The First and Second Stiefel-Whitney Classes; Orientation and Spin Structure
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Diagonal Lifts of Metrics to Coframe Bundle
Proceedings of the Institute of Mathematics and Mechanics, National Academy of Sciences of Azerbaijan Volume 44, Number 2, 2018, Pages 328{337 DIAGONAL LIFTS OF METRICS TO COFRAME BUNDLE HABIL FATTAYEV AND ARIF SALIMOV Abstract. In this paper the diagonal lift Dg of a Riemannian metric g ∗ of a manifold Mn to the coframe bundle F (Mn) is defined, Levi-Civita connection, Killing vector fields with respect to the metric Dg and also an almost paracomplex structures in the coframe bundle are studied. 1. Introduction The Riemannian metrics in the tangent bundle firstly has been investigated by the Sasaki [14]. Tondeur [16] and Sato [15] have constructed Riemannian metrics on the cotangent bundle, the construction being the analogue of the metric Sasaki for the tangent bundle. Mok [7] has defined so-called the diagonal lift of metric to the linear frame bundle, which is a Riemannian metric resembles the Sasaki metric of tangent bundle. Some properties and applications for the Riemannian metrics of the tangent, cotangent, linear frame and tensor bundles are given in [1-4,7-9,12,13]. This paper is devoted to the investigation of Riemannian metrics in the coframe bundle. In 2 we briefly describe the definitions and results that are needed later, after which the diagonal lift Dg of a Riemannian metric g is constructed in 3. The Levi-Civita connection of the metric Dg is determined in In 4. In 5 we consider Killing vector fields in coframe bundle with respect to Riemannian metric Dg. An almost paracomplex structures in the coframe bundle equipped with metric Dg are studied in 6. -
The Jouanolou-Thomason Homotopy Lemma
The Jouanolou-Thomason homotopy lemma Aravind Asok February 9, 2009 1 Introduction The goal of this note is to prove what is now known as the Jouanolou-Thomason homotopy lemma or simply \Jouanolou's trick." Our main reason for discussing this here is that i) most statements (that I have seen) assume unncessary quasi-projectivity hypotheses, and ii) most applications of the result that I know (e.g., in homotopy K-theory) appeal to the result as merely a \black box," while the proof indicates that the construction is quite geometric and relatively explicit. For simplicity, throughout the word scheme means separated Noetherian scheme. Theorem 1.1 (Jouanolou-Thomason homotopy lemma). Given a smooth scheme X over a regular Noetherian base ring k, there exists a pair (X;~ π), where X~ is an affine scheme, smooth over k, and π : X~ ! X is a Zariski locally trivial smooth morphism with fibers isomorphic to affine spaces. 1 Remark 1.2. In terms of an A -homotopy category of smooth schemes over k (e.g., H(k) or H´et(k); see [MV99, x3]), the map π is an A1-weak equivalence (use [MV99, x3 Example 2.4]. Thus, up to A1-weak equivalence, any smooth k-scheme is an affine scheme smooth over k. 2 An explicit algebraic form Let An denote affine space over Spec Z. Let An n 0 denote the scheme quasi-affine and smooth over 2m Spec Z obtained by removing the fiber over 0. Let Q2m−1 denote the closed subscheme of A (with coordinates x1; : : : ; x2m) defined by the equation X xixm+i = 1: i Consider the following simple situation. -
Vector Bundles on Projective Space
Vector Bundles on Projective Space Takumi Murayama December 1, 2013 1 Preliminaries on vector bundles Let X be a (quasi-projective) variety over k. We follow [Sha13, Chap. 6, x1.2]. Definition. A family of vector spaces over X is a morphism of varieties π : E ! X −1 such that for each x 2 X, the fiber Ex := π (x) is isomorphic to a vector space r 0 0 Ak(x).A morphism of a family of vector spaces π : E ! X and π : E ! X is a morphism f : E ! E0 such that the following diagram commutes: f E E0 π π0 X 0 and the map fx : Ex ! Ex is linear over k(x). f is an isomorphism if fx is an isomorphism for all x. A vector bundle is a family of vector spaces that is locally trivial, i.e., for each x 2 X, there exists a neighborhood U 3 x such that there is an isomorphism ': π−1(U) !∼ U × Ar that is an isomorphism of families of vector spaces by the following diagram: −1 ∼ r π (U) ' U × A (1.1) π pr1 U −1 where pr1 denotes the first projection. We call π (U) ! U the restriction of the vector bundle π : E ! X onto U, denoted by EjU . r is locally constant, hence is constant on every irreducible component of X. If it is constant everywhere on X, we call r the rank of the vector bundle. 1 The following lemma tells us how local trivializations of a vector bundle glue together on the entire space X. -
Notes on the Atiyah-Singer Index Theorem Liviu I. Nicolaescu
Notes on the Atiyah-Singer Index Theorem Liviu I. Nicolaescu Notes for a topics in topology course, University of Notre Dame, Spring 2004, Spring 2013. Last revision: November 15, 2013 i The Atiyah-Singer Index Theorem This is arguably one of the deepest and most beautiful results in modern geometry, and in my view is a must know for any geometer/topologist. It has to do with elliptic partial differential opera- tors on a compact manifold, namely those operators P with the property that dim ker P; dim coker P < 1. In general these integers are very difficult to compute without some very precise information about P . Remarkably, their difference, called the index of P , is a “soft” quantity in the sense that its determination can be carried out relying only on topological tools. You should compare this with the following elementary situation. m n Suppose we are given a linear operator A : C ! C . From this information alone we cannot compute the dimension of its kernel or of its cokernel. We can however compute their difference which, according to the rank-nullity theorem for n×m matrices must be dim ker A−dim coker A = m − n. Michael Atiyah and Isadore Singer have shown in the 1960s that the index of an elliptic operator is determined by certain cohomology classes on the background manifold. These cohomology classes are in turn topological invariants of the vector bundles on which the differential operator acts and the homotopy class of the principal symbol of the operator. Moreover, they proved that in order to understand the index problem for an arbitrary elliptic operator it suffices to understand the index problem for a very special class of first order elliptic operators, namely the Dirac type elliptic operators. -
Fermionic Finite-Group Gauge Theories and Interacting Symmetric
Fermionic Finite-Group Gauge Theories and Interacting Symmetric/Crystalline Orders via Cobordisms Meng Guo1;2;3, Kantaro Ohmori4, Pavel Putrov4;5, Zheyan Wan6, Juven Wang4;7 1Department of Mathematics, Harvard University, Cambridge, MA 02138, USA 2Perimeter Institute for Theoretical Physics, Waterloo, ON, N2L 2Y5, Canada 3Department of Mathematics, University of Toronto, Toronto, ON M5S 2E4, Canada 4School of Natural Sciences, Institute for Advanced Study, Princeton, NJ 08540, USA 5 ICTP, Trieste 34151, Italy 6School of Mathematical Sciences, USTC, Hefei 230026, China 7Center of Mathematical Sciences and Applications, Harvard University, Cambridge, MA, USA Abstract We formulate a family of spin Topological Quantum Filed Theories (spin-TQFTs) as fermionic generalization of bosonic Dijkgraaf-Witten TQFTs. They are obtained by gauging G-equivariant invertible spin-TQFTs, or, in physics language, gauging the interacting fermionic Symmetry Protected Topological states (SPTs) with a finite group G symmetry. We use the fact that the latter are classified by Pontryagin duals to spin-bordism groups of the classifying space BG. We also consider unoriented analogues, that is G-equivariant invertible pin±-TQFTs (fermionic time-reversal-SPTs) and their gauging. We compute these groups for various examples of abelian G using Adams spectral sequence and describe all corresponding TQFTs via certain bordism invariants in dimensions 3, 4, and other. This gives explicit formulas for the partition functions of spin-TQFTs on closed manifolds with possible extended operators inserted. The results also provide explicit classification of 't Hooft anomalies of fermionic QFTs with finite abelian group symmetries in one dimension lower. We construct new anomalous boundary deconfined spin-TQFTs (surface fermionic topological orders). -
K-Theoryand Characteristic Classes
MATH 6530: K-THEORY AND CHARACTERISTIC CLASSES Taught by Inna Zakharevich Notes by David Mehrle [email protected] Cornell University Fall 2017 Last updated November 8, 2018. The latest version is online here. Contents 1 Vector bundles................................ 3 1.1 Grassmannians ............................ 8 1.2 Classification of Vector bundles.................... 11 2 Cohomology and Characteristic Classes................. 15 2.1 Cohomology of Grassmannians................... 18 2.2 Characteristic Classes......................... 22 2.3 Axioms for Stiefel-Whitney classes................. 26 2.4 Some computations.......................... 29 3 Cobordism.................................. 35 3.1 Stiefel-Whitney Numbers ...................... 35 3.2 Cobordism Groups.......................... 37 3.3 Geometry of Thom Spaces...................... 38 3.4 L-equivalence and Transversality.................. 42 3.5 Characteristic Numbers and Boundaries.............. 47 4 K-Theory................................... 49 4.1 Bott Periodicity ............................ 49 4.2 The K-theory spectrum........................ 56 4.3 Some properties of K-theory..................... 58 4.4 An example: K-theory of S2 ..................... 59 4.5 Power Operations............................ 61 4.6 When is the Hopf Invariant one?.................. 64 4.7 The Splitting Principle........................ 66 5 Where do we go from here?........................ 68 5.1 The J-homomorphism ........................ 70 5.2 The Chern Character and e invariant............... -
Isometry Types of Frame Bundles
Pacific Journal of Mathematics ISOMETRY TYPES OF FRAME BUNDLES WOUTER VAN LIMBEEK Volume 285 No. 2 December 2016 PACIFIC JOURNAL OF MATHEMATICS Vol. 285, No. 2, 2016 dx.doi.org/10.2140/pjm.2016.285.393 ISOMETRY TYPES OF FRAME BUNDLES WOUTER VAN LIMBEEK We consider the oriented orthonormal frame bundle SO.M/ of an oriented Riemannian manifold M. The Riemannian metric on M induces a canon- ical Riemannian metric on SO.M/. We prove that for two closed oriented Riemannian n-manifolds M and N, the frame bundles SO.M/ and SO.N/ are isometric if and only if M and N are isometric, except possibly in di- mensions 3, 4, and 8. This answers a question of Benson Farb except in dimensions 3, 4, and 8. 1. Introduction 393 2. Preliminaries 396 3. High dimensional isometry groups of manifolds 400 4. Geometric characterization of the fibers of SO.M/ ! M 403 5. Proof for M with positive constant curvature 415 6. Proof of the main theorem for surfaces 422 Acknowledgements 425 References 425 1. Introduction Let M be an oriented Riemannian manifold, and let X VD SO.M/ be the oriented orthonormal frame bundle of M. The Riemannian structure g on M induces in a canonical way a Riemannian metric gSO on SO.M/. This construction was first carried out by O’Neill[1966] and independently by Mok[1978], and is very similar to Sasaki’s[1958; 1962] construction of a metric on the unit tangent bundle of M, so we will henceforth refer to gSO as the Sasaki–Mok–O’Neill metric on SO.M/. -
Arxiv:1910.04634V1 [Math.DG] 10 Oct 2019 ˆ That E Sdnt by Denote Us Let N a En H Subbundle the Define Can One of Points Bundle
SPIN FRAME TRANSFORMATIONS AND DIRAC EQUATIONS R.NORIS(1)(2), L.FATIBENE(2)(3) (1) DISAT, Politecnico di Torino, C.so Duca degli Abruzzi 24, I-10129 Torino, Italy (2)INFN Sezione di Torino, Via Pietro Giuria 1, I-10125 Torino, Italy (3) Dipartimento di Matematica – University of Torino, via Carlo Alberto 10, I-10123 Torino, Italy Abstract. We define spin frames, with the aim of extending spin structures from the category of (pseudo-)Riemannian manifolds to the category of spin manifolds with a fixed signature on them, though with no selected metric structure. Because of this softer re- quirements, transformations allowed by spin frames are more general than usual spin transformations and they usually do not preserve the induced metric structures. We study how these new transformations affect connections both on the spin bundle and on the frame bundle and how this reflects on the Dirac equations. 1. Introduction Dirac equations provide an important tool to study the geometric structure of manifolds, as well as to model the behaviour of a class of physical particles, namely fermions, which includes electrons. The aim of this paper is to generalise a key item needed to formulate Dirac equations, the spin structures, in order to extend the range of allowed transformations. Let us start by first reviewing the usual approach to Dirac equations. Let (M,g) be an orientable pseudo-Riemannian manifold with signature η = (r, s), such that r + s = m = dim(M). R arXiv:1910.04634v1 [math.DG] 10 Oct 2019 Let us denote by L(M) the (general) frame bundle of M, which is a GL(m, )-principal fibre bundle. -
The Atiyah-Singer Index Theorem*
CHAPTER 5 The Atiyah-Singer Index Theorem* Peter B. Gilkey Mathematics Department, University of Oregon, Eugene, OR 97403, USA E-mail: gilkey@ math. uo regon, edu Contents 0. Introduction ................................................... 711 1. Clifford algebras and spin structures ..................................... 711 2. Spectral theory ................................................. 718 3. The classical elliptic complexes ........................................ 725 4. Characteristic classes of vector bundles .................................... 730 5. Characteristic classes of principal bundles .................................. 737 6. The index theorem ............................................... 739 References ..................................................... 745 *Research partially supported by the NSF (USA) and MPIM (Germany). HANDBOOK OF DIFFERENTIAL GEOMETRY, VOL. I Edited by EJ.E. Dillen and L.C.A. Verstraelen 2000 Elsevier Science B.V. All fights reserved 709 The Atiyah-Singer index theorem 711 O. Introduction Here is a brief outline to the paper. In Section 1, we review some basic facts concerning Clifford algebras and spin structures. In Section 2, we discuss the spectral theory of self- adjoint elliptic partial differential operators and give the Hodge decomposition theorem. In Section 3, we define the classical elliptic complexes: de Rham, signature, spin, spin c, Yang-Mills, and Dolbeault; these elliptic complexes are all of Dirac type. In Section 4, we define the various characteristic classes for vector bundles that we shall need: Chern forms, Pontrjagin forms, Chern character, Euler form, Hirzebruch L polynomial, A genus, and Todd polynomial. In Section 5, we discuss the characteristic classes for principal bundles. In Section 6, we give the Atiyah-Singer index theorem; the Chern-Gauss-Bonnet formula, the Hirzebruch signature formula, and the Riemann-Roch formula are special cases of the index theorem. We also discuss the equivariant index theorem and the index theorem for manifolds with boundary. -
Characteristic Classes and Smooth Structures on Manifolds Edited by S
7102 tp.fh11(path) 9/14/09 4:35 PM Page 1 SERIES ON KNOTS AND EVERYTHING Editor-in-charge: Louis H. Kauffman (Univ. of Illinois, Chicago) The Series on Knots and Everything: is a book series polarized around the theory of knots. Volume 1 in the series is Louis H Kauffman’s Knots and Physics. One purpose of this series is to continue the exploration of many of the themes indicated in Volume 1. These themes reach out beyond knot theory into physics, mathematics, logic, linguistics, philosophy, biology and practical experience. All of these outreaches have relations with knot theory when knot theory is regarded as a pivot or meeting place for apparently separate ideas. Knots act as such a pivotal place. We do not fully understand why this is so. The series represents stages in the exploration of this nexus. Details of the titles in this series to date give a picture of the enterprise. Published*: Vol. 1: Knots and Physics (3rd Edition) by L. H. Kauffman Vol. 2: How Surfaces Intersect in Space — An Introduction to Topology (2nd Edition) by J. S. Carter Vol. 3: Quantum Topology edited by L. H. Kauffman & R. A. Baadhio Vol. 4: Gauge Fields, Knots and Gravity by J. Baez & J. P. Muniain Vol. 5: Gems, Computers and Attractors for 3-Manifolds by S. Lins Vol. 6: Knots and Applications edited by L. H. Kauffman Vol. 7: Random Knotting and Linking edited by K. C. Millett & D. W. Sumners Vol. 8: Symmetric Bends: How to Join Two Lengths of Cord by R. -
Recent Developments in Representation Theory
RECENT DEVELOPMENTS IN REPRESENTATION THEORY Wilfried 5chmid* Department of Mathematics Harvard University Cambridge, MA 02138 For the purposes of this lecture, "representation theory" means representation theory of Lie groups, and more specifically, of semisimple Lie groups. I am interpreting my assignment to give a survey rather loosely: while I shall touch upon various major advances in the subject, I am concentrating on a single development. Both order and emphasis of my presentation are motivated by expository considerations, and do not reflect my view of the relative importance of various topics. Initially G shall denote a locally compact topological group which is unimodular -- i.e., left and right Haar measure coincide -- and H C G a closed unimodular subgroup. The quotient space G/H then carries a G- invariant measure, so G acts unitarily on the Hilbert space L2(G/H). In essence, the fundamental problem of harmonic analysis is to decompose L2(G/H) into a direct "sum" of irreducibles. The quotation marks allude to the fact that the decomposition typically involves the continuous ana- logue of a sum, namely a direct integral, as happens already for non- compact Abelian groups. If G is of type I -- loosely speaking, if the unitary representations of G behave reasonably -- the abstract Plan- cherel theorem [12] asserts the existence of such a decomposition. This existence theorem raises as many questions as it answers: to make the decomposition useful, one wants to know it explicitly and, most impor- tantly, one wants to understand the structure of the irreducible sum- mands. In principle, any irreducible unitary representation of G can occur as a constituent of L2(G/H), for some H C G. -
Crystalline Topological Phases As Defect Networks
Crystalline topological phases as defect networks The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Else, Dominic V. and Ryan Thorngren. "Crystalline topological phases as defect networks." Physical Review B 99, 11 (March 2019): 115116 © 2019 American Physical Society As Published http://dx.doi.org/10.1103/PhysRevB.99.115116 Publisher American Physical Society Version Final published version Citable link http://hdl.handle.net/1721.1/120966 Terms of Use Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. PHYSICAL REVIEW B 99, 115116 (2019) Editors’ Suggestion Crystalline topological phases as defect networks Dominic V. Else Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA and Department of Physics, University of California, Santa Barbara, California 93106, USA Ryan Thorngren Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot 7610001, Israel and Department of Mathematics, University of California, Berkeley, California 94720, USA (Received 10 November 2018; published 14 March 2019) A crystalline topological phase is a topological phase with spatial symmetries. In this work, we give a very general physical picture of such phases: A topological phase with spatial symmetry G (with internal symmetry Gint G) is described by a defect network,aG-symmetric network of defects in a topological phase with internal symmetry Gint. The defect network picture works both for symmetry-protected topological (SPT) and symmetry-enriched topological (SET) phases, in systems of either bosons or fermions.