Triangle Seminars
Monday, 22 Apr 2024
Lonti: Geodesics and Singularity Theorems in General Relativity (3/4)
Sunil Mukhi
(IISER, Pune)
Abstract:
These lectures will summarise mathematical aspects of classical General Relativity that are helpful in understanding current developments in the field. Lecture I will focus on Lorentzian-signature geometry, with an emphasis on causal structure. Some topological notions will also be introduced. In Lecture II we will go on to study the behaviour of geodesics in General Relativity and derive the famous Raychaudhuri equation. The null version of this equation, due to Sachs, will also be derived. Lecture III will focus on the "Hawking singularity theorem", namely that cosmological spacetimes with positive local Hubble constant are geodesically incomplete in the past under suitable conditions. In Lecture IV we will discuss the "Penrose singularity theorem" for black holes.
These lectures will summarise mathematical aspects of classical General Relativity that are helpful in understanding current developments in the field. Lecture I will focus on Lorentzian-signature geometry, with an emphasis on causal structure. Some topological notions will also be introduced. In Lecture II we will go on to study the behaviour of geodesics in General Relativity and derive the famous Raychaudhuri equation. The null version of this equation, due to Sachs, will also be derived. Lecture III will focus on the "Hawking singularity theorem", namely that cosmological spacetimes with positive local Hubble constant are geodesically incomplete in the past under suitable conditions. In Lecture IV we will discuss the "Penrose singularity theorem" for black holes.
Posted by: andrea
Wednesday, 24 Apr 2024
Holography in the Gravitational Wave Era
π London
David Mateos
(ICC Universitat de Barcelona and ICREA)
Abstract:
The discovery of gravitational waves has opened a new experimental window into the Universe. The fact that the relevant dynamics is often out of equilibrium offers a golden opportunity for holography to make a unique impact on cosmology and astrophysics. I will illustrate this with applications to cosmological phase transitions, to neutron star mergers and to the BKL dynamics near a cosmological singularity.
The discovery of gravitational waves has opened a new experimental window into the Universe. The fact that the relevant dynamics is often out of equilibrium offers a golden opportunity for holography to make a unique impact on cosmology and astrophysics. I will illustrate this with applications to cosmological phase transitions, to neutron star mergers and to the BKL dynamics near a cosmological singularity.
Posted by: QMUL2
On beta functions in the first-order sigma models
π London
Oleksandr Gamayun
(LIMS, London)
Abstract:
I will introduce a first-order formalism for two-dimensional sigma models with the KΓΒ€hler target space. I will explain how to compute the metric beta function in this approach using the conformal perturbation methods. Comparing the answer with the standard geometric background field methods we observe certain anomalies, which we later resolve with supersymmetric completion. Based on 2312.01885 and 2307.04665.
I will introduce a first-order formalism for two-dimensional sigma models with the KΓΒ€hler target space. I will explain how to compute the metric beta function in this approach using the conformal perturbation methods. Comparing the answer with the standard geometric background field methods we observe certain anomalies, which we later resolve with supersymmetric completion. Based on 2312.01885 and 2307.04665.
Posted by: andrea
Thursday, 25 Apr 2024
Lonti: Geodesics and Singularity Theorems in General Relativity (4/4)
Sunil Mukhi
(IISER, Pune)
Abstract:
These lectures will summarise mathematical aspects of classical General Relativity that are helpful in understanding current developments in the field. Lecture I will focus on Lorentzian-signature geometry, with an emphasis on causal structure. Some topological notions will also be introduced. In Lecture II we will go on to study the behaviour of geodesics in General Relativity and derive the famous Raychaudhuri equation. The null version of this equation, due to Sachs, will also be derived. Lecture III will focus on the "Hawking singularity theorem", namely that cosmological spacetimes with positive local Hubble constant are geodesically incomplete in the past under suitable conditions. In Lecture IV we will discuss the "Penrose singularity theorem" for black holes.
These lectures will summarise mathematical aspects of classical General Relativity that are helpful in understanding current developments in the field. Lecture I will focus on Lorentzian-signature geometry, with an emphasis on causal structure. Some topological notions will also be introduced. In Lecture II we will go on to study the behaviour of geodesics in General Relativity and derive the famous Raychaudhuri equation. The null version of this equation, due to Sachs, will also be derived. Lecture III will focus on the "Hawking singularity theorem", namely that cosmological spacetimes with positive local Hubble constant are geodesically incomplete in the past under suitable conditions. In Lecture IV we will discuss the "Penrose singularity theorem" for black holes.
Posted by: andrea
From Correlators to massive amplitudes in N = 4 SYM
π London
Frank Coronado
(ETH Zurich)
Abstract:
In planar N=4 SYM, massless scattering amplitudes are dual to null
polygonal Wilson loops (T-duality) or the same as the
four-dimensional null limit of stress-tensor correlators. I will present
a (conjectured) generalization of this duality which equates correlators
of determinant operators, in a special ten-dimensional null limit, with
massive scattering amplitudes in the Coulomb branch of N=4. This
determinant operator is a generating function of all half-BPS
single-traces operators. By taming it on twistor space I will show its
correlators have ten dimensional poles which combine 4d space-time and
6d R-charge kinematics.
In planar N=4 SYM, massless scattering amplitudes are dual to null
polygonal Wilson loops (T-duality) or the same as the
four-dimensional null limit of stress-tensor correlators. I will present
a (conjectured) generalization of this duality which equates correlators
of determinant operators, in a special ten-dimensional null limit, with
massive scattering amplitudes in the Coulomb branch of N=4. This
determinant operator is a generating function of all half-BPS
single-traces operators. By taming it on twistor space I will show its
correlators have ten dimensional poles which combine 4d space-time and
6d R-charge kinematics.
Posted by: QMW
Friday, 26 Apr 2024
Non-invertible symmetries for qubits
π London
Shu-Heng Shao
(Stony Brook)
Abstract:
I'll discuss the exact non-invertible Kramers-Wannier symmetry of 1+1d lattice models on a tensor product Hilbert space of qubits. This symmetry mixes with lattice translations, and obeys a different algebra compared to the continuum one. The non-invertible symmetry leads to a constraint similar to that of Lieb-Schultz-Mattis, implying that the system cannot have a unique gapped ground state. It is either in a gapless phase or in a gapped phase with three (or a multiple of three) ground states, associated with the spontaneous breaking of the non-invertible symmetry.
I'll discuss the exact non-invertible Kramers-Wannier symmetry of 1+1d lattice models on a tensor product Hilbert space of qubits. This symmetry mixes with lattice translations, and obeys a different algebra compared to the continuum one. The non-invertible symmetry leads to a constraint similar to that of Lieb-Schultz-Mattis, implying that the system cannot have a unique gapped ground state. It is either in a gapless phase or in a gapped phase with three (or a multiple of three) ground states, associated with the spontaneous breaking of the non-invertible symmetry.
Posted by: QMW