Introduction to Wigner-Weyl Calculus
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Dirac Brackets in Geometric Dynamics Annales De L’I
ANNALES DE L’I. H. P., SECTION A JEDRZEJ S´ NIATYCKI Dirac brackets in geometric dynamics Annales de l’I. H. P., section A, tome 20, no 4 (1974), p. 365-372 <http://www.numdam.org/item?id=AIHPA_1974__20_4_365_0> © Gauthier-Villars, 1974, tous droits réservés. L’accès aux archives de la revue « Annales de l’I. H. P., section A » implique l’accord avec les conditions générales d’utilisation (http://www.numdam. org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Ann. Inst. Henri Poincaré, Section A : Vol. XX, n° 4, 1974, 365 Physique théorique. Dirac brackets in geometric dynamics Jedrzej 015ANIATYCKI The University of Calgary, Alberta, Canada. Department of Mathematics Statistics and Computing Science ABSTRACT. - Theory of constraints in dynamics is formulated in the framework of symplectic geometry. Geometric significance of secondary constraints and of Dirac brackets is given. Global existence of Dirac brackets is proved. 1. INTRODUCTION The successes of the canonical quantization of dynamical systems with a finite number of degrees of freedom, the experimental necessity of quan- tization of electrodynamics, and the hopes that quantization of the gravi- tational field could resolve difficulties encountered in quantum field theory have given rise to thorough investigation of the canonical structure of field theories. It has been found that the standard Hamiltonian formu- lation of dynamics is inadequate in the physically most interesting cases of electrodynamics and gravitation due to existence of constraints. -
Infinitely Many Star Products to Play With
DSF{40{01 BiBoS 01-12-068 ESI 1109 hep{th/0112092 December 2001 Infinitely many star products to play with J.M. Gracia-Bond´ıa a;b, F. Lizzi b, G. Marmo b and P. Vitale c a BiBoS, Fakult¨atder Physik, Universit¨atBielefeld, 33615 Bielefeld, Germany b Dipartimento di Scienze Fisiche, Universit`adi Napoli Federico II and INFN, Sezione di Napoli, Monte S. Angelo Via Cintia, 80126 Napoli, Italy [email protected], [email protected] c Dipartimento di Fisica, Universit`adi Salerno and INFN Gruppo Collegato di Salerno, Via S. Allende 84081 Baronissi (SA), Italy [email protected] Abstract While there has been growing interest for noncommutative spaces in recent times, most examples have been based on the simplest noncommutative algebra: [xi; xj] = iθij. Here we present new classes of (non-formal) deformed products k associated to linear Lie algebras of the kind [xi; xj] = icijxk. For all possible three- dimensional cases, we define a new star product and discuss its properties. To complete the analysis of these novel noncommutative spaces, we introduce noncom- pact spectral triples, and the concept of star triple, a specialization of the spectral triple to deformations of the algebra of functions on a noncompact manifold. We examine the generalization to the noncompact case of Connes' conditions for non- commutative spin geometries, and, in the framework of the new star products, we exhibit some candidates for a Dirac operator. On the technical level, properties of 2n the Moyal multiplier algebra M(Rθ ) are elucidated. 1 Introduction Over five years ago, Connes gave the first axiomatics for first-quantized fermion fields on (compact) noncommutative varieties, the so-called spectral triples [1]. -
Non-Abelian Conversion and Quantization of Non-Scalar Second
FIAN-TD/05-01 hep-th/0501097 Non-Abelian Conversion and Quantization of Non-scalar Second-Class Constraints I. Batalin,a M. Grigoriev,a and S. Lyakhovichb aTamm Theory Department, Lebedev Physics Institute, Leninsky prospect 53, 119991 Moscow, Russia bTomsk State University, prospect Lenina 36, 634050 Tomsk, Russia ABSTRACT. We propose a general method for deformation quantization of any second-class constrained system on a symplectic manifold. The constraints deter- mining an arbitrary constraint surface are in general defined only locally and can be components of a section of a non-trivial vector bundle over the phase-space manifold. The covariance of the construction with respect to the change of the constraint basis is provided by introducing a connection in the “constraint bundle”, which becomes a key ingredient of the conversion procedure for the non-scalar constraints. Unlike arXiv:hep-th/0501097v1 13 Jan 2005 in the case of scalar second-class constraints, no Abelian conversion is possible in general. Within the BRST framework, a systematic procedure is worked out for con- verting non-scalar second-class constraints into non-Abelian first-class ones. The BRST-extended system is quantized, yielding an explicitly covariant quantization of the original system. An important feature of second-class systems with non-scalar constraints is that the appropriately generalized Dirac bracket satisfies the Jacobi identity only on the constraint surface. At the quantum level, this results in a weakly associative star-product on the phase space. 2 BATALIN, GRIGORIEV, AND LYAKHOVICH CONTENTS 1. Introduction 2 2. Geometry of constrained systems with locally defined constraints 5 3. -
Phase Space Quantum Mechanics Is Such a Natural Formulation of Quantum Theory
Phase space quantum mechanics Maciej B laszak, Ziemowit Doma´nski Faculty of Physics, Adam Mickiewicz University, Umultowska 85, 61-614 Pozna´n, Poland Abstract The paper develope the alternative formulation of quantum mechanics known as the phase space quantum mechanics or deformation quantization. It is shown that the quantization naturally arises as an appropriate deformation of the classical Hamiltonian mechanics. More precisely, the deformation of the point-wise prod- uct of observables to an appropriate noncommutative ⋆-product and the deformation of the Poisson bracket to an appropriate Lie bracket is the key element in introducing the quantization of classical Hamiltonian systems. The formalism of the phase space quantum mechanics is presented in a very systematic way for the case of any smooth Hamiltonian function and for a very wide class of deformations. The considered class of deformations and the corresponding ⋆-products contains as a special cases all deformations which can be found in the literature devoted to the subject of the phase space quantum mechanics. Fundamental properties of ⋆-products of observables, associated with the considered deformations are presented as well. Moreover, a space of states containing all admissible states is introduced, where the admissible states are appropriate pseudo-probability distributions defined on the phase space. It is proved that the space of states is endowed with a structure of a Hilbert algebra with respect to the ⋆-multiplication. The most important result of the paper shows that developed formalism is more fundamental then the axiomatic ordinary quantum mechanics which appears in the presented approach as the intrinsic element of the general formalism. -
Turbulence, Entropy and Dynamics
TURBULENCE, ENTROPY AND DYNAMICS Lecture Notes, UPC 2014 Jose M. Redondo Contents 1 Turbulence 1 1.1 Features ................................................ 2 1.2 Examples of turbulence ........................................ 3 1.3 Heat and momentum transfer ..................................... 4 1.4 Kolmogorov’s theory of 1941 ..................................... 4 1.5 See also ................................................ 6 1.6 References and notes ......................................... 6 1.7 Further reading ............................................ 7 1.7.1 General ............................................ 7 1.7.2 Original scientific research papers and classic monographs .................. 7 1.8 External links ............................................. 7 2 Turbulence modeling 8 2.1 Closure problem ............................................ 8 2.2 Eddy viscosity ............................................. 8 2.3 Prandtl’s mixing-length concept .................................... 8 2.4 Smagorinsky model for the sub-grid scale eddy viscosity ....................... 8 2.5 Spalart–Allmaras, k–ε and k–ω models ................................ 9 2.6 Common models ........................................... 9 2.7 References ............................................... 9 2.7.1 Notes ............................................. 9 2.7.2 Other ............................................. 9 3 Reynolds stress equation model 10 3.1 Production term ............................................ 10 3.2 Pressure-strain interactions -
Canonical Quantization of the Self-Dual Model Coupled to Fermions∗
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server Canonical Quantization of the Self-Dual Model coupled to Fermions∗ H. O. Girotti Instituto de F´ısica, Universidade Federal do Rio Grande do Sul Caixa Postal 15051, 91501-970 - Porto Alegre, RS, Brazil. (March 1998) Abstract This paper is dedicated to formulate the interaction picture dynamics of the self-dual field minimally coupled to fermions. To make this possible, we start by quantizing the free self-dual model by means of the Dirac bracket quantization procedure. We obtain, as result, that the free self-dual model is a relativistically invariant quantum field theory whose excitations are identical to the physical (gauge invariant) excitations of the free Maxwell-Chern-Simons theory. The model describing the interaction of the self-dual field minimally cou- pled to fermions is also quantized through the Dirac-bracket quantization procedure. One of the self-dual field components is found not to commute, at equal times, with the fermionic fields. Hence, the formulation of the in- teraction picture dynamics is only possible after the elimination of the just mentioned component. This procedure brings, in turns, two new interac- tions terms, which are local in space and time while non-renormalizable by power counting. Relativistic invariance is tested in connection with the elas- tic fermion-fermion scattering amplitude. We prove that all the non-covariant pieces in the interaction Hamiltonian are equivalent to the covariant minimal interaction of the self-dual field with the fermions. The high energy behavior of the self-dual field propagator corroborates that the coupled theory is non- renormalizable. -
Weyl Quantization and Wigner Distributions on Phase Space
faculteit Wiskunde en Natuurwetenschappen Weyl quantization and Wigner distributions on phase space Bachelor thesis in Physics and Mathematics June 2014 Student: R.S. Wezeman Supervisor in Physics: Prof. dr. D. Boer Supervisor in Mathematics: Prof. dr H. Waalkens Abstract This thesis describes quantum mechanics in the phase space formulation. We introduce quantization and in particular the Weyl quantization. We study a general class of phase space distribution functions on phase space. The Wigner distribution function is one such distribution function. The Wigner distribution function in general attains negative values and thus can not be interpreted as a real probability density, as opposed to for example the Husimi distribution function. The Husimi distribution however does not yield the correct marginal distribution functions known from quantum mechanics. Properties of the Wigner and Husimi distribution function are studied to more extent. We calculate the Wigner and Husimi distribution function for the energy eigenstates of a particle trapped in a box. We then look at the semi classical limit for this example. The time evolution of Wigner functions are studied by making use of the Moyal bracket. The Moyal bracket and the Poisson bracket are compared in the classical limit. The phase space formulation of quantum mechanics has as advantage that classical concepts can be studied and compared to quantum mechanics. For certain quantum mechanical systems the time evolution of Wigner distribution functions becomes equivalent to the classical time evolution stated in the exact Egerov theorem. Another advantage of using Wigner functions is when one is interested in systems involving mixed states. A disadvantage of the phase space formulation is that for most problems it quickly loses its simplicity and becomes hard to calculate. -
Matrix Bases for Star Products: a Review?
Symmetry, Integrability and Geometry: Methods and Applications SIGMA 10 (2014), 086, 36 pages Matrix Bases for Star Products: a Review? Fedele LIZZI yzx and Patrizia VITALE yz y Dipartimento di Fisica, Universit`adi Napoli Federico II, Napoli, Italy E-mail: [email protected], [email protected] z INFN, Sezione di Napoli, Italy x Institut de Ci´enciesdel Cosmos, Universitat de Barcelona, Catalonia, Spain Received March 04, 2014, in final form August 11, 2014; Published online August 15, 2014 http://dx.doi.org/10.3842/SIGMA.2014.086 Abstract. We review the matrix bases for a family of noncommutative ? products based on a Weyl map. These products include the Moyal product, as well as the Wick{Voros products and other translation invariant ones. We also review the derivation of Lie algebra type star products, with adapted matrix bases. We discuss the uses of these matrix bases for field theory, fuzzy spaces and emergent gravity. Key words: noncommutative geometry; star products; matrix models 2010 Mathematics Subject Classification: 58Bxx; 40C05; 46L65 1 Introduction Star products were originally introduced [34, 62] in the context of point particle quantization, they were generalized in [9, 10] to comprise general cases, the physical motivations behind this was the quantization of phase space. Later star products became a tool to describe possible noncommutative geometries of spacetime itself (for a review see [4]). In this sense they have become a tool for the study of field theories on noncommutative spaces [77]. In this short review we want to concentrate on one particular aspect of the star product, the fact that any action involving fields which are multiplied with a star product can be seen as a matrix model. -
A Functorial Construction of Quantum Subtheories
entropy Article A Functorial Construction of Quantum Subtheories Ivan Contreras 1 and Ali Nabi Duman 2,* 1 Department of Mathematics, University of Illinois at Urbana-Champain, Urbana, IL 61801, USA; [email protected] 2 Department of Mathematics and Statistics, King Fahd University of Petroleum and Minerals, Dhahran 31261, Saudi Arabia * Correspondence: [email protected]; Tel.: +966-138-602-632 Academic Editors: Giacomo Mauro D’Ariano, Andrei Khrennikov and Massimo Melucci Received: 2 March 2017; Accepted: 4 May 2017; Published: 11 May 2017 Abstract: We apply the geometric quantization procedure via symplectic groupoids to the setting of epistemically-restricted toy theories formalized by Spekkens (Spekkens, 2016). In the continuous degrees of freedom, this produces the algebraic structure of quadrature quantum subtheories. In the odd-prime finite degrees of freedom, we obtain a functor from the Frobenius algebra of the toy theories to the Frobenius algebra of stabilizer quantum mechanics. Keywords: categorical quantum mechanics; geometric quantization; epistemically-restricted theories; Frobenius algebras 1. Introduction The aim of geometric quantization is to construct, using the geometry of the classical system, a Hilbert space and a set of operators on that Hilbert space that give the quantum mechanical analogue of the classical mechanical system modeled by a symplectic manifold [1–3]. Starting with a symplectic space M corresponding to the classical phase space, the square integrable functions over M is the first Hilbert space in the construction, called the prequantum Hilbert space. In this case, the classical observables are mapped to the operators on this Hilbert space, and the Poisson bracket is mapped to the commutator. -
An Extension of the Dirac and Gotay-Nester Theories of Constraints for Dirac Dynamical Systems
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Servicio de Difusión de la Creación Intelectual An extension of the Dirac and Gotay-Nester theories of constraints for Dirac dynamical systems Hern´anCendraa;1, Mar´ıaEtchechouryb and Sebasti´anJ. Ferraroc a Departamento de Matem´atica Universidad Nacional del Sur, Av. Alem 1253 8000 Bah´ıaBlanca and CONICET, Argentina. [email protected] b Laboratorio de Electr´onicaIndustrial, Control e Instrumentaci´on, Facultad de Ingenier´ıa,Universidad Nacional de La Plata and Departamento de Matem´atica, Facultad de Ciencias Exactas, Universidad Nacional de La Plata. CC 172, 1900 La Plata, Argentina. [email protected] c Departamento de Matem´aticaand Instituto de Matem´aticaBah´ıaBlanca Universidad Nacional del Sur, Av. Alem 1253 8000 Bah´ıaBlanca, and CONICET, Argentina [email protected] Abstract This paper extends the Gotay-Nester and the Dirac theories of constrained systems in order to deal with Dirac dynamical systems in the integrable case. In- tegrable Dirac dynamical systems are viewed as constrained systems where the constraint submanifolds are foliated, the case considered in Gotay-Nester theory being the particular case where the foliation has only one leaf. A Constraint Al- gorithm for Dirac dynamical systems (CAD), which extends the Gotay-Nester algorithm, is developed. Evolution equations are written using a Dirac bracket adapted to the foliations and an abridged total energy which coincides with the total Hamiltonian in the particular case considered by Dirac. The interesting example of LC circuits is developed in detail. The paper emphasizes the point of view that Dirac and Gotay-Nester theories are dual and that using a com- bination of results from both theories may have advantages in dealing with a given example, rather than using systematically one or the other. -
University of Groningen Hamiltonian Formulation of the Supermembrane
University of Groningen Hamiltonian formulation of the supermembrane Bergshoeff, E.; Sezgin, E.; Tanii, Y. Published in: Nuclear Physics B DOI: 10.1016/0550-3213(88)90309-4 IMPORTANT NOTE: You are advised to consult the publisher's version (publisher's PDF) if you wish to cite from it. Please check the document version below. Document Version Publisher's PDF, also known as Version of record Publication date: 1988 Link to publication in University of Groningen/UMCG research database Citation for published version (APA): Bergshoeff, E., Sezgin, E., & Tanii, Y. (1988). Hamiltonian formulation of the supermembrane. Nuclear Physics B, 298(1). https://doi.org/10.1016/0550-3213(88)90309-4 Copyright Other than for strictly personal use, it is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), unless the work is under an open content license (like Creative Commons). Take-down policy If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. Downloaded from the University of Groningen/UMCG research database (Pure): http://www.rug.nl/research/portal. For technical reasons the number of authors shown on this cover page is limited to 10 maximum. Download date: 24-09-2021 Nuclear Physics B298 (1988) 187-204 North-Holland, Amsterdam HAMILTONIAN FORMULATION OF THE SUPERMEMBRANE E. BERGSHOEFF*, E. SEZGIN and Y. TAN11 International Centre for Theoretical Physics, Trieste, It& Received 15 June 1987 The hamiltonian formulation of the supermembrane theory in eleven dimensions is given. -
Abstracts for 18 Category Theory; Homological 62 Statistics Algebra 65 Numerical Analysis Syracuse, October 2–3, 2010
A bstr bstrActs A A cts mailing offices MATHEMATICS and additional of Papers Presented to the Periodicals postage 2010 paid at Providence, RI American Mathematical Society SUBJECT CLASSIFICATION Volume 31, Number 4, Issue 162 Fall 2010 Compiled in the Editorial Offices of MATHEMATICAL REVIEWS and ZENTRALBLATT MATH 00 General 44 Integral transforms, operational calculus 01 History and biography 45 Integral equations Editorial Committee 03 Mathematical logic and foundations 46 Functional analysis 05 Combinatorics 47 Operator theory Robert J. Daverman, Chair Volume 31 • Number 4 Fall 2010 Volume 06 Order, lattices, ordered 49 Calculus of variations and optimal Georgia Benkart algebraic structures control; optimization 08 General algebraic systems 51 Geometry Michel L. Lapidus 11 Number theory 52 Convex and discrete geometry Matthew Miller 12 Field theory and polynomials 53 Differential geometry 13 Commutative rings and algebras 54 General topology Steven H. Weintraub 14 Algebraic geometry 55 Algebraic topology 15 Linear and multilinear algebra; 57 Manifolds and cell complexes matrix theory 58 Global analysis, analysis on manifolds 16 Associative rings and algebras 60 Probability theory and stochastic 17 Nonassociative rings and algebras processes Abstracts for 18 Category theory; homological 62 Statistics algebra 65 Numerical analysis Syracuse, October 2–3, 2010 ....................... 655 19 K-theory 68 Computer science 20 Group theory and generalizations 70 Mechanics of particles and systems Los Angeles, October 9–10, 2010 .................. 708 22 Topological groups, Lie groups 74 Mechanics of deformable solids 26 Real functions 76 Fluid mechanics 28 Measure and integration 78 Optics, electromagnetic theory Notre Dame, November 5–7, 2010 ................ 758 30 Functions of a complex variable 80 Classical thermodynamics, heat transfer 31 Potential theory 81 Quantum theory Richmond, November 6–7, 2010 ..................