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We predict branching ratios and CP asymmetries of the $B\to KK$ decays using perturbative QCD factorization theorem, in which tree, penguin, and annihilation contributions, including both factorizable and nonfactorizable ones, are expressed…

High Energy Physics - Phenomenology · Physics 2009-10-31 Chuan-Hung Chen , Hsiang-nan Li

We study CP asymmetries in penguin-induced b -> s\bar{s}s decays in general left-right models without imposing manifest or pseudomanifest left-right symmetry. Using the effective Hamiltonian approach, we evaluate CP asymmetries in B^\pm ->…

High Energy Physics - Phenomenology · Physics 2011-03-23 Soo-hyeon Nam

We formulate the most-general time-dependent decay distributions of $B_s\to J/\psi (\to l^+l^-) \phi(\to K^+K^-)$ in which the direct CP violation is explicitly incorporated. We then investigate the $B \to J/\psi V$ decays in the…

High Energy Physics - Phenomenology · Physics 2015-07-13 Xin Liu , Wei Wang , Yuehong Xie

We discuss the correlations of charming penguin contributions to $B\to\pi\pi$, $\pi K$ and KK using approximate flavor SU(3) symmetry. Strong constraints are found from the direct CP asymmetries especially in $\pi K$ modes. We make a global…

High Energy Physics - Phenomenology · Physics 2010-01-21 Yue-Liang Wu , Yu-Feng Zhou , Ci Zhuang

Major new experimental efforts on detecting CP violation in $B$ decays will very soon go on the air. Recent developments suggest that final state interaction phases in exclusive decays of $B$ are unlikely to be small indicating the…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. Atwood , A. Soni

It is commonly believed that a careful investigation of the subleading terms is crucial for a better understanding of the $QCD$ factorization in charmless B decays. In this work the penguin-dominated $B\to K\pi$ decays are discussed…

High Energy Physics - Phenomenology · Physics 2011-01-27 Tao Huang , Lin Li , Xue-Qian Li , Zuo-Hong Li , Xiang-Yao Wu

In the Standard Model (SM) charmless hadronic decays $B_s^0 \rightarrow \eta^\prime \eta$ proceed via tree-level $b\to u$ and penguin $b\to s$ transitions. Penguin transitions are sensitive to Beyond-the-Standard-Model (BSM) physics…

High Energy Physics - Experiment · Physics 2020-09-15 Belle Collaboration , A. Abdesselam , I. Adachi , K. Adamczyk , J. K. Ahn , H. Aihara , S. Al Said , K. Arinstein , Y. Arita , D. M. Asner , H. Atmacan , V. Aulchenko , T. Aushev , R. Ayad , T. Aziz , V. Babu , S. Bahinipati , A. M. Bakich , Y. Ban , E. Barberio , M. Barrett , M. Bauer , P. Behera , C. Beleño , K. Belous , J. Bennett , M. Berger , F. Bernlochner , M. Bessner , D. Besson , V. Bhardwaj , B. Bhuyan , T. Bilka , J. Biswal , T. Bloomfield , A. Bobrov , A. Bondar , G. Bonvicini , A. Bozek , M. Bračko , N. Braun , F. Breibeck , T. E. Browder , M. Campajola , L. Cao , G. Caria , D. Červenkov , M. -C. Chang , P. Chang , Y. Chao , V. Chekelian , A. Chen , K. -F. Chen , Y. Chen , Y. -T. Chen , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -J. Cho , V. Chobanova , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , J. Crnkovic , S. Cunliffe , T. Czank , S. Das , N. Dash , G. De Nardo , R. Dhamija , F. Di Capua , J. Dingfelder , Z. Doležal , T. V. Dong , D. Dossett , Z. Drásal , S. Dubey , S. Eidelman , D. Epifanov , M. Feindt , T. Ferber , A. Frey , O. Frost , B. G. Fulsom , R. Garg , V. Gaur , N. Gabyshev , A. Garmash , M. Gelb , J. Gemmler , D. Getzkow , F. Giordano , A. Giri , P. Goldenzweig , B. Golob , D. Greenwald , M. Grosse Perdekamp , J. Grygier , O. Grzymkowska , Y. Guan , E. Guido , H. Guo , J. Haba , C. Hadjivasiliou , P. Hamer , K. Hara , T. Hara , O. Hartbrich , J. Hasenbusch , K. Hayasaka , H. Hayashii , X. H. He , M. Heck , M. T. Hedges , D. Heffernan , M. Heider , A. Heller , M. Hernandez Villanueva , T. Higuchi , S. Hirose , K. Hoshina , W. -S. Hou , Y. B. Hsiung , C. -L. Hsu , K. Huang , M. Huschle , Y. Igarashi , T. Iijima , M. Imamura , K. Inami , G. Inguglia , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , S. Iwata , W. W. Jacobs , I. Jaegle , E. -J. Jang , H. B. Jeon , S. Jia , Y. Jin , D. Joffe , M. Jones , C. W. Joo , K. K. Joo , T. Julius , J. Kahn , H. Kakuno , A. B. Kaliyar , J. H. Kang , K. H. Kang , P. Kapusta , G. Karyan , S. U. Kataoka , Y. Kato , H. Kawai , T. Kawasaki , T. Keck , H. Kichimi , C. Kiesling , B. H. Kim , C. H. Kim , D. Y. Kim , H. J. Kim , H. -J. Kim , J. B. Kim , K. -H. Kim , K. T. Kim , S. H. Kim , S. K. Kim , Y. J. Kim , Y. -K. Kim , T. Kimmel , H. Kindo , K. Kinoshita , C. Kleinwort , J. Klucar , N. Kobayashi , P. Kodyš , Y. Koga , I. Komarov , T. Konno , S. Korpar , D. Kotchetkov , P. Križan , R. Kroeger , J. -F. Krohn , P. Krokovny , B. Kronenbitter , T. Kuhr , R. Kulasiri , M. Kumar , R. Kumar , K. Kumara , T. Kumita , E. Kurihara , Y. Kuroki , A. Kuzmin , P. Kvasnička , Y. -J. Kwon , Y. -T. Lai , K. Lalwani , J. S. Lange , I. S. Lee , J. K. Lee , J. Y. Lee , S. C. Lee , M. Leitgab , R. Leitner , D. Levit , P. Lewis , C. H. Li , H. Li , J. Li , L. K. Li , Y. Li , Y. B. Li , L. Li Gioi , J. Libby , K. Lieret , A. Limosani , Z. Liptak , C. Liu , Y. Liu , D. Liventsev , A. Loos , R. Louvot , M. Lubej , T. Luo , J. MacNaughton , M. Masuda , T. Matsuda , D. Matvienko , J. T. McNeil , M. Merola , F. Metzner , K. Miyabayashi , Y. Miyachi , H. Miyake , H. Miyata , Y. Miyazaki , R. Mizuk , G. B. Mohanty , S. Mohanty , H. K. Moon , T. J. Moon , T. Mori , T. Morii , H. -G. Moser , M. Mrvar , T. Müller , N. Muramatsu , R. Mussa , Y. Nagasaka , Y. Nakahama , I. Nakamura , K. R. Nakamura , E. Nakano , T. Nakano , M. Nakao , H. Nakayama , H. Nakazawa , T. Nanut , K. J. Nath , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , C. Ng , C. Niebuhr , M. Niiyama , N. K. Nisar , S. Nishida , K. Nishimura , O. Nitoh , A. Ogawa , K. Ogawa , S. Ogawa , T. Ohshima , S. Okuno , S. L. Olsen , H. Ono , Y. Onuki , P. Oskin , W. Ostrowicz , C. Oswald , H. Ozaki , P. Pakhlov , G. Pakhlova , B. Pal , T. Pang , E. Panzenböck , S. Pardi , C. -S. Park , C. W. Park , H. Park , K. S. Park , S. -H. Park , S. Patra , S. Paul , T. K. Pedlar , T. Peng , L. Pesántez , R. Pestotnik , M. Peters , L. E. Piilonen , T. Podobnik , V. Popov , K. Prasanth , E. Prencipe , M. T. Prim , K. Prothmann , M. V. Purohit , A. Rabusov , J. Rauch , B. Reisert , P. K. Resmi , E. Ribežl , M. Ritter , M. Röhrken , J. Rorie , A. Rostomyan , N. Rout , M. Rozanska , G. Russo , D. Sahoo , Y. Sakai , M. Salehi , S. Sandilya , D. Santel , L. Santelj , T. Sanuki , J. Sasaki , N. Sasao , Y. Sato , V. Savinov , T. Schlüter , O. Schneider , G. Schnell , M. Schram , J. Schueler , C. Schwanda , A. J. Schwartz , B. Schwenker , R. Seidl , Y. Seino , D. Semmler , K. Senyo , O. Seon , I. S. Seong , M. E. Sevior , L. Shang , M. Shapkin , C. Sharma , V. Shebalin , C. P. Shen , T. -A. Shibata , H. Shibuya , S. Shinomiya , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , J. B. Singh , R. Sinha , K. Smith , A. Sokolov , Y. Soloviev , E. Solovieva , S. Stanič , M. Starič , M. Steder , Z. Stottler , J. F. Strube , J. Stypula , S. Sugihara , A. Sugiyama , M. Sumihama , K. Sumisawa , T. Sumiyoshi , W. Sutcliffe , K. Suzuki , K. Suzuki , S. Suzuki , S. Y. Suzuki , H. Takeichi , M. Takizawa , U. Tamponi , M. Tanaka , S. Tanaka , K. Tanida , N. Taniguchi , Y. Tao , G. N. Taylor , F. Tenchini , Y. Teramoto , A. Thampi , K. Trabelsi , T. Tsuboyama , M. Uchida , I. Ueda , S. Uehara , T. Uglov , Y. Unno , S. Uno , P. Urquijo , Y. Ushiroda , Y. Usov , S. E. Vahsen , C. Van Hulse , R. Van Tonder , P. Vanhoefer , G. Varner , K. E. Varvell , K. Vervink , A. Vinokurova , V. Vorobyev , A. Vossen , M. N. Wagner , E. Waheed , B. Wang , C. H. Wang , E. Wang , M. -Z. Wang , P. Wang , X. L. Wang , M. Watanabe , Y. Watanabe , S. Watanuki , R. Wedd , S. Wehle , E. Widmann , J. Wiechczynski , K. M. Williams , E. Won , X. Xu , B. D. Yabsley , S. Yamada , H. Yamamoto , Y. Yamashita , W. Yan , S. B. Yang , S. Yashchenko , H. Ye , J. Yelton , J. H. Yin , Y. Yook , C. Z. Yuan , Y. Yusa , C. C. Zhang , J. Zhang , L. M. Zhang , Z. P. Zhang , L. Zhao , V. Zhilich , V. Zhukova , V. Zhulanov , T. Zivko , A. Zupanc , N. Zwahlen

I review recent progress on exclusive hadronic B meson decays in the perturbative QCD approach, with focus on puzzles in the branching ratios and the CP asymmetries of the B -> pi K and B -> pi pi modes, and polarization fractions in B ->…

High Energy Physics - Phenomenology · Physics 2007-05-23 Satoshi Mishima

We update the profile of the CKM matrix. The apex (rhobar,etabar) of the Unitarity Triangle is given by means of a global fit. We propose to include therein sin2alpha from the CP-violating asymmetries in B0->rho+rho-, using isospin to…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. Charles , A. Hocker , H. Lacker , S. Laplace , F. R. Le Diberder , J. Malcles , J. Ocariz , M. Pivk , L. Roos

The integrated branching fraction of the process $B\to X_s l^+l^-$ is dominated by resonance background from narrow charmonium states, such as $B\to X_s\psi\to X_s l^+l^-$, which exceeds the non-resonant charm-loop contribution by two…

High Energy Physics - Phenomenology · Physics 2009-07-22 M. Beneke , G. Buchalla , M. Neubert , C. T. Sachrajda

Based upon flavor SU(3) symmetry, we perform global fits to charmless B decays into one pseudoscalar meson and one vector meson in the final states. We consider different symmetry breaking schemes and find that the one implied by na{\"i}ve…

High Energy Physics - Phenomenology · Physics 2009-03-27 Cheng-Wei Chiang , Yu-Feng Zhou

We discuss the perturbative QCD approach for the exclusive two body B-meson decays to light mesons. We briefly review its ingredients and some important theoretical issues on factorization approach. We show numerical results which are…

High Energy Physics - Phenomenology · Physics 2014-11-17 Y. Y. Keum , A. I. Sanda

We show that the presence of intrinsic charm in the hadrons' light-cone wave functions, even at a few percent level, provides new, competitive decay mechanisms for B decays which are nominally CKM-suppressed. For example, the weak decays of…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. J. Brodsky , S. Gardner

With the wealth of new data from the B-factories, b -> d penguin decays become available for study, in addition to their b -> s counterparts that have proven an indespensable tool for the exploration of new-physics effects in flavour…

High Energy Physics - Phenomenology · Physics 2007-05-23 Robert Fleischer , Stefan Recksiegel

Inspired by the recent LHCb measurements and forthcoming great potential on $B_{c}$ meson, we study the exclusive $B_{c}$ ${\to}$ $B_{q}P$, $B_{q}V$ decays with the perturbative QCD approach, where $q$ $=$ $u$, $d$, $s$; $P$ and $V$ denote…

High Energy Physics - Phenomenology · Physics 2015-06-22 Junfeng Sun , Yueling Yang , Qin Chang , Gongru Lu

CP-violating effects in decays of B mesons offer a wide spectrum of probes for testing the phase structure of the quark-flavour sector of the Standard Model. After a brief discussion of the picture emerging from the current LHC data, the…

High Energy Physics - Phenomenology · Physics 2015-06-22 Robert Fleischer

An important experimental effort has been accomplished in recent years in the measurement of rates, polarization and CP observables in $B$ decays into two light vector mesons. On the theoretical side, after a very consistent effort done…

High Energy Physics - Phenomenology · Physics 2024-03-29 Roy Aleksan , Luis Oliver

We analyzed the nonleptonic decays $B/B_s\to \psi(2S) V $ with $V=(\rho, \omega, K^{*}, \phi)$ by employing the perturbative QCD (PQCD) factorization approach. Here the branching ratios, the $CP$ asymmetries and the complete set of…

High Energy Physics - Phenomenology · Physics 2017-09-18 Zhou Rui , Ya Li , Zhen-Jun Xiao

We investigate the $B_{d,s}^0 \to f_1 f_1$ decays in the framework of perturbative QCD(PQCD) approach with a referenced value $\phi_{f_1} \sim 24^\circ$. Here, $f_1$ denotes the axial-vector mesons $f_1(1285)$ and $f_1(1420)$ with mixing…

High Energy Physics - Phenomenology · Physics 2021-04-15 Zewen Jiang , De-Hua Yao , Zhi-Tian Zou , Xin Liu , Ying Li , Zhen-Jun Xiao

We study the nonleptonic charmless $B_{u,d,s} \to K_0^*(1430)P$ $(P=K\,, \pi)$ and $ K_0^*(1430)V$ $ (V=K^*\,, \rho\,, \omega\,, \phi)$ decays. The amplitudes are calculated within the QCD factorization, and the non-perturbative quantities…

High Energy Physics - Phenomenology · Physics 2022-01-06 Lili Chen , Mengfei Zhao , Yunyun Zhang , Qin Chang