The Simplicial Complex
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Introduction to Dynamical Triangulations
Introduction to Dynamical Triangulations Andrzej G¨orlich Niels Bohr Institute, University of Copenhagen Naxos, September 12th, 2011 Andrzej G¨orlich Causal Dynamical Triangulation Outline 1 Path integral for quantum gravity 2 Causal Dynamical Triangulations 3 Numerical setup 4 Phase diagram 5 Background geometry 6 Quantum fluctuations Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum mechanics A classical particle follows a unique trajectory. Quantum mechanics can be described by Path Integrals: All possible trajectories contribute to the transition amplitude. To define the functional integral, we discretize the time coordinate and approximate each path by linear pieces. space classical trajectory t1 time t2 Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum mechanics A classical particle follows a unique trajectory. Quantum mechanics can be described by Path Integrals: All possible trajectories contribute to the transition amplitude. To define the functional integral, we discretize the time coordinate and approximate each path by linear pieces. quantum trajectory space classical trajectory t1 time t2 Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum mechanics A classical particle follows a unique trajectory. Quantum mechanics can be described by Path Integrals: All possible trajectories contribute to the transition amplitude. To define the functional integral, we discretize the time coordinate and approximate each path by linear pieces. quantum trajectory space classical trajectory t1 time t2 Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum gravity General Relativity: gravity is encoded in space-time geometry. The role of a trajectory plays now the geometry of four-dimensional space-time. All space-time histories contribute to the transition amplitude. -
Topics in Equivariant Cohomology
Topics in Equivariant Cohomology Luke Keating Hughes Thesis submitted for the degree of Master of Philosophy in Pure Mathematics at The University of Adelaide Faculty of Mathematical and Computer Sciences School of Mathematical Sciences February 1, 2017 Contents Abstract v Signed Statement vii Acknowledgements ix 1 Introduction 1 2 Classical Equivariant Cohomology 7 2.1 Topological Equivariant Cohomology . 7 2.1.1 Group Actions . 7 2.1.2 The Borel Construction . 9 2.1.3 Principal Bundles and the Classifying Space . 11 2.2 TheGeometryofPrincipalBundles. 20 2.2.1 The Action of a Lie Algebra . 20 2.2.2 Connections and Curvature . 21 2.2.3 Basic Di↵erentialForms ............................ 26 2.3 Equivariant de Rham Theory . 28 2.3.1 TheWeilAlgebra................................ 28 2.3.2 TheWeilModel ................................ 34 2.3.3 The Chern-Weil Homomorphism . 35 2.3.4 The Mathai-Quillen Isomorphism . 36 2.3.5 The Cartan Model . 37 3 Simplicial Methods 39 3.1 SimplicialandCosimplicialObjects. 39 3.1.1 The Simplicial Category . 39 3.1.2 CosimplicialObjects .............................. 41 3.1.3 SimplicialObjects ............................... 43 3.1.4 The Nerve of a Category . 47 3.1.5 Geometric Realisation . 49 iii 3.2 A Simplicial Construction of the Universal Bundle . 53 3.2.1 Basic Properties of NG ........................... 53 | •| 3.2.2 Principal Bundles and Local Trivialisations . 56 3.2.3 The Homotopy Extension Property and NDR Pairs . 57 3.2.4 Constructing Local Sections . 61 4 Simplicial Equivariant de Rham Theory 65 4.1 Dupont’s Simplicial de Rham Theorem . 65 4.1.1 The Double Complex of a Simplicial Space . -
Vertex-Unfoldings of Simplicial Manifolds Erik D
Masthead Logo Smith ScholarWorks Computer Science: Faculty Publications Computer Science 2002 Vertex-Unfoldings of Simplicial Manifolds Erik D. Demaine Massachusetts nI stitute of Technology David Eppstein University of California, Irvine Jeff rE ickson University of Illinois at Urbana-Champaign George W. Hart State University of New York at Stony Brook Joseph O'Rourke Smith College, [email protected] Follow this and additional works at: https://scholarworks.smith.edu/csc_facpubs Part of the Computer Sciences Commons, and the Geometry and Topology Commons Recommended Citation Demaine, Erik D.; Eppstein, David; Erickson, Jeff; Hart, George W.; and O'Rourke, Joseph, "Vertex-Unfoldings of Simplicial Manifolds" (2002). Computer Science: Faculty Publications, Smith College, Northampton, MA. https://scholarworks.smith.edu/csc_facpubs/60 This Article has been accepted for inclusion in Computer Science: Faculty Publications by an authorized administrator of Smith ScholarWorks. For more information, please contact [email protected] Vertex-Unfoldings of Simplicial Manifolds Erik D. Demaine∗ David Eppstein† Jeff Erickson‡ George W. Hart§ Joseph O’Rourke¶ Abstract We present an algorithm to unfold any triangulated 2-manifold (in particular, any simplicial polyhedron) into a non-overlapping, connected planar layout in linear time. The manifold is cut only along its edges. The resulting layout is connected, but it may have a disconnected interior; the triangles are connected at vertices, but not necessarily joined along edges. We extend our algorithm to establish a similar result for simplicial manifolds of arbitrary dimension. 1 Introduction It is a long-standing open problem to determine whether every convex polyhe- dron can be cut along its edges and unfolded flat in one piece without overlap, that is, into a simple polygon. -
From Double Lie Groupoids to Local Lie 2-Groupoids
Smith ScholarWorks Mathematics and Statistics: Faculty Publications Mathematics and Statistics 12-1-2011 From Double Lie Groupoids to Local Lie 2-Groupoids Rajan Amit Mehta Pennsylvania State University, [email protected] Xiang Tang Washington University in St. Louis Follow this and additional works at: https://scholarworks.smith.edu/mth_facpubs Part of the Mathematics Commons Recommended Citation Mehta, Rajan Amit and Tang, Xiang, "From Double Lie Groupoids to Local Lie 2-Groupoids" (2011). Mathematics and Statistics: Faculty Publications, Smith College, Northampton, MA. https://scholarworks.smith.edu/mth_facpubs/91 This Article has been accepted for inclusion in Mathematics and Statistics: Faculty Publications by an authorized administrator of Smith ScholarWorks. For more information, please contact [email protected] FROM DOUBLE LIE GROUPOIDS TO LOCAL LIE 2-GROUPOIDS RAJAN AMIT MEHTA AND XIANG TANG Abstract. We apply the bar construction to the nerve of a double Lie groupoid to obtain a local Lie 2-groupoid. As an application, we recover Haefliger’s fun- damental groupoid from the fundamental double groupoid of a Lie groupoid. In the case of a symplectic double groupoid, we study the induced closed 2-form on the associated local Lie 2-groupoid, which leads us to propose a definition of a symplectic 2-groupoid. 1. Introduction In homological algebra, given a bisimplicial object A•,• in an abelian cate- gory, one naturally associates two chain complexes. One is the diagonal complex diag(A) := {Ap,p}, and the other is the total complex Tot(A) := { p+q=• Ap,q}. The (generalized) Eilenberg-Zilber theorem [DP61] (see, e.g. [Wei95, TheoremP 8.5.1]) states that diag(A) is quasi-isomorphic to Tot(A). -
Locally Solid Riesz Spaces with Applications to Economics / Charalambos D
http://dx.doi.org/10.1090/surv/105 alambos D. Alipr Lie University \ Burkinshaw na University-Purdue EDITORIAL COMMITTEE Jerry L. Bona Michael P. Loss Peter S. Landweber, Chair Tudor Stefan Ratiu J. T. Stafford 2000 Mathematics Subject Classification. Primary 46A40, 46B40, 47B60, 47B65, 91B50; Secondary 28A33. Selected excerpts in this Second Edition are reprinted with the permissions of Cambridge University Press, the Canadian Mathematical Bulletin, Elsevier Science/Academic Press, and the Illinois Journal of Mathematics. For additional information and updates on this book, visit www.ams.org/bookpages/surv-105 Library of Congress Cataloging-in-Publication Data Aliprantis, Charalambos D. Locally solid Riesz spaces with applications to economics / Charalambos D. Aliprantis, Owen Burkinshaw.—2nd ed. p. cm. — (Mathematical surveys and monographs, ISSN 0076-5376 ; v. 105) Rev. ed. of: Locally solid Riesz spaces. 1978. Includes bibliographical references and index. ISBN 0-8218-3408-8 (alk. paper) 1. Riesz spaces. 2. Economics, Mathematical. I. Burkinshaw, Owen. II. Aliprantis, Char alambos D. III. Locally solid Riesz spaces. IV. Title. V. Mathematical surveys and mono graphs ; no. 105. QA322 .A39 2003 bib'.73—dc22 2003057948 Copying and reprinting. Individual readers of this publication, and nonprofit libraries acting for them, are permitted to make fair use of the material, such as to copy a chapter for use in teaching or research. Permission is granted to quote brief passages from this publication in reviews, provided the customary acknowledgment of the source is given. Republication, systematic copying, or multiple reproduction of any material in this publication is permitted only under license from the American Mathematical Society. -
Homological Pairs on Simplicial Manifolds
DISS. ETH NO. ................... HOMOLOGICAL PAIRS ON SIMPLICIAL MANIFOLDS A thesis submitted to attain the degree of DOCTOR OF SCIENCES of ETH ZURICH (Dr. sc. ETH Zurich) presented by Claudio Sibilia MSc. Math., ETHZ Born on 23.12.1987 Citizen of Italy accepted on the recommendation of Prof. Dr. Giovanni Felder Prof. Dr. Damien Calaque Prof. Dr. Benjamin Enriquez 2017 ii Abstract In this thesis we study the relation between Chen theory of formal homology connection, Universal Knizh- nik{Zamolodchikov connection and Universal Knizhnik{Zamolodchikov-Bernard connection. In the first chapter, we give a summary of some results of Chen. In the second chapter we extend the notion of formal homology connection to simplicial manifolds. In particular, this allows us to construct formal homology connection on manifolds M equipped with a smooth/holomorphic properly discontinuos group action of a discrete group G. We prove that the monodromy represetation of that connection coincides with the Malcev completion of the group M=G. In the second chapter, we use this theory to produces holomorphic flat connections and we show that the universal Universal Knizhnik{Zamolodchikov-Bernard connection on the punctured elliptic curve can be constructed as a formal homology connection. Moreover, we produce an algorithm to construct such a connection by using the homotopy transfer theorem. In the third chapter, we extend this procedure for the configuration space of points of the punctured elliptic curve. Our approach is very general and it can be used to construct flat connections on more challenging manifolds equipped with a group action. For example it can be used for the configuration space of points of a higher genus Riemann surface. -
Integrating Lo -Algebras
Compositio Math. 144 (2008) 1017–1045 doi:10.1112/S0010437X07003405 Integrating L∞-algebras Andr´e Henriques Abstract Given a Lie n-algebra, we provide an explicit construction of its integrating Lie n-group. This extends work done by Getzler in the case of nilpotent L∞-algebras. When applied to an ordinary Lie algebra, our construction yields the simplicial classifying space of the corresponding simply connected Lie group. In the case of the string Lie 2-algebra of Baez and Crans, we obtain the simplicial nerve of their model of the string group. 1. Introduction 1.1 Homotopy Lie algebras Stasheff [Sta92] introduced L∞-algebras, or strongly homotopy Lie algebras, as a model for ‘Lie algebras that satisfy Jacobi up to all higher homotopies’ (see also [HS93]). A (non-negatively graded) L∞-algebra is a graded vector space L = L0 ⊕ L1 ⊕ L2 ⊕··· equipped with brackets []:L → L, [ , ]:Λ2L → L, [ ,,]:Λ3L → L, ··· (1) of degrees −1, 0, 1, 2 ..., where the exterior powers are interpreted in the graded sense. Thereafter, all L∞-algebras will be assumed finite-dimensional in each degree. The axioms satisfied by the brackets can be summarized as follows. ∨ ∗ R ∗ Let L be the graded vector space with Ln−1 =Hom(Ln−1, )indegreen,andletC (L):= Sym(L∨) be its symmetric algebra, again interpreted in the graded sense ∗ ∗ 2 ∗ ∗ 3 ∗ ∗ ∗ ∗ C (L)=R ⊕ [L0] ⊕ [Λ L0 ⊕ L1] ⊕ [Λ L0 ⊕ (L0 ⊗ L1) ⊕ L2] 2 (2) 4 ∗ 2 ∗ ∗ ∗ ⊕ [Λ L0 ⊕ (Λ L0 ⊗ L1) ⊕ Sym L1 ⊕···] ⊕··· . The transpose of the brackets (1) can be assembled into a degree one map L∨ → C∗(L), which extends uniquely to a derivation δ : C∗(L) → C∗(L). -
Arxiv:1608.00296V2
Continuous point symmetries in Group Field Theories Alexander Kegeles∗ and Daniele Oriti† Max Planck Institute for Gravitational Physics (Albert Einstein Institute), Am Mühlenberg 1, 14476 Potsdam-Golm, Germany, EU We discuss the notion of symmetries in non-local field theories characterized by integro-differential equations of motion, from a geometric perspective. We then focus on Group Field Theory (GFT) models of quantum gravity and provide a general analysis of their continuous point symmetry transformations, including the generalized conservation laws following from them. Introduction a quite extensive literature available on this subject [12– 14]. However, in contrast to local field theories, the meth- Symmetry principles are omni-present in modern physics, ods and strategies of analysis strongly vary from case to and especially in the quantum field theory formulation case, and no universal method is known yet. As a result, of fundamental interactions. They enter crucially in we do not know a priori which of the known methods the very definition of fundamental fields and particles, can be suitable adapted for the analysis of group field they dictate the allowed interactions between them, and theories. Particular examples for symmetry calculations capture key features of such interactions in terms of for several GFT models were calculated in [15] but no conservation laws. They also offer powerful conceptual systematic treatment was proposed there. tools, for example, in the characterization of macroscopic In this paper we investigate the variational symmetry phases of quantum systems, as well as many computa- groups of various prominent models in Group Field The- tional simplifications and powerful mathematical tech- ory, that is symmetries of the action and not the (wider) niques for numerical and analytical calculations. -
Notes on Convex Sets, Polytopes, Polyhedra, Combinatorial Topology, Voronoi Diagrams and Delaunay Triangulations
Notes on Convex Sets, Polytopes, Polyhedra, Combinatorial Topology, Voronoi Diagrams and Delaunay Triangulations Jean Gallier and Jocelyn Quaintance Department of Computer and Information Science University of Pennsylvania Philadelphia, PA 19104, USA e-mail: [email protected] April 20, 2017 2 3 Notes on Convex Sets, Polytopes, Polyhedra, Combinatorial Topology, Voronoi Diagrams and Delaunay Triangulations Jean Gallier Abstract: Some basic mathematical tools such as convex sets, polytopes and combinatorial topology, are used quite heavily in applied fields such as geometric modeling, meshing, com- puter vision, medical imaging and robotics. This report may be viewed as a tutorial and a set of notes on convex sets, polytopes, polyhedra, combinatorial topology, Voronoi Diagrams and Delaunay Triangulations. It is intended for a broad audience of mathematically inclined readers. One of my (selfish!) motivations in writing these notes was to understand the concept of shelling and how it is used to prove the famous Euler-Poincar´eformula (Poincar´e,1899) and the more recent Upper Bound Theorem (McMullen, 1970) for polytopes. Another of my motivations was to give a \correct" account of Delaunay triangulations and Voronoi diagrams in terms of (direct and inverse) stereographic projections onto a sphere and prove rigorously that the projective map that sends the (projective) sphere to the (projective) paraboloid works correctly, that is, maps the Delaunay triangulation and Voronoi diagram w.r.t. the lifting onto the sphere to the Delaunay diagram and Voronoi diagrams w.r.t. the traditional lifting onto the paraboloid. Here, the problem is that this map is only well defined (total) in projective space and we are forced to define the notion of convex polyhedron in projective space. -
Convex Sets and Convex Functions 1 Convex Sets
Convex Sets and Convex Functions 1 Convex Sets, In this section, we introduce one of the most important ideas in economic modelling, in the theory of optimization and, indeed in much of modern analysis and computatyional mathematics: that of a convex set. Almost every situation we will meet will depend on this geometric idea. As an independent idea, the notion of convexity appeared at the end of the 19th century, particularly in the works of Minkowski who is supposed to have said: \Everything that is convex interests me." We discuss other ideas which stem from the basic definition, and in particular, the notion of a convex and concave functions which which are so prevalent in economic models. The geometric definition, as we will see, makes sense in any vector space. Since, for the most of our work we deal only with Rn, the definitions will be stated in that context. The interested student may, however, reformulate the definitions either, in an ab stract setting or in some concrete vector space as, for example, C([0; 1]; R)1. Intuitively if we think of R2 or R3, a convex set of vectors is a set that contains all the points of any line segment joining two points of the set (see the next figure). Here is the definition. Definition 1.1 Let u; v 2 V . Then the set of all convex combinations of u and v is the set of points fwλ 2 V : wλ = (1 − λ)u + λv; 0 ≤ λ ≤ 1g: (1.1) In, say, R2 or R3, this set is exactly the line segment joining the two points u and v. -
OPTIMIZATION METHODS: CLASS 3 Linearity, Convexity, ANity
OPTIMIZATION METHODS: CLASS 3 Linearity, convexity, anity The exercises are on the opposite side. D: A set A ⊆ Rd is an ane space, if A is of the form L + v for some linear space L and a shift vector v 2 Rd. By A is of the form L + v we mean a bijection between vectors of L and vectors of A given as b(u) = u + v. Each ane space has a dimension, dened as the dimension of its associated linear space L. D: A vector is an ane combination of a nite set of vectors if Pn , where x a1; a2; : : : an x = i=1 αiai are real number satisfying Pn . αi i=1 αi = 1 A set of vectors V ⊆ Rd is anely independent if it holds that no vector v 2 V is an ane combination of the rest. D: GIven a set of vectors V ⊆ Rd, we can think of its ane span, which is a set of vectors A that are all possible ane combinations of any nite subset of V . Similar to the linear spaces, ane spaces have a nite basis, so we do not need to consider all nite subsets of V , but we can generate the ane span as ane combinations of the base. D: A hyperplane is any ane space in Rd of dimension d − 1. Thus, on a 2D plane, any line is a hyperplane. In the 3D space, any plane is a hyperplane, and so on. A hyperplane splits the space Rd into two halfspaces. We count the hyperplane itself as a part of both halfspaces. -
Background Geometry in 4D Causal Dynamical Triangulations
Background Geometry in 4D Causal Dynamical Triangulations Andrzej G¨orlich Institute of Physics, Jagiellonian University, Kraków Zakopane, June 17, 2008 Andrzej G¨orlich Background Geometry in 4D Causal Dynamical Triangulations Outline 1 Path integral formulation of Quantum Gravity 2 Causal Dynamical Triangulations 3 Monte Carlo Simulations 4 Phase diagram 5 Background geometry Andrzej G¨orlich Background Geometry in 4D Causal Dynamical Triangulations Path integral formulation of Quantum Gravity The partition function of quantum gravity is defined as a formal integral over all geometries weighted by the Einstein-Hilbert action. To make sense of the gravitational path integral one uses the standard method of regularization - discretization. The path integral is written as a nonperturbative sum over all causal triangulations T . Wick rotation is well defined due to global proper-time foliation. Using Monte Carlo techniques we can calculate expectation values of observables. Z X 1 Regge DM[g] iSEH [g] Z = eiS [g] Z = e → s(T ) DiffM T Causal Dynamical Triangulations (CDT) is a background independent approach to quantum gravity. Andrzej G¨orlich Background Geometry in 4D Causal Dynamical Triangulations Path integral formulation of Quantum Gravity The partition function of quantum gravity is defined as a formal integral over all geometries weighted by the Einstein-Hilbert action. To make sense of the gravitational path integral one uses the standard method of regularization - discretization. The path integral is written as a nonperturbative sum over all causal triangulations T . Wick rotation is well defined due to global proper-time foliation. Using Monte Carlo techniques we can calculate expectation values of observables. Z X 1 Regge DM[g] iSEH [g] Z = eiS [g] Z = e → s(T ) DiffM T Causal Dynamical Triangulations (CDT) is a background independent approach to quantum gravity.