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Related papers: Microscopic study of the string breaking in QCD

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Virtual quark effects in lattice QCD are studied in an approach where the infrared modes are included in a precise and gauge-invariant manner. At fixed physical volume the required number of modes does not increase in the continuum limit,…

High Energy Physics - Lattice · Physics 2009-10-31 A. Duncan , E. Eichten , H. Thacker

In this article, the tensor-vector-pseudoscalar type of vertex is analyzed with the QCD sum rules and the local-QCD sum rules. Correspondingly, the hadronic coupling constants of D2*(2460), Ds2*(2573), B2*(5747) and Bs2*(5840), and their…

High Energy Physics - Phenomenology · Physics 2016-03-01 Zhen-Yu Li , Zhi-Gang Wang , Guo-Liang Yu

Estimating decay parameters in lattice simulations is a computationally demanding problem, requiring several volumes and momenta. We explore an alternative approach, where the transition amplitude can be extracted from the spectral…

High Energy Physics - Lattice · Physics 2025-04-22 Benoît Blossier , Jochen Heitger , Jan Neuendorf , Teseo San José

We calculate the decay constants of light and heavy-light pseudoscalar and vector mesons with improved soft-wall holographic wavefuntions, which take into account the effects of both quark masses and dynamical spins. We find that the…

High Energy Physics - Phenomenology · Physics 2018-05-15 Qin Chang , Xiao-Nan Li , Xin-Qiang Li , Fang Su

Virtual quark pair screening leads to breaking of the string between fundamental representation quarks in QCD. For unquenched four dimensional lattice QCD, this (so far elusive) phenomenon is studied using the recently developed truncated…

High Energy Physics - Lattice · Physics 2009-12-31 A. Duncan , E. Eichten , H. Thacker

Presented here is a study of well-posedness and asymptotic stability of a "degenerately damped" PDE modeling a vibrating elastic string. The coefficient of the damping may vanish at small amplitudes thus weakening the effect of the…

False vacuum decay typically proceeds via the nucleation of spherical bubbles of true vacuum, described by $O(4)$ symmetric field configurations in Euclidean time. In this work, we investigate how the presence of cosmic strings can catalyze…

Cosmology and Nongalactic Astrophysics · Physics 2026-01-30 Aleksandr Chatrchyan , Florian Niedermann , Phoebe Richman-Taylor

We study the QCD--DM scenario by analyzing the imprint of energy injection from decaying dark-sector particles on the spectral distortions (SDs) of the Cosmic Microwave Background (CMB). We adopt a unified framework capable of describing…

Cosmology and Nongalactic Astrophysics · Physics 2025-11-12 Jorge Mastache , Raúl Henriquez-Ortiz

We summarize recently improved results for the pseudoscalar [1,2] and vector [3] meson decay constants and their ratios from QCD spectral sum rules where N2LO + estimate of the N3LO PT and power corrections up to d< 6 dimensions have been…

High Energy Physics - Phenomenology · Physics 2015-12-01 Stephan Narison

In string theory the coupling ``constants'' appearing in the low-energy effective Lagrangian are determined by the vacuum expectation values of some (a priori) massless scalar fields (dilaton, moduli). This naturally leads one to expect a…

General Relativity and Quantum Cosmology · Physics 2014-11-17 Thibault Damour

We argue that in the context of string theory a large number N of connected degenerate vacua that mix will lead to a ground state with much lower energy, essentially because of the standard level repulsion of quantum theory for the…

High Energy Physics - Theory · Physics 2007-05-23 G. L. Kane , M. J. Perry , A. N. Zytkow

The separation of a heavy quark and antiquark pair leads to the formation of a tube of flux, or "string", which should break in the presence of light quark-antiquark pairs. This expected zero-temperature phenomenon has proven elusive in…

High Energy Physics - Lattice · Physics 2008-11-26 C. Bernard , T. DeGrand , C. DeTar , S. Gottlieb , U. M. Heller , J. Hetrick , P. Lacock , K. Orginos , R. L. Sugar , D. Toussaint

We use a covariant supermultiplet theory to determine the primary coupling constant associated with several types of two-body meson decay. Despite the diverse range of decays considered the primary coupling constant is surprisingly uniform.…

High Energy Physics - Phenomenology · Physics 2015-06-25 N. Jones , R. Delbourgo

The various decay modes of the type $B \to \gamma D^* $ are dynamically different. In general there are factorizable contributions, and there are pole diagrams and pseudoscalar exchange contributions at meson level. The purpose of this…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. O. Eeg J. A. Macdonald Sørensen

SU(3) gauge theory with eight massless fundamental fermions seems to be near the conformal boundary, and is a candidate theory of walking technicolor. Along the series of study by LatKMI collaboration using HISQ fermions, S-parameter and…

As we pointed out recently, the neutral decays $B_d\to\pi^\mp K^\pm$ and $B_d\to\pi^0K$ may provide non-trivial bounds on the CKM angle $\gamma$. In this paper, we reconsider this approach in the light of recent CLEO data, which look very…

High Energy Physics - Phenomenology · Physics 2008-11-26 Andrzej J. Buras , Robert Fleischer

We show that a linear scaling between the weak decay constants of pseudoscalar and the vector mesons masses is supported by the available experimental data. The decay constant scale as $f_m/f_{pi}=M_V/M_{\rho}$ (f_m is decay constant and…

High Energy Physics - Phenomenology · Physics 2015-06-25 L. A. M. Salcedo , J. P. B. C. de Melo , D. Hadjmichef , T. Frederico

We study the decay law for a moving unstable particle. The usual time-dilatation formula states that the decay width for an unstable state moving with a momentum $p$ and mass $M$ is $\tilde{\Gamma}_{p}=\Gamma M/\sqrt{p^{2}+M^{2}}$ with…

High Energy Physics - Phenomenology · Physics 2016-11-03 Francesco Giacosa

We derive analytic formulae for the energy average (including the energy average of the fluctuation contribution) and variance of the intraband decay intensity of a superdeformed band. Our results may be expressed in terms of three…

Nuclear Theory · Physics 2009-11-07 A. J. Sargeant , M. S. Hussein , M. P. Pato , M. Ueda

The attenuation factor F responsible for the decay out of a superdeformed (SD) band is calculated with the help of a statistical model. This factor is given by 1/F = (1 + Gamma(down) / Gamma(S)). Here, Gamma(S) is the width for the…

Nuclear Theory · Physics 2009-01-23 H. A. Weidenmueller , P. von Brentano , B. R. Barrett