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<metadata xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:dc="http://purl.org/dc/elements/1.1/"><dc:title>Measurement of branching fractions for $B \to J/\psi \eta K$ decays and search for a narrow resonance in the $J/\psi \eta$ final state</dc:title><dc:creator>Iwashita,	T.	(Avtor)
	</dc:creator><dc:creator>Bračko,	Marko	(Avtor)
	</dc:creator><dc:creator>Golob,	Boštjan	(Avtor)
	</dc:creator><dc:creator>Klučar,	Jure	(Avtor)
	</dc:creator><dc:creator>Korpar,	Samo	(Avtor)
	</dc:creator><dc:creator>Križan,	Peter	(Avtor)
	</dc:creator><dc:creator>Pestotnik,	Rok	(Avtor)
	</dc:creator><dc:creator>Petrič,	Marko	(Avtor)
	</dc:creator><dc:creator>Stanič,	Samo	(Drugo)
	</dc:creator><dc:creator>Starič,	Marko	(Avtor)
	</dc:creator><dc:creator>Šantelj,	Luka	(Avtor)
	</dc:creator><dc:creator>Zupanc,	Anže	(Avtor)
	</dc:creator><dc:subject>C07</dc:subject><dc:subject>C21</dc:subject><dc:subject>particle properties</dc:subject><dc:subject>lepton collider experiments</dc:subject><dc:subject>experimental particle physics</dc:subject><dc:description>We report an observation of the $B^{\pm } \to J/\psi \eta K^{\pm }$ and $B^0 \to J/\psi \eta K^0_S$ decays using $772\times 10^{6}B\overline {B}$ pairs collected at the $\Upsilon (4S)$ resonance with the Belle detector at the KEKB asymmetric-energy $e^+e^-$ collider. We obtain the branching fractions ${\mathcal B}(B^{\pm }\rightarrow J/\psi \eta K^{\pm })=(1.27\pm 0.11(\hbox {stat.})\pm 0.11(\hbox {syst.}))\times 10^{-4}$ and ${\mathcal B}(B^0\to J/\psi \eta K^0_S)=(5.22 \pm 0.78 (\hbox {stat.}) \pm 0.49 (\hbox {syst.}))\times 10^{-5}$. We search for a new narrow charmonium(-like) state $X$ in the $ J/\psi \eta$ mass spectrum and find no significant excess. We set upper limits on the product of branching fractions, ${\mathcal B}(B^\pm \to XK^\pm){\mathcal B}(X \to J/\psi \eta)$, at $3872\,\hbox {MeV}\,c^{-2}$ where a $C$-odd partner of $X(3872)$ may exist, at $\psi (4040)$ and $\psi (4160)$ assuming their known mass and width, and over a range from 3.8 to $4.8\,\hbox {GeV}\,c^{-2}$. The obtained upper limits at 90% confidence level for $X^{C\hbox {-}{\rm odd}}(3872)$, $\psi (4040)$, and $\psi (4160)$ are $3.8\times 10^{-6}$, $15.5\times 10^{-6}$, and $7.4\times 10^{-6}$, respectively.</dc:description><dc:date>2014</dc:date><dc:date>2017-07-21 12:45:37</dc:date><dc:type>Znanstveno delo</dc:type><dc:identifier>66977</dc:identifier><dc:identifier>ISSN: 2050-3911</dc:identifier><dc:identifier>UDK: 539.1</dc:identifier><dc:identifier>OceCobissID: 2704635</dc:identifier><dc:identifier>COBISS_ID: 28162343</dc:identifier><dc:identifier>DOI: 10.1093/ptep/ptu043</dc:identifier><dc:identifier>ISSN pri članku: 2050-3911</dc:identifier><dc:identifier>NUK URN: URN:SI:UM:DK:GX0ZKAEF</dc:identifier><dc:language>sl</dc:language></metadata>
