1991
DOI: 10.1016/0550-3213(91)90102-4
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c -theorem and spectral representation

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Cited by 218 publications
(362 citation statements)
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“…As we discussed earlier in this section, by choosing 23) and combining equation (B.13)and (B.21) we can conclude that the on-shell action with the boundary data A (0) and π (0) must take the following form: 24) with the understanding that A (0) and π (0) are completely free parameters in the above expression.…”
Section: A1 Conformal Radial Coordinatementioning
confidence: 99%
See 1 more Smart Citation
“…As we discussed earlier in this section, by choosing 23) and combining equation (B.13)and (B.21) we can conclude that the on-shell action with the boundary data A (0) and π (0) must take the following form: 24) with the understanding that A (0) and π (0) are completely free parameters in the above expression.…”
Section: A1 Conformal Radial Coordinatementioning
confidence: 99%
“…In fact we can construct a cfunction along the RG flow, which is defined for all energy scales and is equal to c UV and c IR , respectively, at the UV and IR fixed point. To state this in a bit more detail, note that we can write [23] …”
Section: Jhep02(2015)056mentioning
confidence: 99%
“…We now plug (3.4) and (3.8) into (2.24) and expand to quadratic order in δA. Notice that, to this order, N µ P µ = 0, and N H = H (2) . After integration by parts, the terms S grav + S matter of the action expanded to quadratic order can be brought to the form…”
Section: Jhep03(2016)033mentioning
confidence: 99%
“…Here unitarity of Θ(x) implies Zamolodchikov's c-theorem, and its two-point function yields the sum rule [1,2] C UV − C IR = 3π d 2 x x 2 0|Θ(x)Θ(0)|0 , (1.2) where C UV and C IR are the central charges of the UV and IR fixed points. The situation in higher dimensions is more complicated and interesting.…”
Section: Jhep03(2016)033mentioning
confidence: 99%
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