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We discuss chiral perturbation theory for two and three quark flavors in the epsilon expansion at next-to-next-to-leading order (NNLO) including a small imaginary chemical potential. We calculate finite-volume corrections to the low-energy…

High Energy Physics - Lattice · Physics 2014-11-20 Christoph Lehner , Shoji Hashimoto , Tilo Wettig

There exist experimental hints from the B sector for CP violation beyond the Standard Model (SM) CKM paradigm. An anomalous dimuon asymmetry was reported by the D0 collaboration, while tension exists between $B \to \tau \nu$ and $S_{\psi…

High Energy Physics - Phenomenology · Physics 2011-09-08 Sean Tulin , Peter Winslow

The flavor changing neutral current processes $K_L \to \pi^0 e^+ e^-$, $B \to X_s e^+ e^-$ and $B \to X_s \mu^+ \mu^-$ are studied within the minimal supersymmetric extension of the Standard Model. We first examine the rates for these decay…

High Energy Physics - Phenomenology · Physics 2009-10-28 Peter Cho , Mikolaj Misiak , Daniel Wyler

We present the results of the first lattice QCD calculation of the $K \to \pi$ matrix elements of the chromomagnetic operator $O_{CM} = g\, \bar s\, \sigma_{\mu\nu} G_{\mu\nu} d$, which appears in the effective Hamiltonian describing…

High Energy Physics - Lattice · Physics 2018-04-11 M. Constantinou , M. Costa , R. Frezzotti , V. Lubicz , G. Martinelli , D. Meloni , H. Panagopoulos , S. Simula

We report on an ongoing non-perturbative computation of RI-MOM scheme renormalization constants for the lattice action with four dynamical flavours currently in use by ETMC. For this goal dedicated simulations with four degenerate sea quark…

High Energy Physics - Lattice · Physics 2015-03-17 P. Dimopoulos , R. Frezzotti , G. Herdoiza , K. Jansen , V. Lubicz , D. Palao , G. C. Rossi

The mass and weak interaction eigenstates for the quarks of the third generation are very well aligned, an empirical fact for which the Standard Model offers no explanation. We explore the possibility that this alignment is due to an…

High Energy Physics - Phenomenology · Physics 2018-01-17 K. S. Babu , A. Friedland , P. A. N. Machado , I. Mocioiu

We analyze in detail the constraints on SUSY-model parameters obtained from K-Kbar mixing in the hypothesis of a splitted SUSY spectrum. FCNC contributions from gluino-squark-quark interactions are studied in the so-called mass insertion…

High Energy Physics - Phenomenology · Physics 2011-09-13 Roberto Contino , Ignazio Scimemi

The recent evidence for the decay $B^+ \to K^+ \nu \bar{\nu}$ reported by the Belle II collaboration, combined with the existing constraints on the neutral mode $B^0 \to K^{*0} \nu \bar{\nu}$, implies a deviation from the Standard Model…

High Energy Physics - Phenomenology · Physics 2026-01-27 Xin-Shuai Yan , Wen-Feng Liu , Qin Chang , Ya-Dong Yang

Flavour physics represents a unique test bench for the Standard Model (SM). New analyses performed at the LHC experiments are now providing unprecedented insights into CKM metrology and new evidences for rare decays. The CKM picture can…

In light of recent measurements suggesting potential lepton flavor universality violations in semileptonic decays at collider experiments, this article provides a concise study of tree- and loop-level $B$-hadron semileptonic decays, $b \to…

High Energy Physics - Phenomenology · Physics 2025-02-05 Sonali Patnaik , Lopamudra Nayak , Rajeev Singh

Flavor mixing is scrutinized at 1-loop in a SU(2)_L gauge theory of massive fermions. The main issue is to cope with kinetic-like, momentum (p^2) dependent effective interactions that arise at this order. They spoil the unitarity of the…

High Energy Physics - Phenomenology · Physics 2010-06-16 Bruno Machet

We discuss the theory prediction of epsilon_K and the rare K -> pi nu nu-bar decays and review the structure and current status of higher-order contributions to these flavour changing processes in the standard model in some detail. This…

High Energy Physics - Phenomenology · Physics 2010-04-23 Martin Gorbahn

We present new results for the renormalisation and subtraction constants for the four fermion Delta F=2 operators, computed non-perturbatively in the RI-MOM scheme (in the Landau gauge). From our preliminary analysis of the lattice data at…

High Energy Physics - Lattice · Physics 2015-06-25 D. Becirevic , V. Gimenez , V. Lubicz , G. Martinelli , M. Papinutto , J. Reyes

We present the status of our calculation of hadronic matrix elements for $D$- and $B$-meson mixing. We use a large set of the MILC collaboration's $N_f=2+1$ asqtad ensembles, which includes lattice spacings in the range $a\approx0.12$-0.045…

High Energy Physics - Lattice · Physics 2013-11-28 C. C. Chang , C. Bernard , C. M. Bouchard , A. X. El-Khadra , E. D. Freeland , E. Gámiz , A. S. Kronfeld , J. Laiho , R. S. van de Water

We presents results for the matrix elements of a variety of four-fermion operators calculated using quenched Wilson fermions. Our simulations are done on 170 lattices of size $32^3 x 64$ at $\beta = 6.0$. We find $B_K=0.74 +- 0.04 +- 0.05$,…

High Energy Physics - Lattice · Physics 2008-02-03 Rajan Gupta , Tanmoy Bhattacharya , Stephen Sharpe

The precise determination of the CKM matrix element $\left| V_{cb}\right|$ is important for carrying out tests of the flavour sector of the Standard Model. In this article we present a preliminary analysis of the $\bar B^0 \to D^{*\,+} \,…

High Energy Physics - Experiment · Physics 2017-02-15 The Belle Collaboration , A. Abdesselam , I. Adachi , K. Adamczyk , H. Aihara , S. Al Said , K. Arinstein , Y. Arita , D. M. Asner , T. Aso , H. Atmacan , V. Aulchenko , T. Aushev , R. Ayad , T. Aziz , V. Babu , I. Badhrees , S. Bahinipati , A. M. Bakich , A. Bala , Y. Ban , V. Bansal , E. Barberio , M. Barrett , W. Bartel , A. Bay , P. Behera , M. Belhorn , K. Belous , M. Berger , F. U. Bernlochner , D. Besson , V. Bhardwaj , B. Bhuyan , J. Biswal , T. Bloomfield , S. Blyth , A. Bobrov , A. Bondar , G. Bonvicini , C. Bookwalter , C. Boulahouache , A. Bozek , M. Bračko , N. Braun , F. Breibeck , J. Brodzicka , T. E. Browder , E. Waheed , D. Červenkov , M. -C. Chang , P. Chang , Y. Chao , V. Chekelian , A. Chen , K. -F. Chen , P. Chen , B. G. Cheon , K. Chilikin , R. Chistov , K. Cho , V. Chobanova , S. -K. Choi , Y. Choi , D. Cinabro , J. Crnkovic , J. Dalseno , M. Danilov , N. Dash , S. Di Carlo , J. Dingfelder , Z. Doležal , D. Dossett , Z. Drásal , A. Drutskoy , S. Dubey , D. Dutta , K. Dutta , S. Eidelman , D. Epifanov , S. Falke , H. Farhat , J. E. Fast , M. Feindt , T. Ferber , A. Frey , O. Frost , B. G. Fulsom , V. Gaur , N. Gabyshev , S. Ganguly , A. Garmash , M. Gelb , J. Gemmler , D. Getzkow , R. Gillard , F. Giordano , R. Glattauer , Y. M. Goh , P. Goldenzweig , B. Golob , D. Greenwald , M. Grosse Perdekamp , J. Grygier , O. Grzymkowska , Y. Guan , E. Guido , H. Guo , J. Haba , P. Hamer , Y. L. Han , K. Hara , T. Hara , Y. Hasegawa , J. Hasenbusch , K. Hayasaka , H. Hayashii , X. H. He , M. Heck , M. T. Hedges , D. Heffernan , M. Heider , A. Heller , T. Higuchi , S. Himori , S. Hirose , T. Horiguchi , Y. Hoshi , K. Hoshina , W. -S. Hou , Y. B. Hsiung , C. -L. Hsu , M. Huschle , H. J. Hyun , Y. Igarashi , T. Iijima , M. Imamura , K. Inami , G. Inguglia , A. Ishikawa , K. Itagaki , R. Itoh , M. Iwabuchi , M. Iwasaki , Y. Iwasaki , S. Iwata , W. W. Jacobs , I. Jaegle , H. B. Jeon , S. Jia , Y. Jin , D. Joffe , M. Jones , 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 , E. Kato , Y. Kato , P. Katrenko , H. Kawai , T. Kawasaki , T. Keck , H. Kichimi , C. Kiesling , B. H. Kim , D. Y. Kim , H. J. Kim , H. -J. Kim , J. B. Kim , J. H. Kim , K. T. Kim , M. J. Kim , S. H. Kim , S. K. Kim , Y. J. Kim , K. Kinoshita , C. Kleinwort , J. Klucar , B. R. Ko , N. Kobayashi , S. Koblitz , P. Kodyš , Y. Koga , S. Korpar , D. Kotchetkov , R. T. Kouzes , P. Križan , P. Krokovny , B. Kronenbitter , T. Kuhr , R. Kulasiri , R. Kumar , T. Kumita , E. Kurihara , Y. Kuroki , A. Kuzmin , P. Kvasnička , Y. -J. Kwon , Y. -T. Lai , J. S. Lange , D. H. Lee , I. S. Lee , S. -H. Lee , M. Leitgab , R. Leitner , D. Levit , P. Lewis , C. H. Li , H. Li , J. Li , L. Li , X. Li , Y. Li , L. Li Gioi , J. Libby , A. Limosani , C. Liu , Y. Liu , Z. Q. Liu , D. Liventsev , A. Loos , R. Louvot , M. Lubej , P. Lukin , T. Luo , J. MacNaughton , M. Masuda , T. Matsuda , D. Matvienko , A. Matyja , F. Metzner , S. McOnie , Y. Mikami , K. Miyabayashi , Y. Miyachi , H. Miyake , H. Miyata , Y. Miyazaki , R. Mizuk , G. B. Mohanty , S. Mohanty , D. Mohapatra , A. Moll , H. K. Moon , T. Mori , T. Morii , H. -G. Moser , M. Mrvar , T. Müller , N. Muramatsu , R. Mussa , T. Nagamine , Y. Nagasaka , Y. Nakahama , I. Nakamura , K. R. Nakamura , E. Nakano , H. Nakano , T. Nakano , M. Nakao , H. Nakayama , H. Nakazawa , T. Nanut , K. J. Nath , Z. Natkaniec , M. Nayak , E. Nedelkovska , K. Negishi , K. Neichi , C. Ng , C. Niebuhr , M. Niiyama , N. K. Nisar , S. Nishida , K. Nishimura , O. Nitoh , T. Nozaki , A. Ogawa , S. Ogawa , T. Ohshima , S. Okuno , S. L. Olsen , H. Ono , Y. Ono , Y. Onuki , W. Ostrowicz , C. Oswald , H. Ozaki , P. Pakhlov , G. Pakhlova , B. Pal , H. Palka , E. Panzenböck , C. -S. Park , C. W. Park , H. Park , K. S. Park , S. Paul , L. S. Peak , T. K. Pedlar , T. Peng , L. Pesántez , R. Pestotnik , M. Peters , M. Petrič , L. E. Piilonen , A. Poluektov , K. Prasanth , M. Prim , K. Prothmann , C. Pulvermacher , M. V. Purohit , J. Rauch , B. Reisert , E. Ribežl , M. Ritter , J. Rorie , A. Rostomyan , M. Rozanska , S. Rummel , S. Ryu , H. Sahoo , M. Salehi , T. Saito , K. Sakai , Y. Sakai , S. Sandilya , D. Santel , L. Santelj , T. Sanuki , J. Sasaki , N. Sasao , Y. Sato , V. Savinov , T. Schlüter , O. Schneider , G. Schnell , P. Schönmeier , M. Schram , 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 , V. Shebalin , C. P. Shen , T. -A. Shibata , H. Shibuya , N. Shimizu , S. Shinomiya , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , J. B. Singh , R. Sinha , P. Smerkol , Y. -S. Sohn , A. Sokolov , Y. Soloviev , E. Solovieva , S. Stanič , M. Starič , M. Steder , J. F. Strube , J. Stypula , S. Sugihara , A. Sugiyama , M. Sumihama , K. Sumisawa , T. Sumiyoshi , K. Suzuki , K. Suzuki , S. Suzuki , S. Y. Suzuki , Z. Suzuki , H. Takeichi , M. Takizawa , U. Tamponi , M. Tanaka , S. Tanaka , K. Tanida , N. Taniguchi , G. N. Taylor , F. Tenchini , Y. Teramoto , I. Tikhomirov , K. Trabelsi , V. Trusov , T. Tsuboyama , M. Uchida , T. Uchida , S. Uehara , K. Ueno , T. Uglov , Y. Unno , S. Uno , S. Uozumi , P. Urquijo , Y. Ushiroda , Y. Usov , S. E. Vahsen , C. Van Hulse , 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 , J. Wang , M. -Z. Wang , P. Wang , X. L. Wang , M. Watanabe , Y. Watanabe , R. Wedd , S. Wehle , E. White , E. Widmann , J. Wiechczynski , K. M. Williams , E. Won , B. D. Yabsley , S. Yamada , H. Yamamoto , J. Yamaoka , Y. Yamashita , M. Yamauchi , S. Yashchenko , H. Ye , J. Yelton , Y. Yook , C. Z. Yuan , Y. Yusa , C. C. Zhang , L. M. Zhang , Z. P. Zhang , L. Zhao , V. Zhilich , V. Zhukova , V. Zhulanov , M. Ziegler , T. Zivko , A. Zupanc , N. Zwahlen

In view of the recent start of the NA62 experiment at CERN that is expected to measure the $K^+\to\pi^+\nu\bar\nu$ branching ratio with a precision of 10%, we summarise the present status of this promising decay within the Standard Model…

High Energy Physics - Phenomenology · Physics 2015-12-10 Andrzej J. Buras , Dario Buttazzo , Jennifer Girrbach-Noe , Robert Knegjens

Models of new physics induce K-Kbar mixing operators having Dirac structures other than the "left-left" form of the Standard Model. We calculate the functional form of the corresponding B-parameters at next-to-leading order in both SU(3)…

High Energy Physics - Lattice · Physics 2013-05-30 Jon A. Bailey , Hyung-Jin Kim , Weonjong Lee , Stephen R. Sharpe

We derive explicit transformation formulae relating the renormalized quark mass and field as defined in the MS-bar scheme with the corresponding quantities defined in any other scheme. By analytically computing the three-loop quark…

High Energy Physics - Phenomenology · Physics 2010-04-06 K. G. Chetyrkin , A. Retey

The quantity R_K = Gamma(K -> e nu)/Gamma(K -> mu nu) studied by the experiment NA62 at CERN is known to probe lepton-flavour violating (LFV) parameters of the Minimal Supersymmetric Standard Model (MSSM). A non-zero parameter…

High Energy Physics - Phenomenology · Physics 2012-02-23 Jennifer Girrbach , Ulrich Nierste