2021
DOI: 10.1007/jhep06(2021)079
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Coadjoint representation of the BMS group on celestial Riemann surfaces

Abstract: The coadjoint representation of the BMS group in four dimensions is constructed in a formulation that covers both the sphere and the punctured plane. The structure constants are worked out for different choices of bases. The conserved current algebra of non-radiative asymptotically flat spacetimes is explicitly interpreted in these terms.

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Cited by 49 publications
(87 citation statements)
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“…It vanishes for the round metricq. We can also understand the vacuum sector as an orbit of the BMSW group (see [90,106] for an orbit analysis of the original BMS group). To do so we introduce the BMSW group elements 21 g (T,W,Y ) = e δ T e δ W e δ Y .…”
Section: Vacuum Structurementioning
confidence: 99%
“…It vanishes for the round metricq. We can also understand the vacuum sector as an orbit of the BMSW group (see [90,106] for an orbit analysis of the original BMS group). To do so we introduce the BMSW group elements 21 g (T,W,Y ) = e δ T e δ W e δ Y .…”
Section: Vacuum Structurementioning
confidence: 99%
“…In [18], the coadjoint representation of the BMS group in four dimensions has been constructed. It acts on a set of conformal fields that have been identified with local expressions of the solution space of non-radiative asymptotically flat spacetimes at null infinity JHEP11(2021)040 through a (pre-)momentum map.…”
Section: Introductionmentioning
confidence: 99%
“…In terms of it, we examined physically relevant non-central extensions and came up with some simple free field realizations. Remarkably, the two-punctured Riemann sphere, where the conformal subalgebra of (3.2) and of (3.6) is consistently realized, has been argued to be the relevant one for celestial scattering amplitudes and soft theorems in the context of bms [37,[54][55][56]. Analogously, we expect the complete (3.2) and (3.6) to play the equivalent role for gbms.…”
Section: Jhep10(2021)133 4 Summary and Conclusionmentioning
confidence: 66%