Triangle Seminars
Wednesday, 21 Nov 2018
Wilson Surface Central Charge
๐ London
Andy O'Bannon
(University of Southampton)
Abstract:
M-theory is currently our best candidate for a theory of everything, but remains mysterious. We know M-theory has M2- and M5-branes. The low-energy theory on a stack of coincident M2-branes is well-understood: it is maximally supersymmetric Chern-Simons-matter theory. However, the low-energy theory on a stack of coincident M5-branes remains poorly-understood: it is a maximally supersymmetric theory of self-dual strings with zero tension. In this talk I will discuss one type of probe of the M5-brane theory, namely self-dual strings with infinite tension. These play a role analogous to Wilson lines in gauge theories, but are two-dimensional surfaces rather than lines, and hence are called Wilson surfaces. I will describe holographic calculations of entanglement entropy associated with these infinite-tension self-dual strings, from which we extract a key parameter characterizing them, their central charge. This provides a count of the number of massless degrees of freedom living on them, and thus may shed light on some of the fundamental degrees of freedom of M-theory.
M-theory is currently our best candidate for a theory of everything, but remains mysterious. We know M-theory has M2- and M5-branes. The low-energy theory on a stack of coincident M2-branes is well-understood: it is maximally supersymmetric Chern-Simons-matter theory. However, the low-energy theory on a stack of coincident M5-branes remains poorly-understood: it is a maximally supersymmetric theory of self-dual strings with zero tension. In this talk I will discuss one type of probe of the M5-brane theory, namely self-dual strings with infinite tension. These play a role analogous to Wilson lines in gauge theories, but are two-dimensional surfaces rather than lines, and hence are called Wilson surfaces. I will describe holographic calculations of entanglement entropy associated with these infinite-tension self-dual strings, from which we extract a key parameter characterizing them, their central charge. This provides a count of the number of massless degrees of freedom living on them, and thus may shed light on some of the fundamental degrees of freedom of M-theory.
Posted by: KCL
Polygon Seminar: Hugh Osborn: Seeking fixed points
Hugh Osborn
(DAMTP, Cambridge University)
Abstract:
Fixed points are crucial in understanding the RG flow of quantum field
theories. The conformal bootstrap has proved a wonderful tool in
determining the properties of CFTs at fixed points but tends to require
guidance in terms of what symmetries to impose and what is the spectrum of
relevant operators. Here I review what can be said in general by using the
time honoured epsilon expansion. Although qualitatively this is not
nowadays the most efficient method it provides qualitative information
about possible fixed points. Finding fixed points which cannot be linked to
the epsilon expansion could provide a clue to non Lagrangian theories.
Fixed points are crucial in understanding the RG flow of quantum field
theories. The conformal bootstrap has proved a wonderful tool in
determining the properties of CFTs at fixed points but tends to require
guidance in terms of what symmetries to impose and what is the spectrum of
relevant operators. Here I review what can be said in general by using the
time honoured epsilon expansion. Although qualitatively this is not
nowadays the most efficient method it provides qualitative information
about possible fixed points. Finding fixed points which cannot be linked to
the epsilon expansion could provide a clue to non Lagrangian theories.
Posted by: IC
Polygon Seminar: Exploring generalised dualities and integrable deformations
Daniel C Thompson
(Swansea)
Abstract:
Extensions of target space T-duality to non-Abelian isometry groups and even to spaces without isometry have found recent utility within the AdS/CFT correspondence and have played a central role in the development of new classes of integrable string backgrounds called \(\eta\) and \(\lambda\)-models. After a pedagogical introduction to the topic I will outline some recent results concerning the open sector of \(\lambda\)-models and the interpretation of these theories within the formalism of double field theory.
Extensions of target space T-duality to non-Abelian isometry groups and even to spaces without isometry have found recent utility within the AdS/CFT correspondence and have played a central role in the development of new classes of integrable string backgrounds called \(\eta\) and \(\lambda\)-models. After a pedagogical introduction to the topic I will outline some recent results concerning the open sector of \(\lambda\)-models and the interpretation of these theories within the formalism of double field theory.
Posted by: IC
Thursday, 22 Nov 2018
Holographic relative entropy in infinite-dimensional Hilbert spaces
Monica Kang
(Harvard)
Abstract:
Quantum error correction provides a convenient setup where bulk operators are defined only on a code subspace of the physical Hilbert space of the conformal field theory. I will first reformulate entanglement wedge reconstruction in the language of operator-algebra quantum error correction with infinite-dimensional physical and code Hilbert spaces. I will streamline my proof that for infinite-dimensional Hilbert spaces, the entanglement wedge reconstruction is identical to the equivalence of the boundary and bulk relative entropies. I will discuss its implications for holographic theories with the Reeh-Schlieder theorem.
Quantum error correction provides a convenient setup where bulk operators are defined only on a code subspace of the physical Hilbert space of the conformal field theory. I will first reformulate entanglement wedge reconstruction in the language of operator-algebra quantum error correction with infinite-dimensional physical and code Hilbert spaces. I will streamline my proof that for infinite-dimensional Hilbert spaces, the entanglement wedge reconstruction is identical to the equivalence of the boundary and bulk relative entropies. I will discuss its implications for holographic theories with the Reeh-Schlieder theorem.
Posted by: QMW
Friday, 23 Nov 2018
Goldstone pairs at the Fermi surface
Alberto Nicolis
(Columbia)
Abstract:
I will adapt the Goldstone theorem to spontaneously broken boosts, and show that, while still predicting gapless Goldstone states, it is quite forgiving regarding the nature of such states. In particular, I will show that while for solids and superfluids the role of the boost Goldstone states is played by phonon single-particle states, for a Fermi liquid such a role is played by the particle-hole continuum, that is, by two-particle states.
I will adapt the Goldstone theorem to spontaneously broken boosts, and show that, while still predicting gapless Goldstone states, it is quite forgiving regarding the nature of such states. In particular, I will show that while for solids and superfluids the role of the boost Goldstone states is played by phonon single-particle states, for a Fermi liquid such a role is played by the particle-hole continuum, that is, by two-particle states.
Posted by: IC