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Related papers: The $B_K$ Parameter in the $1/N_c$ Expansion

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We investigate a chirally imbalanced medium in the context of the two-flavor Nambu--Jona-Lasinio model using both the large-$N_c$ (LN) and beyond large-$N_c$ (BLN) approximations. To incorporate BLN effects, we consider the optimized…

High Energy Physics - Phenomenology · Physics 2025-10-21 André G. da Silva , Dyana C. Duarte , Ricardo L. S. Farias , Marcus Benghi Pinto , Rudnei O. Ramos , William R. Tavares

We calculate the $c\bar{b}$ mass spectrum, the splitting values and some other properties in the framework of the semi-relativistic equation by applying the shifted large-N expansion technique. We use seven different central potentials…

High Energy Physics - Phenomenology · Physics 2011-03-23 Sameer M. Ikhdair , Ramazan Sever

We calculate the neutral kaon mixing parameter B_K in unquenched lattice QCD using asqtad-improved staggered sea quarks and domain-wall valence quarks. We use the "2+1" flavor gauge configurations generated by the MILC Collaboration, and…

High Energy Physics - Lattice · Physics 2010-04-28 C. Aubin , Jack Laiho , Ruth S. Van de Water

In this paper, we investigate the vertex corrections and spectator hard scattering contributions to $B \to \chi_{c0,2}K$ decays, which has no leading contribution from naive factorization scheme. A non-zero binding energy $b=2m_c-M$ is…

High Energy Physics - Phenomenology · Physics 2015-06-25 T. N. Pham , Guohuai Zhu

We compute the $\widehat B_K$ parameter and the mass difference $\Delta M_{LS}$ of the $K^0-\bar K^0$ system by means of the chiral quark model. The chiral coefficients of the relevant $\Delta S=2$ and $\Delta S=1$ chiral lagrangians are…

High Energy Physics - Phenomenology · Physics 2014-11-17 V. Antonelli , S. Bertolini , M. Fabbrichesi , E. I. Lashin

We study the B-parameter (``bag factor'') for B-anti-B mixing within a recently developed heavy-light chiral quark model. Non-factorizable contributions in terms of gluon condensates and chiral corrections are calculated. In addition, we…

High Energy Physics - Phenomenology · Physics 2015-06-25 A. Hiorth , J. O. Eeg

We present results for $B_K$ calculated using HYP-smeared improved staggered fermions on the MILC asqtad lattices. In this report, the data is analyzed using the results of SU(2) staggered chiral perturbation theory (SChPT). We outline the…

High Energy Physics - Lattice · Physics 2010-11-05 Hyung-Jin Kim , Taegil Bae , Jangho Kim , Jongjeong Kim , Kwangwoo Kim , Boram Yoon , Weonjong Lee , Chulwoo Jung , Stephen R. Sharpe

The computation on the lattice of the bag parameter $B_{B_s}$ associated to the $B_s - \bar{B_s}$ mixing amplitude in the Standard Model is presented. The estimation has been made by combining the static limit of HQET and the Neuberger…

High Energy Physics - Lattice · Physics 2008-11-26 B. Blossier

We report the first lattice QCD calculation of the form factors for the standard model tree-level decay $B_s\to K \ell\nu$. In combination with future measurement, this calculation will provide an alternative exclusive semileptonic…

High Energy Physics - Lattice · Physics 2014-10-08 C. M. Bouchard , G. Peter Lepage , Christopher Monahan , Heechang Na , Junko Shigemitsu

A detailed investigation of the low-energy chiral expansion is presented within a model truncation of QCD. The truncation allows for a phenomenological description of the quark-quark interaction in a framework which maintains the global…

Nuclear Theory · Physics 2008-11-26 M. R. Frank , T. Meissner

Indirect CP violation in K \rightarrow {\pi}{\pi} decays plays a central role in constraining the flavor structure of the Standard Model (SM) and in the search for new physics. For many years the leading uncertainty in the SM prediction of…

High Energy Physics - Lattice · Physics 2011-11-10 S. Durr , Z. Fodor , C. Hoelbling , S. D. Katz , S. Krieg , T. Kurth , L. Lellouch , T. Lippert , C. McNeile , A. Portelli , K. K. Szabo

The $B_K$ parameter is computed in quenched lattice QCD with Wilson twisted mass fermions. Two variants of tmQCD are used; in both of them the relevant $\Delta S = 2$ four-fermion operator is renormalised multiplicatively. The…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. Dimopoulos , J. Heitger , F. Palombi , C. Pena , S. Sint , A. Vladikas

We use lattice QCD to calculate the form factors $f_+(q^2)$ and $f_0(q^2)$ for the semileptonic decay $B_s\to K\ell\nu$. Our calculation uses six MILC asqtad 2+1 flavor gauge-field ensembles with three lattice spacings. At the smallest and…

We present preliminary results for the calculation of the Kaon Bag parameter $B_K$ in $N_f=2+1$ lattice QCD, using M\"obius Domain Wall Fermion ensembles generated by the RBC-UKQCD collaboration. This computation is done directly at…

High Energy Physics - Lattice · Physics 2013-12-10 Julien Frison , Peter Boyle , Norman H. Christ , Nicolas Garron , Robert Mawhinney , Chris T. Sachrajda , Hantao Yin

We discuss nonfactorizable $1/N_c$ contributions in the amplitudes of non-leptonic exclusive decays of the type $B\rightarrow D\pi$ ($N_c$ is the number of colors). In a certain kinematical limit rather reliable estimates are possible. It…

High Energy Physics - Phenomenology · Physics 2010-11-01 B. Blok , M. Shifman

We propose a method to non-perturbatively calculate the forward-scattering matrix elements relevant to inclusive semi-leptonic B meson decays. Corresponding hadronic structure functions at unphysical kinematics are accessible through…

High Energy Physics - Lattice · Physics 2019-12-06 Shoji Hashimoto

We calculate the kaon B-parameter, B_K, to next-to-leading order in staggered chiral perturbation theory. We extend the usual power counting to include the effects of using perturbative (rather than non-perturbative) matching factors. Taste…

High Energy Physics - Lattice · Physics 2007-05-23 Ruth S. Van de Water , Stephen R. Sharpe

Theoretical predictions for B decay rates are rewritten in terms of the Upsilon(1S) meson mass instead of the b quark mass, using a modified perturbation expansion. The theoretical consistency of this expansion is shown both at low and high…

High Energy Physics - Phenomenology · Physics 2009-10-31 Andre H. Hoang , Zoltan Ligeti , Aneesh V. Manohar

The baryon Dirac form factor is computed at one-loop order in large-N_c baryon chiral perturbation theory, where N_c is the number of color charges. Loop graphs with octet and decuplet intermediate states are systematically incorporated…

High Energy Physics - Phenomenology · Physics 2015-12-09 Ruben Flores-Mendieta , Mayra Alejandra Rivera-Ruiz

The non-Fermi liquid physics at the edge of fractional quantum Hall systems is described by specific chiral Conformal Field Theories with central charge c=1. The charged quasi-particles in these theories have fractional charge and obey a…

Mesoscale and Nanoscale Physics · Physics 2008-11-26 R. A. J. van Elburg , K. Schoutens