Search results for "Chiral symmetry"

showing 5 items of 75 documents

New Angle on the Strong CP and Chiral Symmetry Problems from a Rotating Mass Matrix

2007

It is shown that when the mass matrix changes in orientation (i.e. rotates) in generation space for a changing energy scale, the masses of the lower generations are not given just by its eigenvalues. In particular, these masses need not be zero even when the eigenvalues are zero. In that case, the strong CP problem can be avoided by removing the unwanted theta term by a chiral transformation not in contradiction with the nonvanishing quark masses experimentally observed. Similarly, a rotating mass matrix may shed new light on the problem of chhiral symmetry breaking. That the fermion mass matrix may so rotate with the scale has been suggested before as a possible explanation for up-down fer…

QuarkPhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeFOS: Physical sciencesFísicaAstronomy and AstrophysicsFermionSpace (mathematics)Mass matrixAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Quantum mechanicsStrong CP problemChiral symmetry breakingEigenvalues and eigenvectorsMixing (physics)
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Nucleon and delta masses in QCD

1992

Using the positivity of the path integral measure of $QCD$ and defining a structure for the quark propagator in a background field according to the fluxon scenario for confinement, we calculate and compare the correlators for nucleon and delta. From their shape we elucidate about the origin of their mass difference, which in our simplified scenario is due to the tensor structure in the propagator. This term arises due to a dynamical mechanism which is responsible simultaneously for confinement and spontaneous chiral symmetry breaking. Finally we discuss, by comparing the calculated correlators with the Lehmann representation, the possibility that a strong CP and/or P violation occurs as a c…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsField (physics)PropagatorFOS: Physical sciencesCromodinàmica quànticaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Violació CP (Física nuclear)Path integral formulationTensorChiral symmetry breakingNucleon
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Quark gap equation within the analytic approach to QCD

2005

The compatibility between the QCD analytic invariant charge and chiral symmetry breaking is examined in detail. The coupling in question incorporates asymptotic freedom and infrared enhancement into a single expression, and contains only one adjustable parameter with dimension of mass. When inserted into the standard form of the quark gap-equation it gives rise to solutions displaying singular confining behavior at the origin. By relating these solutions to the pion decay constant, a rough estimate of about 880 MeV is obtained for the aforementioned mass-scale.

QuarkPhysicsQuantum chromodynamicsStandard formHigh Energy Physics - TheoryNuclear and High Energy PhysicsHigh Energy Physics::LatticeFísicaFOS: Physical sciencesAsymptotic freedomAtomic and Molecular Physics and OpticsTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Chiral symmetry breakingPion decay constant
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πB8B8andσB8B8couplings from a chiral quark potential model

2008

From an SU(2)$\ensuremath{\bigotimes}$SU(2) chiral quark potential model incorporating spontaneous chiral symmetry breaking the asymptotic $\ensuremath{\pi}$ and $\ensuremath{\sigma}$ exchange pieces of the $\mathit{NN}$ potential are generated. From them the $\ensuremath{\pi}\mathit{NN}$ and $\ensuremath{\sigma}\mathit{NN}$ coupling constants can be extracted. The generalization to SU(3)$\ensuremath{\bigotimes}$SU(3) allows for a determination of $\ensuremath{\pi}{B}_{8}{B}_{8}$ and $\ensuremath{\sigma}{B}_{8}{B}_{8}$ coupling constants according to exact SU(3) hadron symmetry. The implementation of the values of the couplings at ${Q}^{2}=0$ provided by QCD sum rules and/or phenomenology m…

QuarkQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsQCD sum rulesMesonHigh Energy Physics::PhenomenologyHadronQuark modelSymmetry breakingChiral symmetry breakingPhysical Review C
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Chiral symmetry andπ-πscattering in the covariant spectator theory

2014

The π-π scattering amplitude calculated with a model for the quark-antiquark interaction in the framework of the Covariant Spectator Theory (CST) is shown to satisfy the Adler zero constraint imposed by chiral symmetry. The CST formalism is established in Minkowski space and our calculations are performed in momentum space. We prove that the axial-vector Ward-Takahashi identity is satisfied by our model. Then we show that, similarly to what happens within the Bethe-Salpeter formalism, application of the axial-vector Ward Takahashi identity to the CST π-π scattering amplitude allows us to sum the intermediate quark-quark interactions to all orders. Thus, the Adler self-consistency zero for π…

Ward–Takahashi identityPhysicsNuclear and High Energy PhysicsChiral symmetryBethe–Salpeter equation010308 nuclear & particles physicsScatteringHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyPosition and momentum space01 natural sciencesScattering amplitudeQuantum mechanics0103 physical sciencesMinkowski spaceCovariant transformation010306 general physicsPhysical Review D
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