Fermions in random gauge fields and chiral-symmetry breaking

Random superpositions of gauge fields such that a fermion can propagate in them along the same one-dimensional trajectory in four-dimensional space over arbitrary distances without reduction of the amplitude are considered. Conditions are found under which such structures possess a finite density of fermion zero modes. The possibility of chiral-symmetry breaking in these configurations of gauge fields is explored.     

Ambiguities in chiral-symmetry breaking using the effective potential approach

Using a form of the effective potential for composite operators with a variational approach we show that it is possible to get different directions of the chiral phase transition in QCD. Which one occurs depends on the way the Schwinger-Dyson equation for the fermion self-energy is used in the 2-loop term of the effective potential. We must choose the 2-loop term which agrees with phenomenology in each form of the effective potential.     

Holographic solitons in centrosymmetric photorefractive crystals

The conditions necessary for obtaining holographic solitons in centrosymmetric photorefractive crystals are discussed. When both the intensity modulation of the two interacting waves and the angle between the vector of each beam and the longitudinal axis are small, centrosymmetric photorefractive crystals with a positive (or negative ) effective quadratic electro-optic coefficient are able to support bright (or dark) holographic solitons. The intensity width at half maximum of bright and dark solitons is inversely proportional to the external bias field. The holographic solitons can also exit in dissipative centrosymmetric photorefractive crystals when the applied external bias field is large enough.     

A comparative study of the chiral-symmetry breaking solutions in QCD

We make a comparative study of the different asymptotic forms of the dynamical mass in quantum chomodynamics. Using the effective potential for composite operator we can determine which one of those dynamical mass correspond to a chiral-symmetry breaking à 1 a Nambu-Goldstone.     

Spontaneous chiral-symmetry breaking of lattice QCD with massless dynamical quarks

One of the most challenging issues in QCD is the investigation of spontaneous chiral-symmetry breaking, which is characterized by the non-vanishing chiral condensate when the bare fermion mass is zero. In standard methods of the lattice gauge theory, one has to perform expensive simulations at multiple bare quark masses, and employ some modeled functions to extrapolate the data to the chiral limit. This paper applies the probability distribution function method to computing the chiral condensate in lattice QCD with massless dynamical quarks, without any ambiguous mass extrapolation. The results for staggered quarks indicate that this might be a promising and efficient method for investigating the spontaneous chiral-symmetry breaking in lattice QCD, which deserves further investigation.