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Lecture Notes in Mathematics Editors: J.-M Morel, Cachan F Takens, Groningen B Teissier, Paris 1887 K Habermann · L Habermann Introduction to Symplectic Dirac Operators ABC Authors Katharina Habermann State and University Library Göttingen Platz der Göttinger Sieben 37073 Göttingen Germany e-mail: habermann@sub.uni-goettingen.de Lutz Habermann Department of Mathematics University of Hannover Welfengarten 30167 Hannover Germany e-mail: habermann@math.uni-hannover.de Library of Congress Control Number: 2006924i23 Mathematics Subject Classification (2000): 53-02, 53Dxx, 58-02, 58Jxx ISSN print edition: 0075-8434 ISSN electronic edition: 1617-9692 ISBN-10 3-540-33420-3 Springer Berlin Heidelberg New York ISBN-13 978-3-540-33420-0 Springer Berlin Heidelberg New York DOI 10.1007/b138212 This work is subject to copyright All rights are reserved, whether the whole or part of the material is concerned, specifically the rights of translation, reprinting, reuse of illustrations, recitation, broadcasting, reproduction on microfilm or in any other way, and storage in data banks Duplication of this publication or parts thereof is permitted only under the provisions of the German Copyright Law of September 9, 1965, in its current version, and permission for use must always be obtained from Springer Violations are liable for prosecution under the German Copyright Law Springer is a part of Springer Science+Business Media springer.com c Springer-Verlag Berlin Heidelberg 2006 Printed in The Netherlands The use of general descriptive names, registered names, trademarks, etc in this publication does not imply, even in the absence of a specific statement, that such names are exempt from the relevant protective laws and regulations and therefore free for general use A EX package Typesetting: by the authors and SPI Publisher Services using a Springer LT Cover design: design & production GmbH, Heidelberg Printed on acid-free paper SPIN: 11736684 V A 41/3100/ SPI 543210 To Karen Preface This book aims to give a systematic and self-contained introduction to the theory of symplectic Dirac operators and to reflect the current state of the subject At the same time, it is intended to establish the idea that symplectic spin geometry and symplectic Dirac operators may give valuable tools in symplectic geometry and symplectic topology, which have become important fields and very active areas of mathematical research The basic idea of symplectic spin geometry goes back to the early 1970s, when Bertram Kostant introduced symplectic spinors in order to give the construction of the half-form bundle and the half-form pairings in the context of geometric quantization [37] During the next two decades, however, almost no attention has been given to a closer study of symplectic spin geometry itself In 1995, the first author introduced symplectic Dirac operators [24] and started a systematical investigation [25, 26, 27] These symplectic Dirac operators are called Dirac operators, since they are defined in an analogous way as the classical Riemannian Dirac operator known from Riemannian spin geometry (cf e.g [21]) They are called symplectic because they are constructed by use of the symplectic setting of the underlying symplectic manifold All tools which were necessary for that construction have already been known and accepted, mainly in mathematical physics These are the symplectic Clifford algebra (also known as Weyl algebra), the metaplectic group, the metaplectic representation (Segal–Shale–Weil representation) acting on L2 (Rn ), metaplectic structures, and symplectic connections One of the basic ideas in differential geometry is that the study of analytic properties of certain differential operators acting on sections of vector bundles yields geometric and topological properties of the underlying base manifold There are several classical results in that direction An example is Hodge– de Rham theory Here, one considers the Hodge–Laplace–Beltrami operator ∆ VIII Preface acting on differential forms This operator is one of the most studied operators in global Riemannian geometry and his spectrum gives important topological invariants In particular, the dimension of the kernel of ∆ on p-forms over a closed Riemannian manifold is the p-th Betti number Other well known and well studied operators are the Kodaira–Hodge–Laplace operator on differential forms with values in a holomorphic vector bundle or the classical Dirac operator on Riemannian manifolds Now, symplectic spinor fields are sections in an L2 (Rn )-Hilbert space bundle over a symplectic manifold and symplectic Dirac operators, acting on symplectic spinor fields, are associated to the symplectic manifold in a very natural way Hence they may be expected to give interesting applications in symplectic geometry and symplectic topology It is our opinion that, besides the already stated, there are further close relations to mathematical physics Some steps towards this direction have been made by the first author and Andreas Klein in [28, 29, 30] Another perspective could be the extension of Clifford analysis and spin geometry to super differential geometry According to the most used version of super geometry developed by Bertram Kostant, geometrical structures over a supermanifold consist of Z2 -graded objects and thus have an even as well as an odd part Then one can imagine that a metric has to satisfy some kind of graded symmetry which, roughly speaking, corresponds to a symmetric object on the even part as well as to a skew symmetric object on the odd part of the supermanifold For the first one, we have the classical Riemannian spin geometry, whereas the second one is basically given by symplectic spin geometry The main aspects of that idea are treated in a paper by Frank Sommen [45] Although the construction of symplectic Dirac operators follows the same procedure as for the classical Riemannian Dirac operator, using the symplectic structure of the underlying manifold instead of the Riemannian metric, there are essential differences to the Riemannian case These are caused by the fact that the algebraic structure of the symplectic Clifford algebra is completely different from that of Riemannian spin geometry For the classical Clifford algebra, we have the relation v2 = − v , whereas the algebraic structure of the symplectic Clifford algebra is given by v · w − w · v = −ω0 (v, w) This implies essentially different properties for the Clifford multiplications, which enter into the definition of the Dirac operators Moreover, the non-compactness of the symplectic group leads to analytic difficulties Namely, since the typical fiber of the symplectic spinor bundle is the Hilbert space L2 (Rn ), we deal with operators acting on sections of a vector bundle of infinite rank For elliptic formally self-adjoint pseudo-differential operators with positive definite leading symbol acting on sections in a vector bundle of finite rank, one has a completely developed theory So, in order to be able to apply these techniques, we are interested in equivariance properties Preface IX of our operators with respect to a certain decomposition of the symplectic spinor bundle into a series of subbundles of finite rank It turns out that an associated second order operator respects this decomposition provided that a technical assumption, which always can be realized, holds true Let us now briefly describe the content of each chapter of this book The first chapter is introductory It contains preliminaries and basic material needed for our considerations Chapter is devoted to symplectic connections In particular, we introduce a further Ricci tensor, which we will call symplectic Ricci tensor To our knowledge, no attention has been given to this tensor in previous studies In fact, this symplectic Ricci tensor is a new object in the case of non-vanishing torsion To date, mostly only torsion-free symplectic connections have been considered It turns out that, in our context, it is convenient to work also with symplectic connections with torsion and that the symplectic Ricci tensor is more suitable for our purposes The next chapter introduces the symplectic spinor bundle and the spinor derivative and analyzes a splitting property of the spinor bundle In Chapter 4, we give the definition of symplectic Dirac operators and describe in detail how these operators depend on the objects from which they are built Chapter is concerned with an associated second order operator of Laplace type and addresses properties of this operator The objective of Chapter is the situation for a special class of symplectic manifolds, namely Kă ahler manifolds Here, we also investigate the example of CP The aim of Chapter is to construct a Fourier transform for symplectic spinor fields and to derive consequences for the symplectic Dirac operators The last chapter focuses on relations to mathematical physics, in particular to quantization This closes the circle to the beginnings by Bertram Kostant The present text is originated in research ideas of the first author and provides an extended version of her “Habilitationsschrift”, which was never published separately Starting with helpful discussions from the beginning of the investigations and proposing many improvements in the selection and presentation of the material, the second author became more and more involved into the subject We decided to write this book tree years ago and, for this book, he made a thorough revision of the material, in particular, to improve the strictness of the presentation Then it took time to compose it in a natural and organic way Furthermore, our working places are no longer as close to each other as before and it became difficult to keep our discussions at its intensive level Now we consider the text ready for publication and hope to present the reader a mature work During the work on the book, we received financial support from DFG, the German Research Foundation, contract HA 3056/1-1,2 Many thanks are due to our students Paul Rosenthal and Steffen Rudnick for proof-reading the LATEX-type-written manuscript X Preface We dedicate this book to our daughter Karen She accepts our mathematical family circle and enriches it with her interest We are grateful to being able to give her an understanding of the fascination of mathematics Karen, you are a wonderful teenager which makes us enjoying the challenge of teaching mathematics Gă ottingen and Greifswald, November 2004 Katharina & Lutz Habermann Contents Background on Symplectic Spinors 1.1 Symplectic Group and Clifford Algebra 1.2 The Stone–von Neumann Theorem 1.3 Metaplectic Representation 1.4 Symplectic Clifford Multiplication 11 1.5 Hermite Functions 16 Symplectic Connections 21 2.1 Symplectic Manifolds 21 2.2 Constructions and Torsion 25 2.3 Symplectic Curvature and Ricci Tensors 29 Symplectic Spinor Fields 35 3.1 Metaplectic Structures 35 3.2 Symplectic Spinor Bundle 37 3.3 Splitting of the Spinor Bundle 43 Symplectic Dirac Operators 49 4.1 Definition of the Operators 49 4.2 Dependence on the Symplectic Connection 52 4.3 Dependence on the Metaplectic Structure 57 4.4 Dependence on the Almost Complex Structure 62 4.5 Formal Self-Adjointness 64 XII Contents An Associated Second Order Operator 67 5.1 Definition and Ellipticity 67 5.2 A Weitzenbă ock Formula 68 5.3 Splitting of the Operator 74 The Kă ahler Case 81 6.1 The Operator P on Kă ahler Manifolds 81 6.2 Lower Bound Estimates 86 6.3 The Spectrum of P on CP 87 Fourier Transform for Symplectic Spinors 97 7.1 Definition of the Transform 97 7.2 Basic Properties 98 7.3 Symmetry of the Spectra of D and D 99 Lie Derivative and Quantization 101 8.1 Lie Derivative of Symplectic Spinor Fields 101 8.2 Schră odinger Equation for Quadratic Hamiltonians 109 8.3 Lie Derivative as Quantization 111 References 115 Index 119 8.2 Schră odinger Equation for Quadratic Hamiltonians 109 According to Proposition 3.2.9 and Lemma 8.1.11, i 2n ∇X ∇Jej Y · ej − ∇Y ∇Jej X · ej − ∇Jej [X, Y ] · ej · ϕ j=1 = i 2n R(X, Y )(Jej ) · ej + ∇[X,Jej ] Y · ej − ∇[Y,Jej ] X · ej · ϕ j=1 = RQ (X, Y )ϕ + i 2n ∇[X,Jej ] Y · ej − ∇[Y,Jej ] X · ej · ϕ j=1 By Lemmas 8.1.9 and 8.1.10 and the torsion-freeness of ∇, it follows that [LX , LY ]ϕ − L[X,Y ] ϕ = − i 2n ∇Jej Y · ∇X ej − ∇Jej X · ∇Y ej j=1 +∇[X,Jej ] Y · ej − ∇[Y,Jej ] X · ej · ϕ − (∇X · ∇Y · ϕ − ∇Y · ∇X · ϕ) = i 2n ∇∇X (Jej ) Y · ej − ∇∇Y (Jej ) X · ej j=1 −∇[X,Jej ] Y · ej + ∇[Y,Jej ] X · ej −∇∇Jej X Y · ej + ∇∇Jej Y X · ej · ϕ =0, and the proposition is proved 8.2 Schră odinger Equation for Quadratic Hamiltonians We consider R2n with its standard symplectic structure ω0 and a quadratic Hamiltonian u on R2n , i.e a function u : R2n → Rn defined by u(v) = Υ v, v , where Υ is any symmetric real 2n × 2n-matrix First we note that the Hamiltonian vector field Xu of u is given by an element of the Lie algebra sp(n, R) Lemma 8.2.1 (1) One has Xu (v) = −2J0 Υ v for all v ∈ R2n 110 Lie Derivative and Quantization (2) J0 Υ and Υ J0 lie in sp(n, R) Proof Assertion (1) follows from (du)v (w) = Υ v, w = −2ω0 (J0 Υ v, w) for any v, w ∈ R2n To verify (2), use the fact that a real 2n × 2n-matrix A is an element of sp(n, R) if and only if AT J0 + J0 A = Let Hu denote the Hamilton operator associated to u via normal ordering quantization That means that n ( Υ , aj Qi ◦ Qj + Υ , bj (Qi ◦ Pj + Pj ◦ Qi ) Hu = i,j=1 + Υ b i , b j Pi ◦ Pj ) , where Qi and Pi are again the position and momentum operators Lemma 8.2.2 One has the relation i m∗ ◦ ρ−1 ∗ (Υ J0 ) = − Hu Proof By Lemma 1.3.1, ρ−1 ∗ (Υ J0 ) = = n (ai · Υ + bi · Υ bi ) i=1 n ( Υ , a j a i · a j + Υ a i , b j a i · b j i,j=1 + Υ bi , aj bi · aj + Υ bi , bj bi · bj ) n = ( Υ , aj · aj + Υ , bj (ai · bj + bj · ) i,j=1 + Υ bi , bj bi · bj ) Now apply Equation (1.4.2) Let (AΥt ) be the one parameter subgroup of Sp(n, R) generated by 2Υ J0 , i.e AΥt = exp(2tΥ J0 ) for t ∈ R, and let (qtΥ ) denote the lift of (AΥt ) to Mp(n, R) 8.3 Lie Derivative as Quantization 111 Proposition 8.2.3 For any f ∈ S(Rn ), the curve (m(qtΥ )f ) in S(Rn ) satises the Schră odinger equation d m(qtΥ )f = −iHu m(qtΥ )f dt Proof We have ρ∗ d Υ q ds s Hence = s=0 d ρ(q Υ ) ds s d Υ q ds s = s=0 d Υ A ds s = 2Υ J0 s=0 = ρ−1 ∗ (Υ J0 ) s=0 By means of Lemma 8.2.2, we get d d m(qtΥ )f = m(qsΥ )m(qtΥ )f dt ds s=0 d Υ q = m∗ m(qtΥ )f ds s s=0 Υ = m∗ ρ−1 ∗ (Υ J0 ) m(qt )f = −iHu m(qtΥ )f for any f ∈ S(Rn ) 8.3 Lie Derivative as Quantization We use the symplectic standard basis (a1 , , an , b1 , , bn ) understood as a global section of the symplectic frame bundle R of (R2n , ω0 ) to identify R2n × Sp(n, R) with R That means, we assign to (v, A) ∈ R2n × Sp(n, R) the symplectic basis (Aa1 , , Aan , Ab1 , , Abn ) of Tv R2n = R2n The metaplectic structure of (R2n , ω0 ) is then simply the product bundle P = R2n × Mp(n, R) , where the map FP : P → R is given by FP (v, q) = (v, ρ(q)) We identify R2n × L2 (Rn ) with the symplectic spinor bundle Q via (v, f ) ∈ R2n × L2 (Rn ) → v, e+ , f ∈ Q , where e+ denotes the unit element of Mp(n, R) Then sections of Q are maps ϕ : R2n → L2 (Rn ) In the next lemma, we use that elements of Sp(n, R) can also be considered as symplectomorphisms of R2n 112 Lie Derivative and Quantization Lemma 8.3.1 Let B ∈ Sp(n, R) and let qB ∈ Mp(n, R) such that ρ(qB ) = B Then one has ˜ : R → R induced by B is given by (1) The isomorphism B ˜ B(v, A) = (Bv, BA) for (v, A) ∈ R2n × Sp(n, R) ¯ : P → P defined by (2) The isomorphism B ¯ B(v, q) = (Bv, qB q) ˜ for (v, q) ∈ R2n × Mp(n, R) is a lift of B (3) It is ¯ −1 )∗ ϕ (v) = m q −1 ϕ(Bv) (B B for ϕ ∈ Γ(Q) and v ∈ R2n Proof Assertion (1) follows from (dB)v (w) = Bw for v, w ∈ R2n Assertion (2) is easily checked To see (3), first observe that the Mp(n, R)-equivariant mapping ϕˆ : P → L2 (Rn ) corresponding to ϕ ∈ Γ(Q) is given by ϕ(v, ˆ q) = m q −1 ϕ(v) for v ∈ R2n and q ∈ Mp(n, R) Hence, by (2), −1 ¯ ϕ(Bv) ϕˆ ◦ B(v, q) = m q −1 m qB This implies the stated relation We now give an interpretation of the Lie derivative in the direction of an Hamiltonian vector field in the language of normal ordering quantization For this, let f for f ∈ S(Rn ) denote the symplectic spinor field over R2n that is constantly equal to f Proposition 8.3.2 Let u be a quadratic Hamiltonian on R2n Then LXu f = −i F −1 ◦ Hu ◦ F(f ) for any f ∈ S(Rn ) Proof Let Υ , (AΥt ) and (qtΥ ) be as in Section 8.2 By Lemma 8.2.1, the flow (θt ) of the Hamiltonian vector field Xu is θt = exp(−2tJ0 Υ ) = J0 AΥ−t J0−1 8.3 Lie Derivative as Quantization 113 By Proposition 1.3.7(1) and Lemma 8.3.1, it follows that (θ¯t−1 )∗ f = F −1 ◦ m(qtΥ ) ◦ F(f ) for f ∈ S(Rn ) Now, using Proposition 8.2.3, one gets the assertion Although the above relation cannot be carried over to arbitrary manifolds, we can prove a Heisenberg relation in the general situation Proposition 8.3.3 Let (M, ω) be a symplectic manifold that admits a metaplectic structure Setting q(u)ϕ = iLXu ϕ , one has [q(u), q(v)]ϕ = −iq({u, v})ϕ for all u, v ∈ C ∞ (M ) and all symplectic spinor fields ϕ over M with respect to any metaplectic structure Proof By Propositions 2.1.9 and 8.1.8, one concludes that [q(u), q(v)]ϕ = − [LXu , LXv ] ϕ = −L[Xu ,Xv ] ϕ = LX{u,v} ϕ = −iq({u, v})ϕ References A.O Barut, R Raczka: Theory of group representations and applications 2nd rev ed Singapore: World Scientic (1986) H Baum: Spin-Strukturen und Dirac-Operatoren u ăber pseudoriemannschen Mannigfaltigkeiten Teubner-Texte zur Mathematik, Bd 41 Leipzig: BSB B G Teubner Verlagsgesellschaft (1981) N Berline, E Getzler, M Vergne: Heat Kernels and Dirac Operators Grundlehren der Mathematischen Wissenschaften 298 Berlin etc.: SpringerVerlag (1992) R.J Blattner: Some remarks on quantization Symplectic geometry and mathematical physics, Proc Colloq., Aix-en-Provence/Fr 1990, Prog Math 99, 37-47 (1991) A Borel, N Wallach: Continuous cohomology, discrete subgroups, and representations of reductive groups 2nd ed Mathematical Surveys and Monographs 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metaplectic representation and Lagrangian quantization Mathematical Research 95 Berlin: Akademie Verlag (1997) 13 C Emmrich, A Weinstein: The differential geometry of Fedosov’s quantization Brylinski, Jean-Luc (ed.) et al., Lie theory and geometry: in honor of Bertram 116 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 References Kostant on the occasion of his 65th birthday Invited papers, some originated at a symposium held at MIT, Cambridge, MA, USA in May 1993 Boston, MA: Birkhă auser Prog Math 123, 217-239 (1994) B.V Fedosov: A simple geometrical construction of deformation quantization J Differ Geom 40, No.2, 213-238 (1994) B.V Fedosov: Deformation quantization and index theory Mathematical Topics Berlin: Akademie Verlag (1996) G.B Folland: Harmonic analysis in phase space Annals of Mathematics Studies, 122 Princeton, NJ: Princeton University Press (1989) M Forger, H Hess: Universal metaplectic structures and geometric quantization Commun Math Phys 64, 269-278 (1979) Th 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13, 155-168 (1995) K Habermann: Basic Properties of Symplectic Dirac Operators Commun Math Phys 184, 629-652 (1997) K Habermann: Harmonic Symplectic Spinors on Riemann Surfaces Manuscr Math 94, 465-484 (1997) K Habermann: Symplectic Dirac Operators on Kă ahler Manifolds Math Nachr 211, 37-62 (2000) K Habermann: An M pC -spinorial approach to a geometric-type quantization for symplectic manifolds Gesztesy, Fritz (ed.) et al., Stochastic processes, physics and geometry: New interplays II A volume in honor of Sergio Albeverio Proceedings of the conference on infinite dimensional (stochastic) analysis and quantum physics, Leipzig, Germany, January 18-22, 1999 Providence, RI: American Mathematical Society (AMS) CMS Conf Proc 29, 259-268 (2000) K Habermann, A Klein: A Fourier transform for symplectic spinors and applications Preprint, Greifswald University (2002) K Habermann, A Klein: Lie derivative of symplectic spinor fields, metaplectic representation, and quantization Rostocker Math Kolloq 57, 71-91 (2003) H Hofer, E Zehnder: Symplectic invariants and Hamiltonian dynamics Birkhă auser Advanced Texts Basel: Birkhă auser (1994) M Kashiwara, M Vergne: On the Segal-Shale-Weil representations and harmonic polynomials Invent Math 44, 1-47 (1978) References 117 33 A.A Kirillov: Geometric quantization Dynamical systems IV Symplectic geometry and its applications, Encycl Math Sci 4, 137-172 (1990); translation from Itogi Nauki Tekh., Ser Sovrem Probl Mat., Fundam Napravleniya 4, 141-178 (1985) 34 A Klein: Eine Fouriertransformation fă ur symplektische Spinoren und Anwendungen in der Quantisierung Diploma Thesis, Technische Universită at Berlin (2000) 35 S Kobayashi, K Nomizu: Foundations of differential geometry I New YorkLondon: Interscience Publishers, a division of John Wiley & Sons XI (1963) 36 S Kobayashi, K Nomizu: Foundations of Differential Geometry Vol II New York-London-Sydney: Interscience Publishers a division of John Wiley and Sons (1969) 37 B Kostant: Symplectic Spinors Symp math 14, Geom simplett., Fis mat., Teor geom Integr Var minim., Convegni 1973, 139-152 (1974) 38 A Lichnerowicz: Spineurs harmoniques C R Acad Sci., Paris 257, 7-9 (1963) 39 D McDuff, D Salamon: Introduction to symplectic topology Oxford Mathematical Monographs Oxford: Clarendon Press (1995) 40 I Niven, H.S Zuckerman: An introduction to the theory of numbers 3rd ed New York etc.: John Wiley & Sons, Inc XII (1972) 41 M.J Pflaum: The normal symbol on Riemannian manifolds New York J Math 4, 97-125, electronic only (1998) 42 P.L Robinson, J.H Rawnsley: The metaplectic representation, M pc structures and geometric quantization Mem Am Math Soc 410 (1989) 43 E Schră odinger: Diracsches Elektron im Schwerefeld I Sitzungsber Preuß Akad Wiss., Phys.-Math Kl 1932, No 11/12, 105-128 (1932) 44 M Shubin: A sequence of connections and a characterization of Kă ahler manifolds Farber, Michael (ed.) et al., Tel Aviv topology conference: Rothenberg Festschrift Proceedings of the international conference on topology, Tel Aviv, Israel, June 1-5, 1998 dedicated to Mel Rothenberg on the occasion of his 65th birthday Providence, RI: American Mathematical Society Contemp Math 231, 265-270 (1999) 45 F Sommen: An extension of Clifford analysis towards super-symmetry Ryan, John (ed.) et al., Clifford algebras and their applications in mathematical physics Papers of the 5th international conference, Ixtapa-Zihuatanejo, Mexico, June 27-July 4, 1999 Volume 2: Clifford analysis Boston, MA: Birkhă auser Prog Phys 19, 199-224 (2000) 46 Ph Tondeur: Ane Zusammenhă ange auf Mannigfaltigkeiten mit fast-symplektischer Struktur Comment Math Helv 36, 234-244 (1961) 47 I Vaisman: Symplectic curvature tensors Monatsh Math 100, 299-327 (1985) 48 N.R Wallach: Harmonic Analysis on Homogeneous Spaces Pure and Applied Mathematics 19 New York: Marcel Dekker, Inc (1973) 49 N.R Wallach: Symplectic Geometry and Fourier Analysis With an appendix on quantum mechanics by Robert Hermann Lie Groups: History, Frontiers and Applications Vol V Brookline, Mass.: Math Sci Press (1977) 50 A Weil: Sur certains groupes d’op´ erateurs unitaires Acta Math 111, 143-211 (1964) 51 N.M.J Woodhouse: Geometric quantization 2nd ed Oxford Mathematical Monographs Oxford: Clarendon Press (1997) 52 Ch Wyss: Symplektische Diracoperatoren auf dem komplexen projektiven Raum Diploma Thesis, Universită at Bremen (2003) 118 References ˇ 53 D.P Zelobenko: Compact Lie Groups and their representations Translated from the Russian by Israel Program for Scientific Translations Translations of Mathematical Monographs Vol 40 Providence, R.I.: American Mathematical Society (AMS) VIII (1973) Index almost complex structure, 23 ω-compatible, 23 anti-canonical line bundle, 46 Baum, 49 Bianchi identity, 29 Bourgeois, 21 Cahen, 21 Casimir operator, 90 Cauchy–Riemann equation generalized, 79 Chern class first, 36 complex projective space, 36, 87, 92 complex torus, 85 connection canonical, 90 Hermitian, 27 Levi–Civita, 34, 81 symplectic, 25 reducible, 33 torsion-free, 27 cotangent bundle, 22, 36 curvature, 29 of the spinor derivative, 42 Darboux theorem, 22 deformation of metaplectic structures, 58 divergence, 27 Einstein manifold, 84 Fedosov, 21 flow, 102, 112 formally self-adjoint, 64, 66, 81 Fourier transform, for symplectic spinors, 97 Friedrich, 49 Frobenius reciprocity, 91, 92 Fubini–Study metric, 36, 88 G˚ arding, Gelfand, 21 Gutt, 21 Hamiltonian quadratic, 109 vector field, 24 harmonic oscillator, 17 Heisenberg group, relation, 113 Hermite function, 17, 89 Hermitian connection, 27 structure, 39 holomorphic sectional curvature constant, 33, 84, 94 invariant subspace, Kă ahler form, 22, 81 manifold, 22, 81 Lie derivative, 102 120 Index of symplectic spinor fields, 103 metaplectic group, representation, 10 differential of, 14 structure, 35 momentum operator, 11 normal ordering quantization, 110, 112 orthogonal group, Pell’s equation, 95 Poisson bracket, 24 position operator, 11 quadratic Hamiltonian, 109 quantization, 97, 101 normal ordering, 110, 112 Rawnsley, 21 representation, adjoint, 88 differential of, equivalent, unitary, irreducible, isotropy, 88 metaplectic, 10 differential of, 14 projective unitary, unitary, Retakh, 21 Ricci tensor, 31 symplectic, 31 scalar curvature, 34 symplectic, 34 Schră odinger equation, 111 representation, Schur’s lemma, 5, 93 Schwartz space, sectional curvature, 84 holomorphic, 33, 84 Segal–Shale–Weil representation, 10 Shubin, 21 smooth section, 37 vector, spectrum, 93, 100 spinor derivative, 39 curvature of, 42 Stiefel–Whitney class first, 36 second, 36 Stone–von Neumann theorem, symmetric space, 88 symplectic basis, 1, 23 Clifford algebra, multiplication, 13, 38 connection, 25 curvature tensor, 29 Dirac operator, 50 form, frame, 23 frame bundle, 23 gradient, 24 group, Lie algebra, manifold, 22 Ricci tensor, 31 scalar curvature, 34 spinor, 10 bundle, 37 field, 37 Laplacian, 70 structure, 22 vector field, 102 symplectomorphic, 22 symplectomorphism, 22 Tondeur, 21 torsion, 27 vector field, 27 unitary frame, 24 group, Vaisman, 21 vector field Hamiltonian, 24 symplectic, 102 volume element, 28 weight, 90, 92 Weil, Weitzenbă ock formula, 72, 82 Weyl algebra, Lecture Notes in Mathematics For information about earlier volumes please contact your bookseller or Springer LNM Online archive: springerlink.com Vol 1681: G J Wirsching, The Dynamical System Generated by the 3n+1 Function (1998) Vol 1682: H.-D Alber, Materials with Memory (1998) Vol 1683: A Pomp, The Boundary-Domain Integral Method for Elliptic Systems (1998) Vol 1684: C A Berenstein, P F Ebenfelt, S G Gindikin, S Helgason, A E Tumanov, Integral Geometry, Radon Transforms and Complex Analysis Firenze, 1996 Editors: E Casadio Tarabusi, M A Picardello, G Zampieri (1998) Vol 1685: S König, A Zimmermann, Derived Equivalences for Group Rings (1998) Vol 1686: J Azéma, M Émery, M Ledoux, M Yor (Eds.), Séminaire de Probabilités XXXII (1998) Vol 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(2001) Vol 1638: P Vanhaecke, Integrable Systems in the realm of Algebraic Geometry 1996 – Second Edition (2001) Vol 1702: J Ma, J Yong, Forward-Backward Stochastic Differential Equations and their Applications 1999 – Corrected 3rd printing (2005) .. .K Habermann · L Habermann Introduction to Symplectic Dirac Operators ABC Authors Katharina Habermann State and University Library Göttingen Platz... 11736684 V A 41/3100/ SPI 543210 To Karen Preface This book aims to give a systematic and self-contained introduction to the theory of symplectic Dirac operators and to reflect the current state of... (1.5.8) Symplectic Connections In order to define symplectic Dirac operators, we have to fix a symplectic connection on the underlying symplectic manifold Every symplectic manifold admits symplectic