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Related papers: Pseudoscalar Vertex and Quark Masses

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We develop quenched chiral perturbation theory for vector mesons made of light quarks, in the limit where the vector meson masses are much larger than the pion mass. We use this theory to extract the leading nonanalytic dependence of the…

High Energy Physics - Phenomenology · Physics 2009-10-30 Michael Booth , George Chiladze , Adam F. Falk

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

The masses of $uudd\bar s $, $uudd\bar d$ and $uuss\bar d$ pentaquarks are evaluated in a framework of both the Effective Hamiltonian approach to QCD and spinless Salpeter using the Jaffe--Wilczek diquark approximation and the string…

High Energy Physics - Phenomenology · Physics 2009-11-11 I. M. Narodetskii , C. Semay , B. Silvestre-Brac , Yu. A. Simonov , M. A. Trusov

Because quarks in hadronic states are subjected to strong QCD forces, it is not straight-forward to apply calculation obtained at the quark level to physical processes involving hadrons. In this paper we present a new approach to treat the…

High Energy Physics - Phenomenology · Physics 2013-04-15 Swee Ping Chia

A short overview of recent progress in describing kaon and pion decays within Chiral Perturbation Theory is presented. Particular attention is devoted to the issues of final-state interactions and isospin breaking in $K \to 2 \pi$, as well…

High Energy Physics - Phenomenology · Physics 2017-08-23 Gino Isidori

We discuss the modified top quark condensation model proposed in \cite{VZ2015}. This construction was inspired by the top - seesaw scenario, in which the extra heavy fermion $\chi$ is added that may be paired with the top quark. Besides,…

High Energy Physics - Phenomenology · Physics 2017-08-29 Z. V. Khaidukov , M. A. Zubkov

We point out that it is possible to associate the electroweak Higgs boson with the pseudo-Goldstone boson of broken scale invariance, thus resolving the hierarchy problem in a technically natural way. We illustrate this idea with two…

High Energy Physics - Phenomenology · Physics 2008-11-26 Robert Foot , Archil Kobakhidze , Raymond R. Volkas

We argue that the axion arising in the solution of the strong CP problem can be identified with the Majoron, the (pseudo-)Goldstone boson of spontaneously broken lepton number symmetry. At low energies, the associated $U(1)_L$ becomes, via…

High Energy Physics - Phenomenology · Physics 2011-02-08 Adam Latosinski , Krzysztof A. Meissner , Hermann Nicolai

The $\sigma$ mesons may be considered as the Higgs boson of strong interaction. While the observation of the electroweak Higgs boson is the primary goal in ongoing experiments at the LHC, the $\sigma$ meson is by now well studied both as an…

High Energy Physics - Phenomenology · Physics 2011-07-22 Martin Schumacher

We introduce coupled channels of Bethe-Salpeter mesons both in the boundstate equation for mesons and in the mass gap equation for chiral symmetry. Consistency is insured by the Ward Identities for axial currents, which preserve the…

Nuclear Theory · Physics 2010-11-15 Pedro Bicudo

The decay constants of pseudoscalar and vector heavy-light mesons are calculated in the framework of the relativistic quark model with the completely relativistic treatment of the light quark. It is argued that relativistic effects play a…

High Energy Physics - Phenomenology · Physics 2009-11-07 D. Ebert , R. N. Faustov , V. O. Galkin

We use the covariant spectator theory with an effective quark-antiquark interaction, containing Lorentz scalar, pseudoscalar, and vector contributions, to calculate the masses and vertex functions of, simultaneously, heavy and heavy-light…

High Energy Physics - Phenomenology · Physics 2017-10-25 Sofia Leitão , Alfred Stadler , M. T. Peña , Elmar P. Biernat

The nucleon-nucleon problem is studied as a six-quark system in a nonrelativistic chiral constituent quark model where the Hamiltonian contains a linear confinement and a pseudoscalar meson (Goldstone boson) exchange interaction between the…

High Energy Physics - Phenomenology · Physics 2009-11-07 D. Bartz

In Little Higgs models, the Higgs mass is stabilized at the one-loop level by the mechanism of collective symmetry breaking. Typically, the basic ingredient of these models is a large(r) global symmetry group spontaneously broken at a scale…

High Energy Physics - Phenomenology · Physics 2014-11-18 Wolfgang Kilian , David Rainwater , Juergen Reuter

We present a consistent analysis of $\Upsilon$ sum rules and $B$-meson semileptonic width in the next-to-next-to-leading order in the strong coupling constant. The analysis is based on the analytical result for the heavy quark vector…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. A. Penin , A. A. Pivovarov

We argue that for a Higgs boson mass M_H ~125 GeV, as suggested by recent Higgs searches at the LHC, the inclusion of electroweak radiative corrections in the relationship between the pole and MS-bar masses of the top quark reduces the…

High Energy Physics - Phenomenology · Physics 2015-06-12 Fred Jegerlehner , Mikhail Yu. Kalmykov , Bernd A. Kniehl

The relativistic four-quark equations are found in the framework of coupled-channel formalism. The dynamical mixing of the meson-meson states with the four-quark states is considered. The four-quark amplitudes of the tetraquarks with hidden…

High Energy Physics - Phenomenology · Physics 2008-12-02 S. M. Gerasyuta , V. I. Kochkin

We investigate the efficiency of single timeslice stochastic sources for the calculation of light meson masses on the lattice as one varies the quark mass. Simulations are carried out with Nf = 2 flavours of non-perturbatively O(a) improved…

High Energy Physics - Lattice · Physics 2011-11-28 E. Endress , A. Jüttner , H. Wittig

We base our chiral symmetry approach on the quark-level linear sigma model Lagrangian. Then we review the Nambu--Goldstone theorem with vanishing pi, K, eta_8 masses. Next we dynamically generate the pi, K, eta_8 masses away from the chiral…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. Kekez , D. Klabucar , M. D. Scadron

Certain dark matter interactions with nuclei are mediated possibly by a scalar or pseudoscalar Higgs boson. The estimation of the corresponding cross sections requires a correct evaluation of the couplings between the scalar or pseudoscalar…

High Energy Physics - Phenomenology · Physics 2015-06-04 Hai-Yang Cheng , Cheng-Wei Chiang
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