scholarly journals Axial anomaly with the overlap-Dirac operator in arbitrary dimensions

2002 ◽  
Vol 2002 (09) ◽  
pp. 025-025 ◽  
Author(s):  
Takanori Fujiwara ◽  
Keiichi Nagao ◽  
Hiroshi Suzuki
1996 ◽  
Vol 11 (12) ◽  
pp. 979-986
Author(s):  
ALEXANDER MOROZ

The Dirac–Hamiltonian with the Aharonov–Bohm potential provides an example of a non-Fredholm operator for which all spectral asymmetry comes entirely from the continuous spectrum. In this case one finds that the use of standard definitions of the resolvent regularized, the heat kernel regularized, and the Witten indices misses the contribution coming from the continuous spectrum and gives vanishing spectral asymmetry and axial anomaly. This behavior in the case of the continuous spectrum seems to be general and its origin is discussed.


2018 ◽  
Vol 175 ◽  
pp. 04006 ◽  
Author(s):  
Mario Kieburg ◽  
Tim R. Würfel

It is well-known that staggered fermions do not necessarily satisfy the same global symmetries as the continuum theory. We analyze the mechanism behind this phenomenon for arbitrary dimension and gauge group representation. For this purpose we vary the number of lattice sites between even and odd parity in each single direction. Since the global symmetries are manifest in the lowest eigenvalues of the Dirac operator, the spectral statistics and also the symmetry breaking pattern will be affected. We analyze these effects and compare our predictions with Monte-Carlo simulations of naive Dirac operators in the strong coupling limit. This proceeding is a summary of our work [1].


1999 ◽  
Vol 463 (1) ◽  
pp. 63-68 ◽  
Author(s):  
Takanori Fujiwara ◽  
Hiroshi Suzuki ◽  
Ke Wu

2007 ◽  
Vol 16 (01) ◽  
pp. 59-67 ◽  
Author(s):  
M. DILLIG

We formulate natural regularization (NR) as a variant of dimensional regularization (DR). We replace the conventional dimensional reduction by a dimensionless regulator, allowing a transparent regularization of standard D-dimensional Feynman integrals. For arbitrary dimensions, we motivate and demonstrate explicitly the transition from the dimensionally reduced integration space to natural regularization. We establish the relation to cut-off regularization and point out the basic differences from dimensional regularization. Possible applications, such as to the axial anomaly or to gauge theories are briefly touched upon.


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