2016
DOI: 10.1103/physrevd.93.026003
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Burg-Metzner-Sachs symmetry, string theory, and soft theorems

Abstract: We study the action of the BMS group in critical, bosonic string theory living on a target space of the formand C is an arbitrary compactification. We provide a treatment of generalized WardTakahashi identities and derive consistent boundary conditions for any d from string theory considerations. Finally, we derive BMS transformations in higher dimensional spacetimes and show that the generalized Ward-Takahashi identity of BMS produces Weinberg's soft theorem in string theory.

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Cited by 48 publications
(48 citation statements)
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References 70 publications
(131 reference statements)
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“…We are interested in these expressions at the leading terms in the large-r expansion which are known to be gauge-invariant [21]. The action of the hard charge Q H on a Fock state of N massive particles can be expressed as [20] …”
Section: Jhep02(2018)171mentioning
confidence: 99%
“…We are interested in these expressions at the leading terms in the large-r expansion which are known to be gauge-invariant [21]. The action of the hard charge Q H on a Fock state of N massive particles can be expressed as [20] …”
Section: Jhep02(2018)171mentioning
confidence: 99%
“…The utility of this gauge choice in the context of the IR triangle was originally suggested in [19].…”
Section: Soft Theorem As Ward Identitymentioning
confidence: 99%
“…We would now like to express the generator of soft supertranslations in terms of the creation and annihilation operators. To do this, we will be using the results of [22,23], where it was shown that to leading order in the asymptotic expansion, the soft supertranslations generator is gauge-invariant. Therefore, instead of performing the computation in the general Gupta-Bleuler quantization that we have been using so far, we can go further and fix the residual gauge freedom left after setting the harmonic gauge.…”
Section: Jhep01(2018)142mentioning
confidence: 99%
“…As explained above, that will not change the result since, to leading order in the asymptotic expansion, the soft supertranslation generator is independent of the gauge choice [22,23]. Using this and the plane wave expansion (for example see appendix A of [13]), we write the radiative data as [10] …”
Section: Jhep01(2018)142mentioning
confidence: 99%