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From the pudding cake to the Super Symmetry
From the pudding cake to the Super Symmetry

Slide - University of Maryland
Slide - University of Maryland

... But now consider any smoothly related gauge (“P-smooth gauges”), (Xi smooth) It is of course still true that h-hS is sufficiently regular. ...
Interaction-induced Lipkin-Meshkov-Glick model in a Bose
Interaction-induced Lipkin-Meshkov-Glick model in a Bose

... 26 October 2009 / Vol. 17, No. 22 / OPTICS EXPRESS 19682 ...
On the quantization of the superparticle action in proper time and the
On the quantization of the superparticle action in proper time and the

(4)
(4)

Is there a problem with quantum wormhole states in N= 1
Is there a problem with quantum wormhole states in N= 1

Particle Physics on Noncommutative Spaces
Particle Physics on Noncommutative Spaces

... gauge theory based on the group SU(3)SU(2)U(1), emerge as a low energy action of a noncommutative gauge theory? • The main difficulty is to implement symmetries on NC spaces. • We need to understand how to implement SU(N) gauge symmetries on NC spaces. • Are there space-time symmetries (Lorentz in ...
PDF
PDF

Two-State Vector Formalism
Two-State Vector Formalism

2 + 1 dimensional gravity as an exactly soluble system
2 + 1 dimensional gravity as an exactly soluble system

Einstein Finds Past Events Not Knowable with
Einstein Finds Past Events Not Knowable with

... This amazing extension of the prin- 1905 applied the quantum theory of ciples of the new physics is contained energy to light and electricity. The in a letter to the editor of the Physical quantum idea that energy is not conReview, journal of the American Phys- tinuous but in packetsor gobs like mat ...
Lecture 2: Bogoliubov theory of a dilute Bose gas Abstract
Lecture 2: Bogoliubov theory of a dilute Bose gas Abstract

... infinite volume V but finite particle density, I want to investigate more closely the consequences of having a nondegenerate ground state. I consider the cases of both noninteracting many-body Hamiltonians such as Ĥ in Eq. (2.12) and interacting many-body Hamiltonians5 that commute with Q̂. The Hil ...
4-Space Dirac Theory and LENR A. B. Evans Research Article ∗
4-Space Dirac Theory and LENR A. B. Evans Research Article ∗

... Little-known versions of QED, known collectively as parametrized relativistic quantum theories [1,2], have for decades been investigated intermittently by researchers looking for models that clearly avoid any suggestion of a preferred frame of reference. In these models, the space-time coordinates X ...
Introduction to loop quantum gravity
Introduction to loop quantum gravity

Read PDF - Physics (APS)
Read PDF - Physics (APS)

Space, time and Riemann zeros (Madrid, 2013)
Space, time and Riemann zeros (Madrid, 2013)

... • The xp model is a promissing candidate to yield a spectral interpretation of the Riemann zeros • Connes xp -> Landau xy model -> Analogue of Hawking radiation in the FQHE (Stone). No connection with Riemann zeros. • Berry-Keating xp -> Dirac fermion in Rindler space • Conjecture: b-c field theory ...
Transparencies
Transparencies

... Also sounds good, but requires a fixed causal structure. (Terno reports on some developments) What is an event when we sum over causal histories? Maybe quantum theory should come from quantum gravity and not the other way around?? ...
Deformation quantization for fermionic fields
Deformation quantization for fermionic fields

... infinite number of degrees of freedom, that besides be consistent with the Lorentz invariance and with the gauge invariance. In this work we present the formalism of Weyl-WignerMoyal for fermionic fields, and it is applied to Dirac field as an example. ...
Dispersion Relation of Longitudinal Waves in
Dispersion Relation of Longitudinal Waves in

M Theory Model of a Big Crunch/Big Bang Transition Abstract
M Theory Model of a Big Crunch/Big Bang Transition Abstract

Get PDF - OSA Publishing
Get PDF - OSA Publishing

Second quantization and tight binding models
Second quantization and tight binding models

One-loop partition function of three
One-loop partition function of three

l = 0
l = 0

CS286.2 Lectures 5-6: Introduction to Hamiltonian Complexity, QMA
CS286.2 Lectures 5-6: Introduction to Hamiltonian Complexity, QMA

< 1 ... 16 17 18 19 20 21 22 23 24 ... 38 >

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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