First evidence for $\cos 2\beta>0$ and resolution of the CKM Unitarity Triangle ambiguity by a time-dependent Dalitz plot analysis of $B^{0} \to D^{(*)} h^{0}$ with $D \to K_{S}^{0} \pi^{+} \pi^{-}$ decays

I. Adachi,G. Simi, S. Vahsen, G. Marchiori,R. Prepost,K. Tanida,M. Carpinelli,T. Uglov,E. Won,D. Matvienko,P. Ongmongkolkul,K. Cho, Z. P. Zhang,M. Iwasaki,R. Godang,R. Faccini,R. Kowalewski, Y. Watanabe,F. Ferroni, D. J. Lange,T. S. Miyashita,F. C. Porter,L. Santelj,H. Hayashii,J. B. Kim,W. S. Lockman, Y. Sakai, J. Haba, A. Lusiani,A. Palano,V. Poireau,Vladimir Popov, M. Piccolo, E. Solovieva, A. V. Gritsan, G. Varner, J. P. Coleman,N. Arnaud,T.-A. Shibata,T. Leddig,P. Kim,M. T. Hedges,H. Ono,H. Miyata, D. Červenkov, D. N. Brown,M. Gelb,F. Forti,S. Akar,T. Luo, M. Nayak,W.-S. Hou,S. Eidelman,H. Ahmed,R. Mussa,R. Kroeger, H. Aihara,T. Schroeder, S. Prell,T. Sanuki, M. Wang, H. K. Moon,J. G. Smith,T. Sumiyoshi, A. Chen,G. Cowan, S. R. Wagner,M. Starič,T. E. Browder, K. J. Nath, N. Guttman,P. Pakhlov,D. M. Asner,E. M. T. Puccio,M. Salehi, K. Senyo,V. Bansal, D. Hutchcroft,V. Shebalin,M. Rotondo, C. H. Wang,R. F. Schwitters,C. Hast,E. Grauges, E. Fioravanti,I. Badhrees,D. Bettoni, A. Filippi, D. Kotchetkov,A. Kuzmin,R. Calabrese,H. M. Lacker,Yu. I. Skovpen, S. J. Sekula,T. Nanut, T. Hara,A. Calcaterra,J. Chauveau,Somnath Choudhury,M. V. Purohit, B. K. Pal,M. Uchida, P. K. Behera, M. Margoni, D. Liventsev,R. Kulasiri,H. Kichimi,H. Ye,M. Takizawa,M. Davier,K. Hayasaka, T. Adye,I. S. Lee, I. Garzia,T. Mori, C. Z. Yuan, K.Yu. Todyshevx,G. B. Mohanty,G. Vasseur, N. Shimizu,G. J. King,V. Zhukova,A. Giri,A. M. Eisner,V. P. Druzhinin,C. Cartaro,A. R. Buzykaev, J. Ocariz,B. Dey,J. Libby,G. De Nardo,M. Rama,R. Cowan,M. Heck,Rocky Bala Garg, A. Zallo, C. Bünger,P.K. Resmi, A. Hafner, R. Waldi,M. Heß, Y. Guan,Z. Huard, S. Luitz,J. G. Shiu, G. Karyan, C. Bozzi,L. E. Piilonen,S. Dittrich, A. J. Bevan, E. P. Solodov, F. Martinez-Vidal, M. Posocco,W. W. Jacobs,A. M. Lutz,M. Lubej,G. Rizzo,D. A. Roberts, S. Hirose,E. Luppi, Yongmin Li,J. W. Gary, T. Ferber,G. Wormser,S. Emery,R. Y. So,A. Jawahery,Z. Doležal,V. Zhulanov,R. Ayad,D. W. G. S. Leith,C. Hsu,R. Cenci,S. Martellotti, J. A. McKenna,G. Batignani,W. Panduro Vazquez, T. Gershon, D. B. MacFarlane, A. J. Schwartz, C. P. Jessop,P. R. Burchat,A. G. Denig,J. L. Ritchie,M. T. Graham, N. Neri, G. Cibinetto,Songkyo Lee,A. Garmash, M. K. Sullivan,M. Ebert,A. Beaulieu,G. Raven, K. T. Kim,C. Van Hulse, R. Itoh, R. J. Sobie, Y. Iwasaki,K. Honscheid,D. R. Muller,K. T. Flood, V. Savinov,F. Bianchi,B. Oberhof, E. Nakano, S. Nishida,T. Aushev,D. Aston, E. Ben-Haim,A. M. Bakich,S. Di Carlo,I. M. Peruzzi,R. C. Field,J. MacNaughton,G. D. Lafferty,F. Le Diberder,J. P. Lees, G. Eigen,E. Guido, C. P. Shen,M. Masuda, K. Sumisawa, C. Patrignani,V. Vorobyev, Y. Choi,K. K. Joo, M. Bračko, H. Park,M. Verderi,A. B. Kaliyar, M. Chrzaszcz,E. Manoni,P. Kodys,B. G. Cheon,B. G. Pushpawela, S. L. Wu,R. Cheaib,E. Waheed,S. I. Serednyakov,R. Kass,Sokoloff,S. Zakharov, R. J. Barlow, B. Echenard,M. Merola,F. Di Lodovico, F. F. Wilson,V. Zhilich,S. Uno, F. Anulli, S. Korpar,D. M. Wright, A. J. S. Smith,R. de Sangro,R. Mizuk,T. Matsuda, D. Y. Kim,M. Bellis,N. K. Nisar,D. S. Chao, K. Griessinger,W. Gradl, O. Schneider,B. T. Meadows, Y. Kwon, H. Atmacan,J. Va'vra,O. Seon,M. E. Sevior,B. N. Ratcliff,S. Bettarini, F. Simonetto,J. Walsh,A. Randle-Conde, Y. Jin,U. Tamponi, G. Finocchiaro,P. Križan, C. Schwanda,T. S. Mattison, D. J. Payne, D. Bernard,V. E. Blinov,L. Li, K. Chilikin, F. Tenchini, R. Gorodeisky,D. Gamba,Sw. Banerjee,J. M. LoSecco,T. Muller,S. Paul,C. Voß,A. Pilloni,Alam,E. Paoloni,Bingran Wang,K. R. Schubert,W. Dunwoodie,A. Bondar,L. Lanceri,O. Long, D. Cinabro, A. Oyanguren, G. Calderini,L. Cremaldi, R. Stroili,A. J. Lankford,O. Grünberg, K. Miyabayashi,J. M. Izen,W. J. Wisniewski, M. Biasini,T. Kumita, C. Chen, S. Sandilya, L. Sun, X. C. Lou,V. Santoro, C. Sciacca, Y. Onuki, J. S. Lange,A. P. Onuchin, F. U. Bernlochner,J. Kim, D. Epifanov,R. Pestotnik,I. M. Nugent,V. Babu,S. Al Said, M. Bomben,M. Röhrken,S. H. Robertson, S. H. Kim,P. Taras,D. J. Summers,G. Russo,M. Ritter, P. Wang,B. Golob, A. Ishikawa,B. G. Fulsom, J. Cochran,A. Bozek, J. Biswal, A. M. Rossi, G. Inguglia,J. Fast, H. Koch, J. Albert,L. Vitale,E. A. Kravchenko, K. Inami,S. Ogawa,V. B. Golubev,T. Julius,T. E. Latham,S. Cunliffe,D. R. Peimer, Z. Drásal, P. Patteri,T. K. Pedlar, I. Pavelkin,B. Bhuyan,M. Rozanska,K. Kinoshita, C. H. Cheng, Yu. G. Kolomensky, Giorgi,Y. Li,V. Bhardwaj,V. Gaur, R. Sacco, Y. Unno,A. Roodman, K. H. Kang,D. G. Hitlin,P. F. Harrison, G. R. Bonneaud,A. Gaz, A. Zupanc, M. Nakao,M. Feindt, P. Goldenzweig,J. Ernst, T. Lueck,F. Palombo, S. Jia, J. R. Wilson,G. Casarosa,P. Krokovny,C. Touramanis, S. Passaggio,J. Dorfan,F. Simon,N. Dash, S. Pardi, Y. Seino,H. Neal,S. M. Spanier,J.K. Ahn,T. Kuhr,U. Mallik, Y. Yusa,R.M. Seddon, F. Ferrarotto,G. Schnell, C. Hearty,J. M. Roney,L. Zani,C. L. Davis, G. Pakhlova, L. Li Gioi, G.Piredda affiliation{INFN Sezione di Roma, A. Soffer, V. Tisserand,M. Fritsch,N. Tasneem,M. R. Convery,F. De Mori

arXiv: High Energy Physics - Experiment(2018)

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摘要
We present first evidence that the cosine of the CP-violating weak phase $2beta$ is positive, and hence exclude trigonometric multifold solutions of the CKM Unitarity Triangle using a time-dependent Dalitz plot analysis of $B^{0} D^{(*)} h^{0}$ with $D K_{S}^{0} pi^{+} pi^{-}$ decays, where $h^{0} {pi^{0}, eta, omega }$ denotes a light unflavored and neutral hadron. The measurement is performed combining the final data sets of the BaBar and Belle experiments collected at the $Upsilon(4S)$ resonance at the asymmetric-energy B factories PEP-II at SLAC and KEKB at KEK, respectively. The data samples contain $( 471 pm 3 )times 10^6, Bbar{B}$ pairs recorded by the BaBar detector and $( 772 pm 11 )times 10^6, Bbar{B}$ pairs recorded by the Belle detector. The results of the measurement are $sin{2beta} = 0.80 pm 0.14 ,(rm{stat.}) pm 0.06 ,(rm{syst.}) pm 0.03 ,(rm{model})$ and $cos{2beta} = 0.91 pm 0.22 ,(rm{stat.}) pm 0.09 ,(rm{syst.}) pm 0.07 ,(rm{model})$. The result for the direct measurement of the angle $beta$ of the CKM Unitarity Triangle is $beta = left( 22.5 pm 4.4 ,(rm{stat.}) pm 1.2 ,(rm{syst.}) pm 0.6 ,(rm{model}) right)^{circ}$. The quoted model uncertainties are due to the composition of the $D^{0} K_{S}^{0} pi^{+} pi^{-}$ decay amplitude model, which is newly established by performing a Dalitz plot amplitude analysis using a high-statistics $e^{+}e^{-} cbar{c}$ data sample. CP violation is observed in $B^{0} D^{(*)} h^{0}$ decays at the level of $5.1$ standard deviations. The significance for $cos{2beta}u003e0$ is $3.7$ standard deviations. The trigonometric multifold solution $pi/2 - beta = (68.1 pm 0.7)^{circ}$ is excluded at the level of $7.3$ standard deviations. The measurement resolves an ambiguity in the determination of the apex of the CKM Unitarity Triangle.
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