Results 61 to 70 of about 278,956 (259)
Phase structure of NJL model with finite quark mass and QED correction [PDF]
We study QED corrections to the chiral symmetry breaking in Nambu-Jona-Lasinio (NJL) model with two flavors of quarks. In the model the isospin symmetry is broken by differences of the current quark masses and the electromagnetic charges between up and ...
Fujihara, Takahiro+2 more
core +3 more sources
A Master Formula for Chiral Symmetry Breaking [PDF]
We derive a master formula for chiral $SU(2)\times SU(2)$ breaking, based on the Veltman-Bell equations and the Peierls-Dyson relation. Our approach does not rely on the use of the soft pion limit or an expansion around the chiral limit, and yields exact results for on-shell pions. Threshold theorems for $ N\rightarrow N$, $ N\rightarrow N$, $ N\
Hidenaga Yamagishi, Ismail Zahed
openaire +3 more sources
On the Bose symmetry and the left- and right-chiral anomalies
It is generally assumed that in order to preserve Bose symmetry in the left- (or right-chiral) current it is necessary to equally distribute the chiral anomaly between the vectorial and the axial Ward identities, requiring the use of counterterms to ...
J. S. Porto+4 more
doaj +1 more source
We study in detail the effect of the finite current quark mass on chiral symmetry breaking, in the framework of truncated Coulomb gauge QCD with a linear confining quark-antiquark potential. In the chiral limit of massless current quarks, the breaking of
Adler+38 more
core +1 more source
Schwinger-Dyson equations are used to study spontaneous chiral and parity symmetry breaking of three dimensional quantum electrodynamics with two-component fermions. This theory admits a topological photon mass that explicitly breaks parity symmetry and generates a fermion mass.
arxiv +1 more source
Abelian dominance in chiral symmetry breaking [PDF]
Calculations of the chiral condensate $\langle \bar \rangle$ on the lattice using staggered fermions and the Lanczos algorithm are presented. Three gauge fields are considered: the quenched non-Abelian field, the Abelian field projected in the maximal Abelian gauge, and the monopole field further decomposed from the Abelian field.
Frank X. Lee+2 more
openaire +3 more sources
Chiral symmetry breaking in the truncated Coulomb Gauge II. Non-confining power law potentials
In this paper we study the breaking of chiral symmetry with non-confining power-like potentials. The region of allowed exponents is identified and, after the previous study of confining (positive exponent) potentials, we now specialize in shorter range ...
D. Klabucar, O. Kaczmarek, P. Bicudo
core +1 more source
Criterion for dynamical chiral symmetry breaking [PDF]
10 pages, 2 figures; made minor changes, published ...
Bithika Jain+3 more
openaire +3 more sources
Four-fermion deformations of the massless Schwinger model and confinement
We consider the massless charge-N Schwinger model and its deformation with two four-fermion operators. Without the deformations, this model exhibits chiral symmetry breaking without confinement. It is usually asserted that the massless Schwinger model is
Aleksey Cherman+4 more
doaj +1 more source
Inhomogeneous phases and chiral symmetry breaking
Presented at ICHEP-2014, Valencia ...
Vivian de la Incera+2 more
openaire +3 more sources