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Measurements of branching fractions of tau lepton decays with one or more K-S(0)

Authors
Ryu, S[Ryu, S.]Adachi, I[Adachi, I.]Aihara, H[Aihara, H.]Asner, DM[Asner, D. M.]Aulchenko, V[Aulchenko, V.]Aushev, T[Aushev, T.]Bakich, AM[Bakich, A. M.]Bala, A[Bala, A.]Bhuyan, B[Bhuyan, B.]Bobrov, A[Bobrov, A.]Bondar, A[Bondar, A.]Bonvicini, G[Bonvicini, G.]Bozek, A[Bozek, A.]Bracko, M[Bracko, M.]Browder, TE[Browder, T. E.]Cervenkov, D[Cervenkov, D.]Chekelian, V[Chekelian, V.]Cheon, BG[Cheon, B. G.]Chilikin, K[Chilikin, K.]Chistov, R[Chistov, R.]Cho, K[Cho, K.]Chobanova, V[Chobanova, V.]Choi, SK[Choi, S. -K.]Choi, Y[Choi, Y.]Dalseno, J[Dalseno, J.]Dolezal, Z[Dolezal, Z.]Dutta, D[Dutta, D.]Eidelman, S[Eidelman, S.]Epifanov, D[Epifanov, D.]Farhat, H[Farhat, H.]Fast, JE[Fast, J. E.]Ferber, T[Ferber, T.]Gaur, V[Gaur, V.]Gabyshev, N[Gabyshev, N.]Ganguly, S[Ganguly, S.]Garmash, A[Garmash, A.]Gillard, R[Gillard, R.]Goh, YM[Goh, Y. M.]Golob, B[Golob, B.]Haba, J[Haba, J.]Hayasaka, K[Hayasaka, K.]Hayashii, H[Hayashii, H.]Hoshi, Y[Hoshi, Y.]Hou, WS[Hou, W. -S.]Iijima, T[Iijima, T.]Inami, K[Inami, K.]Ishikawa, A[Ishikawa, A.]Iwashita, T[Iwashita, T.]Julius, T[Julius, T.]Kato, E[Kato, E.]Kiesling, C[Kiesling, C.]Kim, BH[Kim, B. H.]Kim, DY[Kim, D. Y.]Kim, JB[Kim, J. B.]Kim, JH[Kim, J. H.]Kim, KT[Kim, K. T.]Kim, MJ[Kim, M. J.]Kim, SK[Kim, S. K.]Kim, YJ[Kim, Y. J.]Ko, BR[Ko, B. R.]Kodys, P[Kodys, P.]Krizan, P[Krizan, P.]Krokovny, P[Krokovny, P.]Kuhr, T[Kuhr, T.]Kuzmin, A[Kuzmin, A.]Kwon, YJ[Kwon, Y. -J.]Lee, SH[Lee, S. -H.]Li, J[Li, J.]Libby, J[Libby, J.]Liventsev, D[Liventsev, D.]Lukin, P[Lukin, P.]MacNaughton, J[MacNaughton, J.]Matvienko, D[Matvienko, D.]Miyabayashi, K[Miyabayashi, K.]Miyata, H[Miyata, H.]Mizuk, R[Mizuk, R.]Moll, A[Moll, A.]Mori, T[Mori, T.]Mussa, R[Mussa, R.]Nakano, E[Nakano, E.]Nakao, M[Nakao, M.]Nakazawa, H[Nakazawa, H.]Nayak, M[Nayak, M.]Nedelkovska, E[Nedelkovska, E.]Nisar, NK[Nisar, N. K.]Nishida, S[Nishida, S.]Nitoh, O[Nitoh, O.]Okuno, S[Okuno, S.]Olsen, SL[Olsen, S. L.]Pakhlov, P[Pakhlov, P.]Pakhlova, G[Pakhlova, G.]Park, CW[Park, C. W.]Park, H[Park, H.]Park, HK[Park, H. K.]Pedlar, TK[Pedlar, T. K.]Petric, M[Petric, M.]Piilonen, LE[Piilonen, L. E.]Ritter, M[Ritter, M.]Rohrken, M[Roehrken, M.]Rostomyan, A[Rostomyan, A.]Sahoo, H[Sahoo, H.]Saito, T[Saito, T.]Sakai, Y[Sakai, Y.]Santelj, L[Santelj, L.]Sanuki, T[Sanuki, T.]Savinov, V[Savinov, V.]Schneider, O[Schneider, O.]Schnell, G[Schnell, G.]Schwanda, C[Schwanda, C.]Semmler, D[Semmler, D.]Seon, O[Seon, O.]Shebalin, V[Shebalin, V.]Shen, CP[Shen, C. P.]Shibata, TA[Shibata, T. -A.]Shiu, JG[Shiu, J. -G.]Shwartz, B[Shwartz, B.]Sibidanov, A[Sibidanov, A.]Simon, F[Simon, F.]Sohn, YS[Sohn, Y. -S.]Sokolov, A[Sokolov, A.]Solovieva, E[Solovieva, E.]Stanic, S[Stanic, S.]Staric, M[Staric, M.]Sumiyoshi, T[Sumiyoshi, T.]Tamponi, U[Tamponi, U.]Tatishvili, G[Tatishvili, G.]Teramoto, Y[Teramoto, Y.]Uchida, M[Uchida, M.]Uehara, S[Uehara, S.]Unno, Y[Unno, Y.]Uno, S[Uno, S.]Van Hulse, C[Van Hulse, C.]Vanhoefer, P[Vanhoefer, P.]Varner, G[Varner, G.]Vinokurova, A[Vinokurova, A.]Vorobyev, V[Vorobyev, V.]Wagner, MN[Wagner, M. N.]Wang, CH[Wang, C. H.]Wang, P[Wang, P.]Watanabe, M[Watanabe, M.]Watanabe, Y[Watanabe, Y.]Won, E[Won, E.]Yamashita, Y[Yamashita, Y.]Yashchenko, S[Yashchenko, S.]Yook, Y[Yook, Y.]Yuan, CZ[Yuan, C. Z.]Zhang, ZP[Zhang, Z. P.]Zhilich, V[Zhilich, V.]Zhulanov, V[Zhulanov, V.]Zupanc, A[Zupanc, A.]
Issue Date
9-Apr-2014
Publisher
AMER PHYSICAL SOC
Citation
PHYSICAL REVIEW D, v.89, no.7
Indexed
SCIE
SCOPUS
Journal Title
PHYSICAL REVIEW D
Volume
89
Number
7
URI
https://scholarworks.bwise.kr/skku/handle/2021.sw.skku/53337
DOI
10.1103/PhysRevD.89.072009
ISSN
1550-7998
Abstract
We report measurements of branching fractions of tau lepton decays to final states with a K-S(0) meson using a 669 fb(-1) data sample accumulated with the Belle detector at the KEKB asymmetric-energy e(+)e(-) collider. The inclusive branching fraction is measured to be beta(tau(-) -> (KSX-)-X-0 nu(tau)) = (9.15 +/- 0.01 +/- 0.15) X 10(-3), where X- can be anything; the exclusive branching fractions are beta(tau(-) -> pi(-) K-S(0)nu(tau)) = (4.16 +/- 0.01 +/- 0.08) X 10(-3), beta(tau(-) -> K- K-S(0)nu(tau)) = (7.40 +/- 0.07 +/- 0.27) X 10(-4), beta(tau(-) -> pi(-) K-S(0)pi(0)nu(tau)) = (1.93 +/- 0.02 +/- 0.07) X 10(-3), beta(tau(-) -> K- K-S(0)pi(0)nu(tau)) = (7.48 +/- 0.10 +/- 0.37) X 10(-4), beta(tau(-) -> pi(-) (KSKS0)-K-0 nu(tau)) = (2.33 +/- 0.03 +/- 0.09) X 10(-4), beta(tau(-) -> pi(-) (KSKS0)-K-0 pi(0)nu(tau)) = (2.00 +/- 0.22 +/- 0.20) X 10(-5), where the first uncertainty is statistical and the second is systematic. For each mode, the accuracy is improved over that of pre-B-factory measurements by a factor ranging from five to ten. In tau(-) -> pi(-) (KSKS0)-K-0 pi(0)nu(tau) decays, clear signals for the intermediate states tau(-) -> pi(-) f(1)(1285)nu(tau) and tau(-) -> K*- K-S(0)pi(0)nu(tau) are observed.
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