2000
DOI: 10.1016/s0370-2693(00)01180-1
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Dimensional regularization of nonlinear sigma models on a finite time interval

Abstract: We extend dimensional regularization to the case of compact spaces. Contrary to previous regularization schemes employed for nonlinear sigma models on a finite time interval ("quantum mechanical path integrals in curved space") dimensional regularization requires only a covariant finite two-loop counterterm. This counterterm is nonvanishing and given by 1 8h 2 R.

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Cited by 28 publications
(61 citation statements)
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“…We have used the recently developed dimensional regularization scheme for quantum mechanical path integrals [10] to compute the trace anomaly for a scalar field in six dimensions. The identification of the full anomaly required a complete 4-loop quantum mechanical computation.…”
Section: Discussionmentioning
confidence: 99%
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“…We have used the recently developed dimensional regularization scheme for quantum mechanical path integrals [10] to compute the trace anomaly for a scalar field in six dimensions. The identification of the full anomaly required a complete 4-loop quantum mechanical computation.…”
Section: Discussionmentioning
confidence: 99%
“…In mode regularization and time slicing such counterterms are noncovariant. In the DR scheme the counterterm is covariant and equal to V DR = R 8 , as demonstrated in [10,11]. Now, let us describe the DR scheme which we are going to apply in the next section.…”
Section: Dimensional Regularization Of the Path Integralmentioning
confidence: 99%
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“…The nonlinearities present in the kinetic term make the definition of the path integral rather subtle, carrying the necessity of specifying a regularization scheme together with the fixing of corresponding finite counterterms. The latter are needed for specifying a well-defined quantum theory; see [2][3][4][5] for the known regularization schemes. The development of those regularization schemes was prompted by the a e-mail: fiorenzo.bastianelli@bo.infn.it b e-mail: olindo.corradini@unimore.it desire of extending the quantum mechanical method of computing chiral anomalies [6][7][8] to trace anomalies [9,10].…”
Section: Introductionmentioning
confidence: 99%
“…The complete counterterm was found in [33,34]. The extensions to N = 1 and N = 2 were studied in [18] and [19], respectively.…”
Section: Introductionmentioning
confidence: 99%