1996
DOI: 10.1016/0550-3213(95)00593-5
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Loop calculations in quantum mechanical non-linear sigma models with fermions and applications to anomalies

Abstract: We construct the path integral for one-dimensional non-linear sigma models, starting from a given Hamiltonian operator and states in a Hilbert space. By explicit evaluation of the discretized propagators and vertices we find the correct Feynman rules which differ from those often assumed. These rules, which we previously derived in bosonic systems [1], are now extended to fermionic systems. We then generalize the work of Alvarez-Gaumé and Witten [2] by developing a framework to compute anomalies of an n-dimens… Show more

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Cited by 60 publications
(83 citation statements)
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“…Furthermore we showed in section 3 that for the N = 2 model mode regularization gives a non-covariant, susy-breaking counterterm Γ 2 /24, while both dimensional regularization and time slicing [19,31] give a vanishing counterterm. In MR, one may interpret the vanishing of N = 1 counterterm as due to the fact that this model is supersymmetric even off-shell (we have an equal number of bosonic and fermionic fields); and as a signal that such regularization scheme preserves the symmetry.…”
Section: Discussionmentioning
confidence: 89%
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“…Furthermore we showed in section 3 that for the N = 2 model mode regularization gives a non-covariant, susy-breaking counterterm Γ 2 /24, while both dimensional regularization and time slicing [19,31] give a vanishing counterterm. In MR, one may interpret the vanishing of N = 1 counterterm as due to the fact that this model is supersymmetric even off-shell (we have an equal number of bosonic and fermionic fields); and as a signal that such regularization scheme preserves the symmetry.…”
Section: Discussionmentioning
confidence: 89%
“…(2.10) This result can be compared with the one obtained employing other regularization schemes [31,18] that reads…”
Section: Flat Indicesmentioning
confidence: 97%
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“…Since the Atiyah-Singer index theorem is related to the chiral anomaly, the methods used here can be looked upon as yet another derivation of the theorem, when the background is nongravitational. These anomalies were first formulated in terms of worldline pathintegrals in [35] and were put on more rigorous footing in [36] and the analysis finally culminated in a book [37]. One can compare the methods in these references with the methods here to appreciate the economy of arguments and calculational steps.…”
Section: Advances In High Energy Physicsmentioning
confidence: 99%
“…where we have taken thėcorrelator from [36] and used the fact that one-point functions vanish. Thus doing the integral in (55), one gets, upon using…”
Section: Propagator For the Spin-one Particlementioning
confidence: 99%