1992
DOI: 10.1007/bf01555530
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Unique effective action in two dimensional induced quantum gravity

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1993
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Cited by 4 publications
(6 citation statements)
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“…This technique applies only to some restricted class of operators called minimal operators. Although the technique can be extended to non-minimal operators as well following the work of Barvinsky and Vilkovisky [29] (see [11,[30][31][32][33][34][35] for its applications), it is still very difficult to implement it in practice. As such we resort to the perturbative expansion technique as follows (for application of this technique see [12,25,36,37]).…”
Section: Some Essential Preliminaries For the Computation Of Divergen...mentioning
confidence: 99%
“…This technique applies only to some restricted class of operators called minimal operators. Although the technique can be extended to non-minimal operators as well following the work of Barvinsky and Vilkovisky [29] (see [11,[30][31][32][33][34][35] for its applications), it is still very difficult to implement it in practice. As such we resort to the perturbative expansion technique as follows (for application of this technique see [12,25,36,37]).…”
Section: Some Essential Preliminaries For the Computation Of Divergen...mentioning
confidence: 99%
“…and then employ heat kernel technique [17,19] to compute the divergences in effective action. However, this technique is applicable to some restricted class of operators called minimal operators and can, in certain cases, be extended to non-minimal ones following the work of Barvinsky & Vilkovisky [20] (see [21][22][23][24][25][26][27] for its applications). Owing to a highly non-trivial form of the operator, we instead resort to the perturbative expansion technique.…”
Section: Some Essential Preliminaries For Computation Of Divergences ...mentioning
confidence: 99%
“…[8], where the path integral (2) without torsion and in the self-dual limit ρ 0 → ∞ has been studied. Presumably, such limit describes the infrared dynamics of four-dimensional quantum gravity [9] (see also [10]). When ρ 0 → ∞, the path integral over g µν becomes the integral over conformally self-dual metrics.…”
mentioning
confidence: 99%
“…where the last term in both brackets is the contribution of ∆ to the conformal anomaly [10,12], and the last terms in (14) and (15) are the a 0 + a L and b 0 + b L found in [12], respectively. These contributions are equal to the trace anomaly coefficients of conformal quantum gravity 3 (see ref.…”
mentioning
confidence: 99%
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