Erratum to: Superboost transitions, refraction memory and super-Lorentz charge algebra

Hereby, we bring to your attention the following typos and mistakes in [1].


List of corrections
Hereby, we bring to your attention the following typos and mistakes in [1].
After correcting one algebraic mistake and one typo, equation (5.31) must read as / δH (1.1) Equation (5.32) is the modification of the surface charge codimension 2-form k ξ [g, δg] under the incorporation of a covariant Iyer-Wald ambiguity Y [g, δg]. Its proof involves Cartan's magic formula acting on Y . Here however, Y is not proven to be covariant in terms of the bulk metric alone and therefore that identity cannot be used. As a consequence, although (5.33)-(5.36) are correct, the comment just below (5.36) must be deleted.
Instead, the boundary counterterm Y removes all linear in r divergences without affecting the finite pieces by construction. According to (1.1), the finite charge in (5.37) must read as Open Access, c The Authors. Article funded by SCOAP 3 . https://doi.org/10.1007/JHEP04(2020)172

JHEP04(2020)172
We checked that the u derivative of this charge is equal to the symplectic flux where ω r is defined in (5.26). The surface charge expression is therefore now correct. (5.38) is therefore incorrect and the non-integrable part reads as Due to the modification of the surface charge (5.37), the algebra of charges, described in (5.68)-(5.70), closes under the modified bracket. (5.68) should be replaced by There is no anomalous term and (5.70) should be removed. Equation (5.69) should be replaced by (1.5) The comments under (5.72) must be modified as follows: "The charge algebra (5.68) closes under the modified bracket introduced in [2]. Even staying. . . ". Accordingly, the last sentence of the introduction before the Note added should read as "We finally show that the generalized BMS charges obey the algebra under the modified Dirac bracket introduced in [2]". The technical restriction (2.4) can be better reformulated as the boundary condition √ q = √q where ∂ uq = 0 and δq = 0. Then ∂ u q AB = 0 follows from Einstein's equations. The residual diffeomorphisms (2.10) preserve the condition √ q = √q . In the introduction of section 2.1., r is a parameter along the null geodesic congruence which is not necessarily affine. The right-hand side of (2.23) needs to include the additional term In addition, note that all d 2 Ω should read as d 2 Ω, C AB = (u −1 ) in footnotes 4 and 5 should read as C AB = o(u −1 ); the subscripts c in section 3.1 are better written C in order to avoid confusion with the indices a, b, c; all subscripts (0) in section 5.3 are better written as (fin) in order to match the notation of section 5.4. The integration variable in (5.10) should be dudrd 2 x while d 2 Ω in (5.21) is √ qd 2 x; the sign of the r divergent part in (5.24) should be the opposite; in the first term of (5.26), the q AB should be q AB ; there is a "hat" missing on N vac A in (5.65). Finally, the "spin effect" in the box in figure 2 should better be called "spin and center-of-mass memory".
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