Anomalies at finite density and chiral fermions
arXiv:0906.5188 · doi:10.1103/PhysRevD.81.034501
Abstract
Using perturbation theory in the Euclidean (imaginary time) formalism as well as the non-perturbative Fujikawa method, we verify that the chiral anomaly equation remains unaffected in the presence of nonzero chemical potential, . We extend our considerations to fermions with exact chiral symmetry on the lattice and discuss the consequences for the recent Bloch-Wettig proposal for the Dirac operator at finite chemical potential. We propose a new simpler method of incorporating and compare it with the Bloch-Wettig idea.
12 pages, 3 figures,some typos corrected, a better proof for the μindependence of anomaly is given in section IIB, v4: the published version
References in corpus (5)
Cited by in corpus (15)
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