2017
DOI: 10.1007/jhep04(2017)007
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Holographic Ward identities for symmetry breaking in two dimensions

Abstract: We investigate symmetry breaking in two-dimensional field theories which have a holographic gravity dual. Being at large N, the Coleman theorem does not hold and Goldstone bosons are expected. We consider the minimal setup to describe a conserved current and a charged operator, and we perform holographic renormalization in order to find the correct Ward identities describing symmetry breaking. This involves some subtleties related to the different boundary conditions that a vector can have in the three-dimensi… Show more

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Cited by 13 publications
(21 citation statements)
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References 161 publications
(346 reference statements)
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“…We extend the analysis of [16] to the above mentioned case of d ď z`1. As in the relativistic case [7], we find that alternative quantization for the vector is needed, albeit in the present case of Lifshitz scaling, only the temporal component of the vector is involved. This quantization which treats differently space and time is actually needed to enforce the proper gauge invariance of the generating functional.…”
Section: Introductionmentioning
confidence: 47%
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“…We extend the analysis of [16] to the above mentioned case of d ď z`1. As in the relativistic case [7], we find that alternative quantization for the vector is needed, albeit in the present case of Lifshitz scaling, only the temporal component of the vector is involved. This quantization which treats differently space and time is actually needed to enforce the proper gauge invariance of the generating functional.…”
Section: Introductionmentioning
confidence: 47%
“…It is important for the following to note thatã 0 is a gauge invariant quantity and therefore cannot be the source for the temporal part of a conserved current. Note that in the limiting, relativistic, case where d " 2 and z " 1, i.e.d " 2, all leading and subleading terms of the vector modes have the same order in r respectively : This case was already discussed in [7] (see also [21,22]) so we will keepd ą 2 from now on.…”
Section: Quantum Corrections To the Symmetry Breaking Vevmentioning
confidence: 98%
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