluded that strong El Niño events are associated with summer monsoon
flooding over the Yangtze River, which is consistent with our results. The
distribution of rainy-season precipitation for developing El Niño is
also in agreement with the research by Zhang et al. (2011).
Northern China had an opposite PARS pattern for developing El Niño Modoki,
in comparison to developing CEN (Fig. 3b). Nonetheless, the two phases showed
similar precipitation distribution, with reduced precipitation in central
China (approximately <inline-formula><mml:math id="M70" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10 <inline-formula><mml:math id="M71" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula>) and enhanced precipitation in southern China.
Typically, developing CEN demonstrated more obvious wet or dry signals
compared to MEN. Moreover, the wet and dry condition for developing CEN is
the most serious among all ENSO and ENSO Modoki regimes in both developing
and decaying phases, with the largest precipitation anomaly reaching 50 <inline-formula><mml:math id="M72" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula>
above average precipitation amount and lowest 30 <inline-formula><mml:math id="M73" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula> below. This means that
developing CEN should be paid urgent attention to for flooding and drought
monitoring. The spatial pattern of PARS for developing CLN presented similar
signals with developing MEN, with a shorter wet precipitation band in
northern China for developing CLN (Fig. 3c). The increased precipitation was
shifted westwards for the developing MLN, compared to cold episodes of
conventional ENSO (Fig. 3d). ENSO and ENSO Modoki regimes in the developing
phase presented various distribution of precipitation anomalies. Wet or dry
signals are more easily shown for the warm episodes of conventional ENSO, in
comparison to the other three regimes. Similar patterns of PARS for
developing CLN and MEN should be further studied.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p>Composites of 850 <inline-formula><mml:math id="M74" display="inline"><mml:mi mathvariant="normal">mbar</mml:mi></mml:math></inline-formula>
vector wind for mainland
China during CPW, EPC and EPW developing (0) and decaying (1) phases. Arrows
show the direction of wind (<inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>); grey shaded areas denote wind speed above
3 <inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/21/5415/2017/hess-21-5415-2017-f05.png"/>

        </fig>

      <p>Decaying ENSO and ENSO Modoki years showed different features of PARS
(Fig. 4). Most parts of China presented increasing precipitation for decaying
CEN, with more than 30 <inline-formula><mml:math id="M77" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula> above average precipitation identified in
northern
China (Fig. 4a). The decaying phase of MEN (Fig. 4b) presented shrinking
extent of enhanced precipitation, which was condensed in the central parts
of China, ranging between 0 and 10 <inline-formula><mml:math id="M78" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula>. The result is consistent with
conclusions from Feng et al. (2011), who found obvious rainfall
anomalies in southern China for decaying El Niño and no prominent
rainfall variations in the corresponding phase of El Niño Modoki. In
terms of the cold episodes of ENSO (Fig. 4c), approximately 95 <inline-formula><mml:math id="M79" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula> of China
showed dry signals, and the condition was more serious eastwards, being
30 <inline-formula><mml:math id="M80" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula> below average precipitation amount. We can see that the spatial
pattern of PARS for the decaying CLN is opposite to that of CEN. Decaying
MLN (Fig. 4d) showed a larger extent of enhanced precipitation in a band
stretching from western China to parts of the Yellow River basin, in
comparison to CLN. In conclusion, the decaying phases of conventional ENSO
showed more obvious wet or dry signals compared to ENSO Modoki, with most
parts of China displaying increasing (decreasing) precipitation for the CEN
(CLN).</p>
      <p>This study analyzed spatial patterns of precipitation under different ENSO
regimes, since ENSO is the leading driver of precipitation anomaly in China
(Xiao et al., 2015). Xu et al. (2016) revealed that
increasing autumn precipitation in southern China is due to the combined
ENSO and Indian Ocean Dipole (IOD) events. Other researchers also concluded
that IOD and ENSO have mutual impact on precipitation anomalies in China
(Weng et al., 2011; Liu et al., 2009; Wu et al., 2012). Moreover, Pacific
Decadal Oscillation, subtropical high, also influences the distribution of
Chinese precipitation (Chan, 2005; Wang et al., 2008; Chang et al.,
2000; Niu and Li, 2008; Ouyang et al., 2014). As a result, the spatial
patterns of PARS under ENSO regimes may be determined not only by ENSO but
also by the combination of various drivers, which ought to be studied
further.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p>Composites of 850 <inline-formula><mml:math id="M81" display="inline"><mml:mi mathvariant="normal">mbar</mml:mi></mml:math></inline-formula> vector wind for mainland
China during ENSO and ENSO Modoki developing (0) phases. Arrows show the
direction of wind (<inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>); grey shaded areas denote wind speed above 3 <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/21/5415/2017/hess-21-5415-2017-f06.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><caption><p>Composites of 850 <inline-formula><mml:math id="M84" display="inline"><mml:mi mathvariant="normal">mbar</mml:mi></mml:math></inline-formula> vector wind for mainland
China during ENSO and ENSO Modoki decaying (1) phases. Arrows show the
direction of wind (<inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>); grey shaded areas denote wind speed above 3 <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/21/5415/2017/hess-21-5415-2017-f07.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS3">
  <title>Composites of circulation</title>
      <p>Figure 5 presents the composites of 850 <inline-formula><mml:math id="M87" display="inline"><mml:mi mathvariant="normal">mbar</mml:mi></mml:math></inline-formula> vector wind for three types of
ENSO. There is a strengthening of westerly and southwesterly wind in the
decaying year of CPW (Fig. 5b), which brings more moisture to China, compared
to developing CPW (Fig. 5a). This may explain the enhanced precipitation in
decaying CPW (Fig. 2b). The difference between developing and decaying EPC
(Fig. 5c–d) lies in the shift of anti-cyclonic flow in the western part of
North Pacific (WNP). The eastward anti-cyclone for the decaying EPC weakened
the transportation of moisture in eastern China and caused reduced
precipitation (Fig. 2d). The decaying EPW (Fig. 5f) experienced stronger
western and southwestern wind but weakened anti-cyclone compared to the
developing phase (Fig. 5e). The WNP anti-cyclone could bring plentiful
moisture to China, so weakened anti-cyclonic flow will cause reduced
precipitation (Feng et al., 2011). However, most parts of China
presented wetter signals in the phase of decaying EPW in comparison to
developing EPW. Therefore, it can be pointed out that the India monsoon
plays a more significant role in the formation of rainy-season precipitation
during EPW phases compared to the atmospheric circulation.</p>
      <p>Figure 6 shows the underlying causes of different performance of
conventional ENSO and ENSO Modoki in the developing phase by analysis of the
850 <inline-formula><mml:math id="M88" display="inline"><mml:mi mathvariant="normal">hp</mml:mi></mml:math></inline-formula> wind. Compared to developing CEN, developing MEN experienced reduced
precipitation in western China and generally enhanced precipitation in
eastern parts under the combined influence of stronger monsoon and weakened
anti-cyclone (Fig. 6a–b). Stronger anti-cyclonic flow in the phase of
developing La Niña Modoki (Fig. 6d) may cause the enhanced precipitation
in western parts of China compared to conventional La Niña regime in
developing years (Fig. 6c).</p>
      <p>The wind composites of warm and cold episodes of decaying ENSO and ENSO
Modoki are presented in Fig. 7. Compared to decaying CEN, the wet signal of
precipitation is weaker in the decaying year of MEN, which may be attributed
to the weakened anti-cyclonic flow in WNP and western winds for the decaying
MEN. The difference of wind composites between decaying CLN and MLN
indicates similar configuration, with stronger westerly wind and
anti-cyclone causing enhanced precipitation for decaying MLN.</p>
      <p>In summary, westerly winds seem to play more significant role in the phase
of CPW and EPW, while developing La Niña and La Niña Modoki are
dominated by the anti-cyclone. The spatial pattern of PARS is the reflection
of combined influence of westerly winds and anti-cyclonic flow for the EPC
and decaying ENSO and ENSO Modoki regimes.</p>
      <p>It can be seen that the spatial pattern of precipitation during the rainy
season in China is dominated by westerly winds from India and anti-cyclone
in WNP, which is equivalent to the results by Dai and Wigley
(2000), Feng and Li (2011), and Wu et al. (2003). Generally,
stronger western and southwestern winds are related to increasing
precipitation. It is in agreement with the research of Zhang et
al. (1996) and Wang et al. (2000), who pointed out that southeastern
and southwestern winds could substantially enhance the moisture
transportation to China. Wu et al. (2003) also found that East
Asian monsoon is positively related to precipitation variations, which is
consistent with our result. Likewise, the westward and stronger anti-cyclone
is related to enhanced PARS. Wu et al. (2003) reported that the
anomalous low-level anti-cyclone is determined by large-scale equatorial
heating anomalies and local air–sea interactions. Westerlies and
anti-cyclone are of dominant importance for the ENSO-induced precipitation
during the rainy season. However, cyclonic flow may have larger influence on
Chinese precipitation under certain circumstances. For example, the autumn
drought in southwest China in 2009 was determined by a strong cyclone in WNP
for ENSO Modoki (W. Zhang et al., 2013b). Feng et al. (2011)
also revealed that the WNP circulation is cyclonic in winter and then
becomes weak in the following spring and anti-cyclonic flow in summer for El Niño
Modoki. As a consequence, WNP anti-cyclone has a larger effect on
East Asian precipitation on the inter-annual or inter-decadal scale, but
anti-cyclone and cyclone are both crucial for the determination of
precipitation on the annual or smaller scale.</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <title>Conclusion</title>
      <p>This study investigated the distribution of PARS under various ENSO types in
developing and decaying phases and their underlying causes. It was found
that northwestern, central and southeastern China experience increasing
precipitation for decaying CPW and EPW, and positive precipitation anomaly
ranges from 0 to 30 <inline-formula><mml:math id="M89" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula> due to the stronger westerly and southwesterly
winds. The developing phase of EPW presents overall negative rainy-season
precipitation anomalies in China with more than 30 <inline-formula><mml:math id="M90" display="inline"><mml:mi mathvariant="normal">%</mml:mi></mml:math></inline-formula> below average
precipitation identified in many parts of the country, which is a result
of weak westerly winds. The different spatial distribution of rainy-season
precipitation under developing and decaying ENSO and ENSO Modoki regimes was
also examined. Conventional El Niño in developing years showed larger
influence on precipitation during rainy season in China as compared to
developing CLN, MEN and MLN. Conventional ENSO in the decaying phase is
more likely to show wet and dry signals in comparison to the corresponding
ENSO Modoki regimes. Different performance of conventional ENSO and ENSO
Modoki is a reflection of combined influence of the India monsoon and the
WNP anti-cyclone. This study improved our understanding on the spatial
variability of ENSO-induced precipitation during rainy season in China and
the underlying causes. These results suggest that improved predictability
can be achieved for rainy-season precipitation related to ENSO regimes. We
suggest that further work should focus on the influence of interactive ENSO
and other drivers on precipitation to evaluate and improve the predictive
ability.</p>
</sec>

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

      <p>The daily precipitation, NOAA extended reconstructed SST, ENSO Modoki index
(EMI) and the NCEP-NCAR reanalysis datasets used in this study are available
for download under the following URLs:
<list list-type="bullet"><list-item>
      <p>daily precipitation:
<uri>http://data.cma.cn/data/detail/dataCode/SURF_CLI_CHN_MUL_DAY_V3.0.html</uri>
(Ren et al., 2012)</p></list-item><list-item>
      <p>NOAA extended reconstructed SST:
<uri>https://data.nodc.noaa.gov/cgi-bin/iso?id=gov.noaa.ncdc:C00884</uri> (Huang et al., 2015)</p></list-item><list-item>
      <p>EMI:
<uri>http://www.jamstec.go.jp/frsgc/research/d1/iod/DATA/emi.monthly.txt</uri> (Japan Agency for Marine Science and Technology, 2017)</p></list-item><list-item>
      <p>NCEP/NCAR reanalysis data:
<uri>https://www.esrl.noaa.gov/psd/data/gridded/data.ncep.reanalysis.html</uri> (Kalnay et al., 1996)</p></list-item></list></p>
  </notes><notes notes-type="authorcontribution">

      <p>QC, ZH and FY conceived the study. All authors
contributed to writing the paper.</p>
  </notes><notes notes-type="competinginterests">

      <p>The authors declare that they have no conflict of
interest.</p>
  </notes><ack><title>Acknowledgements</title><p>Funding from the National Key Research Projects (grant no. 2016YFC0402704)
and the National Natural Science Foundation of China (grant no. 41371047)
are gratefully acknowledged. Support from the China Postdoctoral Science
Foundation (grant no. 2016M601711) and the Jiangsu Planned Projects for
Postdoctoral Research Funds (grant no. 1601027B) are appreciated.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: Luis Samaniego <?xmltex \hack{\newline}?>
Reviewed by: two anonymous referees</p></ack><ref-list>
    <title>References</title>

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    <!--<article-title-html>Impact of ENSO regimes on developing- and decaying-phase precipitation during rainy season in China</article-title-html>
<abstract-html><p class="p">This study investigated the influence of five El Niño–Southern
Oscillation (ENSO) types on rainy-season precipitation in China: central Pacific warming (CPW), eastern
Pacific cooling (EPC), eastern Pacific warming (EPW), conventional ENSO and
ENSO Modoki. The multi-scale moving
<i>t</i> test was applied to determine the onset and withdrawal of rainy season.
Results showed that the precipitation anomaly can reach up to 30 % above
average precipitation during decaying CPW and EPW phases. Developing EPW
could cause decreasing precipitation over large areas in China with 10–30 %
lower than average precipitation in most areas. Conventional El Niño in
the developing phase had the largest influence on ENSO-related precipitation
among developing ENSO and ENSO Modoki regimes. Decaying ENSO also showed a
larger effect on precipitation anomalies, compared to decaying ENSO Modoki.
The difference between rainy-season precipitation under various ENSO regimes
may be attributed to the combined influence of anti-cyclone in the western
North Pacific and the Indian monsoon. Stronger monsoon and anti-cyclone are
associated with enhanced rainy-season precipitation. The results suggest a
certain predictability of rainy-season precipitation related to ENSO regimes.</p></abstract-html>
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