The Unitary Group in Its Strong Topology
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1. INTRODUCTION 1.1. Introductory Remarks on Supersymmetry. 1.2
1. INTRODUCTION 1.1. Introductory remarks on supersymmetry. 1.2. Classical mechanics, the electromagnetic, and gravitational fields. 1.3. Principles of quantum mechanics. 1.4. Symmetries and projective unitary representations. 1.5. Poincar´esymmetry and particle classification. 1.6. Vector bundles and wave equations. The Maxwell, Dirac, and Weyl - equations. 1.7. Bosons and fermions. 1.8. Supersymmetry as the symmetry of Z2{graded geometry. 1.1. Introductory remarks on supersymmetry. The subject of supersymme- try (SUSY) is a part of the theory of elementary particles and their interactions and the still unfinished quest of obtaining a unified view of all the elementary forces in a manner compatible with quantum theory and general relativity. Supersymme- try was discovered in the early 1970's, and in the intervening years has become a major component of theoretical physics. Its novel mathematical features have led to a deeper understanding of the geometrical structure of spacetime, a theme to which great thinkers like Riemann, Poincar´e,Einstein, Weyl, and many others have contributed. Symmetry has always played a fundamental role in quantum theory: rotational symmetry in the theory of spin, Poincar´esymmetry in the classification of elemen- tary particles, and permutation symmetry in the treatment of systems of identical particles. Supersymmetry is a new kind of symmetry which was discovered by the physicists in the early 1970's. However, it is different from all other discoveries in physics in the sense that there has been no experimental evidence supporting it so far. Nevertheless an enormous effort has been expended by many physicists in developing it because of its many unique features and also because of its beauty and coherence1. -
Projective Unitary Representations of Infinite Dimensional Lie Groups
Projective unitary representations of infinite dimensional Lie groups Bas Janssens and Karl-Hermann Neeb January 5, 2015 Abstract For an infinite dimensional Lie group G modelled on a locally convex Lie algebra g, we prove that every smooth projective unitary represen- tation of G corresponds to a smooth linear unitary representation of a Lie group extension G] of G. (The main point is the smooth structure on G].) For infinite dimensional Lie groups G which are 1-connected, regular, and modelled on a barrelled Lie algebra g, we characterize the unitary g-representations which integrate to G. Combining these results, we give a precise formulation of the correspondence between smooth pro- jective unitary representations of G, smooth linear unitary representations of G], and the appropriate unitary representations of its Lie algebra g]. Contents 1 Representations of locally convex Lie groups 5 1.1 Smooth functions . 5 1.2 Locally convex Lie groups . 6 2 Projective unitary representations 7 2.1 Unitary representations . 7 2.2 Projective unitary representations . 7 3 Integration of Lie algebra representations 8 3.1 Derived representations . 9 3.2 Globalisation of Lie algebra representations . 10 3.2.1 Weak and strong topology on V . 11 3.2.2 Regular Lie algebra representations . 15 4 Projective unitary representations and central extensions 20 5 Smoothness of projective representations 25 5.1 Smoothness criteria . 25 5.2 Structure of the set of smooth rays . 26 1 6 Lie algebra extensions and cohomology 28 7 The main theorem 31 8 Covariant representations 33 9 Admissible derivations 36 9.1 Admissible derivations . -
Unitary Group - Wikipedia
Unitary group - Wikipedia https://en.wikipedia.org/wiki/Unitary_group Unitary group In mathematics, the unitary group of degree n, denoted U( n), is the group of n × n unitary matrices, with the group operation of matrix multiplication. The unitary group is a subgroup of the general linear group GL( n, C). Hyperorthogonal group is an archaic name for the unitary group, especially over finite fields. For the group of unitary matrices with determinant 1, see Special unitary group. In the simple case n = 1, the group U(1) corresponds to the circle group, consisting of all complex numbers with absolute value 1 under multiplication. All the unitary groups contain copies of this group. The unitary group U( n) is a real Lie group of dimension n2. The Lie algebra of U( n) consists of n × n skew-Hermitian matrices, with the Lie bracket given by the commutator. The general unitary group (also called the group of unitary similitudes ) consists of all matrices A such that A∗A is a nonzero multiple of the identity matrix, and is just the product of the unitary group with the group of all positive multiples of the identity matrix. Contents Properties Topology Related groups 2-out-of-3 property Special unitary and projective unitary groups G-structure: almost Hermitian Generalizations Indefinite forms Finite fields Degree-2 separable algebras Algebraic groups Unitary group of a quadratic module Polynomial invariants Classifying space See also Notes References Properties Since the determinant of a unitary matrix is a complex number with norm 1, the determinant gives a group 1 of 7 2/23/2018, 10:13 AM Unitary group - Wikipedia https://en.wikipedia.org/wiki/Unitary_group homomorphism The kernel of this homomorphism is the set of unitary matrices with determinant 1. -
An Overview of Topological Groups: Yesterday, Today, Tomorrow
axioms Editorial An Overview of Topological Groups: Yesterday, Today, Tomorrow Sidney A. Morris 1,2 1 Faculty of Science and Technology, Federation University Australia, Victoria 3353, Australia; [email protected]; Tel.: +61-41-7771178 2 Department of Mathematics and Statistics, La Trobe University, Bundoora, Victoria 3086, Australia Academic Editor: Humberto Bustince Received: 18 April 2016; Accepted: 20 April 2016; Published: 5 May 2016 It was in 1969 that I began my graduate studies on topological group theory and I often dived into one of the following five books. My favourite book “Abstract Harmonic Analysis” [1] by Ed Hewitt and Ken Ross contains both a proof of the Pontryagin-van Kampen Duality Theorem for locally compact abelian groups and the structure theory of locally compact abelian groups. Walter Rudin’s book “Fourier Analysis on Groups” [2] includes an elegant proof of the Pontryagin-van Kampen Duality Theorem. Much gentler than these is “Introduction to Topological Groups” [3] by Taqdir Husain which has an introduction to topological group theory, Haar measure, the Peter-Weyl Theorem and Duality Theory. Of course the book “Topological Groups” [4] by Lev Semyonovich Pontryagin himself was a tour de force for its time. P. S. Aleksandrov, V.G. Boltyanskii, R.V. Gamkrelidze and E.F. Mishchenko described this book in glowing terms: “This book belongs to that rare category of mathematical works that can truly be called classical - books which retain their significance for decades and exert a formative influence on the scientific outlook of whole generations of mathematicians”. The final book I mention from my graduate studies days is “Topological Transformation Groups” [5] by Deane Montgomery and Leo Zippin which contains a solution of Hilbert’s fifth problem as well as a structure theory for locally compact non-abelian groups. -
UC Riverside UC Riverside Previously Published Works
UC Riverside UC Riverside Previously Published Works Title Universal topological quantum computation from a superconductor-abelian quantum hall heterostructure Permalink https://escholarship.org/uc/item/3nm3m6f2 Journal Physical Review X, 4(1) ISSN 2160-3308 Authors Mong, RSK Clarke, DJ Alicea, J et al. Publication Date 2014 DOI 10.1103/PhysRevX.4.011036 Peer reviewed eScholarship.org Powered by the California Digital Library University of California Universal topological quantum computation from a superconductor/Abelian quantum Hall heterostructure Roger S. K. Mong,1 David J. Clarke,1 Jason Alicea,1 Netanel H. Lindner,1 Paul Fendley,2 Chetan Nayak,3, 4 Yuval Oreg,5 Ady Stern,5 Erez Berg,5 Kirill Shtengel,6, 7 and Matthew P. A. Fisher4 1Department of Physics, California Institute of Technology, Pasadena, CA 91125, USA 2Department of Physics, University of Virginia, Charlottesville, VA 22904, USA 3Microsoft Research, Station Q, University of California, Santa Barbara, CA 93106, USA 4Department of Physics, University of California, Santa Barbara, CA 93106, USA 5Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot, 76100, Israel 6Department of Physics and Astronomy, University of California, Riverside, California 92521, USA 7Institute for Quantum Information, California Institute of Technology, Pasadena, CA 91125, USA Non-Abelian anyons promise to reveal spectacular features of quantum mechanics that could ultimately pro- vide the foundation for a decoherence-free quantum computer. A key breakthrough in the pursuit of these exotic particles originated from Read and Green’s observation that the Moore-Read quantum Hall state and a (relatively simple) two-dimensional p + ip superconductor both support so-called Ising non-Abelian anyons. -
Notes on Principal Bundles and Classifying Spaces
Notes on principal bundles and classifying spaces Stephen A. Mitchell August 2001 1 Introduction Consider a real n-plane bundle ξ with Euclidean metric. Associated to ξ are a number of auxiliary bundles: disc bundle, sphere bundle, projective bundle, k-frame bundle, etc. Here “bundle” simply means a local product with the indicated fibre. In each case one can show, by easy but repetitive arguments, that the projection map in question is indeed a local product; furthermore, the transition functions are always linear in the sense that they are induced in an obvious way from the linear transition functions of ξ. It turns out that all of this data can be subsumed in a single object: the “principal O(n)-bundle” Pξ, which is just the bundle of orthonormal n-frames. The fact that the transition functions of the various associated bundles are linear can then be formalized in the notion “fibre bundle with structure group O(n)”. If we do not want to consider a Euclidean metric, there is an analogous notion of principal GLnR-bundle; this is the bundle of linearly independent n-frames. More generally, if G is any topological group, a principal G-bundle is a locally trivial free G-space with orbit space B (see below for the precise definition). For example, if G is discrete then a principal G-bundle with connected total space is the same thing as a regular covering map with G as group of deck transformations. Under mild hypotheses there exists a classifying space BG, such that isomorphism classes of principal G-bundles over X are in natural bijective correspondence with [X, BG]. -
Topological Groups
Topological Groups Siyan Daniel Li-Huerta September 8, 2020 Definition A topological group is a group G with a topological space structure such that The multiplication map µ : G × G ! G is continuous, The inverse map ι : G ! G is continuous. Example Any group G with the discrete topology, The group R under addition with the Euclidean topology, × The group C under multiplication with the Euclidean topology, 1 × × The subgroup S = fz 2 C j jzj = 1g ⊂ C , The group GLn(R) = fA 2 Matn×n(R) j det A 6= 0g under multiplication with the Euclidean topology. Remark Any finite Hausdorff topological group G must be discrete. 2 / 9 Let G be a topological group, and let g be in G. Then left translation (i.e. multiplication) by g equals the composite (g;id) µ G / fgg × G / G; so it's continuous. Its inverse is left translation by g −1, so it's even a homeomorphism. The same holds for right translation. Definition Let X be a topological space. We say X is homogeneous if, for every x and y in X , there exists a homeomorphism f : X ! X such that f (x) = y. Example Any topological group G is homogeneous (using left translation), n n+1 The n-sphere S = f~v 2 R j k~vk= 1g is homogeneous (using rotations). Thus topological groups are very special topological spaces: they look \the same" around every point. So it often suffices to study neighborhoods of one point. Let's pick the point 1! 3 / 9 Proposition Let G be a topological group, and let U be a neighborhood of 1. -
The Unitary Group in Its Strong Topology Martin Schottenloher Mathematisches Institut LMU M¨Unchen Theresienstr
The Unitary Group In Its Strong Topology Martin Schottenloher Mathematisches Institut LMU M¨unchen Theresienstr. 39, 80333 M¨unchen [email protected], +49 89 21804435 Abstract. The unitary group U(H) on an infinite dimensional complex Hilbert space H in its strong topology is a topological group and has some further nice properties, e.g. it is metrizable and contractible if H is separa- ble. As an application Hilbert bundles are classified by homotopy. Keywords: Unitary Operator, Strong Operator Topology, Topological Group, Infinite Dimensional Lie Group, Contractibility, Hilbert bundle, Classifying Space 2000 Mathematics Subject Classification: 51 F 25, 22 A 10, 22 E 65, 55 R 35, 57 T 20 It is easy to show and well-known that the unitary group U(H) – the group of all unitary operators H→Hon a complex Hilbert space H – is a topological group with respect to the norm topology on U(H). However, for many purposes in mathematics the norm topology is too strong. For example, for a compact topological group G with Haar measure μ the left regular representation on H = L2(G, μ) −1 L : G → U(H),g → Lg : H→H,Lgf(x)=f(g x) is continuous for the strong topology on U(H),butL is not continuous when U(H) is equipped with the norm topology, except for finite G. This fact makes the norm topology on U(H) useless in representation theory and its applications as well as in many areas of physics or topology. The continuity property which is mostly used in case of a topological space W and a general Hilbert space H and which seems to be more natural is the continuity of a left action on H Φ:W ×H→H, in particular, in case of a left action of a topological group G on H: Note that the above left regular representation is continuous as a map: L : G ×H→H. -
A Linear Algebraic Group? Skip Garibaldi
WHATIS... ? a Linear Algebraic Group? Skip Garibaldi From a marketing perspective, algebraic groups group over F, a Lie group, or a topological group is are poorly named.They are not the groups you met a “group object” in the category of affine varieties as a student in abstract algebra, which I will call over F, smooth manifolds, or topological spaces, concrete groups for clarity. Rather, an algebraic respectively. For algebraic groups, this implies group is the analogue in algebra of a topological that the set G(K) is a concrete group for each field group (fromtopology) or a Liegroup (from analysis K containing F. and geometry). Algebraic groups provide a unifying language Examples for apparently different results in algebra and The basic example is the general linear group number theory. This unification can not only sim- GLn for which GLn(K) is the concrete group of plify proofs, it can also suggest generalizations invertible n-by-n matrices with entries in K. It is the and bring new tools to bear, such as Galois co- collection of solutions (t, X)—with t ∈ K and X an homology, Steenrod operations in Chow theory, n-by-n matrix over K—to the polynomial equation etc. t ·det X = 1. Similar reasoning shows that familiar matrix groups such as SLn, orthogonal groups, Definitions and symplectic groups can be viewed as linear A linear algebraic group over a field F is a smooth algebraic groups. The main difference here is that affine variety over F that is also a group, much instead of viewing them as collections of matrices like a topological group is a topological space over F, we view them as collections of matrices that is also a group and a Lie group is a smooth over every extension K of F. -
Arxiv:1305.5974V1 [Math-Ph]
INTRODUCTION TO SPORADIC GROUPS for physicists Luis J. Boya∗ Departamento de F´ısica Te´orica Universidad de Zaragoza E-50009 Zaragoza, SPAIN MSC: 20D08, 20D05, 11F22 PACS numbers: 02.20.a, 02.20.Bb, 11.24.Yb Key words: Finite simple groups, sporadic groups, the Monster group. Juan SANCHO GUIMERA´ In Memoriam Abstract We describe the collection of finite simple groups, with a view on physical applications. We recall first the prime cyclic groups Zp, and the alternating groups Altn>4. After a quick revision of finite fields Fq, q = pf , with p prime, we consider the 16 families of finite simple groups of Lie type. There are also 26 extra “sporadic” groups, which gather in three interconnected “generations” (with 5+7+8 groups) plus the Pariah groups (6). We point out a couple of physical applications, in- cluding constructing the biggest sporadic group, the “Monster” group, with close to 1054 elements from arguments of physics, and also the relation of some Mathieu groups with compactification in string and M-theory. ∗[email protected] arXiv:1305.5974v1 [math-ph] 25 May 2013 1 Contents 1 Introduction 3 1.1 Generaldescriptionofthework . 3 1.2 Initialmathematics............................ 7 2 Generalities about groups 14 2.1 Elementarynotions............................ 14 2.2 Theframeworkorbox .......................... 16 2.3 Subgroups................................. 18 2.4 Morphisms ................................ 22 2.5 Extensions................................. 23 2.6 Familiesoffinitegroups ......................... 24 2.7 Abeliangroups .............................. 27 2.8 Symmetricgroup ............................. 28 3 More advanced group theory 30 3.1 Groupsoperationginspaces. 30 3.2 Representations.............................. 32 3.3 Characters.Fourierseries . 35 3.4 Homological algebra and extension theory . 37 3.5 Groupsuptoorder16.......................... -
Appendix a Topological Groups and Lie Groups
Appendix A Topological Groups and Lie Groups This appendix studies topological groups, and also Lie groups which are special topological groups as well as manifolds with some compatibility conditions. The concept of a topological group arose through the work of Felix Klein (1849–1925) and Marius Sophus Lie (1842–1899). One of the concrete concepts of the the- ory of topological groups is the concept of Lie groups named after Sophus Lie. The concept of Lie groups arose in mathematics through the study of continuous transformations, which constitute in a natural way topological manifolds. Topo- logical groups occupy a vast territory in topology and geometry. The theory of topological groups first arose in the theory of Lie groups which carry differential structures and they form the most important class of topological groups. For exam- ple, GL (n, R), GL (n, C), GL (n, H), SL (n, R), SL (n, C), O(n, R), U(n, C), SL (n, H) are some important classical Lie Groups. Sophus Lie first systematically investigated groups of transformations and developed his theory of transformation groups to solve his integration problems. David Hilbert (1862–1943) presented to the International Congress of Mathe- maticians, 1900 (ICM 1900) in Paris a series of 23 research projects. He stated in this lecture that his Fifth Problem is linked to Sophus Lie theory of transformation groups, i.e., Lie groups act as groups of transformations on manifolds. A translation of Hilbert’s fifth problem says “It is well-known that Lie with the aid of the concept of continuous groups of transformations, had set up a system of geometrical axioms and, from the standpoint of his theory of groups has proved that this system of axioms suffices for geometry”. -
An Introduction to Topological Groups
An Introduction to Topological Groups by Dylan Spivak A project submitted to the Department of Mathematical Sciences in conformity with the requirements for Math 4301 (Honours Seminar) Lakehead University Thunder Bay, Ontario, Canada copyright c (2015) Dylan Spivak Abstract This project is a survey of topological groups. Specifically, our goal is to investigate properties and examples of locally compact topological groups. Our project is structured as follows. In Chapter 2, we review the basics of topology and group theory that will be needed to understand topological groups. This summary in- cludes definitions and examples of topologies and topological spaces, continuity, the prod- uct topology, homeomorphism, compactness and local compactness, normal subgroups and quotient groups. In Chapter 3, we discuss semitopological groups. This includes the left and right translations of a group G, the left and right embeddings of G, products of semitopological groups and compact semitopological groups. Chapter 4 is on topological groups, here we discuss subgroups, quotient groups, and products of topological groups. We end the project with locally compact topological groups; here we investigate compact- ness and local compactness in topological groups. An important class of locally compact topological groups are groups of matrices. These structures are important in physics, we go over some of their basic properties. i Acknowledgements I would like to thank my supervisor Dr. Monica Ilie for taking the time to meet with me every week, for carefully editing all of my proofs, and for working with me during the summer. Her kindness and experience made this project a pleasure to work on. I would also like to thank Dr.