Nonresonant three-body decays of charmed mesons in chiral perturbation theory

In this paper, the non-leptonic three-body decays [Formula: see text], [Formula: see text], [Formula: see text] are studied by introducing two-meson distribution amplitude for the [Formula: see text], [Formula: see text] and [Formula: see text] pairs in naive and QCD factorization (QCDF) approaches, such that the analysis is simplified into quasi-two body decays. By considering that the vector meson is being ejected in factorization, the resonant and non-resonant contributions are analyzed by using intermediate mesons in Breit–Wigner resonance formalism and the heavy meson chiral perturbation theory (HMChPT), respectively. The calculated values of the resonant and non-resonant branching ratio of [Formula: see text], [Formula: see text] and [Formula: see text] decay modes are compared with the experimental data. For [Formula: see text] and [Formula: see text], the non-resonant contributions are about 70–80% of experimental data, for which the total results by considering resonant contributions are in good agreement with the experiment.

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Excited charmed mesons in chiral perturbation theory

Physics Letters B ◽

10.1016/0370-2693(92)91115-p ◽

1992 ◽

Vol 288 (3-4) ◽

pp. 360-366 ◽

Cited By ~ 47

Author(s):

Ulrich Kilian ◽

Jürgen G. Körner ◽

Dan Pirjol

Keyword(s):

Perturbation Theory ◽

Chiral Perturbation Theory ◽

Chiral Perturbation ◽

Charmed Mesons

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Accurate nucleon-nucleon potential based upon chiral perturbation theory

10.1063/1.1469952 ◽

2002 ◽

Author(s):

D. R. Entem ◽

R. Machleidt

Keyword(s):

Perturbation Theory ◽

Chiral Perturbation Theory ◽

Nucleon Nucleon ◽

Chiral Perturbation ◽

Nucleon Potential

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The axion-baryon coupling in SU(3) heavy baryon chiral perturbation theory

Journal of High Energy Physics ◽

10.1007/jhep08(2021)024 ◽

2021 ◽

Vol 2021 (8) ◽

Author(s):

Thomas Vonk ◽

Feng-Kun Guo ◽

Ulf-G. Meißner

Keyword(s):

Perturbation Theory ◽

Chiral Perturbation Theory ◽

Heavy Baryon ◽

Power Counting ◽

Flavor Symmetry ◽

Chiral Perturbation ◽

Third Order ◽

Stellar Objects ◽

The Past ◽

Dense Nuclear Matter

Abstract In the past, the axion-nucleon coupling has been calculated in the framework of SU(2) heavy baryon chiral perturbation theory up to third order in the chiral power counting. Here, we extend these earlier studies to the case of heavy baryon chiral perturbation theory with SU(3) flavor symmetry and derive the axion coupling to the full SU(3) baryon octet, showing that the axion also significantly couples to hyperons. As studies on dense nuclear matter suggest the possible existence of hyperons in stellar objects such as neutron stars, our results should have phenomenological implications related to the so-called axion window.

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Light front Hamiltonian for boson form of QED (1 + 1) in Pauli–Villars regularization

International Journal of Modern Physics A ◽

10.1142/s0217751x19501136 ◽

2019 ◽

Vol 34 (21) ◽

pp. 1950113

Author(s):

V. A. Franke ◽

M. Yu. Malyshev ◽

S. A. Paston ◽

E. V. Prokhvatilov ◽

M. I. Vyazovsky

Keyword(s):

Perturbation Theory ◽

Chiral Perturbation Theory ◽

Chiral Condensate ◽

Light Front ◽

Coupling Constants ◽

Hamiltonian Approach ◽

Chiral Perturbation ◽

Dimensional Models ◽

Villars Regularization ◽

Ultraviolet Regularization

Light front (LF) Hamiltonian for QED in [Formula: see text] dimensions is constructed using the boson form of this model with additional Pauli–Villars-type ultraviolet regularization. Perturbation theory, generated by this LF Hamiltonian, is proved to be equivalent to usual covariant chiral perturbation theory. The obtained LF Hamiltonian depends explicitly on chiral condensate parameters which enter in a form of some renormalization of coupling constants. The obtained results can be useful when one attempts to apply LF Hamiltonian approach for [Formula: see text]-dimensional models like QCD.

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