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        <jpcoar:jpcoar xmlns:datacite="https://schema.datacite.org/meta/kernel-4/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:dcndl="http://ndl.go.jp/dcndl/terms/" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:jpcoar="https://github.com/JPCOAR/schema/blob/master/1.0/" xmlns:oaire="http://namespace.openaire.eu/schema/oaire/" xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:rioxxterms="http://www.rioxx.net/schema/v2.0/rioxxterms/" xmlns:xs="http://www.w3.org/2001/XMLSchema" xmlns="https://github.com/JPCOAR/schema/blob/master/1.0/" xsi:schemaLocation="https://github.com/JPCOAR/schema/blob/master/1.0/jpcoar_scm.xsd">
          <dc:title>Study of B meson decays with J/ψ　and φ in the final states</dc:title>
          <dc:title xml:lang="en">Study of B meson decays with J/ψ　and φ in the final states</dc:title>
          <jpcoar:creator>
            <jpcoar:creatorName>LIU, YANG</jpcoar:creatorName>
          </jpcoar:creator>
          <jpcoar:creator>
            <jpcoar:creatorName>リュウ, ヤン</jpcoar:creatorName>
          </jpcoar:creator>
          <jpcoar:creator>
            <jpcoar:creatorName xml:lang="en">LIU, Yang</jpcoar:creatorName>
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          <datacite:description descriptionType="Other">We study the decay modes of &lt;i&gt;B&lt;/i&gt; meson decay to final states including &lt;i&gt;J/ψ&lt;/i&gt; and&#13;
&lt;i&gt;Φ&lt;/i&gt; mesons based on a large amount of data sample at the &amp;upsih;(4S) state collected with&#13;
Belle detector in KEKB asymmetric energy &lt;i&gt;e&lt;/i&gt;&lt;sup&gt;+&lt;/sup&gt;&lt;i&gt;e&lt;/i&gt;&lt;sup&gt;-&lt;/sup&gt; collider.&#13;
　　The decay &lt;i&gt;B&lt;/i&gt;&lt;sup&gt;0&lt;/sup&gt; → &lt;i&gt;J /ψΦ&lt;/i&gt;&lt;/sup&gt; is expected to involve W-exchange and final state interac-&#13;
tion (FSI) processes. The mechanisms contributing to this decay can be divided into&#13;
four categories: 1) The photo-production; 2) The tri-gluon fusion; 3) The rescattering&lt;br /&gt;effect; 4) The &lt;i&gt;ω - Φ&lt;/i&gt; mixing. The dominant contribution is from &lt;i&gt;ω- Φ&lt;/i&gt; mixing and the&#13;
branching fraction for this decay is estimated to be (1.8 ± 0.3) × 10&lt;sup&gt;-7&lt;/sup&gt;.&#13;
　　We perform a search for &lt;i&gt;B&lt;/i&gt;&lt;sup&gt;0&lt;/sup&gt; → &lt;i&gt;J /ψΦ&lt;/i&gt; decays using a data sample of 605 fb&lt;sup&gt;-1&lt;/sup&gt;&#13;
 containing 657 × 10&lt;sup&gt;6&lt;/sup&gt; &lt;i&gt;BB&lt;/i&gt;&lt;/span&gt;pairs.&#13;
　　We reconstruct &lt;i&gt;B&lt;/i&gt; mesons from the decays &lt;i&gt;J/ψ&lt;/i&gt; → &lt;i&gt;l&lt;sup&gt;+&lt;/sup&gt;l&lt;sup&gt;-&lt;/sup&gt; (l = e,μ)&lt;/i&gt; and &lt;i&gt;Φ&lt;/i&gt; →&#13;
&lt;i&gt;K&lt;sup&gt;+&lt;/sup&gt; K&lt;sup&gt;-&lt;/sup&gt;&lt;/i&gt;. Events are required to pass a basic hadronic event selection. We identify &lt;i&gt;B&lt;/i&gt;&#13;
candidates using two widely used kinematic variable calculated in the center-of-mass&#13;
system:the beam-energy constrained mass (&lt;i&gt;M&lt;/i&gt;&lt;small&gt;bc&lt;/small&gt; &amp;equiv; &lt;big&gt;&amp;radic;&lt;/big&gt;E&lt;sup&gt;2&lt;/sup&gt;&lt;small&gt;beam&lt;/small&gt;　―　P&lt;sup&gt;2&lt;/sup&gt;&lt;small&gt;B&lt;/small&gt;) and the energy&#13;
difference (△&lt;i&gt;E&lt;/i&gt; &amp;equiv; &lt;i&gt;E&lt;small&gt;B&lt;/i&gt;&lt;/small&gt; - &lt;i&gt;E&lt;/i&gt;&lt;small&gt;beam&lt;/small&gt;), where &lt;i&gt;E&lt;/i&gt;&lt;small&gt;beam&lt;/small&gt; is the beam energy, &lt;i&gt;P&lt;small&gt;B&lt;/i&gt;&lt;/small&gt; and &lt;i&gt;E&lt;small&gt;B&lt;/small&gt;&lt;/i&gt; are the&#13;
reconstructed momentum and energy of the B&lt;sup&gt;0&lt;/sup&gt; candidate. We select &lt;i&gt;B&lt;/i&gt; candidates&#13;
within the range -0.2 GeV &lt; △&lt;i&gt;E&lt;/i&gt; &lt; 0.3 GeV and 5.27 GeV / &lt;i&gt;c&lt;/i&gt;&lt;sup&gt;2&lt;/sup&gt; ＜ &lt;i&gt;M&lt;/i&gt;&lt;small&gt;bc&lt;/small&gt; &lt; 5.29 GeV / &lt;i&gt;c&lt;/i&gt;&lt;sup&gt;2&lt;/sup&gt;&#13;
for final analysis.&#13;
　　We study reconstruction efficiency and event selection criteria using a large signal&#13;
Monte Calor (MC) sample. To study the background, we use a MC sample corre-&#13;
sponding to 3.86 × 10&lt;sup&gt;6&lt;/sup&gt;generic &lt;i&gt;BB&lt;/i&gt; decays (59 times that of real data) that includes&#13;
all known &lt;i&gt;B&lt;/i&gt; →　&lt;i&gt;J/ψX&lt;/i&gt; processes as well as sideband region.&#13;
　　The dominant background comes from &lt;i&gt;BB&lt;/i&gt; events with &lt;i&gt;B&lt;/i&gt; decays to &lt;i&gt;J/ψ&lt;/i&gt;. We&#13;
 find that the dominant backgrounds come B&lt;sup&gt;0&lt;/sup&gt; → &lt;i&gt;J/ψK&lt;/i&gt;*&lt;sup&gt;0&lt;/sup&gt;(892)[→&lt;i&gt;K&lt;/i&gt;&lt;sup&gt;-&lt;/sup&gt;π&lt;sup&gt;+&lt;/sup&gt;] and&lt;br /&gt;B&lt;sup&gt;0-&lt;/sup&gt; → &lt;i&gt;J/ψK&lt;/i&gt;&lt;small&gt;1&lt;/small&gt;(1270)[→ &lt;i&gt;K&lt;/i&gt;&lt;sup&gt;-&lt;/sup&gt;π&lt;sup&gt;+&lt;/sup&gt;π&lt;sup&gt;0/-&lt;/sup&gt;]. In both cases, a pion is misidentified as a kaon,&#13;
and in the latter case, the other pion is missed. The former has a peak at △&lt;i&gt;E&lt;/i&gt; ～0.1～&lt;br /&gt;GeV, while the latter has a broad peak in the negative △&lt;i&gt;E&lt;/i&gt; region. The remaining&#13;
background is due to random combinations of &lt;i&gt;J/ψ&lt;/i&gt;and &lt;i&gt;Φ&lt;/i&gt; candidates and does not&#13;
have structure in the △&lt;i&gt;E&lt;/i&gt; distribution (referred to as combinatorial background).&#13;
　　The signal yield is extracted by performing an unbinned extended maximum-&#13;
likelihood fit to the △&lt;i&gt;E&lt;/i&gt; distribution of candidate events. The signal PDF is mod-&#13;
eled by a sum of two Gaussians. The background PDFs are two Gaussians for the&#13;
&lt;i&gt;J/ψK&lt;/i&gt;&lt;small&gt;1&lt;/small&gt; component, a bifurcated Gaussian for the &lt;i&gt;J/ψK&lt;/i&gt;&lt;sup&gt;*0&lt;/sup&gt; component and a second-&#13;
order polynomial for combinatorial background, respectively. The parameters of these&#13;
PDFs are determined from MC simulations.&#13;
　　We obtain a signal yield of 4.6&lt;sup&gt;+3.1&lt;/sup&gt;&lt;small&gt;-2.5&lt;/small&gt; events with a statistical significance of 2.3σ.&#13;
As no significant signal is found for the &lt;i&gt;B&lt;/i&gt;&lt;sup&gt;0&lt;/sup&gt; →　&lt;i&gt;J /ψΦ&lt;/i&gt; decay mode, we an upper&#13;
limit on the yield at the 90% confidence level by a frequentist method using ensembles&#13;
of pseudo-experiments. Finally an upper limit at the 90% confidence level is obtained:&#13;
&#13;
　　　　　　　　　　　　　　&lt;i&gt;β&lt;/i&gt;(&lt;i&gt;B&lt;/i&gt;&lt;sup&gt;0&lt;/sup&gt; → &lt;i&gt;J /ψΦ&lt;/i&gt;)&lt; 9.4 × 10&lt;sup&gt;-7&lt;/sup&gt;.   　　　　　 (1)&#13;
&#13;
　　This result improves upon the previous result by about a factor of 10 and is&#13;
consistent with the theory prediction. The result shows that a large enhancement&#13;
 from rescattering is not likely in this decay mode. To check the prediction more&#13;
precisely, a larger data sample is needed.</datacite:description>
          <datacite:description descriptionType="Other">総研大甲第1196号</datacite:description>
          <dc:language>eng</dc:language>
          <dc:type rdf:resource="http://purl.org/coar/resource_type/c_46ec">thesis</dc:type>
          <jpcoar:identifier identifierType="URI">https://ir.soken.ac.jp/records/711</jpcoar:identifier>
          <dcndl:degreeName>博士（理学）</dcndl:degreeName>
          <dcndl:dateGranted>2008-09-30</dcndl:dateGranted>
          <jpcoar:degreeGrantor>
            <jpcoar:degreeGrantorName>総合研究大学院大学</jpcoar:degreeGrantorName>
          </jpcoar:degreeGrantor>
          <jpcoar:file>
            <jpcoar:URI label="要旨・審査要旨">https://ir.soken.ac.jp/record/711/files/甲1196_要旨.pdf</jpcoar:URI>
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            <jpcoar:extent>252.8 kB</jpcoar:extent>
            <datacite:date dateType="Available">2016-02-17</datacite:date>
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          <jpcoar:file>
            <jpcoar:URI label="本文">https://ir.soken.ac.jp/record/711/files/甲1196_本文.pdf</jpcoar:URI>
            <jpcoar:mimeType>application/pdf</jpcoar:mimeType>
            <jpcoar:extent>23.0 MB</jpcoar:extent>
            <datacite:date dateType="Available">2016-02-17</datacite:date>
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