1986
DOI: 10.1103/physrevd.33.2875
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Renormalizing (φ3)6theory in curved space-time

Abstract: The renormalization of 43 theory in a six-dimensional conformally flat space-time is discussed at the two-loop level. The background-field method and the momentum-space representation of the Feynman propagator are used to calculate the ultraviolet divergences of the effective action. It is shown that (#'& theory is renormalizable in a conformally flat space-time at the two-loop level.The counterterms are given to the two-loop order. The next-to-leading-order term in the B function for the coupling constant of … Show more

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Cited by 6 publications
(6 citation statements)
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“…Eq. ( 11) generalizes the single field result of [23] (see also [20,21,24,25]) to the multi-field case, and agrees with the results of [22,26,27]. The first contribution to ( 12) is non-planar.…”
Section: Results From the Effective Potentialsupporting
confidence: 86%
“…Eq. ( 11) generalizes the single field result of [23] (see also [20,21,24,25]) to the multi-field case, and agrees with the results of [22,26,27]. The first contribution to ( 12) is non-planar.…”
Section: Results From the Effective Potentialsupporting
confidence: 86%
“…Eq. (5.6) reproduces the result of [32] (see also [19][20][21]33]) in the case of a single field φ. In that case β (1) has a negative sign, and hence the corresponding theory is asymptotically-free.…”
Section: Beta Functions and Anomalous Dimensionssupporting
confidence: 75%
“…In the single-field case (5.8) reproduces the result of [32] (see also [19][20][21] 11 ), which, just like β (1) , is also negative.…”
Section: Beta Functions and Anomalous Dimensionssupporting
confidence: 55%
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