Seminars
We host an online seminar series discussing recent papers related to celestial holography. The seminars take place every other Tuesday at noon (EST). To join the mailing list for seminar announcements, please send an email to d.b.skinner@damtp.cam.ac.uk
Upcoming seminars (2026):
- 10 February – Lorenzo Magnea (U Torino & INFN)
- 24 February – A.W. Peet (U Toronto)
- 10 March – Níckolas Alves (Federal University of ABC)
- 24 March – Biswajit Sahoo (KCL)
- 7 April – tba
Past seminars (2025-2026):
- 27 January – Ahmed Sheta (Harvard)
- AdS4 is conformally related to Mink4. In this talk, I will use this relationship to construct a copy of the S algebra in the CFT3 dual to non-abelian gauge theory living on AdS4. In particular, the leading soft generator in flat space is mapped to the light-transform of the conserved current in the CFT3. The subleading S generators are constructed as the SO(3,2) conformal descendants of the leading light-ray operator, and shown to obey the S algebra. This provides a direct connection between the recent progress on flat-space holography and the well-understood AdS holography.
- 13 January – Céline Zwikel (Collège de France & Perimeter Institute)
- Celestial Symmetries of Black Hole Horizons
- I will present a novel correspondence between the gravitational phase space at null infinity and the subleading phase space for finite-distance null hypersurfaces, such as black hole horizons. Using Newman-Penrose formalism and an off-shell Weyl transformation, this construction transfers key structures from asymptotic boundaries to null surfaces in the bulk—for instance, a notion of radiation. Imposing self-duality conditions, I will identify the celestial symmetries and construct their canonical generators for finite-distance null hypersurfaces. This framework provides new observables for black hole physics.
- 9 December – Alfredo Pérez (U San Sebastian, Chile & ESI, Vienna)
- Matching conditions in the presence of logarithms: the role of advanced and retarded radiation
- In this talk, I will present a new perspective on the general matching conditions between the future of past null infinity and the past of future null infinity, emphasizing the role of dominant logarithmic terms in the asymptotic expansion of fields near null infinity. I will explicitly discuss the cases of a massless scalar field and electromagnetism. A key step in the derivation is identifying the physical origin of these logarithms, which are linked to advanced and retarded radiation saturating the finite-energy flux condition at null infinity. The matching conditions then follow from requiring Coulombic (i.e., 1/r) behavior at spatial infinity. The talk is based on arXiv:2510.21072, in collaboration with M. Briceño, H. A. González, and M. Henneaux.
- 25 November – Tianli Wang (Harvard)
- Emergent Flat Space from Quantum Entanglement
- I demonstrate the emergence of bulk Minkowski space from two copies of a boundary CFT for a free scalar. Using celestial holography techniques, I construct “conformal Rindler modes” that, like usual Rindler modes, are supported only on the left or right half of spacetime, and are additionally fully Lorentz covariant. I express the Poincaré-invariant Minkowski vacuum as a thermofield–double state in this basis, naturally connecting the bulk to an entangled pair of boundary CFTs and showing how bulk physics is encoded on the boundary.
- 11 November – Dominik Neuenfeld (Würzberg)
- The Flat Limit of AdS Coupled to a Bath
- In this talk I’ll explain how to take a well-defined flat-space limit of brane models of AdS coupled to a non-gravitating bath. In the dual BCFT this amounts to a triple-scaling limit where both the number of boundary degrees of freedom and the boundary coupling are taken to infinity while the BCFT boundary piecewise approaches a lightcone. The resulting construction offers a new perspective on the flat limit of AdS as well as the potential to carry over ideas from AdS/CFT to flat space. I will discuss some implications for entanglement entropy in flat space, in particular the fact that two different notions of entanglement entropy arise on scri, depending on whether one traces out modes which have left through scri.
- 28 October – Monica Pate (NYU)
- Multi-particle Celestial Operator Product Expansions from the Boundary
- In celestial holography, scattering particles in four-dimensional asymptotically-flat spacetimes are dual to conformal primary field operators on the celestial sphere. Multi-particle celestial operators can be then formulated from regularized coincident limits of single-particle celestial operators. The singular terms in the operator product expansion of multi-particle operators are shown to be fully determined by the singular terms in the operator product expansion between single-particle celestial operators, as is expected in a standard conformal field theory. Boundary operator product expansions in celestial holography are known to be dual to subtle collinear limits of bulk scattering amplitudes. The multi-particle operator product expansions derived from standard conformal field theoretic techniques are shown to reproduce precisely the results from the corresponding bulk collinear limits. Finally, the coefficients of multi-particle celestial operator product expansions are derived from a third complementary method by enforcing bulk four-dimensional translational invariance as a global symmetry of the celestial dual and the results precisely agree with the previous two methods.
- 14 October – Mina Himwich (Princeton)
- Generating Hodges’ Formula with an Lw(1+infinity) Ward Identity
- Hodges’ formula expresses the tree-level all-multiplicity Einstein gravity MHV amplitude as a matrix determinant. In this talk, I will prove that Hodges’ determinant is generated by an Lw(1+infinity) Ward identity on the celestial sphere. The Ward identity takes the form of a recursion relation that has not previously appeared in the literature and is unrelated to BCFW. The proof makes use of the matrix-tree theorem. This talk is based on 2506.05460 with Alfredo Guevara and Noah Miller.
- 30 September – Carlo Heissenberg (IPhT, Saclay)
- Nonlinear gravitational memory from scattering amplitudes
- Scattering amplitudes offer a convenient tool to recast gravitational-wave observables in terms of gauge-invariant building blocks. Amplitude methods are particularly relevant in the the post-Minkowskian (PM) regime, in which sources are far apart and interact weakly. A complementary approach is provided by soft theorems, which apply for small frequencies while retaining exact information on the hard dynamics. In this talk, I will discuss recent progress achieved by combining these two methods to calculate the waveform sourced by the scattering of two compact objects. In particular, I will show how the nonlinear memory effect emerges from amplitudes in the NNLO PM waveform, to leading order in the soft limit, and illustrate how its explicit calculation can be reduced to cut two-loop integrals.
- 16 September – Seraphim Jarov (Perimeter)
- Higher genus twistor spaces and the celestial torus
- In this talk, I will discuss two new deformations of self-dual gauge theory that have the following interesting properties: 1) The theories have celestial CFTs that live on higher genus Riemann surfaces. 2) They exhibit the characteristics of an integrable deformation of self-dual gauge theory. The first example is a deformation of pure self-dual gauge theory with a celestial CFT living on a genus 3 surface, and the second is a deformation of self-dual gauge theory coupled to a massless, complex scalar whose celestial CFT lives on a torus. Using the chiral algebra bootstrap program of Costello and Paquette, I will show that basic amplitudes of the theory vanish, suggesting integrability. I then present the form of higher-order corrections that appear in the theory and explain that the coefficients of these terms are fixed by integrability. Towards the end of the talk, I will explain the twistorial origin of these deformations.
Past seminars (2024-2025):
- 22 July 2025 – Per Kraus (UCLA)
- Carrollian partition functions for Yang-Mills from the bulk path integral
- I will discuss the contents of arxiv: 2503.00916 and related prior work, which develops the relation of the S-matrix to the path integral in Minkowski space with prescribed asymptotic boundary conditions. This approach is well suited to the study of asymptotic symmetries, and is also very natural in the context of the Carrollian approach to flat space holography. The case of Yang-Mills theory will be discussed in detail.
- 24 June 2025 – Sangmin Choi (Amsterdam)
- Log soft theorems and asymptotic symmetries
- Over the past decade, a remarkable connection has been established between soft theorems and the asymptotic symmetries of quantum field theories: soft theorems are the Ward identities of asymptotic symmetries. In particular, at tree level, subleading soft theorems correspond to the Ward identities of the subleading asymptotic symmetries of the theory — divergent gauge transformations in QED and superrotations in gravity. These soft theorems receive loop corrections, and in a series of papers by Laddha, Sahoo and Sen, it was shown that such corrections give rise to a novel, one-loop exact soft theorem with logarithmic dependence on the soft energy. This naturally raises the question: what is the symmetry interpretation of this log soft theorem? In this talk, we explore this question in the context of scalar QED and perturbative gravity. We show that log soft theorems are Ward identities of the subleading asymptotic symmetries, with long-range interactions properly taken into account.
- 10 June 2025 – Tom Wetzstein (LPTHE Jussieu)
- The holographic BMS anomalies
- I will explain the role of anomalies in the extended BMS symmetry of asymptotically flat four-dimensional gravity. I will then classify them from both the bulk gravitational theory and from the boundary field theory perspectives. The two results agree, provided the associated central charges are matched. This is the flat space analogue of the Henningson–Skenderis holographic Weyl anomaly matching in AdS/CFT.
- 27 May 2025 – Nicolas Cresto (Perimeter)
- Asymptotic higher spin symmetries in gravity
- I’ll present the work Laurent and I did during the past couple of years. We constructed a non-perturbative (in a sense I’ll define properly) action of a higher spin symmetry algebroid on the gravitational phase space. It admits a non-linear realization on the asymptotic phase space generated by a Noether charge defined for all spins, which is conserved in the absence of radiation. At non radiative cuts, the algebroid can be restricted to a covariant wedge symmetry algebra. The key ingredient for this construction is to consider field and time dependent symmetry parameters constrained to evolve according to equations of motion dual to (a truncation of) the asymptotic Einstein’s equations. This result then guarantees that the underlying symmetry algebra is also represented canonically. I’ll emphasize how to connect our results with the usual way of presenting the Lw1+infty algebra, pointing out the key differences and the common points, as well as the relation to twistor theory.
- 13 May 2025 – Temple He (Caltech)
- Quantum area fluctuations from gravitational phase space
- We study the gravitational phase space associated to a stretched horizon within a finite-sized causal diamond in (d+2)-dimensional spacetimes. By imposing the Raychaudhuri equation, we obtain its constrained symplectic form using the covariant phase space formalism and derive the relevant quantum commutators by inverting the symplectic form and quantizing. Finally, we compute the area fluctuations of the causal diamond by taking a Carrollian limit of the stretched horizon in pure Minkowski spacetime, and show that the variance of the area fluctuations is proportional to the area itself.
- 29 April 2025 – Christian Ferko (Northeastern)
- Toward flat space holography via interpolating space-times
- In this talk, I will describe recent work on holographic correspondences in spacetimes which interpolate from anti-de Sitter space in the deep bulk to asymptotic regions which share some properties with flat space. Examples include the linear dilaton throat in the F1-NS5 solution and the NCOS decoupling limit of the D1-D5 system. In both examples, null geodesics take infinite coordinate time to reach the boundary, the causal structure resembles that of Minkowski space, and we can sensibly study radiation near future null infinity. These spacetimes are good solutions of string theory and thus might be considered candidates for a top-down sort of celestial holography.
- 1 April 2025 – Lionel Mason (Oxford)
- De Sitter holography for 2+1 Einstein-Weyl spaces and integral formulae near spatial infinity
- This talk starts by addressing integral formulae for wave equations in 2+1 dimensions, and goes on to discuss their relation with Eirnstein-Weyl equations in 2+1 dimensions. With de Sitter asymptotics, in joint work with Claude LeBrun, we show that there is a natural scattering map from past infinity to future infinity arising from the geometry. It is then shown that the 2+1 Einstein-Weyl space can be reconstructed from any choice of such a scattering map giving a 1:1 correspondence. The talk goes on to explain how the linear integral formulae on the standard 2+1 de Sitter to study asymptotics at space-like infinity.
- 18 March 2025 – Iustin Surubaru (Edinburgh)
- Twistorial chiral algebras in higher dimensions
- In four spacetime dimensions, the classically integrable self-dual sectors of gauge theory and gravity have associated chiral algebras, which emerge naturally from their description in twistor space. In this talk I will introduce similar chiral algebras associated to integrable sectors of gauge theory and gravity whenever the spacetime dimension is an integer multiple of four. These sectors have twistor descriptions in terms of certain holomorphic structures that I will introduce. The chiral algebras will then be derived from the symmetries preserving the holomorphic structures. Using twistor sigma models to describe these sectors, I will discuss how the chiral algebras in higher-dimensions also arise as soft symmetry algebras under a certain notion of collinear limit. I will conclude with an example of a tree-level arbitrary multiplicity gauge theory amplitude and the relation between its collinear splitting function and the associated chiral algebra OPE.
- 4 March 2025 – Anthony Morales (Stanford)
- Perturbative consequences of curing twistor anomalies in self-dual Yang-Mills
- Self-dual Yang-Mills (sdYM) obtains a gauge anomaly when uplifted to twistor space, and curing the twistor theory of this anomaly renders the S-matrix of the Minkowski-space theory trivial. We will review the required conditions to cancel the anomaly, then we will explore how the vanishing of the 1-loop amplitude in sdYM implies relations among the gauge-invariant partial amplitudes that comprise the full amplitude. We will then turn our attention to two-loops, where this vanishing will have an effect on the analytic structure of the two-loop all-plus amplitude in massless QCD. In fact, the celestial chiral algebra (CCA) bootstrap can predict two-loop all-plus amplitudes for an arbitrary number of external gluons in theories where the one-loop all-plus amplitude vanishes. Finally, we will see how to leverage the CCA results to more efficiently compute two-loop all-plus amplitudes to higher multiplicity in standard massless QCD.
- 18 February 2025 – Tim Adamo (Edinburgh)
- Flying focus and twistor theory
- Twistor theory is a mathematical framework which manifests the integrability of the self-dual sectors of gauge theory and gravity, and has found many applications in the study of celestial holography. In this talk, I will try to convince you that twistor theory can also be used to address some problems in strong field QFT, where there is considerable interest in background fields which feature spatial focusing. Remarkably, a class of exact solutions to Maxwell’s equations with this property, known as flying focus fields, are self-dual and have a twistor description that enables exact analytic calculations of scattering processes, something which has not been possible with traditional strong-field methods. We will discuss the computation of various scattering amplitudes for QED and Yang-Mills in a flying focus background, their physical interpretation and a generalization to flying focus spacetimes.
- 4 February 2025 – Stefan Prohazka (Vienna)
- Soft gravitons in three dimensions
- We consider quantum gravity with zero cosmological constant in three dimensions. First, we show that pure quantum gravity can be written as a magnetic Carrollian theory living on null infinity, described by Schwarzian-like degrees of freedom. We use this theory to compute the partition function and Hilbert space of pure 3d gravity. Next, we couple quantum gravity to massless matter. Transition amplitudes exhibit several features that resemble soft graviton physics in four dimensions, despite the absence of a propagating graviton. As in four dimensions, we find three equivalent results: a soft graviton theorem, an infinite-dimensional BMS asymptotic symmetry, and a gravitational memory effect. This talk is based on arXiv:2411.13633 [hep-th].
- 21 January 2025 – Farood Moosavian (Oxford)
- How to define spin in the presence of gravity?
- Defining a notion of spin in the presence of gravity is a long-standing question in classical gravitational physics. In this talk, by leveraging the framework of asymptotic symmetries and the method of coadjoint orbits, I will propose a definition of spin for asymptotically-flat spacetimes. I will argue that the appropriate asymptotic symmetries to approach this problem is the generalized BMS (gBMS) algebra, for which the notion of spin exist. I will then discuss the moment map for the action of gBMS algebra, which allows the construction of spin charge on a gravitational phase space. Applying the construction to the case of Kerr black hole, I will explain how its mass, angular momentum, and hence all its multiple moments, can be computed in terms of Casimir functionals associated with the coadjoint orbits of gBMS algebra. I conclude with some of the most interesting questions left to be explored. Based on joint work with Laurent Freidel and Daniele Pranzetti (arXiv:2403.19547).
- 7 January 2025 – Hare Krishna (U Texas)
- A stress tensor for asymptotically flat spacetime
- The stress tensor characterizes the response of the action to arbitrary diffeomorphisms. In this talk, I will briefly review the stress tensor in asymptotically AdS spacetimes which will give us the necessary foundation. The primary focus will be to extend this framework to asymptotically flat spacetimes, particularly at future null infinity of its conformal boundary. The Carrollian structure at null infinity, induced by the null-rigged structure, plays a central role. Both intrinsic and extrinsic data at null infinity are crucial for defining the stress tensor. Through the variational principle, I will derive the expression of the stress tensor and explicitly compute it for Kerr spacetime and more general asymptotically flat spacetimes characterized by Bondi mass, news, shear, and angular momentum. Using this stress tensor, the Brown-York charges will be evaluated and compared with the Wald-Zoupas charges. I will conclude by talking about potential directions for future explorations.
- 10 December 2024 – Kathryn Zurek (Caltech)
- The quantum mechanics of a spherically symmetric causal diamond
- We consider the phase space–and the quantum commutators that arise from canonical quantization—of a spherically symmetric causal diamond in Minkowski space. We find the conjugate pair involves area and time shift operators, and we find two Iyer-Wald charges associated with these operators. The first corresponds to a generator of time translation along the null horizon and is proportional to the area operator, while the second charge generates changes in the size of the causal diamond. We also discuss how very similar structures arise for causal diamonds in JT gravity, and consider implications of the quantum mechanics of causal diamonds for the quantum uncertainty in the spacetime itself as measured by light beams.
- 26 November 2024 – Roland Bittleston (Perimeter)
- Self-dual gauge theory from the top down
- In this talk I will demonstrate how the loop corrected celestial chiral algebra of a particular self-dual gauge theory coupled to massless fermions arises independently as the large N limit of the algebra of operators supported on a 2d holomorphic surface defect. The construction goes via twisted holography for the type I topological string on a Calabi-Yau 5-fold which fibres over twistor space. This duality extends to a large family of self-dual backgrounds. I will explain how to extract flat space form factors from amplitudes in these backgrounds. This allows for the computation of a certian two-loop gauge theory amplitude and form factors of the average null energy operator. Based on joint work with Kevin Costello and Keyou Zeng.
- 12 November 2024 – Adam Tropper (Harvard)
- N = 2 supersymmetry and celestial holography
- I will discuss several aspects of celestial CFTs dual to bulk theories with spacetime supersymmetry. I’ll begin by showing how supersymmetry constrains the structure of soft theorems, asymptotic symmetries, OPEs, and chiral soft algebras — all universal results independent of any specific model. Then, I’ll focus on a fascinating case study: the Seiberg-Witten solution for SU(2) Super Yang-Mills with N = 2 supersymmetry. This theory enjoys a rich moduli space of vacua with singular points encoding the emergence of interesting physical phenomena. Among other things, I’ll explore the interplay between these vacua and the vacua which we are more used to considering in the celestial holography program, i.e. those associated with large gauge transformations.
- 29 October 2024 – Biswajit Sahoo (Kings College London)
- All-order leading-log classical soft photon and soft graviton theorems
- I will discuss the low-frequency expansion of electromagnetic and gravitational waveforms for a generic classical scattering process. The Fourier transform of these waveforms reveals new electromagnetic and gravitational tail memories at both early and late times. Specifically, I will focus on deriving all-order leading-log electromagnetic and gravitational waveforms generated by the acceleration of scattered objects under long-range electromagnetic and gravitational forces, expressed in terms of asymptotic scattering data. Finally, I will explore their connection to the classical limit of all-order leading-log soft theorems to be determined.
- 15 October 2024 – Jordan Cotler (Harvard)
- Quantizing Carrollian field theories
- Carrollian field theories are being explored as potential duals to flat space quantum gravity. Quantizing two-derivative Carrollian theories reveals interesting subtleties such as UV sensitivity, requiring e.g. a lattice regularization and finite inverse temperature. Unlike conventional field theories, details of the lattice regularization remain important at long distances even as the lattice spacing is taken to zero. This limit defines interacting continuum models of generalized free fields with non-Gaussian correlations suppressed by the lattice spacing and unbroken supertranslation symmetry. Our work suggests challenges to having Lagrangian Carrollian field theories which are dual to flat space quantum gravity in 4d and higher dimensions. We also give an example of a Carrollian field theory which is ‘dual’ to pure flat space quantum gravity in 3d.
- 1 October 2024 – Simon Heuveline (Cambridge)
- Towards celestial chiral algebras of self-dual black holes
- This talk is based on 2408.14324 and 2403.18011. We discuss that celestial symmetries get deformed by the presence of a non-zero cosmological constant giving a twistor interpretation of an algebra earlier obtained by Taylor and Zhu. The twistor space of AdS_4 can be further deformed by a backreaction leading to a 2-parameter twistor space of a certain self-dual Taub-NUT AdS_4 spacetime, the Pedersen metric. Its twistor space leads to a 2-parameter deformation of Lw_\wedge which reduces to previously studied algebras in various limits.
- 17 September 2024 – Tristan McLoughlin (Trinity College, Dublin)
- Celestial holography on non-trivial backgrounds
- We will discuss scattering amplitudes on non-trivial, asymptotically-flat, electromagnetic and gravitational backgrounds such as shockwaves, conformal primary waves, and conformally soft modes. We will describe the computation of celestial two-point amplitudes on these backgrounds which have the desirable feature that they are not constrained by the kinematic delta-functions of flat space celestial CFT correlators. We will further describe a number of relations between these backgrounds, CFT three-point functions and, by means of the shadow transform, CFT two-point functions. Finally, by comparing celestial amplitudes on electric and magnetic backgrounds, we will provide evidence that the four-dimensional flat-space holographic dual of S-duality in Abelian gauge theory is two-dimensional T-duality.
- 3 September 2024 – Adam Kmec (Oxford)
- Celestial symmetries from a twistor action
- The celestial Lw1+∞ symmetries in asymptotically flat spacetimes have a natural geometric interpretation on twistor space in terms of Poisson diffeomorphisms. Using this framework, we provide a first-principle derivation of the canonical generators associated with these symmetries starting from the Poisson BF twistor action for self-dual gravity. We express these charges as surface integrals over the celestial sphere in terms of spacetime data at null infinity. The connection between twistor space and spacetime expressions at null infinity is achieved via an integral formula for the asymptotic Bianchi identities due to Bramson and Tod. Finally, we clarify how Lw1+∞ transformations are symmetries of gravity from a phase space perspective by showing the invariance of the asymptotic Bianchi identities. This talk is based on work with Lionel Mason, Romain Ruzziconi, and Akshay Yelleshpur Srikant.
Past seminars (2023-2024):
- 16 July 2024 – Bin Zhu (Edinburgh)
- Eikonal amplitudes on the celestial sphere
- Celestial scattering amplitudes for massless particles are Mellin transforms of momentum-space scattering amplitudes with respect to the energies of the external particles, and behave as conformal correlators on the celestial sphere. However, there are few explicit cases of well-defined celestial amplitudes, particularly for gravitational theories: the mixing between low- and high-energy scales induced by the Mellin transform generically yields divergent integrals. In this talk, we argue that the most natural object to consider is the gravitational amplitude dressed by an oscillating phase arising from semi-classical effects known as eikonal exponentiation. This leads to gravitational celestial amplitudes which are analytic, apart from a set of poles at integer negative conformal dimensions, whose degree and residues we characterize. We also study the large conformal dimension limits, and provide an asymptotic series representation for these celestial eikonal amplitudes. Our investigation covers two different frameworks, related by eikonal exponentiation: 2-2 scattering of scalars in flat spacetime and 1-1 scattering of a probe scalar particle in a curved, stationary spacetime. These provide data which any putative celestial dual for Minkowski, shockwave or black hole spacetimes must reproduce. We also derive dispersion and monodromy relations for these celestial amplitudes and discuss Carrollian eikonal-probe amplitudes in curved spacetimes. This talk is based on the recent work with T. Adamo, W. Bu, and P. Tourkine.
- 2 July 2024 – Akshay Yelleshpur Srikant (Oxford)
- Celestial OPEs from S-Matrix unitarity
- OPE coefficients are essential data in any CFT. In the context of CCFT, they are computed by examining the collinear behavior of scattering amplitudes. However, recent results indicate that the OPE contains more singularities beyond those associated with the collinear limit. In this talk, I will introduce a new method for computing OPEs which is inspired by Cutkosky’s cutting rules and is closely linked to S-Matrix unitarity. I will demonstrate this method can be used to derive compact formulas for OPEs and multi-OPEs for any masses and spins directly from scattering amplitudes.
- 18 Jun 2024 – Sabrina Pasterski (Perimeter)
- Radiation in Holography
- We show how to encode the radiative degrees of freedom in 4-dimensional asymptotically AdS spacetimes, using the boundary Cotton and stress tensors. Background radiation leads to a reduction of the asymptotic symmetry group, in contrast to asymptotically flat spacetimes, where a non-vanishing news tensor does not restrict the asymptotic symmetries. Null gauges, such as Λ-BMS, provide a framework for AdS spacetimes that include radiation in the flat limit. We use this to check that the flat limit of the radiative data matches the expected definition in intrinsically asymptotically flat spacetimes. We further dimensionally reduce our construction to the celestial sphere, and show how the 2-dimensional celestial currents can be extracted from the 3-dimensional boundary data.
- 21 May 2024 – Simone Speziale (CPT, Marseille)
- Different Universal Structures at Scri, Covariance and 2-Cocycles
- In the first part of the talk, I will draw a parallel between
different symmetry groups that arise on null surfaces at a finite
distance, and extensions of the BMS symmetry at future null infinity.
In the second part I will discuss how ambiguities in the charges and
fluxes can be entirely removed thanks to the key property of
covariance, one side of which is the absence of field-dependent
cocycles in the algebra.
- 7 May 2024 – Laurent Freidel (Perimeter)
- Null Raychauduri: Canonical Structure, Dressing Time and Quantisation
- In this talk, I will review our recent work with L. Ciambelli and R. Leigh, focusing on the non-perturbative characterization of the gravitational phase space along null boundaries. I will present the construction of the Carrollian curved geometry, the Poisson bracket and discuss the construction of a field-dependent time called dressing time that allows the construction of a positive definite boost generator for expanding null surfaces. If time permits, I will discuss some elements of the quantization and the appearance of a crucial Quantum central charge. I will also discuss how these results connect to the celestial holography program when one treats the null boundary as an asymptotically null one.
- 23 April 2024 – Temple He (Caltech)
A synergy of shockwaves, edge modes, and infrared physics- In this talk, I will focus on two interesting directions of research in the infrared sector of gauge theories and gravity. First, we study the relationship between shockwave geometries and the gravitational memory effect in four-dimensional asymptotically flat spacetime. In particular, we show the ‘t Hooft commutation relations of shockwave operators are equivalent to the commutation relation between soft and Goldstone modes parametrizing a sector of the gravitational Hilbert space. Second, we present a concrete connection between soft modes on the celestial sphere and entanglement edge modes in QED, paving the way to study entanglement properties of soft modes.
- 2 April 2024 – Walker Melton (Harvard)
- Celestial Leaf Amplitudes
- Celestial amplitudes of massless particles are forced to be distributional at low points due to bulk translation invariance, which is an unusual property for a 2D CFT. However, these distributional amplitudes can be extracted from smooth leaf amplitudes, where a bulk interaction vertex is integrated only over a hyperbolic slice of spacetime. In this talk, I describe the construction of gluon MHV leaf amplitudes, explain how the full scattering amplitude can be extracted from these leaf amplitudes, and describe some properties of their soft and collinear limits. Finally, I will describe how these leaf amplitudes can be generated by a simple 2D system of free fermions and Liouville Theory in the large central charge limit. This talk is based on work done with Andrew Strominger and Atul Sharma [2312.07820, 2402.04150] and [2403.18896] with Andrew Strominger, Atul Sharma, and Tianli Wang.
- 19 March 2024 – Massimo Tarrona (U Napoli & INFN)
- Celestial Holography Revisited
- I will present some recent works in collaboration with Charlotte Sleight where we propose a new extrapolate dictionary for celestial correlators. This new definition is motivated by the AdS/CFT correspondence where the central object under study is not the S-matrix but the boundary limit of time ordered correlation functions. We shall discuss various examples, both perturbatively and non-perturbatively. I will conclude mentioning possible connections with previous proposals based on the S-matrix.
- 5 March 2024 – Yannick Herfray (IDP, Tours)
- Carrollian $Lw_{1+\infty}$ Representation from Twistor Space
- As explained by Tim Adamo, Lionel Mason and Atul Sharma the action of the Lw1+infinity algebra is local and geometrical in twistor space. I will present the main outcome of our recent work with Laurent Freidel and Laura Donnay which is an explicit realization of this action on Carrollian fields (i.e. on scri). The action is derived by direct Penrose transform, and this ensures that the resulting set of differential operators on scri form a representation of the algebra. We also show that this representation, derived from twistor space, coincides with the canonical action of Freidel–Pranzetti–Raclariu.
- 20 Feb 2024 – Sruthi Narayanan (Perimeter)
- Celestial Amplitudes from the Outside In
- Thus far, most of the advances in celestial holography have utilized a mapping between bulk S-matrix elements and boundary conformal correlators to understand more about the structure of celestial CFTs. In this talk I will give some background on what has been done thus far and then discuss how we can study this duality in the opposite way: by considering specific conformal field theories and deducing what bulk theories they should correspond to. This talk is largely based on the paper “Celestial Gluon Amplitudes from the Outside In” from this past December.
- 6 Feb 2024 – Yangrui Hu (Perimeter)
- Celestial Quantum Error Correction
- Quantum gravity in 4D asymptotically flat spacetimes features spontaneous symmetry breaking due to soft radiation hair, intimately tied to the proliferation of IR divergences. A holographic description via a putative 2D CFT is expected free of such redundancies. In this talk, we address this issue by initiating the study of Quantum Error Correction in Celestial CFT (CCFT). We start by constructing a toy model with finite degrees of freedom by revisiting noncommutative geometry in Kleinian hyperkähler spacetimes. The model obeys a Wick algebra that renormalizes in the radial direction and admits an isometric embedding à la Gottesman-Kitaev-Preskill. Then we promote qubits to qunits and construct a toy model of CCFT from the perspective of quantum error-correcting codes. In our code, the hard states with quantized BMS soft hair form the logical subspace. This allows us to reverse errors induced by soft radiation. Technically, the construction relies on the recently studied $w_{1+\infty}$ hierarchy of soft currents and its realization in twistor space.
- 23 Jan 2024 – Francisco Rojas (Adolfo Ibanez U)
- Celestial loop amplitudes in field and string theory
- Due to their exponentially soft behavior in the UV, string amplitudes are an excellent testing ground for studying their corresponding celestial correlators. In this talk, we will review celestial amplitudes in the Type I superstring at one-loop, for the case of external gluons. We will analyze some of its properties and analytic structure. After toroidal compactification to 4 spacetime dimensions, its field theory limit describes gluon amplitudes in N=4 SYM whose planar amplitude is known to all loops in the ‘t Hooft coupling. We will see that, even though each term in the loop expansion produces divergent celestial amplitudes (after the usual Mellin transforms), their all-loop resummation (the BDS formula) yields a convergent expression which is directly related with the known positivity of the cusp anomalous dimension. To conclude, we will briefly comment on ongoing work on how to extract the correct field theory limit from string amplitudes in the conformal basis.
- 9 Jan 2024 – Romain Ruzziconi (Oxford)
- Carrollian Avenue to Celestial Holography
- Carrollian holography aims to express gravity in four dimensional asymptotically flat space-time in terms of a dual three dimensional Carrollian CFT living at null infinity. In this talk, I will review some aspects of Carrollian holography and compare this approach with the AdS/CFT correspondence. I will introduce the notion of Carrollian amplitude and explain how this relates to celestial amplitudes. Finally, I will present recent results concerning Carrollian OPEs and deduce how soft symmetries act at null infinity.
- 12 Dec 2023 – Diksha Jain (TIFR, Mumbai)
- The S-Matrix and Boundary Correlators in Flat Space
- In this talk, I will define and study the boundary correlation functions obtained from the path integral as a functional of boundary values in flat space. The flat space S-matrix can be extracted directly from these boundary correlation functions after smearing. Next, I will derive the constraints on this path-integral that follow from the unitarity of the S-matrix. We then study the locality structure of boundary correlation functions. In the massive case, we find that the boundary correlation functions for generic locations of boundary points are dominated by a saddle point which has the interpretation of particles scattering in a small elevator in the bulk, where the location of the elevator is determined dynamically, and the S-matrix can be recovered after stripping off some dynamically determined but non-local “renormalization” factors. In the massless case, we find that while the boundary correlation functions are generically analytic as a function on the whole manifold of locations of boundary points, they have special singularities on a sub-manifold, points on which correspond to light-like scattering in the bulk. This analysis parallels the analysis of bulk-point singularities in AdS/CFT and generalizes it to the case of multi-bulk point singularities.
- 28 Nov 2023 – Niklas Garner (U Washington)
- Twistorial Monopoles & Chiral Algebras
- Twistor methods are remarkably powerful for studying four-dimensional scattering problems, but a description in terms of a local QFT on six-dimensional twistor space is often obstructed by an anomaly. As observed by Costello and Paquette, when such a description exists the chiral algebra of asymptotic symmetries can also be described as the degrees of freedom living on the boundary of a three-dimensional QFT obtained by reduction from twistor space. In this talk I will describe some recent work with N. Paquette studying non-perturbative aspects of these celestial chiral algebras by combining the above observation with techniques available to three-dimensional, holomorphic-topological gauge theory.
- 14 Nov 2023 – Adam Ball (Perimeter)
- Multicollinear Singularities in Celestial CFT
- After reviewing the celestial OPE, soft current algebras, and the Jacobi identity, I will introduce the holomorphic multicollinear limit and its celestial avatar, the multi-OPE. This new tool provides more information than the usual 2-OPE, and I will use it to show that from the perspective of hard celestial amplitudes the failure of Jacobi is due to the presence of certain branch cuts in the z-dependence. This puts to rest some concerns in the literature that the hard OPE is sick in theories failing Jacobi. Finally, I will use the multi-OPE to show the existence of a new singular term in the OPE between two massless particles, and I will argue it is associated with multi-particle operators.
- 17 Oct 2023 – Hofie Hannesdottir (IAS)
- What can be measured asymptotically?
- In this talk, we consider asymptotic observables in quantum field theories in which the S-matrix makes sense. We argue that in addition to scattering amplitudes, a whole compendium of inclusive observables exists where the time ordering is relaxed. These include expectation values of electromagnetic or gravitational radiation fields as well as out-of-time-order amplitudes. We explain how to calculate them in different ways: by relating them to amplitudes and products of amplitudes and by using a generalization of the LSZ reduction formula. Finally, we discuss how to relate them to one another through new versions of crossing symmetry. As an application, we discuss one-loop contributions to gravitational radiation in the post-Minkowski expansion, emphasizing the role of classical cut contributions and highlighting the infrared physics of in-in observables.
- 3 Oct 2023 – Noah Miller (Harvard)
- Integer modes and Bulk $w_{1+\infty}$ symmetry
- In celestial holography, integer modes with Δ ∈ ℤ have the special importance of generating soft symmetries. In this talk (based on the paper arxiv.org/abs/2302.04905) we prove the completeness of these modes and their descendants (and their shadow pairs) for the massless scalar by reconstructing the positive frequency Wightman function as a sum of these modes. Interestingly, this proof utilizes a novel CFT-like inner product called the RSW inner product.We then discuss how integer modes and descendant wave functions can be used to the bulk spacetime symmetry which satisfies the commutation relations of the (loop algebra of) the S algebra and the w_(1+infinity) algebra in Self Dual Yang Mills and Self Dual Gravity. In these self dual theories, we will find that there is essentially a complete correspondence between radiative modes and “gauge transformations,” once interpreted appropriately.
- 19 Sept 2023 – Wei Bu (Edinburgh)
- Infra-red structures of scattering on self-dual radiative backgrounds
- The scattering of gluons and gravitons in trivial backgrounds is endowed with many surprising infrared features which have interesting conformal interpretations on the two-dimensional celestial sphere. However, the fate of these structures in more general asymptotically flat backgrounds is far from clear. In this paper, we consider holomorphic infrared structures in the presence of non-perturbative, self-dual background gauge and gravitational fields which are determined by freely specified radiative data. We make use of explicit formulae for tree-level gluon and graviton scattering in these self-dual radiative backgrounds, as well as chiral twistor sigma model descriptions of the classical dynamics. Remarkably, we find that the leading holomorphic part of tree-level collinear splitting functions – or celestial OPEs – and infinite-dimensional chiral soft algebras are undeformed by the background. We also compute all-order holomorphic celestial OPEs in the MHV sectors of gauge theory and gravity.