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Related papers: Pole Mass, Width, and Propagators of Unstable Ferm…

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It is shown that conventional mass renormalization, when applied to photonic or gluonic corrections to unstable particle propagators, leads to non-convergent series in the resonance region. A solution of this problem, based on the concepts…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Passera , A. Sirlin

In gauge theories, the mass of a field has been regarded as a purely on-shell concept: the pole mass is gauge-invariant, but the off-shell propagator has had no gauge-invariant definition of mass. We show that renormalization defines a…

High Energy Physics - Theory · Physics 2026-04-07 Kang-Sin Choi

In the gauge theory context, a definition of branching ratios and partial widths of unstable particles is proposed that satisfies the basic principles of additivity and gauge independence. A simpler definition, similar to the conventional…

High Energy Physics - Theory · Physics 2009-10-31 P. A. Grassi , B. A. Kniehl , A. Sirlin

We study the behavior of the pole of the fermion propagator, in QED in $n$-dimensions, in a general class of gauges which interpolate between the covariant, the axial and the Coulomb gauges. We use Nielsen identities, following from the…

High Energy Physics - Theory · Physics 2015-06-16 Ashok K. Das , J. Frenkel

We study the Ward-Takahashi identities in the standard model with the gauge fixing terms given by (1.1) and (1.2). We find that the isolated singularities of the propagators for the unphysical particles are poles of even order, not the…

High Energy Physics - Theory · Physics 2007-05-23 Hung Cheng , S. P. Li

In this review, we present a derivation of the on-shell renormalization conditions for scalar and fermionic fields in theories with and without parity conservation. We also discuss the specifics of Majorana fermions. Our approach only…

High Energy Physics - Phenomenology · Physics 2017-03-22 W. Grimus , M. Löschner

Propagators of unstable particles are considered in the spectral representation which naturally follows from the concept of continuous mass. The spectral functions are found with the help of the most general formal and physical assumptions.…

High Energy Physics - Phenomenology · Physics 2014-09-01 Vladimir Kuksa

The propagators of unstable particles are considered in the framework of the convolution representation. Spectral function was found for a special case when the propagator of scalar unstable particle has Breight-Wigner form. The expressions…

High Energy Physics - Phenomenology · Physics 2015-12-04 Vladimir Kuksa

In order to obtain proper wave-function renormalization constants for unstable fermion and consist with Breit-Wigner formula in the resonant region, We have assumed an extension of the LSZ reduction formula for unstable fermion and adopted…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yong Zhou

A partial resummation of perturbation theory is described for field theories containing spin-1/2 particles in states that may be far from thermal equilibrium. This allows the nonequilibrium state to be characterized in terms of…

High Energy Physics - Phenomenology · Physics 2009-10-31 I. D. Lawrie , D. B. McKernan

Within the Pauli-Villars regularization technique the fermion propagator is studied in the framework of Schwinger-Dyson equations in the Euclidean space. Making the generalization of Fukuda and Kugo proposals, the analytical continuation is…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. Sauli , F. Kleefeld

Unstable particles are notorious in perturbative quantum field theory for producing singular propagators in scattering amplitudes that require regularization by the finite width. In this review I discuss the construction of an effective…

High Energy Physics - Phenomenology · Physics 2015-01-30 M. Beneke

Quantum field model of unstable particles with random mass is suggested to describe the finite-width effects in decay rate. Within the framework of this model we derive the convolution formula for a width of the channels with unstable…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. I. Kuksa

We consider a mixed system of unstable Majorana fermions in a general parity-nonconserving theory and renormalize its propagator matrix to all orders in the pole scheme, in which the squares of the renormalized masses are identified with…

High Energy Physics - Theory · Physics 2014-06-18 Bernd A. Kniehl

Models with extra dimensions may give new effects visible at future experiments. In these models, bulk fields can develop localized corrections to their kinetic terms which can modify the phenomenological predictions in a sizeable way. We…

High Energy Physics - Phenomenology · Physics 2007-05-23 F. del Aguila , M. Perez-Victoria , J. Santiago

The previously developed renormalizable perturbative 1/N-expansion in higher dimensional scalar field theories is extended to gauge theories with fermions. It is based on the $1/N_f$-expansion and results in a logarithmically divergent…

High Energy Physics - Theory · Physics 2007-05-23 D. I. Kazakov , G. S. Vartanov

We discuss theoretical and phenomenological aspects of the use of boson propagators with energy-dependent widths in predictions for high-energy scattering processes. In general, gauge invariance is violated in such calculations. We discuss…

The coupling of an unparticle operator O_U to Standard Model particles opens up the possibility of unparticle decays into standard model fields. We study this issue by analyzing the pole structure (and spectral function) of the unparticle…

High Energy Physics - Phenomenology · Physics 2010-04-23 A. Delgado , J. R. Espinosa , J. M. No , M. Quirós

The different schemes for the definition of the Z boson mass are analyzed. It is shown that the scheme, defining the mass as pole of the real part of the Z boson propagator and the width as the imaginary part of the propagator at the same…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Gegelia , G. Japaridze , A. Tkabladze , A. Khelashvili , K. Turashvili

We construct the propagator for a free fermionic unparticle field from basic considerations of scale and Lorentz invariance. The propagator is fixed up to a normalization factor which is required to recover the result of a free massless…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yi Liao
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