Towards the chiral limit with dynamical blocked Wilson fermions

1992 ◽  
Vol 46 (8) ◽  
pp. 3618-3629 ◽  
Author(s):  
I. Barbour ◽  
E. Laermann ◽  
Th. Lippert ◽  
K. Schilling
Keyword(s):  
1999 ◽  
Vol 73 (1-3) ◽  
pp. 231-233
Author(s):  
A. Hoferichter ◽  
E. Laermann ◽  
V.K. Mitrjushkin ◽  
M. Müller-Preussker ◽  
P. Schmidt
Keyword(s):  

1997 ◽  
Vol 74 (3) ◽  
pp. 541-548 ◽  
Author(s):  
A. Hoferichter ◽  
V.K. Mitrjushkin ◽  
M. Müller-Preussker

1998 ◽  
Vol 63 (1-3) ◽  
pp. 164-166 ◽  
Author(s):  
A. Hoferichter ◽  
E. Laermann ◽  
V.K. Mitrjushkin ◽  
M. Müller-Preussker ◽  
P. Schmidt

1999 ◽  
Vol 466 (2-4) ◽  
pp. 287-292 ◽  
Author(s):  
Christof Gattringer ◽  
Ivan Hip ◽  
C.B. Lang

1990 ◽  
Vol 234 (3) ◽  
pp. 333-338 ◽  
Author(s):  
Khalil Bitar ◽  
A.D. Kennedy ◽  
Pietro Rossi

1992 ◽  
Vol 07 (10) ◽  
pp. 871-880 ◽  
Author(s):  
YOSHIO KIKUKAWA

We formulate lattice SU (N) Thirring model in which two Wilson fermions describe the respective left- and right-handed components of the Dirac fermion in the continuum model. Only chirally projected half components of the Wilson fermions have four-fermion interaction. As to their non-interacting components, there exist shift symmetries discussed by Golterman and Petcher. Axial U (1) Ward-Takahashi identity is examined by weak coupling expansion. It is shown in all orders of the weak coupling expansion that the chiral limit is achieved by simply setting fermion bare mass equal to zero, and that a lattice operator has no mixing due to the Wilson masses with the operators of wrong chiral representation and of lower dimensionality.


1998 ◽  
Vol 58 (11) ◽  
Author(s):  
A. Hoferichter ◽  
V. K. Mitrjushkin ◽  
M. Müller-Preussker ◽  
H. Stüben

1994 ◽  
Vol 34 ◽  
pp. 537-539
Author(s):  
A. Hoferichter ◽  
V.K. Mitrijushkin ◽  
M. Müller-Preussker ◽  
Th. Neuhaus

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