Talks

13105 - 13116 of 20131 Results

Anomaly-induced transport and thermodynamics

Kristan Jensen University of Victoria

November 13, 2012

PIRSA:12110047

High Energy Physics
Stealthy, Composite Stops

Philip Tanedo Cornell University

November 13, 2012

PIRSA:12110063

High Energy Physics
Recent progress on de Sitter S-matrix

Ian Morrison West Chester University

November 13, 2012

PIRSA:12110043

Astrophysics
Statistical Mechanics - Lecture 2

John Berlinsky McMaster University

November 13, 2012

PIRSA:12110020
Quantum Field Theory 2 - Lecture 2

Francois David CEA Saclay

November 13, 2012

PIRSA:12110001

High Energy Physics
Statistical Mechanics - Lecture 1

John Berlinsky McMaster University

November 12, 2012

PIRSA:12110019
Quantum Field Theory 2 - Lecture 1

Francois David CEA Saclay

November 12, 2012

PIRSA:12110000

High Energy Physics
Geometric algebra techniques in flux compactifications

Calin Lazaroiu Horia Hulubei National Institute for R and D in Physics and Nuclear Engineering

November 09, 2012

PIRSA:12110058

Mathematical Physics
Dynamical evaporation of quantum horizons

November 08, 2012

PIRSA:12110064

General Relativity & Quantum Cosmology
Discovery of the Higgs Boson: Sweet Dream or Nightmare

Melissa Franklin Harvard University

November 07, 2012

PIRSA:12110055
An introduction to quantum channels and their capacities

Graeme Smith Institute for Quantum Computing (IQC)

November 07, 2012

PIRSA:12110066

Quantum Physics
What's an unknown POVM, and what does a two qubit state look like?

Matthew Pusey University of York

November 06, 2012

PIRSA:12110068

Anomaly-induced transport and thermodynamics

Kristan Jensen University of Victoria

November 13, 2012

PIRSA:12110047

High Energy Physics

I will discuss recent progress in the study of anomaly-induced transport, focusing on the chiral vortical effect in 3+1 dimensions. Most of my discussion will be framed in light of a larger story, namely progress in making exact statements about finite-temperature quantum field theory, for which the chiral magnetic and vortical effects are instructive prototypes.
Stealthy, Composite Stops

Philip Tanedo Cornell University

November 13, 2012

PIRSA:12110063

High Energy Physics

Light third generation superpartners are one way to avoid bounds on new physics from the early LHC. We will review the theory and phenomenology of light stops and highlight a particular UV model based a partially composite electroweak sector through Seiberg duality.
Recent progress on de Sitter S-matrix

Ian Morrison West Chester University

November 13, 2012

PIRSA:12110043

Astrophysics

The de Sitter S-matrix provides a gauge-invariant and field redefinition-invariant window into de Sitter QFTs and may provide a crucial entry in any dS/CFT dictionary. In this talk I will summarize recent progress on developing the S-matrix for theories with gauge fields and perturbative gravity. Nonrenormalization theorems, hints of supersymmetry, and perturbative stability will be discussed.
Statistical Mechanics - Lecture 2

John Berlinsky McMaster University

November 13, 2012

PIRSA:12110020
Quantum Field Theory 2 - Lecture 2

Francois David CEA Saclay

November 13, 2012

PIRSA:12110001

High Energy Physics
Statistical Mechanics - Lecture 1

John Berlinsky McMaster University

November 12, 2012

PIRSA:12110019
Quantum Field Theory 2 - Lecture 1

Francois David CEA Saclay

November 12, 2012

PIRSA:12110000

High Energy Physics
Geometric algebra techniques in flux compactifications

Calin Lazaroiu Horia Hulubei National Institute for R and D in Physics and Nuclear Engineering

November 09, 2012

PIRSA:12110058

Mathematical Physics

Using techniques originating in a certain approach to Clifford bundles known as "geometric algebra", I discuss a geometric reformulation of constrained generalized Killing spinor equations which proves to be particularly effective in the study and classification of supersymmetric flux compactifications of string and M-theory. As an application, I discuss the most general N=2 compactifications of M-theory to three dimensions, which were never studied in full generality before. I also touch upon the connection of such techniques with a certain variant of the quantization of spin systems.
Dynamical evaporation of quantum horizons

November 08, 2012

PIRSA:12110064

General Relativity & Quantum Cosmology

We describe of the evaporation process as driven by the dynamical evolution of the quantum gravitational degrees of freedom resident at the horizon, as identified by the Loop Quantum Gravity kinematics. Using a parallel with the Brownian motion, we interpret the first law of quantum dynamical horizon in terms of a fluctuation-dissipation relation applied to this fundamental discrete structure. In this way, the horizon evolution is described in terms of relaxation to an equilibrium state balanced by the excitation of Planck scale constituents of the horizon. We show how from this setting the emergence of several conservative scenarios for the final stage of the evaporation process can be microscopically derived. Namely, the leakage of part of the horizon quantum geometry information prior to the Planckian phase and the stabilization of the hole surface shrinkage forming a massive remnant, which can eventually decay, are shown to take place.
Discovery of the Higgs Boson: Sweet Dream or Nightmare

Melissa Franklin Harvard University

November 07, 2012

PIRSA:12110055
An introduction to quantum channels and their capacities

Graeme Smith Institute for Quantum Computing (IQC)

November 07, 2012

PIRSA:12110066

Quantum Physics

A quantum communication channel can be put to many uses: it can transmit classical information, private classical information, or quantum information. It can be used alone, with shared entanglement, or together with other channels. For each of these settings there is a capacity that quantifies a channel's fundamental potential for communication. In this introductory talk, I will discuss what we known about the various capacities of a quantum channel, including a discussion of synergies between different channels and related additivity questions.
What's an unknown POVM, and what does a two qubit state look like?

Matthew Pusey University of York

November 06, 2012

PIRSA:12110068

If probabilities represent knowledge, what is an "unknown
probability"? De Finetti's theorem licenses the view that it is simply a
convenient metaphor for a certain class of knowledge about a series of
events. There are quantum versions for "unknown states" and "unknown
channels". I will explain how "unknown measurements" can be rehabilitated
too.

I will then move to a totally different topic. The Bloch sphere is handy
for representing qubit states, but the equivalent for two qubits is
15-dimensional! I will advocate instead drawing the set of states that Bob
can steer Alice to, the "steering ellipsoid". I will show how entanglement
and discord look from this perspective, and outline a geometric
classification of separable two qubit states.

Title	Date	Collection	Type	Info
Anomaly-induced transport and thermodynamics	2012‑11‑13	Quantum Fields and Strings	Scientific Series	View details
Stealthy, Composite Stops	2012‑11‑13	Particle Physics	Scientific Series	View details
Recent progress on de Sitter S-matrix	2012‑11‑13	Cosmology and Gravitation	Scientific Series	View details
Statistical Mechanics - Lecture 2	2012‑11‑13	12/13 PSI - Statistical Mechanics	Course	View details
Quantum Field Theory 2 - Lecture 2	2012‑11‑13	12/13 PSI - Quantum Field Theory 2	Course	View details
Statistical Mechanics - Lecture 1	2012‑11‑12	12/13 PSI - Statistical Mechanics	Course	View details
Quantum Field Theory 2 - Lecture 1	2012‑11‑12	12/13 PSI - Quantum Field Theory 2	Course	View details
Geometric algebra techniques in flux compactifications	2012‑11‑09	Strings Group Meeting	Scientific Series	View details
Dynamical evaporation of quantum horizons	2012‑11‑08	Quantum Gravity	Scientific Series	View details
Discovery of the Higgs Boson: Sweet Dream or Nightmare	2012‑11‑07	Public Lecture Series	Public Lectures	View details
An introduction to quantum channels and their capacities	2012‑11‑07	Colloquium	Scientific Series	View details
What's an unknown POVM, and what does a two qubit state look like?	2012‑11‑06	Quantum Foundations	Scientific Series	View details

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Format results

Anomaly-induced transport and thermodynamics

Stealthy, Composite Stops

Recent progress on de Sitter S-matrix

Statistical Mechanics - Lecture 2

Quantum Field Theory 2 - Lecture 2

Statistical Mechanics - Lecture 1

Quantum Field Theory 2 - Lecture 1

Geometric algebra techniques in flux compactifications

Dynamical evaporation of quantum horizons

Discovery of the Higgs Boson: Sweet Dream or Nightmare

An introduction to quantum channels and their capacities

What's an unknown POVM, and what does a two qubit state look like?

Anomaly-induced transport and thermodynamics

Stealthy, Composite Stops

Recent progress on de Sitter S-matrix

Statistical Mechanics - Lecture 2

Quantum Field Theory 2 - Lecture 2

Statistical Mechanics - Lecture 1

Quantum Field Theory 2 - Lecture 1

Geometric algebra techniques in flux compactifications

Dynamical evaporation of quantum horizons

Discovery of the Higgs Boson: Sweet Dream or Nightmare

An introduction to quantum channels and their capacities

What's an unknown POVM, and what does a two qubit state look like?