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000208303 0247_ $$2doi$$a10.1103/PhysRevD.91.051101
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000208303 0247_ $$2ISSN$$a1550-2368
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000208303 0247_ $$2arXiv$$aarXiv:1501.06867
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000208303 0881_ $$aBELLE-PREPRINT-2014-22; KEK-PREPRINT-2014-41; arXiv:1501.06867
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000208303 088__ $$2arXiv$$aarXiv:1501.06867
000208303 1001_ $$aBala, A.$$b0
000208303 245__ $$aObservation of $\it{X}$ (3872) in $\it{B}→X$ (3872)$\it{K\pi}$ decays
000208303 260__ $$bAmerican Physical Society$$c2015
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000208303 500__ $$a*Temporary entry*7 pages, 3 figures, submitted to PRD as Rapid Communication / Received 27 January 2015 / Published 2 March 2015
000208303 520__ $$aWe report the first observation of ${B}^{0}\to X\left(3872\right)\left({K}^{+}{\pi }^{-}\right)$ and evidence for ${B}^{+}\to X\left(3872\right)\left({K}^{0}{\pi }^{+}\right)$. We measure the product of branching fractions for the former to be $\mathcal{B}\left({B}^{0}\to X\left(3872\right)\left({K}^{+}{\pi }^{-}\right)\right)×\mathcal{B}\left(X\left(3872\right)\to J/\psi {\pi }^{+}{\pi }^{-}\right)=\left(7.9±1.3\left(\text{stat}\right)±0.4\left(\text{syst}\right)\right)×1{0}^{-6}$ and find that $B^0$$\to X(3872)$$K^*(892)^0$does not dominate the ${B}^{0}\to X\left(3872\right){K}^{+}{\pi }^{-}$ decay mode. We also measure $\mathcal{B}\left({B}^{+}\to X\left(3872\right)\left({K}^{0}{\pi }^{+}\right)\right)×\phantom{\rule{0ex}{0ex}}\mathcal{B}\left(X\left(3872\right)\to J/\psi {\pi }^{+}{\pi }^{-}\right)=\left(10.6±3.0\left(\text{stat}\right)±0.9\left(\text{syst}\right)\right)×1{0}^{-6}$. This study is based on the full data sample of $711\text{}\text{}{\mathrm{fb}}^{-1}$ ($772×1{0}^{6}B\overline{B}$ pairs) collected at the $\mathrm{Υ}\left(4S\right)$ resonance with the Belle detector at the KEKB collider.
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000208303 650_7 $$2INSPIRE$$aelectron positron: annihilation
000208303 650_7 $$2INSPIRE$$aB: pair production
000208303 650_7 $$2INSPIRE$$aX(3872): hadronic decay
000208303 650_7 $$2INSPIRE$$abranching ratio: measured
000208303 650_7 $$2INSPIRE$$aUpsilon(10570)
000208303 650_7 $$2INSPIRE$$aintermediate state
000208303 650_7 $$2INSPIRE$$aexperimental results
000208303 650_7 $$2INSPIRE$$aBELLE
000208303 650_7 $$2INSPIRE$$aKEK-B
000208303 650_7 $$2INSPIRE$$aB --> K pi X(3872)
000208303 650_7 $$2INSPIRE$$aX(3872) --> pi+ pi- J/psi(3100)
000208303 650_7 $$2INSPIRE$$a10.57 GeV-cms
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000208303 77318 $$2Crossref$$3journal-article$$a10.1103/physrevd.91.051101$$b : American Physical Society (APS), 2015-03-02$$n5$$p051101$$tPhysical Review D$$v91$$x1550-7998$$y2015
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000208303 7870_ $$0PUBDB-2015-01056$$aBala, A. et.al.$$d2014$$iIsParent$$rBELLE-PREPRINT-2014-22; arXiv:1501.06867$$tObservation of $X(3872)$ in $B \to X(3872) K\pi$ decays
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