pith. sign in

arxiv: 2501.07136 · v3 · submitted 2025-01-13 · ✦ hep-th · gr-qc

On symmetries of gravitational on-shell boundary action at null infinity

Pith reviewed 2026-05-23 05:58 UTC · model grok-4.3

classification ✦ hep-th gr-qc
keywords gravitational boundary actionnull infinitysoft graviton theoremBMS symmetriessuperrotationsGeroch tensorGoldstone modesasymptotic symmetries
0
0 comments X

The pith

The on-shell gravitational boundary action at null infinity reproduces the subleading soft graviton theorem once the BMS group includes superrotations.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper fixes corner ambiguities in the gravitational boundary action at null infinity by requiring that the exponential of the on-shell action reproduces the tree-level 5-point amplitude in the eikonal approximation for a generic supertranslated vacuum. With this choice the subleading soft graviton theorem follows directly from the action when the BMS group is enlarged by superrotations. The authors further generalize the Geroch tensor to an infinite set of divergence-free symmetric traceless tensors on the sphere; each new tensor supplies a Goldstone mode whose soft insertion produces sub^n-leading contributions to the tree-level S-matrix. A reader cares because the construction ties a classical boundary action to the known soft theorems and supplies a single mechanism that could generate the entire tower of tree-level symmetries.

Core claim

By fixing the corner terms in the boundary action through the 5-point eikonal constraint, the subleading soft graviton theorem emerges naturally from the on-shell action when superrotations are admitted; generalizing the Geroch tensor to a tower of divergence-free symmetric traceless tensors on the sphere then generates an infinite sequence of sub^n-leading soft insertions in the tree-level S-matrix.

What carries the argument

The generalized Geroch tensor, a set of divergence-free symmetric traceless tensors on the sphere that label an infinite tower of Goldstone modes and produce the higher-order soft insertions.

If this is right

  • The subleading soft graviton theorem is recovered directly from the on-shell boundary action.
  • An infinite tower of sub^n-leading soft insertions appears in the tree-level S-matrix.
  • The extended BMS group with superrotations is realized through the boundary action.
  • The construction supplies a uniform origin for the entire hierarchy of tree-level soft symmetries.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Higher soft theorems beyond the subleading order may be derivable from the same boundary action by including still more tensors in the generalized Geroch tower.
  • The framework could be tested by checking whether the action reproduces known higher-point amplitudes that involve multiple soft insertions.
  • Similar boundary-action treatments might apply to other asymptotic symmetry groups, such as those in higher dimensions or with additional matter fields.

Load-bearing premise

Corner ambiguities in the boundary action can be fixed by demanding that the exponential of the on-shell action reproduces the tree-level 5-point amplitude in eikonal approximation in a generic supertranslated vacuum.

What would settle it

An explicit computation showing that the on-shell action, after the proposed corner fixing, fails to reproduce the known subleading soft factor when superrotations are included, or fails to match the 5-point eikonal amplitude.

read the original abstract

We revisit the gravitational boundary action at null infinity of asymptotically flat spacetimes. We fix the corner ambiguities in the boundary action by using the constraint that (exponential of) the on-shell action leads to tree-level 5-point amplitude in eikonal approximation in a generic supertranslated vacuum. The subleading soft graviton theorem follows naturally from the on-shell action when the BMS group is extended to include superrotations. An infinite tower of Goldstone modes is proposed by `generalizing' the Geroch tensor to incorporate a set of divergence-free symmetric traceless tensors on the sphere. This generalization leads to $\text{sub}^{n}$-leading soft insertions in the tree-level $\mathcal{S}$ matrix, thus paving the way to understanding the infinite tower of tree-level symmetries within this framework.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 0 minor

Summary. The manuscript revisits the gravitational on-shell boundary action at null infinity. Corner ambiguities are fixed by the requirement that exp(S_on-shell) reproduces the tree-level 5-point amplitude in eikonal approximation inside a generic supertranslated vacuum. Extending the BMS group to superrotations, the subleading soft graviton theorem is asserted to follow from the action. An infinite tower of Goldstone modes is introduced by generalizing the Geroch tensor to a set of divergence-free symmetric traceless tensors on the sphere; this is claimed to generate sub^n-leading soft insertions in the tree-level S-matrix.

Significance. If the fixing procedure can be shown to be independent of the soft factors being derived and the generalization of the Geroch tensor is placed on a firmer footing, the work would supply a concrete link between boundary actions, extended BMS symmetries, and the infinite tower of soft theorems. Such a framework could clarify the origin of higher-order soft insertions without ad-hoc additions to the symmetry group.

major comments (2)
  1. [Abstract] Abstract (first sentence after 'revisit'): the corner ambiguities are fixed by demanding that the on-shell action reproduce the known 5-point eikonal amplitude in a supertranslated vacuum. Because this amplitude already encodes the leading soft graviton factor (or its Ward identity under supertranslations), the subsequent claim that the subleading soft theorem 'follows naturally' from the same action risks circularity. The manuscript must demonstrate explicitly that the subleading insertion is not already presupposed by the 5-point constraint.
  2. [Abstract] Abstract (paragraph on infinite tower): the generalization of the Geroch tensor to an infinite set of divergence-free symmetric traceless tensors is introduced without a derivation from the boundary action or from the extended BMS algebra. This step appears to be an additional assumption rather than a consequence; the manuscript should supply the explicit map from the action (after the 5-point fixing) to these modes and to the sub^n soft factors.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading and constructive comments. We address the two major points raised in the report below, with clarifications on the logical structure of our arguments and indications of where the manuscript will be revised for greater precision.

read point-by-point responses
  1. Referee: [Abstract] Abstract (first sentence after 'revisit'): the corner ambiguities are fixed by demanding that the on-shell action reproduce the known 5-point eikonal amplitude in a supertranslated vacuum. Because this amplitude already encodes the leading soft graviton factor (or its Ward identity under supertranslations), the subsequent claim that the subleading soft theorem 'follows naturally' from the same action risks circularity. The manuscript must demonstrate explicitly that the subleading insertion is not already presupposed by the 5-point constraint.

    Authors: The 5-point eikonal amplitude constraint is applied exclusively to fix the corner ambiguities so that the on-shell action reproduces the leading soft graviton factor in a supertranslated vacuum. The subleading soft theorem is obtained independently by extending the symmetry group to superrotations and extracting the associated Ward identity from the resulting action. The eikonal 5-point amplitude used for the fixing does not contain or presuppose subleading soft insertions. To eliminate any appearance of circularity, we will revise the abstract and insert an explicit paragraph in Section 3 demonstrating that the 5-point constraint involves only the leading soft factor and is independent of subleading contributions. revision: yes

  2. Referee: [Abstract] Abstract (paragraph on infinite tower): the generalization of the Geroch tensor to an infinite set of divergence-free symmetric traceless tensors is introduced without a derivation from the boundary action or from the extended BMS algebra. This step appears to be an additional assumption rather than a consequence; the manuscript should supply the explicit map from the action (after the 5-point fixing) to these modes and to the sub^n soft factors.

    Authors: The infinite tower is introduced as a proposal that generalizes the Geroch tensor in a manner consistent with the structure of the fixed boundary action and the pattern established by the leading and subleading cases. It is not asserted to follow as a direct derivation within the present work. We agree that an explicit map from the 5-point-fixed action to the full set of modes is not supplied. In revision we will expand the discussion in Section 4 to clarify the status of the proposal, provide the explicit form of the generalized tensors, and sketch how they couple to the action to produce the sub^n soft factors, while noting that a complete algebraic derivation from the extended BMS group remains an open direction. revision: partial

Circularity Check

1 steps flagged

Boundary action fixed by matching to known 5-point eikonal amplitude; soft theorems then extracted as 'natural' consequence

specific steps
  1. fitted input called prediction [Abstract]
    "We fix the corner ambiguities in the boundary action by using the constraint that (exponential of) the on-shell action leads to tree-level 5-point amplitude in eikonal approximation in a generic supertranslated vacuum. The subleading soft graviton theorem follows naturally from the on-shell action when the BMS group is extended to include superrotations."

    The 5-point eikonal amplitude in a supertranslated vacuum already contains the leading soft graviton insertion (via the supertranslation charge). Fixing the action to reproduce this amplitude therefore builds the soft factor into the boundary term by construction; the subsequent claim that the subleading theorem 'follows naturally' from the same action is a direct readout of the fitted input rather than an independent derivation.

full rationale

The paper explicitly tunes corner terms in the on-shell boundary action so that exp(S) reproduces the tree-level 5-point amplitude in the eikonal limit inside a supertranslated vacuum. This amplitude already encodes the leading soft graviton factor through the supertranslation Ward identity. Once the action is fixed by this constraint, the subleading soft theorem is asserted to follow 'naturally' upon extending BMS to superrotations, and an infinite tower is obtained by generalizing the Geroch tensor. The derivation therefore reduces to reading back an input that was inserted via the fixing step.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 1 invented entities

The work rests on standard domain assumptions of asymptotically flat gravity and introduces one new postulated structure (the infinite tower) without independent evidence outside the construction itself.

axioms (2)
  • domain assumption Asymptotically flat spacetimes admit a well-defined gravitational boundary action at null infinity with corner ambiguities
    Invoked in the opening sentence of the abstract as the object being revisited.
  • domain assumption The exponential of the on-shell boundary action must reproduce the tree-level 5-point amplitude in eikonal approximation
    Explicitly used as the constraint to fix corner ambiguities.
invented entities (1)
  • Infinite tower of Goldstone modes obtained by generalizing the Geroch tensor to divergence-free symmetric traceless tensors on the sphere no independent evidence
    purpose: To generate sub^n-leading soft insertions in the tree-level S-matrix
    Proposed in the final two sentences of the abstract; no external falsifiable handle is mentioned.

pith-pipeline@v0.9.0 · 5654 in / 1612 out tokens · 42685 ms · 2026-05-23T05:58:07.564815+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. The gravitational S-matrix from the path integral: asymptotic symmetries and soft theorems

    hep-th 2026-03 unverdicted novelty 6.0

    A path integral with asymptotic boundary conditions produces the gravitational S-matrix and derives soft graviton theorems from extended BMS symmetry Ward identities.

Reference graph

Works this paper leans on

83 extracted references · 83 canonical work pages · cited by 1 Pith paper · 23 internal anchors

  1. [1]

    On-shell boundary term in general relativity 4

  2. [2]

    Boundary terms at null infinity 8

  3. [3]

    Corner term ambiguity 13

  4. [4]

    Subleading symmetry 16

  5. [5]

    subn-leading symmetry 19

  6. [6]

    Preliminaries 22

    Discussion 21 Acknowledgements 22 A. Preliminaries 22

  7. [7]

    Conformal Gaussian null coordinates/Newman-Unti gauge 27 References 28

    Action of superrotations 26 B. Conformal Gaussian null coordinates/Newman-Unti gauge 27 References 28

  8. [8]

    in position space

    INTRODUCTION Over the past decade, there have been several seminal developments in our understanding of the so-called infra-red triangle[1, 2]. Infra-red triangle is a conceptual edifice that con- nects three disparate ideas, namely low-frequency gravitational observables[3–5], asymptotic symmetries[6–10], and quantum soft theorems[11, 12]. Through these ...

  9. [9]

    hat"ˆ. The

    to construct an on-shell boundary action at null infinity in a generic supertranslated vacuum. We show that this action has the so-called corner term ambiguities3. The constraint that the (exponential of this action) leads to 5-point eikonal scattering in a supertranslated background fixes the ambiguities in the corner term. We compute the boundary terms ...

  10. [10]

    ON-SHELL BOUNDAR Y TERM IN GENERAL RELA TIVITY The path integral formulation for theS matrix is S(pin,pout) := ∫ [DϕDg]eiS [ϕ,ˆgab] (2.1) where the integration limits are the asymptotic values of the fieldsϕand the metric ˆgab and S = ∫ Ld4x is the full action of the field theory. At the tree level, the classical path 5 dominates and theS matrix is given ...

  11. [11]

    large gauge

    Null boundaries A proper treatment of counterterms at null boundaries received little attention over time and was examined in [39, 40] and later by LMPS[27] which we now review. Consider a codimension-1 null hypersurface defined byΦ(xa) := 0 for some scalar function Φ that increases towards the future. The null normal to the hypersurface is na =−µ∇aΦ (2.1...

  12. [12]

    conformal frame

    BOUNDAR Y TERMS A T NULL INFINITY In this section, we examine the ambiguity in the boundary action at the past and future null infinity of asymptotically flat spacetimes. We show how these ambiguities can be fixed to formulate a boundary action consistent with the memory effect and Weinberg soft theorem. We will work within the conformal spacetime picture...

  13. [13]

    Since we are working in the conformal picture atI +, we will keep the affine parameter u intact

    Corner term ambiguity As noted by LMPS, there are two types of ambiguities in the boundary action at null boundaries: reparametrization freedom fromλto λ′(λ,xA) and changing the embedding from Φ to Φ′. Since we are working in the conformal picture atI +, we will keep the affine parameter u intact. On the other hand, while we appear to have exhausted the c...

  14. [14]

    In this scenario, the superrotations are generated by holomorphic vector fields that satisfy the conformal killing equation on the sphere

    SUBLEADING SYMMETR Y In this section, we consider the extension of the BMS group to include (holomorphic) superrotations as the asymptotic symmetries onI +. In this scenario, the superrotations are generated by holomorphic vector fields that satisfy the conformal killing equation on the sphere. Unlike meromorphic superrotations (the full extended BMS grou...

  15. [15]

    ρAB is now time-dependent but still defined by the Geroch 24Shear is strictly not a phase space variable since its Poisson bracket with itself is not well defined

    sub n-leading symmetry Consider a ‘generalization’ of the (STF) Geroch tensor TAB→TAB g = ∞∑ n=0 unTAB n+1, T AB 1 :=TAB (4.16) so that25 CAB =σAB + ˆCAB + ∞∑ n=0 un+1TAB n+1 (4.17) Recall that the STF tensorTAB was defined by the condition[13, 50] DATAB + 1 2DBR = 0 (4.18) Equation 4.18 is obeyed at each order inu if we impose that{TAB n ;n≥2}are diverge...

  16. [16]

    We followed the analysis of Lehner, Myers, Poisson, and Sorkin to construct the boundary action at null infinity when the non-trivial memory mode is turned on

    DISCUSSION We have demonstrated in this paper that the corner ambiguities in the boundary action at the null infinity of asymptotically flat spacetimes can be fixed by demanding that the (exponential of) on-shell boundary action factorizes into the Weinberg soft factor and the hard amplitude. We followed the analysis of Lehner, Myers, Poisson, and Sorkin ...

  17. [17]

    The variation of various field quantities under local CKV/Diff(S2) can be found in [41]

    Action of superrotations The vector fields generating superrotations atI + is ξY =α∂u + ( YA−1 rDAα+ 1 2r2CABDBα+O(r−3) ) ∂A + ( −r 2DAYA + 1 2D2α+ 1 r ( −1 2CABDADBα−1 4CABDADBα ) +O(r−2) ) ∂r (A.27) where α= u 2DAYA and YA is a local CKV/smooth vector field on the sphere. The variation of various field quantities under local CKV/Diff(S2) can be found in...

  18. [18]

    Lectures on the Infrared Structure of Gravity and Gauge Theory

    A. Strominger,Lectures on the Infrared Structure of Gravity and Gauge Theory. 3, 2017, [1703.05448]

  19. [19]

    Gravitational Memory, BMS Supertranslations and Soft Theorems

    A. Strominger and A. Zhiboedov,Gravitational Memory, BMS Supertranslations and Soft Theorems, JHEP 01 (2016) 086 [1411.5745]

  20. [20]

    V. B. Braginsky and K. S. Thorne,Gravitational-wave bursts with memory and experimental prospects, Nature 327 (1987) 123

  21. [21]

    Christodoulou,Nonlinear nature of gravitation and gravitational wave experiments, Phys

    D. Christodoulou,Nonlinear nature of gravitation and gravitational wave experiments, Phys. Rev. Lett.67 (1991) 1486

  22. [22]

    An electromagnetic analog of gravitational wave memory

    L. Bieri and D. Garfinkle,An electromagnetic analogue of gravitational wave memory, Class. Quant. Grav. 30 (2013) 195009 [1307.5098]

  23. [23]

    Bondi, M

    H. Bondi, M. G. J. van der Burg and A. W. K. Metzner,Gravitational waves in general relativity. 7. Waves from axisymmetric isolated systems, Proc. Roy. Soc. Lond. A269 (1962) 21

  24. [24]

    R. K. Sachs,On the Characteristic Initial Value Problem in Gravitational Theory, J. Math. Phys. 3 (1962) 908

  25. [25]

    Ashtekar and M

    A. Ashtekar and M. Streubel,Symplectic Geometry of Radiative Modes and Conserved Quantities at Null Infinity, Proc. Roy. Soc. Lond. A376 (1981) 585. 29

  26. [26]

    Ashtekar,ASYMPTOTIC QUANTIZATION: BASED ON 1984 NAPLES LECTURES

    A. Ashtekar,ASYMPTOTIC QUANTIZATION: BASED ON 1984 NAPLES LECTURES. 1987

  27. [27]

    On BMS Invariance of Gravitational Scattering

    A. Strominger,On BMS Invariance of Gravitational Scattering, JHEP 07 (2014) 152 [1312.2229]

  28. [28]

    Weinberg,Infrared photons and gravitons, Phys

    S. Weinberg,Infrared photons and gravitons, Phys. Rev. 140 (1965) B516

  29. [29]

    T. He, V. Lysov, P. Mitra and A. Strominger,BMS supertranslations and Weinberg’s soft graviton theorem, JHEP 05 (2015) 151 [1401.7026]

  30. [30]

    Freidel, D

    L. Freidel, D. Pranzetti and A.-M. Raclariu,Higher spin dynamics in gravity and w1+∞ celestial symmetries, Phys. Rev. D106 (2022) 086013 [2112.15573]

  31. [31]

    S. Choi, A. Laddha and A. Puhm,Asymptotic Symmetries for Logarithmic Soft Theorems in Gauge Theory and Gravity, 2403.13053

  32. [32]

    Symmetries of asymptotically flat 4 dimensional spacetimes at null infinity revisited

    G. Barnich and C. Troessaert,Symmetries of asymptotically flat 4 dimensional spacetimes at null infinity revisited, Phys. Rev. Lett.105 (2010) 111103 [0909.2617]

  33. [33]

    Asymptotic symmetries and subleading soft graviton theorem

    M. Campiglia and A. Laddha,Asymptotic symmetries and subleading soft graviton theorem, Phys. Rev. D90 (2014) 124028 [1408.2228]

  34. [34]

    New symmetries for the Gravitational S-matrix

    M. Campiglia and A. Laddha,New symmetries for the Gravitational S-matrix, JHEP 04 (2015) 076 [1502.02318]

  35. [35]

    Semiclassical Virasoro Symmetry of the Quantum Gravity S-Matrix

    D. Kapec, V. Lysov, S. Pasterski and A. Strominger,Semiclassical Virasoro symmetry of the quantum gravityS-matrix, JHEP 08 (2014) 058 [1406.3312]

  36. [36]

    T. He, P. Mitra, A. P. Porfyriadis and A. Strominger,New Symmetries of Massless QED, JHEP 10 (2014) 112 [1407.3789]

  37. [37]

    BMS Supertranslation Symmetry Implies Faddeev-Kulish Amplitudes

    S. Choi and R. Akhoury,BMS Supertranslation Symmetry Implies Faddeev-Kulish Amplitudes, JHEP 02 (2018) 171 [1712.04551]

  38. [38]

    Prabhu, G

    K. Prabhu, G. Satishchandran and R. M. Wald,Infrared finite scattering theory in quantum field theory and quantum gravity, Phys. Rev. D106 (2022) 066005 [2203.14334]

  39. [39]

    Prabhu and G

    K. Prabhu and G. Satishchandran,Infrared finite scattering theory: Amplitudes and soft theorems, Phys. Rev. D110 (2024) 085022 [2402.18637]

  40. [40]

    Prabhu and G

    K. Prabhu and G. Satishchandran,Infrared finite scattering theory: scattering states and representations of the BMS group, JHEP 08 (2024) 055 [2402.00102]

  41. [41]

    Planckian Energy Scattering and Surface Terms in the Gravitational Action

    M. Fabbrichesi, R. Pettorino, G. Veneziano and G. A. Vilkovisky,Planckian energy scattering and surface terms in the gravitational action, Nucl. Phys. B419 (1994) 147 [hep-th/9309037]

  42. [42]

    I. Y. Arefeva, L. D. Faddeev and A. A. Slavnov,Generating Functional for the s Matrix in Gauge Theories, Teor. Mat. Fiz.21 (1974) 311

  43. [43]

    S. Kim, P. Kraus, R. Monten and R. M. Myers,S-matrix path integral approach to symmetries and soft theorems, JHEP 10 (2023) 036 [2307.12368]

  44. [44]

    Lehner, R

    L. Lehner, R. C. Myers, E. Poisson and R. D. Sorkin,Gravitational action with null boundaries, Physical Review D94 (2016)

  45. [45]

    I. Jubb, J. Samuel, R. Sorkin and S. Surya,Boundary and Corner Terms in the Action for 30 General Relativity, Class. Quant. Grav.34 (2017) 065006 [1612.00149]

  46. [46]

    G. Odak, A. Rignon-Bret and S. Speziale,Wald-Zoupas prescription with soft anomalies, Phys. Rev. D 107 (2023) 084028 [2212.07947]

  47. [47]

    Freidel, R

    L. Freidel, R. Oliveri, D. Pranzetti and S. Speziale,The Weyl BMS group and Einstein’s equations, JHEP 07 (2021) 170 [2104.05793]

  48. [48]

    Penrose,Conformal treatment of infinity,

    R. Penrose,Conformal treatment of infinity,

  49. [49]

    Geroch,Asymptotic Structure of Space-Time, inSymposium on Asymptotic Structure of Space-Time, 1977, DOI

    R. Geroch,Asymptotic Structure of Space-Time, inSymposium on Asymptotic Structure of Space-Time, 1977, DOI

  50. [50]

    Geometry and Physics of Null Infinity

    A. Ashtekar,Geometry and physics of null infinity, Surveys Diff. Geom.20 (2015) 99 [1409.1800]

  51. [51]

    Null infinity, the BMS group and infrared issues

    A. Ashtekar, M. Campiglia and A. Laddha,Null infinity, the BMS group and infrared issues, Gen. Rel. Grav.50 (2018) 140 [1808.07093]

  52. [52]

    Rignon-Bret and S

    A. Rignon-Bret and S. Speziale,Centerless BMS charge algebra, Phys. Rev. D110 (2024) 044050 [2405.01526]

  53. [53]

    D. Jain, S. Kundu, S. Minwalla, O. Parrikar, S. G. Prabhu and P. Shrivastava,The S-matrix and boundary correlators in flat space, 2311.03443

  54. [54]

    He, A.-M

    T. He, A.-M. Raclariu and K. M. Zurek,An Infrared On-Shell Action and its Implications for Soft Charge Fluctuations in Asymptotically Flat Spacetimes, 2408.01485

  55. [55]

    G. W. Gibbons and S. W. Hawking,Cosmological Event Horizons, Thermodynamics, and Particle Creation, Phys. Rev. D15 (1977) 2738

  56. [56]

    On-shell actions with lightlike boundary data

    Y. Neiman,On-shell actions with lightlike boundary data, 1212.2922

  57. [57]

    A Boundary Term for the Gravitational Action with Null Boundaries

    K. Parattu, S. Chakraborty, B. R. Majhi and T. Padmanabhan,A Boundary Term for the Gravitational Action with Null Boundaries, Gen. Rel. Grav.48 (2016) 94 [1501.01053]

  58. [58]

    Compère, A

    G. Compère, A. Fiorucci and R. Ruzziconi,Superboost transitions, refraction memory and super-Lorentz charge algebra, JHEP 11 (2018) 200 [1810.00377], [Erratum: JHEP 04, 172 (2020)]

  59. [59]

    A. M. Grant, K. Prabhu and I. Shehzad,The Wald–Zoupas prescription for asymptotic charges at null infinity in general relativity, Class. Quant. Grav.39 (2022) 085002 [2105.05919]

  60. [60]

    Oliveri and S

    R. Oliveri and S. Speziale,Boundary effects in General Relativity with tetrad variables, Gen. Rel. Grav.52 (2020) 83 [1912.01016]

  61. [61]

    E. T. Newman and T. W. J. Unti,Behavior of Asymptotically Flat Empty Spaces, J. Math. Phys. 3 (1962) 891

  62. [62]

    Bondi-Sachs Formalism

    T. Mädler and J. Winicour,Bondi-Sachs Formalism, Scholarpedia 11 (2016) 33528 [1609.01731]

  63. [63]

    Campiglia and A

    M. Campiglia and A. Laddha,BMS Algebra, Double Soft Theorems, and All That, 2106.14717

  64. [64]

    Vacua of the gravitational field

    G. Compère and J. Long,Vacua of the gravitational field, JHEP 07 (2016) 137 [1601.04958]

  65. [65]

    Donnay, K

    L. Donnay, K. Nguyen and R. Ruzziconi,Loop-corrected subleading soft theorem and the 31 celestial stress tensor, JHEP 09 (2022) 063 [2205.11477]

  66. [66]

    Campiglia and J

    M. Campiglia and J. Peraza,Generalized BMS charge algebra, Phys. Rev. D101 (2020) 104039 [2002.06691]

  67. [67]

    Campiglia and A

    M. Campiglia and A. Sudhakar,Gravitational Poisson brackets at null infinity compatible with smooth superrotations, 2408.13067

  68. [68]

    Infinite Set of Soft Theorems in Gauge-Gravity Theories as Ward-Takahashi Identities

    Y. Hamada and G. Shiu,Infinite Set of Soft Theorems in Gauge-Gravity Theories as Ward-Takahashi Identities, Phys. Rev. Lett.120 (2018) 201601 [1801.05528]

  69. [69]

    Sub-subleading Soft Graviton Theorem in Generic Theories of Quantum Gravity

    A. Laddha and A. Sen,Sub-subleading Soft Graviton Theorem in Generic Theories of Quantum Gravity, JHEP 10 (2017) 065 [1706.00759]

  70. [70]

    Akhtar,On the classical limit of the (sub)n-leading soft graviton theorems in D = 4 without deflection, JHEP 12 (2024) 207 [2409.12898]

    S. Akhtar,On the classical limit of the (sub)n-leading soft graviton theorems in D = 4 without deflection, JHEP 12 (2024) 207 [2409.12898]

  71. [71]

    Damour,ANALYTICAL CALCULATIONS OF GRAVITATIONAL RADIATION, in4th Marcel Grossmann Meeting on the Recent Developments of General Relativity, 6, 1985

    T. Damour,ANALYTICAL CALCULATIONS OF GRAVITATIONAL RADIATION, in4th Marcel Grossmann Meeting on the Recent Developments of General Relativity, 6, 1985

  72. [72]

    S. Nagy, J. Peraza and G. Pizzolo,Infinite-dimensional hierarchy of recursive extensions for all subn-leading soft effects in Yang-Mills, JHEP 12 (2024) 068 [2407.13556]

  73. [73]

    Kraus and R

    P. Kraus and R. M. Myers,Carrollian Partition Functions and the Flat Limit of AdS, 2407.13668

  74. [74]

    Guevara, E

    A. Guevara, E. Himwich, M. Pate and A. Strominger,Holographic symmetry algebras for gauge theory and gravity, JHEP 11 (2021) 152 [2103.03961]

  75. [75]

    Strominger,w1+∞Algebra and the Celestial Sphere: Infinite Towers of Soft Graviton, Photon, and Gluon Symmetries, Phys

    A. Strominger,w1+∞Algebra and the Celestial Sphere: Infinite Towers of Soft Graviton, Photon, and Gluon Symmetries, Phys. Rev. Lett.127 (2021) 221601 [2105.14346]

  76. [76]

    Geiller,Celestial w1+∞charges and the subleading structure of asymptotically-flat spacetimes, 2403.05195

    M. Geiller,Celestial w1+∞charges and the subleading structure of asymptotically-flat spacetimes, 2403.05195

  77. [77]

    Loop Corrections to Soft Theorems in Gauge Theories and Gravity

    S. He, Y.-t. Huang and C. Wen,Loop Corrections to Soft Theorems in Gauge Theories and Gravity, JHEP 12 (2014) 115 [1405.1410]

  78. [78]

    Sahoo and A

    B. Sahoo and A. Sen,Classical and Quantum Results on Logarithmic Terms in the Soft Theorem in Four Dimensions, JHEP 02 (2019) 086 [1808.03288]

  79. [79]

    Agrawal, L

    S. Agrawal, L. Donnay, K. Nguyen and R. Ruzziconi,Logarithmic soft graviton theorems from superrotation Ward identities, JHEP 02 (2024) 120 [2309.11220]

  80. [80]

    Sudhakar and A

    A. Sudhakar and A. Suthar,Phase space of gravity for the dynamical celestial metric, Phys. Rev. D 108 (2023) 104058 [2303.04051]

Showing first 80 references.