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Related papers: Determining weak phases from B->J/Psi P decays

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Recently, $B\to PP$ decays ($B = \{B^0, B^+, B_s^0\}$, $P = \{ \pi, K \}$) were analyzed under the assumption of flavor SU(3) symmetry (SU(3)$_F$). Although the individual fits to $\Delta S=0$ or $\Delta S=1$ decays are good, it was found…

High Energy Physics - Phenomenology · Physics 2025-09-17 Bhubanjyoti Bhattacharya , Marianne Bouchard , Luke Hudy , Alexandre Jean , David London , Christopher MacKenzie

The role of penguin amplitudes in CP violating $B$ decays is reviewed, emphasizing recent progress in the analysis of electroweak penguin contributions. It is shown how these terms are included in a model-independent manner when measuring…

High Energy Physics - Phenomenology · Physics 2007-05-23 Michael Gronau

We present a new method for measuring the CP phase \alpha. It requires the measurement of the pure penguin decays Bd(t) -> K(*) Kbar(*) and B_s -> K(*) Kbar(*). The method is quite clean: we estimate the theoretical uncertainty to be at…

High Energy Physics - Phenomenology · Physics 2017-08-23 Alakabha Datta , David London

A method to extract Standard Model(SM) CP phases involving B decays is presented. The method involves a pair of decays where one decay receives a significant $b \to d$ penguin contribution while the second has a significant $b \to s$…

High Energy Physics - Phenomenology · Physics 2016-09-06 Alakabha Datta

A method based on flavour SU(3) is proposed for identifying and extracting New Physics (NP) amplitudes in charmless $\Delta S=1$ $B_s$ decays using time-dependent CP asymmetries in these decays and in flavour SU(3) related $\Delta S=0$…

High Energy Physics - Phenomenology · Physics 2008-11-26 Robert Fleischer , Michael Gronau

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

We report the first reconstruction in hadron collisions of the suppressed decays B^- -> D(-> K^+ pi^-)K^- and B^- -> D(-> K^+ pi^-)pi^-, sensitive to the CKM phase gamma, using data from 7 fb^-1 of integrated luminosity collected by the CDF…

High Energy Physics - Experiment · Physics 2013-05-29 CDF Collaboration

Measurements of the time-dependent CP asymmetry in the decay $B^0_d (t) \to \pi^+ \pi^-$ and its charge conjugate by the BELLE and BABAR collaborations currently yield $C_{\pi \pi}^{+-} = -0.46 \pm 0.13$ and $S_{\pi \pi}^{+-} = -0.74 \pm…

High Energy Physics - Phenomenology · Physics 2010-11-23 A. Ali , E. Lunghi , A. Ya. Parkhomenko

The Bc -> BP,BV decays are studied with the QCD factorization approach (where P and V denote pseudoscalar and vector mesons, respectively). Considering the contributions of both current-current and penguin operators, the amplitudes of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Junfeng Sun , Yueling Yang , Wenjie Du , Huilan Ma

Time-dependent measurements of the decays B_s^0(t)-->\phi K_s and B_d^0(t) --> K^0 \bar{K}^0 can be used to compare the weak phases of B_d^0-\bar{B}_d^0 mixing and the t-quark contribution to the b->d penguin. Since these two phases are…

High Energy Physics - Phenomenology · Physics 2011-01-13 C. S. Kim , D. London , T. Yoshikawa

The decay rates for $B^0 \to K^+ \pi^-$, $B^+ \to K^0 \pi^+$, and the charge-conjugate processes were found to provide information on the weak phase $\gamma \equiv {\rm Arg}(V_{ub}^*)$ when the ratio $r$ of weak tree and penguin amplitudes…

High Energy Physics - Phenomenology · Physics 2014-11-17 Michael Gronau , Jonathan L. Rosner

Using firmly established experimental inputs such as epsilon_K, Delta M_d, Delta M_s, BR(B -> tau nu), gamma, V_cb along with corresponding lattice matrix elements which have been well studied and are in full QCD such as B_K, SU3 breaking…

High Energy Physics - Phenomenology · Physics 2015-05-27 Enrico Lunghi , Amarjiit Soni

We present the measurement, performed by the BABAR Collaboration, of the weak phase alpha from the time dependent CP asymmetries in B0--> a_1(1260)+- pi-+ decays. The model error induced by penguin contributions to the B0 --> a_1(1260)+-…

High Energy Physics - Experiment · Physics 2019-08-13 Simone Stracka

We analyze the extraction of weak phases from CP violation in $B\to\pi^+\pi^-$ decays. By combining the information on mixing induced CP violation in $B\to\pi^+\pi^-$, namely $S_{\pi\pi}$, with the precision observable $\sin 2\beta$…

High Energy Physics - Phenomenology · Physics 2010-11-23 A. Salim Safir

Recently, we have seen interesting progress in the exploration of CP violation in B^0_d -> pi^+ pi^-: the measurements of mixing-induced CP violation by the BaBar and Belle collaborations are now in good agreement with each other, whereas…

High Energy Physics - Phenomenology · Physics 2008-11-26 Robert Fleischer , Stefan Recksiegel , Felix Schwab

We present preliminary measurements of CP-violating asymmetries in B decays. These include new results on the CKM angle alpha based on studies of the decay B -> rho+ rho- and several charmonium and hadronic penguin modes, sensitive to the…

High Energy Physics - Experiment · Physics 2019-08-14 Giampiero Mancinelli

Based on the low energy effective Hamiltonian with generalized factorization, we calculate the new physics contributions to the branching ratios and CP-violating asymmetries of the two-body charmless hadronic decays $B \to PP, PV$ from the…

High Energy Physics - Phenomenology · Physics 2009-01-07 Zhenjun Xiao , Wenjun Li , Libo Guo , Gongru Lu

We derive constraints for $B\to VV$ modes ($V= vector meson) that allow aquantitative assessment of the contributions from electroweak penguins (EWP) and/or new physics. Interplay of direct CP with oscillation studies then leads to the…

High Energy Physics - Phenomenology · Physics 2009-10-31 David Atwood , Amarjit Soni

We present the contributions of new CP phases in CP asymmetries of two-body neutral $B_s$ decays coming from a left--right model with spontaneous CP violation. Large deviations from the Standard Model predictions can be accommodated in a…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Matias

There are variety of methods which directly test for the presence of new physics in the b -> s flavour-changing neutral current (FCNC), but none which cleanly probe new physics in the b -> d FCNC. One possible idea is to compare the weak…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. London