Introduction to quantum groups 5
Florian Koch - Ludwig-Maximilians-Universität München (LMU)
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Introduction to quantum groups 4
Florian Koch - Ludwig-Maximilians-Universität München (LMU)
Graduate Course on Standard Model & Quantum Field Theory - 10B
Cliff Burgess - McMaster University
Physics of Magnetic Reconnection
Richard Sydora - University of Alberta
Graduate Course on Standard Model & Quantum Field Theory - 10A
Cliff Burgess - McMaster University
Quantum Error Correction 3B
Daniel Gottesman - University of Maryland, College Park
Quantum Error Correction 3A
Daniel Gottesman - University of Maryland, College Park
Domain Lines as Fractional Strings
Roberto Auzzi - University of Minnesota
Quantum Simulations of Quantum and Classical Systems
Rolando Somma - Alphabet (United States)
An Information-Theoretic Approach to Quantum Theory
Philip Goyal - State University of New York (SUNY)
Introduction to quantum groups 3
Florian Koch - Ludwig-Maximilians-Universität München (LMU)
Introduction to quantum groups 2
Florian Koch - Ludwig-Maximilians-Universität München (LMU)
Fundamental Physics Without Colliding Particles
Asimina Arvanitaki - Perimeter Institute for Theoretical Physics
14/15 PSI - Conformal Field Theory - Lecture 12
Freddy Cachazo - Perimeter Institute for Theoretical Physics
14/15 PSI - Quantum Field Theory I (A) - Lecture 12
Tibra Ali - Perimeter Institute for Theoretical Physics , Dan Wohns - Perimeter Institute for Theoretical Physics
Entanglement Entropy and the Area Law - Lecture 3
Rafael Sorkin - Perimeter Institute for Theoretical Physics
Disturbance in weak measurements and the difference between quantum and classical weak values
The role of measurement induced disturbance in weak measurements is of central importance for the interpretation of the weak value. Uncontrolled disturbance can interfere with the postselection process and make the weak value dependent on the details of the measurement process. Here we develop the…
Numerical Study of a Bosonic Topological Insulator in Three Dimensions
Scott Geraedts - California Institute of Technology
We construct a model which realizes a (3+1)-dimensional symmetry-protected topological phase of bosons with U(1) charge conservation and time reversal symmetry, envisioned by A. Vishwanath and T. Senthil [PRX 4 011016]. Our model works by introducing an additional spin degree of freedom, and binding…
14/15 PSI - Conformal Field Theory - Lecture 11
Freddy Cachazo - Perimeter Institute for Theoretical Physics
Three-Point Function in N=4 SYM and Spin Vertex
In this talk I will explain how to compute three-point functions of N=4 SYM theory in the planar limit for tree level and one-loop in perturbation theory. First I will recall how to formulate the problem of computing the three-point function of operators with determined R-charges in the language of…