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Study of the Hadronic Transitions $\Upsilon$(2S)$\rightarrow (\eta,\pi^0)\Upsilon$(1S) at Belle

Authors :
Belle Collaboration
Tamponi, U.
Mussa, R.
Adachi, I.
Aihara, H.
Asner, D. M.
Aulchenko, V.
Aushev, T.
Bakich, A. M.
Barrett, M.
Bhuyan, B.
Bondar, A.
Bozek, A.
Bra\v, M.
Browder, T. E.
Chen, A.
Chen, P.
Cheon, B. G.
Chilikin, K.
Cho, I. -S.
Cho, K.
Choi, Y.
Dalseno, J.
Dole\v, Z.
Drásal, Z.
Dutta, D.
Eidelman, S.
Epifanov, D.
Esen, S.
Farhat, H.
Fast, J. E.
Frey, A.
Gaur, V.
Gillard, R.
Goh, Y. M.
Golob, B.
Hayasaka, K.
Horii, Y.
Hoshi, Y.
Hyun, H. J.
Iijima, T.
Ishikawa, A.
Iwasaki, Y.
Jaegle, I.
Kang, J. H.
Kawasaki, T.
Kim, H. O.
Kim, J. H.
Kim, K. T.
Kim, M. J.
Kim, Y. J.
Klucar, J.
Ko, B. R.
Kody\v, P.
Korpar, S.
Kouzes, R. T.
Kri\v, P.
Krokovny, P.
Kumita, T.
Kuzmin, A.
Lee, S. -H.
Li, Y.
Liu, C.
Liu, Y.
Liu, Z. Q.
Liventsev, D.
Miyata, H.
Mizuk, R.
Mohanty, G. B.
Moll, A.
Muramatsu, N.
Nakao, M.
Natkaniec, Z.
Ng, C.
Nishida, S.
Nitoh, O.
Ogawa, S.
Ohshima, T.
Okuno, S.
Olsen, S. L.
Onuki, Y.
Pakhlov, P.
Park, H. K.
Park, K. S.
Pedlar, T. K.
Pestotnik, R.
Petri\v, M.
Piilonen, L. E.
Röhrken, M.
Sakai, Y.
Sandilya, S.
Santel, D.
Santelj, L.
Sanuki, T.
Schneider, O.
Schnell, G.
Schwanda, C.
Senyo, K.
Shen, C. P.
Shibata, T. -A.
Shiu, J. -G.
Shwartz, B.
Simon, F.
Smerkol, P.
Sohn, Y. -S.
Sokolov, A.
Solovieva, E.
Stari\v, M.
Sumiyoshi, T.
Tanida, K.
Taniguchi, N.
Tatishvili, G.
Teramoto, Y.
Trabelsi, K.
Uehara, S.
Uno, S.
Van Hulse, C.
Vanhoefer, P.
Varner, G.
Wang, C. H.
Wang, M. -Z.
Wang, P.
Wang, X. L.
Watanabe, M.
Watanabe, Y.
Williams, K. M.
Won, E.
Yabsley, B. D.
Yamashita, Y.
Yuan, C. Z.
Zhang, Z. P.
Zhilich, V.
Zhulanov, V.
Zupanc, A.
Publication Year :
2012

Abstract

We study the rare hadronic transitions $\Upsilon(2S)\rightarrow \Upsilon(1S)\eta$ and $\Upsilon(2S)\rightarrow \Upsilon(1S)\pi^0$ using a sample of 158 $\times 10^6$ $\Upsilon(2S)$ decays collected with the Belle detector at the KEKB asymmetric-energy $e^+ e^-$ collider. We observe the $\eta$ meson decay to $\gamma\gamma$ and $\pi^+\pi^-\pi^0$ final states; the $\Upsilon(1S)$ is reconstructed in the $\mu^+\mu^-$ and $e^+e^-$ decay modes. We measure the ratios of branching fractions (${\mathcal B}$) $\frac{{\mathcal B}(\Upsilon(2S)\rightarrow\Upsilon(1S)\eta)}{{\mathcal B}(\Upsilon(2S)\rightarrow\Upsilon(1S)\pi^+\pi^-)}$ = (1.99$\pm$0.14 (stat) $\pm$0.11 (syst)) $\times 10^{-3}$ and $\frac{{\mathcal B}(\Upsilon(2S)\rightarrow\Upsilon(1S)\pi^0)}{{\mathcal B}(\Upsilon(2S)\rightarrow\Upsilon(1S)\pi^+\pi^-)} < 2.3 \times 10^{-4}$ at the 90% confidence level (CL). Assuming the value ${\mathcal B}(\Upsilon(2S) \rightarrow \Upsilon(1S)\pi^-\pi^+)$ = (17.92$\pm$0.26)%, we obtain $ {\mathcal B}(\Upsilon(2S)\rightarrow\Upsilon(1S)\eta) = (3.57 \pm 0.25 ({\rm stat})\ \pm 0.21 ({\rm syst}))\times 10^{-4} $ and $ {\mathcal B}(\Upsilon(2S)\rightarrow\Upsilon(1S)\pi^0) < 4.1\times 10^{-5}\ ({\rm 90%\ CL}). $<br />Comment: 6 pages, 6 figures, submitted to PRD(RC)

Subjects

Subjects :
High Energy Physics - Experiment

Details

Database :
arXiv
Publication Type :
Report
Accession number :
edsarx.1210.6914
Document Type :
Working Paper
Full Text :
https://doi.org/10.1103/PhysRevD.87.011104