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... and (8) must be specified (in place of (5)) by the more general expression ...
PPT | 345.5 KB - Joint Quantum Institute
PPT | 345.5 KB - Joint Quantum Institute

Quanta to Quarks - The University of Sydney
Quanta to Quarks - The University of Sydney

What is quantum chaos?
What is quantum chaos?

... 3. Are there other universality class in quantum chaos? How many? 4. Is localization relevant in quantum chaos? ...
Loop Quantum Gravity and Effective Matter Theories
Loop Quantum Gravity and Effective Matter Theories

Slides
Slides

Metric and curvature in gravitational phase space
Metric and curvature in gravitational phase space

Matteo Bertolini: Research
Matteo Bertolini: Research

QUANTUM MAPS
QUANTUM MAPS

Discrete quantum gravity: a mechanism for selecting the value of
Discrete quantum gravity: a mechanism for selecting the value of

x - PMF
x - PMF

... metric. It is invariant under coordinate transformation on three-space. • No external time parameter is present anymore – theory is “timeless” •Wheeler-DeWitt equation is hyperbolic •this approach is good candidate for a non-perturbative quantum theory of gravity. It should be valid away the Planck ...
The 17st June 2009 This file is intended to provide more information
The 17st June 2009 This file is intended to provide more information

Available PDF download
Available PDF download

Relation Between Schrödinger and Polymer Quantum Mechanics
Relation Between Schrödinger and Polymer Quantum Mechanics

The Lee-Wick Fields out of Gravity
The Lee-Wick Fields out of Gravity

... was argued to be a physical resonance and unitarity is preserved despite the wrong sign in (11). As a result, one is left with a theory containing both massless and massive spin one fields. Similar to photons, the massive Lee-Wick vector fields also serve as mediators of the electromagnetic interac ...
Orthogonal polynomials, special functions and mathematical physics
Orthogonal polynomials, special functions and mathematical physics

... symmetry there corresponds a group. The carrier space of some irreducible representation of a group can be expressed with the help of special functions [15]. In this symposium there have been proposed some particular groups associated to the Lagrangian, with the help of root systems of a classical L ...
Gregory Moore - Rutgers Physics
Gregory Moore - Rutgers Physics

... Mass Formula & Central Charge Given a BPS state ...
20071008133014301
20071008133014301

... In recent years we have realized that strings in 10d are in fact the QCD string… a weird and wonderful alternative description of quarks and glue… Maldacena ...
My Century of Physics
My Century of Physics

Integrable Models in Classical and Quantum Field Theory
Integrable Models in Classical and Quantum Field Theory

Tyler: Quantum Adiabatic Theorem and Berry`s Phase Factor
Tyler: Quantum Adiabatic Theorem and Berry`s Phase Factor

Holonomic Quantum Computation with Josephson Networks
Holonomic Quantum Computation with Josephson Networks

Note 1
Note 1

... S-matrix have particles at infinity, and gauge transformations acting at infinity are true symmetries. They take one physical state to a di↵erent physical state — unlike local gauge transformations, which map a physical state to a di↵erent description of the same physical state. In gravity, local di ...
Isometric and unitary phase operators: explaining the Villain transform
Isometric and unitary phase operators: explaining the Villain transform

to be completed. LECTURE NOTES 1
to be completed. LECTURE NOTES 1

... It is not hard to check that WH is a well-defined continuous map from S to S for any H ∈ S 0 (R2n ). The well-known Schwartz kernel theorem then states that every continuous operator on S can be written as WH for some H ∈ S 0 (R2n ). The map H ∈ S(R2n ) → WH ∈ L(S, S) is called the Weyl corresponden ...
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Canonical quantum gravity

In physics, canonical quantum gravity is an attempt to quantize the canonical formulation of general relativity (or canonical gravity). It is a Hamiltonian formulation of Einstein's general theory of relativity. The basic theory was outlined by Bryce DeWitt in a seminal 1967 paper, and based on earlier work by Peter G. Bergmann using the so-called canonical quantization techniques for constrained Hamiltonian systems invented by Paul Dirac. Dirac's approach allows the quantization of systems that include gauge symmetries using Hamiltonian techniques in a fixed gauge choice. Newer approaches based in part on the work of DeWitt and Dirac include the Hartle–Hawking state, Regge calculus, the Wheeler–DeWitt equation and loop quantum gravity.
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