scholarly journals Perturbation calculation of the axial anomaly of a Ginsparg-Wilson lattice Dirac operator

2002 ◽  
Vol 65 (5) ◽  
Author(s):  
Ting-Wai Chiu ◽  
Tung-Han Hsieh
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.


2021 ◽  
Vol 966 ◽  
pp. 115385
Author(s):  
Emil Mottola ◽  
Andrey V. Sadofyev
Keyword(s):  

2005 ◽  
Vol 315 (2) ◽  
pp. 467-487 ◽  
Author(s):  
A. Kirchberg ◽  
J.D. Länge ◽  
A. Wipf
Keyword(s):  

Author(s):  
Piero D’Ancona ◽  
Luca Fanelli ◽  
Nico Michele Schiavone

AbstractWe prove that the eigenvalues of the n-dimensional massive Dirac operator $${\mathscr {D}}_0 + V$$ D 0 + V , $$n\ge 2$$ n ≥ 2 , perturbed by a potential V, possibly non-Hermitian, are contained in the union of two disjoint disks of the complex plane, provided V is sufficiently small with respect to the mixed norms $$L^1_{x_j} L^\infty _{{\widehat{x}}_j}$$ L x j 1 L x ^ j ∞ , for $$j\in \{1,\dots ,n\}$$ j ∈ { 1 , ⋯ , n } . In the massless case, we prove instead that the discrete spectrum is empty under the same smallness assumption on V, and in particular the spectrum coincides with the spectrum of the unperturbed operator: $$\sigma ({\mathscr {D}}_0+V)=\sigma ({\mathscr {D}}_0)={\mathbb {R}}$$ σ ( D 0 + V ) = σ ( D 0 ) = R . The main tools used are an abstract version of the Birman–Schwinger principle, which allows in particular to control embedded eigenvalues, and suitable resolvent estimates for the Schrödinger operator.


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