Uploaded February 2025 | Updated September 2026, 2 weeks ago
Speaker: Elizabeth Heifenberger (Trinity College Dublin)
Abstract: Renormalization group interfaces are objects formed by taking a field theory at an ultraviolet fixed point and introducing a relevant perturbation on half space. Upon flowing to the far infrared, one ends up with UV and IR theories coupled through a conformal interface. This is an example of a defect conformal field theory (DCFT) as it preserves a subgroup of the conformal group. DCFT has generated much interest in recent years due to wide-ranging applications from condensed matter to string theory. RG interfaces in particular are interesting because of their potential to perhaps help us better understand what IR phases are possible when starting from a given UV theory. In this talk, I will discuss my recent work on RG interfaces described by large-N theories deformed on half space by double-trace operators. I will present some DCFT data that we extracted, as well as the free energy associated with the interface after mapping the theory to a sphere. Finally, I will discuss the dual gravitational description in which a bulk scalar field in AdS satisfies different boundary conditions when taken to either half of the AdS boundary. I show manifest agreement between AdS and CFT calculations.
Speaker: Elizabeth Heifenberger (Trinity College Dublin)
Abstract: Renormalization group interfaces are objects formed by taking a field theory at an ultraviolet fixed point and introducing a relevant perturbation on half space. Upon flowing to the far infrared, one ends up with UV and IR theories coupled through a conformal interface. This is an example of a defect conformal field theory (DCFT) as it preserves a subgroup of the conformal group. DCFT has generated much interest in recent years due to wide-ranging applications from condensed matter to string theory. RG interfaces in particular are interesting because of their potential to perhaps help us better understand what IR phases are possible when starting from a given UV theory. In this talk, I will discuss my recent work on RG interfaces described by large-N theories deformed on half space by double-trace operators. I will present some DCFT data that we extracted, as well as the free energy associated with the interface after mapping the theory to a sphere. Finally, I will discuss the dual gravitational description in which a bulk scalar field in AdS satisfies different boundary conditions when taken to either half of the AdS boundary. I show manifest agreement between AdS and CFT calculations.

![DIAS 85 - STP Workshop - Matrix Membranes and Emergent Spacetime - Day 2
[2025-06-17]
(00:00:00) Simon Catterall - Sneaking up on lattice chiral fermions
(00:56:04) Masanori Hanada - From Banks-Fischler-Shenker-Susskind to Kogut-Susskind: Exponentially Accelerating Quantum Simulations
(01:56:43) David Berenstein - Staggered bosons and supersymmetry
(missing) Antal Jevicki - Finite N and BH Microstates
(02:55:44) Veselin Filev - Holographic probe branes and artificial neural networks DIAS 85 - STP Workshop - Matrix Membranes and Emergent Spacetime - Day 2](https://i.ytimg.com/vi/dTkX9P3BKt0/mqdefault.jpg)




![Multigap Topological Insulators: Non-Abelian Bands, Riemannian Geometry, Quantised Optical Responses
Speaker: Wojciech Jankowski (University of Cambridge)
Abstract: Multigap topological insulators, which fall beyond the conventional classifications of K-theory [1], are of vivid theoretical and experimental interest in condensed matter physics [2,3]. In this seminar, I will first introduce the homotopy classification of multigap topological phases with bulk topological invariants defined under PT (spacetime inversion) symmetry [3]. I will then cohomologically characterise non-Abelian bands of such phases, focusing on recently identified non-Abelian Hopf insulators with invariants underpinned by quaternion algebras [4]. Furthermore, I will discuss the momentum-space Riemannian geometry of quantum states realised by the multigap Bloch bundles, which I will connect to their physical manifestations in optical responses [5]. Finally, as quantised responses constitute a hallmark of topological phases of matter, I will show that three-dimensional multigap topological insulators can host quantised integrated non-linear shift photoconductivities [6]. I will demonstrate how the quantisation emerges from the momentum-space torsion tensors, connecting these to real Chern-Simons forms, and to virtual multiband optical transition amplitudes. Multigap Topological Insulators: Non-Abelian Bands, Riemannian Geometry, Quantised Optical Responses](https://i.ytimg.com/vi/h6-GiN_beZs/mqdefault.jpg)



