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TBA

Florian Girelli University of Waterloo

May 21, 2014

PIRSA:14050121
Gauge theory of gravity and matter

Steven Kerr ThinkTank Maths Ltd.

May 21, 2014

PIRSA:14050120
Equality

Tobias Fritz Universität Innsbruck

May 21, 2014

PIRSA:14050063
New Vacuum and Representation For Loop Quantum Gravity

Bianca Dittrich Perimeter Institute for Theoretical Physics

May 21, 2014

PIRSA:14050119
Designing exotic circuitry with non-Abelian anyons
May 20, 2014

PIRSA:14050029
Condensed Matter
Local quanta, unitary inequivalence, and vacuum entanglement

Hans Westman
May 20, 2014

PIRSA:14050117
Quantum Foundations
M-strings and their orbifolds

Babak Haghighat Harvard University
May 20, 2014

PIRSA:14050005
Quantum Fields and Strings
Black holes and Boyle's Law --- the thermodynamics of Einstein's greatest mistake

Brian Dolan Maynooth University
May 20, 2014

PIRSA:14050093
Cosmology
(Lea Santos) General Features of the Relaxation Dynamics of Isolated Interacting Quantum Systems

May 16, 2014

PIRSA:14050088
Quench dynamics in interacting and disordered field theories in one-dimension

Aditi Mitra New York University (NYU)

May 16, 2014

PIRSA:14050087
(Robert Konik) Glimmers of a Quantum KAM Theorem: Insights from Quantum Quenches in One Dimensional Bose Gases

May 16, 2014

PIRSA:14050086
From locally covariant QFT to quantum gravity

Katarzyna Rejzner University of York
May 15, 2014

PIRSA:14050004
Quantum Gravity

TBA

Florian Girelli University of Waterloo

May 21, 2014

PIRSA:14050121
Gauge theory of gravity and matter

Steven Kerr ThinkTank Maths Ltd.

May 21, 2014

PIRSA:14050120
Equality

Tobias Fritz Universität Innsbruck

May 21, 2014

PIRSA:14050063

Equality of two mathematical objects is a seemingly simple and well-understood concept. In this talk, I will do three things to explain why this is a misconception: I will survey different notions of equality, explain how revising the notion of equality has led to an emerging alternative foundation of mathematics called "homotopy type theory", and try to convince you that thinking about equality is relevant to your research in quantum field theory, quantum gravity or quantum foundations.
New Vacuum and Representation For Loop Quantum Gravity

Bianca Dittrich Perimeter Institute for Theoretical Physics

May 21, 2014

PIRSA:14050119
Designing exotic circuitry with non-Abelian anyons
May 20, 2014

PIRSA:14050029
Condensed Matter
Non-Abelian anyons are widely sought for the exotic fundamental physics they harbor as well as for their possible applications for quantum information processing. Currently, there are numerous blueprints for stabilizing the simplest type of non-Abelian anyon, a Majorana zero energy mode bound to a vortex or a domain wall. One such candidate system, a so-called "Majorana wire" can be made by judiciously interfacing readily available materials; the experimental evidence for the viability of this approach is presently emerging.
Following this idea, we introduce a device fabricated from conventional fractional quantum Hall states, s-wave superconductors and insulators with strong spin-orbit coupling. Similarly to a Majorana wire, the ends of our “quantum wire” would bind "parafermions", exotic non-Abelian anyons which can be viewed as fractionalised Majorana zero modes.
I will discuss their properties and describe how such parafermions can be used to construct new and potentially useful circuit elements which include current and voltage mirrors, transistors for fractional charge currents and "flux capacitors".
Local quanta, unitary inequivalence, and vacuum entanglement

Hans Westman
May 20, 2014

PIRSA:14050117
Quantum Foundations
In this work we develop a formalism for describing localised quanta for a real-valued Klein-Gordon field in a one-dimensional box [0, R]. We quantise the field using non-stationary local modes which, at some arbitrarily chosen initial time, are completely localised within the left or the right side of the box. In this concrete set-up we directly face the problems inherent to a notion of local field excitations, usually thought of as elementary particles. Specifically, by computing the Bogoliubov coefficients relating local and standard (global) quantizations, we show that the local quantisation yields a Fock space F^L which is unitarily inequivalent to the standard one F^G. In spite of this, we find that the local creators and annihilators remain well defined in the global Fock space F^G, and so do the local number operators associated to the left and right partitions of the box. We end up with a useful mathematical toolbox to analyse and characterise local features of quantum states in F^G . Specifically, an analysis of the global vacuum state |0_G> ∈ F^G in terms of local number operators shows, as expected, the existence of entanglement between the left and right regions of the box. The local vacuum |0_L> ∈ F^L , on the contrary, has a very different character. It is neither cyclic nor separating and displays no entanglement. Further analysis shows that the global vacuum also exhibits a distribution of local excitations reminiscent, in some respects, of a thermal bath. We discuss how the mathematical tools developed herein may open new ways for the analysis of fundamental problems in local quantum field theory.
M-strings and their orbifolds

Babak Haghighat Harvard University
May 20, 2014

PIRSA:14050005
Quantum Fields and Strings
We consider M-theory in the presence of M parallel M5-branes probing a transverse A_{N-1} singularity. This leads to a superconformal theory with (1,0) supersymmetry in six dimensions. We compute the supersymmetric partition function of this theory on a two-torus, with arbitrary supersymmetry preserving twists, using the topological vertex formalism. Alternatively, we show that this can also be obtained by computing the elliptic genus of an orbifold of recently studied M-strings. The resulting 2d theory is a (4,0) supersymmetric quiver gauge theory whose Higgs branch corresponds to strings propagating on the moduli space of SU(N)^(M-1) instantons on R^4 where the right-moving fermions are coupled to a particular bundle.
Black holes and Boyle's Law --- the thermodynamics of Einstein's greatest mistake

Brian Dolan Maynooth University
May 20, 2014

PIRSA:14050093
Cosmology
The thermodynamics of black holes will be reviewed and recent developments incorporating pressure into the first law described. The asymptotically AdS Kerr metric has a van der Waals type critical point with a line of first order phase transitions terminating at a critical point with mean field exponents. The phase structure and stability of black holes in higher dimensions will also be described.
(Lea Santos) General Features of the Relaxation Dynamics of Isolated Interacting Quantum Systems

May 16, 2014

PIRSA:14050088

We consider isolated interacting quantum systems that are taken out of equilibrium instantaneously (quenched). We study numerically and analytically the probability of finding the initial state later on in time (the so-called fidelity or Loschmidt echo), the relaxation time of the system, and the evolution of few-body observables. The fidelity decays fastest for systems described by full random matrices, where simultaneous many-body interactions are implied. In the realm of realistic systems with two-body interactions, the dynamics is slower and dependent on the energy of the initial state. The fastest fidelity decay in this case is Gaussian and can persist until saturation. The fidelity also plays a central role in the short-time dynamics of few-body observables that commute with the system Hamiltonian before the quench. Our analyses are mainly developed for initial states that can be prepared in experiments with cold atoms in optical lattices.
Quench dynamics in interacting and disordered field theories in one-dimension

Aditi Mitra New York University (NYU)

May 16, 2014

PIRSA:14050087

I will present results for the quench dynamics of one-dimensional interacting bosons under two circumstances. One is when the bosons are in the vicinity of the superfluid-Mott quantum critical point, while the second is when the bosons are in a disordered potential which can drive the system into a Bose glass phase. I will show that the dynamics following a quench can be quite complex by being characterized by three regimes. One is a short time perturbatively accessible regime which depends on microscopic parameters, the second is an intermediate time prethermalized regime where inelastic effects are weak and correlation functions can show universal scaling behavior which is quantified by a nonequilibrium generalization of the Callan-Symanzik equations. The third is a long time regime where inelastic effects become important. For the dynamics in the inelastic regime I will construct a novel quantum kinetic equation that accounts for multi-particle scattering between bosons, and discuss how the combined effect of interactions and (weak) disorder can thermalize the system.
(Robert Konik) Glimmers of a Quantum KAM Theorem: Insights from Quantum Quenches in One Dimensional Bose Gases

May 16, 2014

PIRSA:14050086

We consider quantum quenches in one dimensional Bose gases where we prepare the gas in the ground state of a parabolic trap and then release it into a small cosine potential. This cosine potential breaks the integrability of the 1D gas which absent the potential is described by the Lieb-Liniger model. We explore the consequences of this cosine potential on the thermalization of the gas. We argue that the integrability breaking of the cosine does not immediately lead to ergodicity inasmuch as we demonstrate that there are residual quasi-conserved quantities post-quench. We demonstrate that the quality of this quasi-conservation can be made arbitrarily good.
From locally covariant QFT to quantum gravity

Katarzyna Rejzner University of York
May 15, 2014

PIRSA:14050004
Quantum Gravity
Locally covariant quantum field theory (LCQFT) has proven to be a very successful framework for QFT on curved spacetimes. It is natural to ask, how far these ideas can be generalized and if one can learn something about quantum gravity, using LCQFT methods. In particular, one can use the relative Cauchy evolution to formulate the notion of background independence. Recently we have proven that background independence in this sense holds for effective quantum gravity, formulated as a perturbative QFT. Remarkably, the formalism of LCQFT can be extended to structures more general than spacetimes. The essential feature is the presence of the causal structure. An example application would be QFT on causal sets (work in progress).

Title	Date	Collection	Type	Info
TBA	2014‑05‑21	Quantum Gravity Day 2014	Conference	View details
Gauge theory of gravity and matter	2014‑05‑21	Quantum Gravity Day 2014	Conference	View details
Equality	2014‑05‑21	Colloquium	Scientific Series	View details
New Vacuum and Representation For Loop Quantum Gravity	2014‑05‑21	Quantum Gravity Day 2014	Conference	View details
Designing exotic circuitry with non-Abelian anyons	2014‑05‑20	Quantum Matter	Scientific Series	View details
Local quanta, unitary inequivalence, and vacuum entanglement	2014‑05‑20	Quantum Foundations	Scientific Series	View details
M-strings and their orbifolds	2014‑05‑20	Quantum Fields and Strings	Scientific Series	View details
Black holes and Boyle's Law --- the thermodynamics of Einstein's greatest mistake	2014‑05‑20	Cosmology and Gravitation	Scientific Series	View details
(Lea Santos) General Features of the Relaxation Dynamics of Isolated Interacting Quantum Systems	2014‑05‑16	Quantum Many-Body Dynamics	Conference	View details
Quench dynamics in interacting and disordered field theories in one-dimension	2014‑05‑16	Quantum Many-Body Dynamics	Conference	View details
(Robert Konik) Glimmers of a Quantum KAM Theorem: Insights from Quantum Quenches in One Dimensional Bose Gases	2014‑05‑16	Quantum Many-Body Dynamics	Conference	View details
From locally covariant QFT to quantum gravity	2014‑05‑15	Quantum Gravity	Scientific Series	View details

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