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Related papers: BSM Kaon Mixing at the Physical Point

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We discuss a simple approach to measure the weak mixing angles phi_s and phi_d of the Bs and Bd systems in the presence of New Physics. We present a new expression that allows one to measure directly the New Physics mixing angles if New…

High Energy Physics - Phenomenology · Physics 2013-05-30 Sebastien Descotes-Genon , Joaquim Matias , Javier Virto

We review the status of heavy quark physics at the Fermilab Tevatron collider by summarizing recent top quark and B physics results from CDF and DO. In particular, we discuss the measurement of the top quark mass and top production cross…

High Energy Physics - Experiment · Physics 2007-05-23 M. Paulini

Full QCD+QED simulations allow to evaluate isospin breaking corrections to hadron masses. With the openQxD code, we are able to perform these simulations employing C-periodic boundary conditions, implemented through a doubling of the…

We present two novelties in our analysis of fully dynamical QCD+QED ensembles with C* boundary conditions. The first one is the explicit computation of the sign of the Pfaffian. We present an algorithm that provides a significant speedup…

We report on the advances in our unquenched calculation of the matrix elements relevant for the analysis of B^0-\bar B^0 mixing using the Asqtad (light quark) and Fermilab (heavy quark) actions. We have calculated the hadronic parameters…

High Energy Physics - Lattice · Physics 2010-11-19 R. Todd Evans , Elvira Gamiz , Aida X. El-Khadra , Massimo Di Pierro

We present results for the light quark masses and the neutral kaon mixing parameter $B_K$ from lattice QCD. Our data set includes lighter than physical light quark masses and 5 lattice spacings so that chiral extrapolation is not necessary…

High Energy Physics - Phenomenology · Physics 2012-07-02 Christian Hoelbling

We study the M1 transitions of ground state heavy baryons within a framework of the modified bag model. Calculations of transition moments and corresponding M1 decay widths are performed. For the spin 1/2 baryons containing three…

High Energy Physics - Phenomenology · Physics 2013-04-24 Andrius Bernotas , Vytautas Šimonis

We review the status of heavy flavour physics at the Fermilab Tevatron collider by summarizing recent top quark and B physics results from CDF and DO. In particular we discuss the measurement of the top quark mass and top production cross…

High Energy Physics - Experiment · Physics 2007-05-23 M. Paulini

We report scale setting and hadronic properties for our new lattice QCD gauge configuration set (HAL-conf-2023). We employ $(2+1)$-flavor nonperturbatively improved Wilson fermions with stout smearing and the Iwasaki gauge action on a…

High Energy Physics - Lattice · Physics 2024-11-12 Tatsumi Aoyama , Takahiro M. Doi , Takumi Doi , Etsuko Itou , Yan Lyu , Kotaro Murakami , Takuya Sugiura

Prompted by the recent surprising results in QCD spectroscopy, we extend the treatment of the constituent quark model showing that mass differences and ratios have the same values when obtained from mesons and baryons. We obtain several new…

High Energy Physics - Phenomenology · Physics 2008-11-26 Marek Karliner , Harry J. Lipkin

We present results for matrix elements of $\Delta S=2$ four-fermion operators arising generically in models of new physics. These are needed to constrain such models using the measured values of $\varepsilon_K$ and $\Delta M_K$. We use…

We introduce a unified Gaussian quantum operator representation for fermions and bosons. The representation extends existing phase-space methods to Fermi systems as well as the important case of Fermi-Bose mixtures. It enables simulations…

Other Condensed Matter · Physics 2009-11-11 P. D. Drummond , J. F. Corney

We present an update of our study of the phase diagram of two-flavour QCD at zero baryon density with dynamical $O(a)$ improved Wilson quarks. All simulations are done on lattices with a temporal extent of $N_t=16$ and spatial extent…

High Energy Physics - Lattice · Physics 2013-11-01 Bastian B. Brandt , Anthony Francis , Harvey B. Meyer , Owe Philipsen , Hartmut Wittig

We present a status report of our ongoing effort toward a precision determination of the kaon $B$ parameter with the Kogut-Susskind quark action in quenched QCD. Results for $B_K$ so far accumulated at $\beta =5.85$, 5.93, 6.0 and 6.2…

High Energy Physics - Lattice · Physics 2015-06-25 JLQCD Collaboration

Charged B decays to three charged kaons are analysed in the framework of the QCD factorization approach. The strong final state K+K-interactions are described using the kaon scalar and vector form factors. The scalar non-strange and strange…

High Energy Physics - Phenomenology · Physics 2011-06-01 Agnieszka Furman , Robert Kaminski , Leonard Lesniak , Piotr Zenczykowski

New sum rules for $B\to \pi,K $ and $B\to \rho,K^*$ form factors are derived from the correlation functions expanded near the light-cone in terms of B-meson distribution amplitudes. The contributions of quark-antiquark and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alexander Khodjamirian , Thomas Mannel , Nils Offen

A new gauge fixing that imposes the U(1) real and quaternion real condition on the correlator of domain wall fermion on the left wall and right wall is proposed. The method is applied to the calculation of the mass function, the QCD…

High Energy Physics - Lattice · Physics 2010-11-05 Sadataka Furui

QCD lattice simulations with 2+1 flavours typically start at rather large up-down and strange quark masses and extrapolate first the strange quark mass to its physical value and then the up-down quark mass. An alternative method of tuning…

Spectra of positively charged kaons in p+C interactions at 31 GeV/c were measured with the NA61/SHINE spectrometer at the CERN SPS. The analysis is based on the full set of data collected in 2007 with a graphite target with a thickness of…

High Energy Physics - Experiment · Physics 2013-05-30 SHINE Collaboration , N. Abgrall , A. Aduszkiewicz , T. Anticic , N. Antoniou , J. Argyriades , B. Baatar , A. Blondel , J. Blumer , M. Bogusz , L. Boldizsar , A. Bravar , W. Brooks , J. Brzychczyk , A. Bubak , S. A. Bunyatov , O. Busygina , T. Cetner , K. -U. Choi , P. Christakoglou , P. Chung , T. Czopowicz , N. Davis , F. Diakonos , S. Di Luise , W. Dominik , J. Dumarchez , R. Engel , A. Ereditato , L. S. Esposito , G. A. Feofilov , Z. Fodor , A. Ferrero , A. Fulop , X. Garrido , M. Gazdzicki , M. Golubeva , K. Grebieszkow , A. Grzeszczuk , F. Guber , A. Haesler , H. Hakobyan , T. Hasegawa , R. Idczak , Y. Ivanov , A. Ivashkin , K. Kadija , A. Kapoyannis , N. Katrynska , D. Kielczewska , D. Kikola , J. -H. Kim , M. Kirejczyk , J. Kisiel , T. Kobayashi , O. Kochebina , V. I. Kolesnikov , D. Kolev , V. P. Kondratiev , A. Korzenev , S. Kowalski , A. Krasnoperov , S. Kuleshov , A. Kurepin , R. Lacey , J. Lagoda , A. Laszlo , V. V. Lyubushkin , M. Mackowiak-Pawlowska , Z. Majka , A. I. Malakhov , A. Marchionni , A. Marcinek , I. Maris , V. Marin , T. Matulewicz , V. Matveev , G. L. Melkumov , A. Meregaglia , M. Messina , St. Mrowczynski , S. Murphy , T. Nakadaira , K. Nishikawa , T. Palczewski , G. Palla , A. D. Panagiotou , T. Paul , W. Peryt , O. Petukhov , R. Planeta , J. Pluta , B. A. Popov , M. Posiadala , S. Pulawski , W. Rauch , M. Ravonel , R. Renfordt , A. Robert , D. Rohrich , E. Rondio , B. Rossi , M. Roth , A. Rubbia , M. Rybczynski , A. Sadovsky , K. Sakashita , T. Sekiguchi , P. Seyboth , M. Shibata , E. Skrzypczak , M. Slodkowski , P. Staszel , G. Stefanek , J. Stepaniak , C. Strabel , H. Strobele , T. Susa , P. Szaflik , M. Szuba , M. Tada , A. Taranenko , V. Tereshchenko , R. Tsenov , L. Turko , R. Ulrich , M. Unger , M. Vassiliou , D. Veberic , V. V. Vechernin , G. Vesztergombi , A. Wilczek , Z. Wlodarczyk , A. Wojtaszek-Szwarc , J. -G. Yi , I. -K. Yoo , L. Zambelli , W. Zipper

We calculate second- and selected fourth-order conserved-charge fluctuations in $(2+1)$-flavor QCD using M\"obius domain-wall fermions (MDWF) along a line of constant physics. Gauge ensembles were generated for two light-to-strange…