Deformation quantization and asymptotic operator representation

1991 ◽  
Vol 25 (3) ◽  
pp. 184-194 ◽  
Author(s):  
B. V. Fedosov
Keyword(s):  
Deformation Quantization ◽  
Operator Representation ◽  
Asymptotic Operator

scholarly journals DEFORMATION QUANTIZATION OF THE ISOTROPIC ROTATOR

1995 ◽  
Vol 10 (05) ◽  
pp. 399-407 ◽  
Author(s):  
A. STERN ◽  
I. YAKUSHIN
Keyword(s):  
Energy Spectrum ◽  
Quantum System ◽  
Chiral Symmetry ◽  
Deformation Quantization ◽  
Rigid Rotator

We perform a deformation quantization of the classical isotropic rigid rotator. The resulting quantum system is not invariant under the usual SU (2) × SU (2) chiral symmetry, but instead [Formula: see text]. We give the energy spectrum for the resulting system.

scholarly journals KONTSEVICH'S UNIVERSAL FORMULA FOR DEFORMATION QUANTIZATION AND THE CAMPBELL–BAKER–HAUSDORFF FORMULA

2000 ◽  
Vol 11 (04) ◽  
pp. 523-551 ◽  
Author(s):  
VINAY KATHOTIA
Keyword(s):  
Lie Algebras ◽  
Deformation Quantization ◽  
Differential Operators ◽  
Main Tool ◽  
Graphical Analysis ◽  
Poisson Structures ◽  
Nilpotent Lie Algebras ◽  
Enveloping Algebra ◽  
Universal Formula ◽  
The Given

We relate a universal formula for the deformation quantization of Poisson structures (⋆-products) on ℝd proposed by Maxim Kontsevich to the Campbell–Baker–Hausdorff (CBH) formula. We show that Kontsevich's formula can be viewed as exp (P) where P is a bi-differential operator that is a deformation of the given Poisson structure. For linear Poisson structures (duals of Lie algebras) his product takes the form exp (C+L) where exp (C) is the ⋆-product given by the universal enveloping algebra via symmetrization, essentially the CBH formula. This is established by showing that the two products are identical on duals of nilpotent Lie algebras where the operator L vanishes. This completely determines part of Kontsevich's formula and leads to a new scheme for computing the CBH formula. The main tool is a graphical analysis for bi-differential operators and the computation of certain iterated integrals that yield the Bernoulli numbers.

scholarly journals Deformation Quantization, Superintegrability and Nambu Mechanics

2004 ◽  
Vol 19 (3-4) ◽  
pp. 199-203 ◽  
Author(s):  
Cosmas K. Zachos ◽  
Thomas L. Curtright
Keyword(s):  
Deformation Quantization ◽  
Nambu Mechanics

scholarly journals Deformation quantization of principal bundles

2016 ◽  
Vol 13 (08) ◽  
pp. 1630010
Author(s):  
Paolo Aschieri
Keyword(s):  
Quantum Group ◽  
Deformation Quantization ◽  
Principal Bundle ◽  
Base Space ◽  
Structure Group ◽  
Galois Extensions ◽  
Principal Bundles ◽  
Group Of Automorphisms ◽  
Drinfeld Twist

We outline how Drinfeld twist deformation techniques can be applied to the deformation quantization of principal bundles into noncommutative principal bundles and, more in general, to the deformation of Hopf–Galois extensions. First, we twist deform the structure group in a quantum group, and this leads to a deformation of the fibers of the principal bundle. Next, we twist deform a subgroup of the group of automorphisms of the principal bundle, and this leads to a noncommutative base space. Considering both deformations, we obtain noncommutative principal bundles with noncommutative fiber and base space as well.

scholarly journals Super Toeplitz operators and non-perturbative deformation quantization of supermanifolds

1993 ◽  
Vol 153 (1) ◽  
pp. 49-76 ◽  
Author(s):  
David Borthwick ◽  
Slawomir Klimek ◽  
Andrzej Lesniewski ◽  
Maurizio Rinaldi
Keyword(s):  
Deformation Quantization ◽  
Toeplitz Operators

scholarly journals Operator Representation of Fermi-Dirac and Bose-Einstein Integral Functions with Applications

2007 ◽  
Vol 2007 ◽  
pp. 1-9 ◽  
Author(s):  
M. Aslam Chaudhry ◽  
Asghar Qadir
Keyword(s):  
Zeta Function ◽  
Riemann Zeta Function ◽  
Statistical Distributions ◽  
Operator Representation ◽  
The Riemann Zeta Function ◽  
Riemann Zeta ◽  
Quantum Statistical ◽  
Bose Einstein ◽  
Operator Representations ◽  
Class Of Functions

Fermi-Dirac and Bose-Einstein functions arise as quantum statistical distributions. The Riemann zeta function and its extension, the polylogarithm function, arise in the theory of numbers. Though it might not have been expected, these two sets of functions belong to a wider class of functions whose members have operator representations. In particular, we show that the Fermi-Dirac and Bose-Einstein integral functions are expressible as operator representations in terms of themselves. Simpler derivations of previously known results of these functions are obtained by their operator representations.

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