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Motivated by recent progress on many flavor QCD on a lattice, we investigate conformal/walking dynamics by using Schwinger-Dyson (SD) equation within an improved ladder approximation for two-loop running coupling. By numerically solving the SD equation, we obtain a pole mass $m_{p}$, pion decay constant $f_{pi}$, and investigate the chiral symmetry breaking and mass anomalous dimension $gamma_{m}$ in the presence of IR cutoffs $Lambda_{mathrm{IR}}$. We find that the chiral symmetry breaking is suppressed if IR cutoff $Lambda_{mathrm{IR}}$ becomes larger than the critical value near the dynamical mass ($Lambda_{mathrm{IR}}$ $simeq m_{D}$) In the conformal phase the $gamma_{m}$ is strongly suppressed by IR cutoffs for $Lambda _{mathrm{IR}}$ $simeq m_{p}$. We, then, obtain finite size hyperscaling (FSS) relation by adapting a linearized approximation for the SD equation, and examine the $gamma_{m}$ The results offer valuable insight and suggestion for analyses in lattice gauge theories.
We study corrections to the conformal hyperscaling relation in the conformal window of the large Nf QCD by using the ladder Schwinger-Dyson (SD) equation as a concrete dynamical model. From the analytical expression of the solution of the ladder SD e
We give a new perspective on the dynamics of conformal theories realized in the SU(N) gauge theory, when the number of flavors N_f is within the conformal window. Motivated by the RG argument on conformal theories with a finite IR cutoff Lambda_{IR},
In the search for a realistic walking technicolor model, QCD with many flavors is an attractive candidate. From the series of studies by the LatKMI collaboration, we present updated results of the scaling properties of various hadron spectra, includi
The dynamics of weakly coupled, non-abelian gauge fields at high temperature is non-perturbative if the characteristic momentum scale is of order |k|~ g^2 T. Such a situation is typical for the processes of electroweak baryon number violation in the
We exactly solve Dyson-Schwinger equations for a massless quartic scalar field theory. n-point functions are computed till n=4 and the exact propagator computed from the two-point function. The spectrum is so obtained, being the same of a harmonic os