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*Chiral* *Symmetry* *Breaking* in QCD

, 2004

"... Chiral Symmetry Breaking (CSB) is derived in QCD starting from the QCD Lagrangian and using Field Correlators Method (FCM). The kernel in the resulting equations responsible for CSB is directly connected to confinement, and therefore both phenomena occur and vanish together as supported by lattice d ..."

Abstract
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*Chiral*

*Symmetry*

*Breaking*(CSB) is derived in QCD starting from the QCD Lagrangian and using Field Correlators Method (FCM). The kernel in the resulting equations responsible for CSB is directly connected to confinement, and therefore both phenomena occur and vanish together as supported by lattice

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*Chiral* *Symmetry* *Breaking* in QCD

"... Chiral Symmetry Breaking (CSB) is derived in QCD starting from the QCD Lagrangian and using Field Correlators Method (FCM). The kernel in the resulting equations responsible for CSB is directly connected to con nement, and therefore both phenomena occur and vanish together as supported by lattice da ..."

Abstract
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*Chiral*

*Symmetry*

*Breaking*(CSB) is derived in QCD starting from the QCD Lagrangian and using Field Correlators Method (FCM). The kernel in the resulting equations responsible for CSB is directly connected to con nement, and therefore both phenomena occur and vanish together as supported by lattice

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*Chiral* *Symmetry* *Breaking* and Pions in

, 2003

"... We study gravity duals of large N non-supersymmetric gauge theories with matter in the fundamental representation by introducing a D7-brane probe into deformed AdS backgrounds. In particular, we consider a D7-brane probe in both the AdS Schwarzschild black hole solution and in the background found b ..."

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background, a quark-bilinear condensate develops only at non-zero quark mass. We speculate on the existence of a third order phase transition at a critical quark mass where the D7 embedding undergoes a geometric transition. In the Constable-Myers background, we find a

*chiral**symmetry**breaking*condensate###
*Chiral* *symmetry* *breaking* and stability of strangelets

, 2008

"... We discuss the stability of strangelets by considering dynamical chiral symmetry breaking and confinement. We use a U(3)L×U(3)R symmetric Nambu–Jona-Lasinio model for chiral symmetry breaking supplemented by a boundary condition for confinement. It is shown that strangelets with baryon number A<2 ..."

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We discuss the stability of strangelets by considering dynamical

*chiral**symmetry**breaking*and confinement. We use a U(3)L×U(3)R symmetric Nambu–Jona-Lasinio model for*chiral**symmetry**breaking*supplemented by a boundary condition for confinement. It is shown that strangelets with baryon number A###
Deconfinement, *Chiral* *Symmetry* *Breaking* and

"... We examine the feasibility of the proposition that there is a temperature range Tc < T < Tch in N f =0 QCD, where real Polyakov line (deconfined) vacuum exhibits valence spontaneous chiral symetry breaking and dynamical chiral polarization of Dirac eigenmodes. Detailed finite–volume analysis c ..."

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We examine the feasibility of the proposition that there is a temperature range Tc < T < Tch in N f =0 QCD, where real Polyakov line (deconfined) vacuum exhibits valence spontaneous

*chiral*symetry*breaking*and dynamical*chiral*polarization of Dirac eigenmodes. Detailed finite–volume analysis###
*Chiral* *symmetry* *breaking* as a consequence of

, 1999

"... A singular configuration of external static magnetic field in the form of a pointlike vortex polarizes the vacuum of quantized massless spinor field in 2+1-dimensional space-time. This results in an analogue of the Bohm-Aharonov effect: the chiral symmetry breaking condensate, energy density and cur ..."

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A singular configuration of external static magnetic field in the form of a pointlike vortex polarizes the vacuum of quantized massless spinor field in 2+1-dimensional space-time. This results in an analogue of the Bohm-Aharonov effect: the

*chiral**symmetry**breaking*condensate, energy density###
*Chiral* *Symmetry* *Breaking* in 2 + 1

, 1998

"... In 2 + 1 dimensional gauge thories with SU(Nc) color and 2Nf flavors of quarks in the fundamental representation, sphalerons, if present may lead to quark condensation and chiral symmetry breaking. The effect is similar to instanton induced chiral symmetry breaking in 3 + 1 dimensions and is due to ..."

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In 2 + 1 dimensional gauge thories with SU(Nc) color and 2Nf flavors of quarks in the fundamental representation, sphalerons, if present may lead to quark condensation and

*chiral**symmetry**breaking*. The effect is similar to instanton induced*chiral**symmetry**breaking*in 3 + 1 dimensions and is due###
*Chiral* *Symmetry* *Breaking* in Graphene

- Proceedings of the Nobel Symposium on Graphene and Quantum Matter, [arXiv:1108.2945 [hep-th

"... ar ..."

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spontaneous *chiral* *symmetry* *breaking*

, 2013

"... This Article is brought to you for free and open access by the Anesthesiology at UKnowledge. It has been accepted for inclusion in Anesthesiology ..."

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This Article is brought to you for free and open access by the Anesthesiology at UKnowledge. It has been accepted for inclusion in Anesthesiology