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Related papers: Getting SM and New Physics CP phases from $B$ Deca…

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The $B_s$-meson system is a key element in the $B$-physics programme of hadron colliders, offering various avenues to explore CP violation and to search for new physics. One of the most prominent decays is $B_s\to J/\psi\phi$, the…

High Energy Physics - Phenomenology · Physics 2010-11-23 Robert Fleischer

Although recent experimental results in b-->s penguin process seem to be roughly consistent with the standard model predictions, there may be still large possibilities of new physics hiding in this processes. Therefore, here we investigate…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. S. Kim , Y. J. Kwon , Jake Lee , T. Yoshikawa

We propose to perform a combined analysis of $B \to \pi\pi$ and $B_s \to K^+ K^-$ modes, in the framework of a global CKM fit. The method optimizes the constraining power of these decays and allows to derive constraints on NP contributions…

High Energy Physics - Phenomenology · Physics 2012-10-17 M. Ciuchini , E. Franco , S. Mishima , L. Silvestrini

Rare $B$, $D$ and $K$ decays provide interesting probes of the Standard Model (SM), with a potential sensitivity to New Physics (NP) higher than other, more common, decays. Their experimental measurement is challenging, and their…

High Energy Physics - Experiment · Physics 2019-01-16 Michel De Cian , Sébastien Descotes-Genon , Karim Massri

The standard CKM model can be tested and New Physics detected using only CP-violating phase measurements in B decays. This requires the measurement of a phase factor which is small in the Standard Model, in addition to the usual large…

High Energy Physics - Phenomenology · Physics 2016-09-06 Joao P. Silva , L. Wolfenstein

The time-dependent angular distributions of certain $B_{d,s}$ decays into final states that are admixtures of CP-even and CP-odd configurations provide valuable information about CKM phases and hadronic parameters. We present the general…

High Energy Physics - Phenomenology · Physics 2016-08-25 Robert Fleischer

We propose two independent methods to determine the CKM phase $\gamma$ and the tree and penguin amplitudes using neutral $B$ decays, assuming that the phase $\beta$ is known. Based on flavor SU(3) symmetry and SU(3) breaking effect, one…

High Energy Physics - Phenomenology · Physics 2007-05-23 N. G. Deshpande , Sechul Oh

We discuss two models with 1 extra CP phase in $b\leftrightarrow s$ transition. The CP phase $\arg (V_{t^\prime s}V_{t^\prime b})$ with fourth generations, previously ignored, could impact on $b\to s\ell^+\ell^-$, $\Delta m_{B_s}$ and…

High Energy Physics - Phenomenology · Physics 2011-09-13 George W. S. Hou

The complex phases $\phi_d$ and $\phi_s$, associated with the mixing between neutral $B_q^0$ and $\bar B_q^0$ mesons ($q\in\{d,s\}$), are key observables to test the Standard Model and search for contributions from new physics. They are…

High Energy Physics - Phenomenology · Physics 2026-03-12 Kristof De Bruyn , Robert Fleischer , Eleftheria Malami

The decays $B_d\to\pi^+\pi^-$ and $B_s\to K^+K^-$ provide an interesting strategy to extract the CKM angle $\gamma$ at ``second-generation'' $B$-physics experiments of the LHC era. A variant for ``first-generation'' experiments can be…

High Energy Physics - Phenomenology · Physics 2010-11-23 Robert Fleischer

In this presentation, we discuss recent key topics in theoretical analyses of CP violation in benchmarks decays of the $B$ meson. We provide the most updated values of the mixing phases and discuss the importance of including the penguin…

High Energy Physics - Phenomenology · Physics 2024-02-28 Eleftheria Malami

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

We present the current wisdom regarding the measurement of the CP-violating phases of the CKM unitarity triangle in $B$-meson decays. After an introduction to the SM picture of CP violation, we review direct and indirect CP violation, the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Oscar F. Hernandez , David London

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

Measurements of CP violation in $B^0_d\to J/\psi K_{\rm S}^0$ and $B^0_s\to J/\psi \phi$ decays play key roles in testing the quark-flavour sector of the Standard Model. The theoretical interpretation of the corresponding observables is…

High Energy Physics - Phenomenology · Physics 2015-03-31 Kristof De Bruyn , Robert Fleischer

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

A new way of determining the phases of weak amplitudes in charged $B$ decays based on SU(3) symmetry is proposed. The CP violating phase $\gamma$ can now be determined without the previous difficulty associated with electroweak penguins.

High Energy Physics - Phenomenology · Physics 2009-10-28 N. G. Deshpande , Xiao-Gang He

We review the theoretical status of b to s hadronic penguin decays in the Standard Model and beyond. We summarize the main theoretical tools to compute Branching Ratios and CP asymmetries for b to s penguin dominated nonleptonic decays, and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Luca Silvestrini

The decays $B_d\to \pi^+ \pi^-$ and $B_s\to K^+ K^-$ are related to each other by interchanging all down and strange quarks, i.e. through the $U$-spin flavour symmetry of strong interactions. A completely general parametrization of the…

High Energy Physics - Phenomenology · Physics 2010-11-23 Robert Fleischer

In left-right models the gluonic penguin contribution to b --> s s-bar s transition is enhanced by m_t/m_b due to the presence of (V+A) currents and by the larger values of loop functions than in the Standard Model. Together those may…

High Energy Physics - Phenomenology · Physics 2009-11-07 Martti Raidal