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Showing papers by "J. Haba published in 2012"


Journal ArticleDOI
Sadaharu Uehara, Y. Watanabe1, H. Nakazawa2, I. Adachi  +156 moreInstitutions (49)
TL;DR: In this paper, the pion transition form factor, F(Q(2)), is measured for the kinematical region 4 GeV2 <= Q(2) <= 40 GeV 2, where -Q 2 is the invariant-mass squared of a virtual photon.
Abstract: We report a measurement of the process gamma gamma* -> pi(0) with a 759 fb(-1) data sample recorded with the Belle detector at the KEKB asymmetric-energy e(+)e(-) collider. The pion transition form factor, F(Q(2)), is measured for the kinematical region 4 GeV2 <= Q(2) <= 40 GeV2, where -Q(2) is the invariant-mass squared of a virtual photon. The measured values of Q(2)vertical bar F(Q(2))vertical bar agree well with the previous measurements below Q(2) similar or equal to 9 GeV2 but do not exhibit the rapid growth in the higher Q(2) region seen in another recent measurement, which exceeds the asymptotic QCD expectation by as much as 50%.

190 citations


Journal ArticleDOI
I. Adachi, H. Aihara1, D. M. Asner2, V.M. Aulchenko3  +172 moreInstitutions (47)
TL;DR: In this paper, a precise measurement of the CP violation parameter sin2 phi(1) and the direct CP violation parameters A(f) using the final data sample of 772 x 10(6) B (B) over bar pairs collected at the gamma(4S) resonance with the Belle detector at the KEKB asymmetric-energy e(+) e(-) collider is presented.
Abstract: We present a precise measurement of the CP violation parameter sin2 phi(1) and the direct CP violation parameter A(f) using the final data sample of 772 x 10(6) B (B) over bar pairs collected at the gamma(4S) resonance with the Belle detector at the KEKB asymmetric-energy e(+) e(-) collider. One neutral B meson is reconstructed in a J/psi K-S(0), psi(2S)K-S(0), chi K-c1(S)0, or J/psi K-L(0) CP eigenstate an(its flavor is identified from the decay products of the accompanying B meson. From the distribution of proper-time intervals between the two B decays, we obtain the following CP violation parameters: sin2 phi(1) 0.667 +/- 0.023(stat) +/- 0.012(syst) and A(f) = 0.006 +/- 0.016(stat) +/- 0.012(syst).

100 citations


Journal ArticleDOI
T. Higuchi, K. Sumisawa, I. Adachi, Hiroaki Aihara1  +175 moreInstitutions (49)
TL;DR: In this article, a new sensitive search for C P T violation was reported, which includes improved measurements of the C p T-violating parameter z and the total decay-width difference normalized to the averaged width delta(d) delta(D) of the two B-d mass eigenstates.
Abstract: We report a new sensitive search for C P T violation, which includes improved measurements of the C P T-violating parameter z and the total decay-width difference normalized to the averaged width delta(d) delta(d) of the two B-d mass eigenstates . The results are based on a data sample of 535 x 10(6) B B pairs collected at the Epsilon(4 S) resonance with the Belle detector at the KEKB asymmetric-energy e(+) e(-) collider. We obtain Re (z) = [+1.9 +/- 3.7 (stat) +/- 3.3 (syst)] x 10(>-2), qm (z) = [-5.7 +/- 3.3 (stat) +/- 3.3 (syst)] x 10(-3), and delta(d) / delta(d) = [-1.7 +/- 1.8 (stat) +/- 1.1 (syst)] x 10(-2), all of which are consistent with zero. This is the most precise single measurement of these parameters in the neutral B-meson system to date.

46 citations


Posted Content
TL;DR: In this article, the authors reported preliminary results on the analysis of the three-body Y(10860)=> B barB pi, Y( 10860) => (B barB* + c.c.c.) pi and Y (10860]=> B* barB*) pi decays as intermediate channels.
Abstract: We report preliminary results on the analysis of the three-body Y(10860)=> B barB pi, Y(10860) => (B barB* + c.c.) pi and Y(10860)=> B* barB* pi decays including an observation of the Y(10860)=> Zb(10610)+- pi-+ => [B barB*+c.c]+- pi-+ and Y(10860)=> Zb(10650)+- pi-+ => [B* barB*]+- pi-+ decays as intermediate channels. We measure branching fractions of the three-body decays to be Br(Y(10860)=> [B barB*+c.c.]+- pi-+)=(28.3+-2.9+-4.6)x10^{-3} and Br(Y(10860)=> [B* barB*]+- pi-+)=(14.1+-1.9+-2.4)x10^{-3} and set 90% C.L. upper limit Br(Y(10860)=> [B barB]+- pi-+) Y(nS)pi+pi-, n=1,2,3 decays and the analysis of the internal structure of the three-body Y(10860)=>hb(mP)pi+pi-, m=1,2 decays. The results are based on a 121.4 1/fb data sample collected with the Belle detector at a center-of-mass energy near the Y(10860).

38 citations


Journal ArticleDOI
B. R. Ko1, E. Won1, I. Adachi, H. Aihara2  +160 moreInstitutions (48)
TL;DR: In this paper, the authors observed evidence for CP violation in the decay D+ → K(S)π+ using a data sample with an integrated luminosity of 977 Ã 0 Ã Ã 1 ) collected by the Belle detector at the KEKB e+ e- asymmetric energy collider.
Abstract: We observe evidence for CP violation in the decay D+ → K(S)(0)π+ using a data sample with an integrated luminosity of 977 fb(-1) collected by the Belle detector at the KEKB e+ e- asymmetric-energy collider. The CP asymmetry in the decay is measured to be (-0.363±0.094±0.067)%, which is 3.2 standard deviations away from zero, and is consistent with the expected CP violation due to the neutral kaon in the final state.

33 citations


Journal ArticleDOI
M. C. Chang1, Y. C. Duh1, J. Y. Lin1, I. Adachi  +152 moreInstitutions (51)
TL;DR: In this paper, the authors measured the branching fractions of B-0 -> J/psi eta((')) decays with the complete Belle data sample of 772 x 10(6) B (B) over bar events collected at the Y(4S) resonance with the Belle detector at the KEKB asymmetric-energy e(+)e(-) collider.
Abstract: We measure the branching fractions of B-0 -> J/psi eta((')) decays with the complete Belle data sample of 772 x 10(6) B (B) over bar events collected at the Y(4S) resonance with the Belle detector at the KEKB asymmetric-energy e(+)e(-) collider. The results for the branching fractions are: B(B-0 -> J/psi eta) = (12.3 +/-(1.8)(1.7)+/- 0.7) x 10(-6) and B(B-0 -> J/psi eta') < 7.4 x 10(-6) at 90% confidence level. The eta-eta' mixing angle is constrained to be less than 42.2 degrees at 90% confidence level.

27 citations


Journal ArticleDOI
J. Li1, I. Adachi, Hiroaki Aihara2, K. Arinstein3  +160 moreInstitutions (51)
TL;DR: In this paper, the first observations of B-s(0)-> J/psi eta were reported from 121.4 fb(-1) of data collected at the Gamma(5S) resonance with the Belle detector at the KEKB e(+)e(-) collider.
Abstract: We report first observations of B-s(0) -> J/psi eta and B-s(0) -> J/psi eta'. The results are obtained from 121.4 fb(-1) of data collected at the Gamma(5S) resonance with the Belle detector at the KEKB e(+)e(-) collider. We obtain the branching fractions B(B-s(0)-> J/psi eta')=[5.10 +/- 0.50(stat)+/- 0.25(syst)(-0.79)(+1.14)(N-Bs(*)(B) over bars(*)] X 10(-4,) B(B-s(0)-> J/psi eta') = [3.71 +/- 0.61(stat)+/-(+0.83)(-0.57)(N-Bs(*)(B) over bars(*)] X 10(-4). The ratio of the two branching fractions is measured to be B(B-s -> J/psi eta')/B(B-s -> J/psi eta) = 0.73 +/- 0.14(stat) +/- 0.02(syst).

23 citations


Journal ArticleDOI
M. Starič, H. Aihara, K. Arinstein, D. M. Asner, T. Aushev, A. M. Bakich, A. Bay, V. Bhardwaj, B. Bhuyan, A. Bozek, M. Bračko, T. E. Browder, A. Chen, Po-Hsun Chen, B. G. Cheon, K. Chilikin, R. Chistov, I. S. Cho, K. Cho, Y. Choi, Z. Doležal, Z. Drásal, S. Eidelman, J. E. Fast, V. Gaur, N. Gabyshev, B. Golob, J. Haba, K. Hayasaka, Yasuyuki Horii, Y. Hoshi, W. S. Hou, Y. B. Hsiung, T. Iijima, K. Inami, A. Ishikawa, R. Itoh, M. Iwabuchi, Y. Iwasaki, T. Iwashita, T. Julius, J. H. Kang, T. Kawasaki, C. Kiesling, Hyunyong Kim, H. O. Kim, J. B. Kim, K. T. Kim, M. J. Kim, Y. J. Kim, K. Kinoshita, Byeong Rok Ko, Nagao Kobayashi, S. Koblitz, Peter Kodys, S. Korpar, P. Križan, T. Kumita, Y. J. Kwon, J. S. Lange, S. H. Lee, J. Li, Y. B. Li, J. Libby, C. Liu, Z. Q. Liu, R. Louvot, S. McOnie, K. Miyabayashi, H. Miyata, Y. Miyazaki, G. B. Mohanty, E. Nakano, Z. Natkaniec, S. Nishida, O. Nitoh, T. Nozaki, T. Ohshima, S. Okuno, S. L. Olsen, G. Pakhlova, H. K. Park, K. S. Park, R. Pestotnik, Marko Petrič, L. E. Piilonen, M. Röhrken, Sunmin Ryu, H. Sahoo, K. Sakai, Y. Sakai, T. Sanuki, O. Schneider, C. Schwanda, A. J. Schwartz, O. Seon, M. E. Sevior, V.E. Shebalin, C. P. Shen, T.-A. Shibata, J. G. Shiu, B. Shwartz, Frank Simon, P. Smerkol, Y. S. Sohn, Andrey Sokolov, Samo Stanič, M. Sumihama, K. Sumisawa, G. Tatishvili, Y. Teramoto, K. Trabelsi, M. Uchida, S. Uehara, T. Uglov, Y. Unno, S. Uno, Phillip Urquijo, G. S. Varner, A. Vossen, C. H. Wang, M. Z. Wang, M. Watanabe, Y. Watanabe, K. M. Williams, E. Won, Bruce Yabsley, Y. Yamashita, C. Z. Yuan, C. C. Zhang, Z. P. Zhang, V.N. Zhilich, V. V. Zhulanov, A. Zupanc 
TL;DR: In this paper, the difference between the $CP$-violating asymmetries for the Cabibbo-suppressed decays was measured, and no evidence for direct violation was found.
Abstract: We search for $CP$ violation in Cabibbo-suppressed charged $D$ meson decays by measuring the difference between the $CP$-violating asymmetries for the Cabibbo-suppressed decays ${D}^{\ifmmode\pm\else\textpm\fi{}}\ensuremath{\rightarrow}{K}^{+}{K}^{\ensuremath{-}}{\ensuremath{\pi}}^{\ifmmode\pm\else\textpm\fi{}}$ and the Cabibbo-favored decays ${D}_{s}^{\ifmmode\pm\else\textpm\fi{}}\ensuremath{\rightarrow}{K}^{+}{K}^{\ensuremath{-}}{\ensuremath{\pi}}^{\ifmmode\pm\else\textpm\fi{}}$ in the ${K}^{+}{K}^{\ensuremath{-}}$ mass region of the $\ensuremath{\phi}$ resonance. Using $955\text{ }\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ of data collected with the Belle detector, we obtain ${A}_{CP}^{{D}^{+}\ensuremath{\rightarrow}\ensuremath{\phi}{\ensuremath{\pi}}^{+}}=(+0.51\ifmmode\pm\else\textpm\fi{}0.28\ifmmode\pm\else\textpm\fi{}0.05)%$. The measurement improves the sensitivity of previous searches by more than a factor of 5. We find no evidence for direct $CP$ violation.

23 citations


Posted Content
TL;DR: In this paper, the first observation of Y(5S) → Y(1S) pi0 pi0 decays at the KEKB asymmetric-energy e+e-collider was reported.
Abstract: We report the first observation of Y(5S) -> Y(1,2S) pi0 pi0 decays. Evidence for the Zb0(10610) with 4.9sigma significance is found in a Dalitz plot analysis of Y(5S) -> Y(2S) pi0 pi0 decays. The results are obtained with a 121.4 fb^-1 data sample collected with the Belle detector at the Y(5S) resonance at the KEKB asymmetric-energy e+e- collider.

20 citations


Journal ArticleDOI
M. Starič, H. Aihara1, K. Arinstein2, D. M. Asner3, T. Aushev, A. M. Bakich4, A. Bay5, V. Bhardwaj6, B. Bhuyan7, A. Bozek8, M. Bračko9, T. E. Browder, A. Chen10, Po-Hsun Chen11, B. G. Cheon12, K. Chilikin, R. Chistov, I. S. Cho13, K. Cho14, Y. Choi15, Z. Doležal16, Z. Drásal16, S.I. Eidelman2, James E. Fast3, V. Gaur17, N. Gabyshev2, B. Golob18, J. Haba, K. Hayasaka19, Yasuyuki Horii20, Y. Hoshi21, W. S. Hou11, Y. B. Hsiung11, T. Iijima19, K. Inami19, A. Ishikawa20, R. Itoh, M. Iwabuchi13, Y. Iwasaki, T. Iwashita22, T. Julius23, J. H. Kang13, T. Kawasaki24, C. Kiesling25, H. J. Kim26, H. O. Kim26, J. B. Kim27, K. T. Kim27, M. J. Kim26, Yongsun Kim14, K. Kinoshita28, B. R. Ko27, Nagao Kobayashi29, S. Koblitz25, Peter Kodys16, S. Korpar9, P. Križan18, T. Kumita30, Y. J. Kwon13, J. S. Lange31, Sang Hoon Lee27, J. Li, Yang Li32, J. Libby33, C. Liu34, Z. Q. Liu, R. Louvot5, S. McOnie4, K. Miyabayashi22, H. Miyata24, Y. Miyazaki19, G. B. Mohanty17, E. Nakano35, Z. Natkaniec8, S. Nishida, O. Nitoh36, T. Nozaki, T. Ohshima19, S. Okuno37, S. L. Olsen38, G. Pakhlova, H. K. Park26, K. S. Park15, R. Pestotnik, Marko Petrič, L. E. Piilonen32, M. Röhrken39, Sunmin Ryu38, H. Sahoo, K. Sakai, Y. Sakai, T. Sanuki20, O. Schneider5, C. Schwanda40, A. J. Schwartz28, O. Seon19, M. E. Sevior23, V.E. Shebalin2, C. P. Shen19, T. A. Shibata29, J. G. Shiu11, B.A. Shwartz2, Frank Simon25, P. Smerkol, Y. S. Sohn13, Andrey Sokolov, Samo Stanič41, M. Sumihama42, K. Sumisawa, G. Tatishvili3, Y. Teramoto35, K. Trabelsi, M. Uchida29, S. Uehara, T. Uglov, Y. Unno12, S. Uno, Phillip Urquijo43, G. S. Varner, A. Vossen44, C. H. Wang45, M. Z. Wang11, M. Watanabe24, Y. Watanabe37, K. M. Williams32, E. Won27, Bruce Yabsley4, Y. Yamashita, C. Z. Yuan, C. C. Zhang, Z. P. Zhang34, V.N. Zhilich2, Vladimir Zhulanov2, Anze Zupanc39 
TL;DR: In this paper, the difference between CP-violating asymmetries for the Cabibbo-suppressed decays D(±)→K(+)K(-)π(±), and the Cabiba-favoured decays was measured.
Abstract: We search for CP violation in Cabibbo-suppressed charged D meson decays by measuring the difference between the CP-violating asymmetries for the Cabibbo-suppressed decays D(±)→K(+)K(-)π(±) and the Cabibbo-favored decays D(s)(±)→K(+)K(-)π(±) in the K(+)K(-) mass region of the ϕ resonance. Using 955 fb(-1) of data collected with the Belle detector, we obtain A(CP)(D+→ϕπ+)=(+0.51±0.28±0.05)%. The measurement improves the sensitivity of previous searches by more than a factor of 5. We find no evidence for direct CP violation.

20 citations


Journal ArticleDOI
TL;DR: In this paper, the authors report measurements of branching fractions and time-dependent $CP$ asymmetries in a data sample that contains pairs collected at the Belle detector at the KEKB asymmetric-energy collider.
Abstract: We report measurements of branching fractions and time-dependent $CP$ asymmetries in ${B}^{0}\ensuremath{\rightarrow}{D}^{+}{D}^{\ensuremath{-}}$ and ${B}^{0}\ensuremath{\rightarrow}{D}^{*\ifmmode\pm\else\textpm\fi{}}{D}^{\ensuremath{\mp}}$ decays using a data sample that contains $(772\ifmmode\pm\else\textpm\fi{}11)\ifmmode\times\else\texttimes\fi{}{10}^{6}B\overline{B}$ pairs collected at the $\ensuremath{\Upsilon}(4S)$ resonance with the Belle detector at the KEKB asymmetric-energy ${e}^{+}{e}^{\ensuremath{-}}$ collider. We determine the branching fractions to be $\mathcal{B}({B}^{0}\ensuremath{\rightarrow}{D}^{+}{D}^{\ensuremath{-}})=(2.12\ifmmode\pm\else\textpm\fi{}0.16\ifmmode\pm\else\textpm\fi{}0.18)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}4}$ and $\mathcal{B}({B}^{0}\ensuremath{\rightarrow}{D}^{*\ifmmode\pm\else\textpm\fi{}}{D}^{\ensuremath{\mp}})=(6.14\ifmmode\pm\else\textpm\fi{}0.29\ifmmode\pm\else\textpm\fi{}0.50)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}4}$. We measure $CP$ asymmetry parameters ${\mathcal{S}}_{{D}^{+}{D}^{\ensuremath{-}}}=\ensuremath{-}{1.06}_{\ensuremath{-}0.14}^{+0.21}\ifmmode\pm\else\textpm\fi{}0.08$ and ${\mathcal{C}}_{{D}^{+}{D}^{\ensuremath{-}}}=\ensuremath{-}0.43\ifmmode\pm\else\textpm\fi{}0.16\ifmmode\pm\else\textpm\fi{}0.05$ in ${B}^{0}\ensuremath{\rightarrow}{D}^{+}{D}^{\ensuremath{-}}$ and ${\mathcal{A}}_{{D}^{*}D}=+0.06\ifmmode\pm\else\textpm\fi{}0.05\ifmmode\pm\else\textpm\fi{}0.02$, ${\mathcal{S}}_{{D}^{*}D}=\ensuremath{-}0.78\ifmmode\pm\else\textpm\fi{}0.15\ifmmode\pm\else\textpm\fi{}0.05$, ${\mathcal{C}}_{{D}^{*}D}=\ensuremath{-}0.01\ifmmode\pm\else\textpm\fi{}0.11\ifmmode\pm\else\textpm\fi{}0.04$, $\ensuremath{\Delta}{\mathcal{S}}_{{D}^{*}D}=\ensuremath{-}0.13\ifmmode\pm\else\textpm\fi{}0.15\ifmmode\pm\else\textpm\fi{}0.04$ and $\ensuremath{\Delta}{\mathcal{C}}_{{D}^{*}D}=+0.12\ifmmode\pm\else\textpm\fi{}0.11\ifmmode\pm\else\textpm\fi{}0.03$ in ${B}^{0}\ensuremath{\rightarrow}{D}^{*\ifmmode\pm\else\textpm\fi{}}{D}^{\ensuremath{\mp}}$, where the first uncertainty is statistical and the second is systematic. We exclude the conservation of $CP$ symmetry in both decays at equal to or greater than $4\ensuremath{\sigma}$ significance.

Journal ArticleDOI
Z. Q. Liu, C. P. Shen1, C. Z. Yuan, T. Iijima1  +160 moreInstitutions (48)
TL;DR: In this paper, the processes γγ → ωϕ, ϕϕ and ωω were measured using an 870 fb(-1) data sample collected with the Belle detector at the KEKB asymmetric-energy e+ e-collider.
Abstract: The processes γγ → ωϕ, ϕϕ, and ωω are measured using an 870 fb(-1) data sample collected with the Belle detector at the KEKB asymmetric-energy e+ e- collider. Production of vector meson pairs is clearly observed and their cross sections are measured for masses that range from threshold to 4.0 GeV. In addition to signals from well established spin-zero and spin-two charmonium states, there are resonant structures below charmonium threshold, which have not been previously observed. We report a spin-parity analysis for the new structures and determine the products of the η(c), χ(c0), and χ(c2) two-photon decay widths and branching fractions to ωϕ, ϕϕ, and ωω.


Journal ArticleDOI
K. Negishi1, Yasuyuki Horii2, Y. Onuki3, T. Sanuki1, Hitoshi Yamamoto1, I. Adachi, Hiroaki Aihara3, D. M. Asner4, Tagir Aushev, A. M. Bakich5, Y. Ban6, K. Belous, B. Bhuyan7, A.E. Bondar8, T. E. Browder, M. C. Chang9, A. Chen10, Po-Hsun Chen11, B. G. Cheon12, K. Chilikin, R. Chistov, I. S. Cho13, K. Cho14, Y. Choi15, J. Dalseno16, Z. Doleal17, Z. Drásal17, A. Drutskoy, Semen Eidelman8, James E. Fast4, V. Gaur18, N. Gabyshev8, Y. M. Goh12, J. Haba, H. Hayashii19, Y. Hoshi20, W. S. Hou11, H. J. Hyun21, Toru Iijima2, K. Inami2, A. Ishikawa1, R. Itoh, M. Iwabuchi13, Y. Iwasaki, T. Iwashita19, T. Julius22, J. H. Kang13, T. Kawasaki23, C. Kiesling16, H. J. Kim21, J. B. Kim24, Jung-Hyun Kim14, K. T. Kim24, M. J. Kim21, Yongsun Kim14, B. R. Ko24, P. Kody17, Samo Korpar25, Richard T. Kouzes4, Pavel Krokovny8, T. Kuhr26, Y. J. Kwon13, S. H. Lee24, J. Libby27, Chang Liu28, Yueh-Feng Liu29, Z. Q. Liu, R. Louvot30, D. Matvienko8, S. McOnie5, K. Miyabayashi19, H. Miyata23, Y. Miyazaki2, D. Mohapatra4, A. Moll16, Norihito Muramatsu1, E. Nakano31, M. Nakao, S. Nishida, K. Nishimura, O. Nitoh32, S. Ogawa33, T. Ohshima2, S. Okuno34, G. Pakhlova, H. K. Park21, T. K. Pedlar35, R. Pestotnik, Marko Petrič, Leo Piilonen36, M. Röhrken26, Sunmin Ryu37, K. Sakai, Y. Sakai, O. Schneider30, C. Schwanda38, A. J. Schwartz29, K. Senyo39, M. E. Sevior22, M. Shapkin, V.E. Shebalin8, T. A. Shibata40, J. G. Shiu11, B.A. Shwartz8, A.L. Sibidanov5, Frank Simon16, P. Smerkol, Y. S. Sohn13, E. Solovieva, Samo Stanič41, M. Starič, M. Sumihama42, T. Sumiyoshi43, S. Suzuki44, G. Tatishvili4, Y. Teramoto31, K. Trabelsi, M. Uchida40, T. Uglov, Y. Unno12, S. Uno, Phillip Urquijo45, G. Varner, Kevin Varvell5, V. Vorobyev8, C. H. Wang46, M. Z. Wang11, P. Wang, M. Watanabe23, Y. Watanabe34, E. Won24, Bruce Yabsley5, Y. Yamashita, C. C. Zhang, Zhenyu Zhang28, V. Zhilich8, Vladimir Zhulanov8, Anze Zupanc26 
TL;DR: In this paper, the decay of B-0 → DK+ pi(-) followed by D-0 or K-pi(+) over bar (0) was investigated. But the decay rate was not shown to be (4.5(-5.0-1.8)) X 10(-2).
Abstract: We report a study of the decay B-0 -> DK+ pi(-) followed by D -> K- pi(+) , where D indicates D-0 or (D) over bar (0). We reconstruct the DK+ pi(-) state in a phase space corresponding to DK*(892)(0). The CP-violating angle phi(3) affects its decay rate via the interference between b -> u and b -> c transitions. The result is obtained from a 711 fb(-1) data sample that contains 772 X 10(6)B (B) over bar pairs collected at the Y(4S) resonance with the Belle detector at the KEKB asymmetric-energy e(+) e(-) collider. We measure the ratio R-DK*0 Gamma(B-0 -> [K- pi(+) ](D)K+ pi(-))/Gamma(B-0 -> [K+ pi(-)](D)K+ pi(-)) to be (4.5(-5.0-1.8)(+5.6+2.8)) X 10(-2), and set an upper limit of R-DK*0 < 0.16 at the 95% credible interval.

Journal ArticleDOI
C. P. Shen1, C. Z. Yuan, Toru Iijima1, I. Adachi, Hiroaki Aihara2, K. Arinstein3, D. M. Asner4, Tagir Aushev, A. M. Bakich5, B Bhuyan6, M. Bischofberger7, A. Bozek8, M. Bračko9, T. E. Browder, M. C. Chang10, A. Chen11, B. G. Cheon12, K. Chilikin, R. Chistov, I. S. Cho13, K. Cho14, S. K. Choi15, Y. Choi16, J. Dalseno17, Z. Drásal18, A. Drutskoy, Semen Eidelman3, J. E. Fast4, V. Gaur19, N. Gabyshev3, A. Garmash3, Y. M. Goh12, J. Haba, T. Hara, K. Hayasaka1, H. Hayashii7, Yasuyuki Horii1, Y. Hoshi20, W. S. Hou21, H. J. Hyun22, A. Ishikawa23, R. Itoh, M. Iwabuchi13, T. Iwashita7, T. Julius24, J. H. Kang13, T. Kawasaki25, H. J. Kim22, H. O. Kim22, J. B. Kim26, K. T. Kim26, M. J. Kim22, Yongsun Kim14, B. R. Ko26, S. Koblitz17, P. Kody18, Samo Korpar9, P. Krian27, P. Krokovny3, T. Kumita28, Y. J. Kwon13, J. S. Lange29, S. H. Lee26, J. Li30, J. Libby31, C. L. Lim13, Chang Liu32, Z. Q. Liu, D. Liventsev, R. Louvot33, S. McOnie5, K. Miyabayashi7, H. Miyata25, Y. Miyazaki1, R. Mizuk, G. B. Mohanty19, A. Moll17, T. Mori1, Norihito Muramatsu34, R. Mussa, E. Nakano35, M. Nakao, H. Nakazawa11, S. Nishida, K. Nishimura, O. Nitoh36, S. Ogawa37, T. Ohshima1, S. Okuno38, Stephen Lars Olsen30, Y. Onuki2, G. Pakhlova, C. W. Park16, H. K. Park22, T. K. Pedlar39, Marko Petrič, Leo Piilonen40, Anton Poluektov3, M. Ritter17, M. Röhrken41, H. Sahoo, Y. Sakai, T. Sanuki23, Y. Sato23, O. Schneider33, C. Schwanda42, K. Senyo43, O. Seon1, M. Shapkin, T. A. Shibata44, J. G. Shiu21, A.L. Sibidanov5, Frank Simon17, Jasvinder A. Singh45, P. Smerkol, Y. S. Sohn13, E. Solovieva, S. Stanič46, M. Starič, T. Sumiyoshi28, G. Tatishvili4, Y. Teramoto35, T. Tsuboyama, M. Uchida44, Sadaharu Uehara, Y. Unno12, S. Uno, Phillip Urquijo47, G. Varner, Kevin Varvell5, C. H. Wang48, P. Wang, X. L. Wang, M. Watanabe25, Y. Watanabe38, E. Won26, Y. Yamashita, Y. Yusa25, Zhenyu Zhang32, V. Zhilich3, Vladimir Zhulanov3, Anze Zupanc41 
TL;DR: In this paper, double-charmonium decays of the P-wave spin-triplet bottomonium states (Y(2S) -> gamma chi(bJ), chi (bJ) = 0.
Abstract: Using a sample of 158 x 10(6) Y(2S) events collected with the Belle detector, we search for the first time for double-charmonium decays of the P-wave spin-triplet bottomonium states (Y(2S) -> gamma chi(bJ), chi(bJ) -> J/psi J/psi, J/psi psi', psi'psi' for J 0, 1, and 2). No significant chi(bJ) signal is observed in the double-charmonium mass spectra, and we obtain the following upper limits: B(chi(bJ) -> J/psi J/psi) J/psi psi') psi'psi') < 3.1 x 10(-5), 6.2 x 10(-5), 1.6 x 10(-5) for J = 0, 1, and 2, respectively, at the 90% confidence level. These limits are significantly lower than the central values (with uncertainties of 50% to 70%) predicted using the light cone formalism but are consistent with calculations using the nonrelativistic QCD (NRQCD) factorization approach.

Journal ArticleDOI
B. Kronenbitter1, I. Adachi, Hiroaki Aihara2, K. Arinstein3  +158 moreInstitutions (42)
TL;DR: In this paper, the branching fraction, the polarization, and the parameters of the time-dependent CP violation in B-0 -> D*(+) D* (-) decays using a data sample of 772 x 10(6)B (B) over bar pairs, collected at the Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric energy e(+)e(-) collider.
Abstract: We report the measurement of the branching fraction, the polarization, and the parameters of the time-dependent CP violation in B-0 -> D*(+) D*(-) decays using a data sample of 772 x 10(6)B (B) over bar pairs, collected at the Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e(+)e(-) collider. We obtain a branching fraction of B = (7.82 +/- 0.38 +/- 0.63) x 10(-4), a CP-odd fraction of R-perpendicular to = 0.138 +/- 0.024 +/- 0.006 and, additionally, a fraction of the longitudinal component in the transversity base of R-0 = 0.624 +/- 0.029 +/- 0.011. The measured values of the parameters of the CP violation are SD*+ D*- = 0.79 +/- 0.13 +/- 0.03 and A(D*+ D*-) 0.15 +/- 0.08 +/- 0.04.

Journal ArticleDOI
Yukinori Sato1, Hitoshi Yamamoto1, H. Aihara2, D. M. Asner3  +158 moreInstitutions (48)
TL;DR: A measurement of the CP-violation parameter sin2φ1 at the Υ(5S) resonance is reported using a new tagging method, called "B-π tagging," which yields results based on 121 fb(-1) of data recorded by the Belle detector at the KEKB e(+)e(-) collider.
Abstract: We report a measurement of the CP-violation parameter sin2 phi(1) at the gamma(5S) resonance using a new tagging method, called "B-pi tagging." In gamma(5S) decays containing a neutral B meson, a charged B, and a charged pion, the neutral B is reconstructed in the J/psi K-S(0) CP-eigenstate decay channel. The initial flavor of the neutral B meson at the moment of the gamma(5S) decay is opposite to that of the charged B and may thus be inferred from the charge of the pion without reconstructing the charged B. From the asymmetry between B-pi(+) and B-pi(-) tagged J/psi K-S(0) yields, we determine sin2 phi(1) 0.57 +/- 0.58(stat) +/- 0.06(syst). The results are based on 121 fb(-1) of data recorded by the Belle detector at the KEKB e(+) e(-) collider.

Journal ArticleDOI
Jung-Hyun Kim1, Jung-Hyun Kim2, M. Nakao, I. Adachi  +148 moreInstitutions (46)
TL;DR: In this article, the authors report on a search for the charmless decays in the Standard Model for the σ-decays of σ + σ σ − σ to σ -π -to σ−σ −σ−π to ρ − ρ -to-π σπ −ρ −toρ σ 0.
Abstract: We report on a search for the charmless decays $B^{+} \to\phi\pi^{+}$ and $B^{0} \to\phi \pi^{0}$ that are strongly suppressed in the Standard Model. The analysis is based on a data sample of $657 \times 10^6$ $B \bar{B}$ pairs collected at the $\Upsilon(4S)$ resonance with the Belle detector at the KEKB asymmetric-energy $e^+ e^-$ collider. We find no significant signal and set upper limits of $3.3 \times 10^{-7}$ for $B^{+} \to \phi \pi^{+}$ and $1.5 \times 10^{-7}$ for $B^0 \to \phi \pi^0$ at the 90% confidence level.

Journal ArticleDOI
J. Stypula1, M. Rozanska1, I. Adachi, K. Adamczyk1  +164 moreInstitutions (46)
TL;DR: In this paper, the decays of B- -> Ds(*)+ K- l- nubar in a data sample containing 657x10^6 BBbar pairs collected with the Belle detector at the KEKB asymmetric-energy e+e- collider were reported.
Abstract: We report measurements of the decays B- -> Ds(*)+ K- l- nubar in a data sample containing 657x10^6 BBbar pairs collected with the Belle detector at the KEKB asymmetric-energy e+e- collider. We observe a signal with a significance of 6 sigma for the combined Ds and Ds* modes and find the first evidence of the B- -> Ds+ K- l- nubar decay with a significance of 3.4 sigma. We measure the following branching fractions: BF(B- -> Ds+ K- l nubar) = (0.30 +/- 0.09(stat) +0.11 -0.08(syst)) x 10^-3 and BF(B- -> Ds*+ K- l- nubar) = (0.59 +/- 0.12(stat) +/- 0.15(syst)) x 10^-3 and set an upper limit BF(B- -> Ds*+ K- l- nubar) < 0.56 x 10^-3 at the 90% confidence level. We also present the first measurement of the Ds+K- invariant mass distribution in these decays, which is dominated by a prominent peak around 2.6 GeV/c^2.

Journal ArticleDOI
C. P. Shen1, C. Z. Yuan, Toru Iijima1, I. Adachi  +151 moreInstitutions (48)
TL;DR: In this article, exclusive hadronic decays of these two bottomonium resonances to the three-body final states phi K+K-, omega pi(+)pi(-) and K*(0)(892)K-pi(+) were studied.
Abstract: Using samples of 102 x 10(6) Gamma(1S) and 158 x 10(6) Gamma(2S) events collected with the Belle detector, we study exclusive hadronic decays of these two bottomonium resonances to the three-body final states phi K+K-, omega pi(+)pi(-) and K*(0)(892)K-pi(+), and to the two-body Vector-Tensor states (phi f'(2)(1525), omega f(2)(1270), rho a(2)(1320) and K*(0)(892)(K) over bar*(0)(2)(1430)) and Axial-vector-Pseudoscalar (K-1(1270)K-+(-), K-1(1400)K-+(-) and b(1)(1235)(+)pi(-)) states. Signals are observed for the first time in the Y(1S) -> phi K+K-, omega pi(+)pi(-), K*K-0(-)pi(+), K*K-0*(0)(2) Gamma(2S) -> phi K+K-, K*K-0(-)pi(+) decay modes. Branching fractions are determined for all the processes, while 90% confidence level upper limits are established on the branching fractions for the modes with a statistical significance less than 3 sigma. The ratios of the branching fractions of Gamma(2S) and Gamma(1S) decays into the same final state are used to test a perturbative QCD prediction for OZI-suppressed bottomonium decays.

Journal ArticleDOI
TL;DR: In this paper, the authors report on a search for the charmless decays that are strongly suppressed in the standard model and find no significant signal and set upper limits of $3.3 and $1.5 at the 90% confidence level.
Abstract: We report on a search for the charmless decays ${B}^{+}\ensuremath{\rightarrow}\ensuremath{\phi}{\ensuremath{\pi}}^{+}$ and ${B}^{0}\ensuremath{\rightarrow}\ensuremath{\phi}{\ensuremath{\pi}}^{0}$ that are strongly suppressed in the standard model. The analysis is based on a data sample of $657\ifmmode\times\else\texttimes\fi{}{10}^{6}$ $B\overline{B}$ pairs collected at the $\ensuremath{\Upsilon}(4S)$ resonance with the Belle detector at the KEKB asymmetric-energy ${e}^{+}{e}^{\ensuremath{-}}$ collider. We find no significant signal and set upper limits of $3.3\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}7}$ for ${B}^{+}\ensuremath{\rightarrow}\ensuremath{\phi}{\ensuremath{\pi}}^{+}$ and $1.5\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}7}$ for ${B}^{0}\ensuremath{\rightarrow}\ensuremath{\phi}{\ensuremath{\pi}}^{0}$ at the 90% confidence level.

Posted Content
23 Aug 2012
TL;DR: In this article, the authors measured the branching fraction of B- -> tau- nu_tau-bar using the full Upsilon(4S) data sample containing 772*10^6 BBbar pairs collected with the Belle detector at the KEKB asymmetric-energy e+e- collider.
Abstract: We measure the branching fraction of B- -> tau- nu_tau-bar using the full Upsilon(4S) data sample containing 772*10^6 BBbar pairs collected with the Belle detector at the KEKB asymmetric-energy e+e- collider. Events with BBbar pairs are tagged by reconstructing one of the B mesons decaying into hadronic final states, and B- -> tau- nu_tau-bar candidates are detected in the recoil. We find evidence for B- -> tau- nu_tau-bar with a significance of 3.0 standard deviations including systematic errors and measure a branching fraction B(B- -> tau- nu_tau-bar) = [0.72^{+0.27}_{-0.25}(stat) +/- 0.11(syst)] * 10^-4.