2001
DOI: 10.1103/physrevd.63.048501
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Comment on “Topological invariants, instantons, and the chiral anomaly on spaces with torsion”

Abstract: In Riemann-Cartan spacetimes with torsion only its axial covector piece A couples to massive Dirac fields. Using renormalization group arguments, we show that in addition to the familiar Riemannian term only the Pontrjagin type four-form dAٙdA arises additionally in the chiral anomaly, but not the Nieh-Yan term d*A, as has been claimed in a recent paper ͓Phys. Rev. D. 55, 7580 ͑1997͔͒.

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Cited by 60 publications
(42 citation statements)
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“…The addition of the Pontrjagin term with respect to the Riemannian curvature R {} αβ and the axial torsion one-form A := * (ϑ α ∧ T α ) is motivated by the the axial anomaly d j 5 2 in the coupling to Dirac fields ψ, cf. [22].…”
Section: Self-dual Sky Gravitymentioning
confidence: 95%
“…The addition of the Pontrjagin term with respect to the Riemannian curvature R {} αβ and the axial torsion one-form A := * (ϑ α ∧ T α ) is motivated by the the axial anomaly d j 5 2 in the coupling to Dirac fields ψ, cf. [22].…”
Section: Self-dual Sky Gravitymentioning
confidence: 95%
“…There is a controversy whether the second term in (4.1), which is by itself a topological invariant, should contribute to the chiral anomaly or not. See [42] and [43] for details. The AdS/CFT correspondence offers a rich ground to test the dependence of the chiral anomaly on torsion.…”
Section: Discussionmentioning
confidence: 99%
“…The latter contains, amongst others, a term proportional to the Riemannian curvature scalar R {} := * (R {}αβ ∧ η β α ) and the axial torsion piece dA ∧ dA of the axial anomaly [32,43] with a relative factor 9. Up to normalizations, the four-forms (26) and (28) are known as Nieh-Yan [52] and gravitational Pontrjagin term, respectively.…”
Section: Appendix A: Riemann-cartan Geometry In Clifford Algebra-valumentioning
confidence: 99%