scholarly journals Running coupling constant and mass anomalous dimension of six-flavor SU(2) gauge theory

2013 ◽  
Vol 88 (9) ◽  
Author(s):  
M. Hayakawa ◽  
K.-I. Ishikawa ◽  
S. Takeda ◽  
N. Yamada
1994 ◽  
Vol 422 (1-2) ◽  
pp. 382-396 ◽  
Author(s):  
G.M. de Divitiis ◽  
R. Frezzotti ◽  
M. Guagnelli ◽  
R. Petronzio

1993 ◽  
Vol 04 (06) ◽  
pp. 1179-1193 ◽  
Author(s):  
G. S. BALI ◽  
K. SCHILLING ◽  
J. FINGBERG ◽  
U. M. HELLER ◽  
F. KARSCH

A detailed investigation of the temperature dependence of the spatial string tension σs in SU(2) gauge theory is presented. A sustained performance of 3 GFLOPS on a 64K Connection Machine CM-2 equivalent has been achieved. Scaling of σs between β = 2.5115 and β = 2.74, on large lattices, is demonstrated. Below the critical temperature, Tc, σs remains constant. For temperatures larger than 2Tc the temperature dependence can be parametrized by σs(T) = (0.369 ± 0.014)2g4(T)T2, where g(T) is a 2-loop running coupling constant with the scale parameter determined as ΛT = (0.076 ± 0.013)Tc.


1989 ◽  
Vol 04 (15) ◽  
pp. 1409-1417 ◽  
Author(s):  
V.A. MIRANSKY ◽  
TATSUHIKO NONOYAMA ◽  
KOICHI YAMAWAKI

In the ladder asymptotically free gauge models with one-loop running coupling constant and additional four-fermion interaction, the structure of the phase diagram in coupling constants is determined. The anomalous dimension γm of the composite operator [Formula: see text] is calculated on the full critical line of the diagram. The possibilities of the examination of the phase diagram of such theories in lattice computer simulations are discussed.


2005 ◽  
Vol 20 (08n09) ◽  
pp. 1955-1958
Author(s):  
A. MIRJALILI ◽  
ALI N. KHORRAMIAN ◽  
S. ATASHBAR TEHRANI

To obtain the improved QCD predictions for the moments of the xF3 structure function in νN scattering, three-loop Wilson coefficients with the corresponding NNLO anomalous dimension coefficients is used. A comparison between QCD predictions and the xF3 data of the CCFR collaboration has been done in which the Bernstein Polynomial method is used in the complete renormalization group improvement approach. A direct fits for [Formula: see text] over the corresponding range of Q2 with five effective quark flavours, is performed.


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