Moving Coframes. I
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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. -
EXAM QUESTIONS (Part Two)
Created by T. Madas MATRICES EXAM QUESTIONS (Part Two) Created by T. Madas Created by T. Madas Question 1 (**) Find the eigenvalues and the corresponding eigenvectors of the following 2× 2 matrix. 7 6 A = . 6 2 2 3 λ= −2, u = α , λ=11, u = β −3 2 Question 2 (**) A transformation in three dimensional space is defined by the following 3× 3 matrix, where x is a scalar constant. 2− 2 4 C =5x − 2 2 . −1 3 x Show that C is non singular for all values of x . FP1-N , proof Created by T. Madas Created by T. Madas Question 3 (**) The 2× 2 matrix A is given below. 1 8 A = . 8− 11 a) Find the eigenvalues of A . b) Determine an eigenvector for each of the corresponding eigenvalues of A . c) Find a 2× 2 matrix P , so that λ1 0 PT AP = , 0 λ2 where λ1 and λ2 are the eigenvalues of A , with λ1< λ 2 . 1 2 1 2 5 5 λ1= −15, λ 2 = 5 , u= , v = , P = − 2 1 − 2 1 5 5 Created by T. Madas Created by T. Madas Question 4 (**) Describe fully the transformation given by the following 3× 3 matrix. 0.28− 0.96 0 0.96 0.28 0 . 0 0 1 rotation in the z axis, anticlockwise, by arcsin() 0.96 Question 5 (**) A transformation in three dimensional space is defined by the following 3× 3 matrix, where k is a scalar constant. 1− 2 k A = k 2 0 . 2 3 1 Show that the transformation defined by A can be inverted for all values of k . -
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/. -
Two-Dimensional Geometric Transformations
Two-Dimensional Geometric Transformations 1 Basic Two-Dimensional Geometric Transformations 2 Matrix Representations and Homogeneous Coordinates 3 Inverse Transformations 4 Two-Dimensional Composite Transformations 5 Other Two-Dimensional Transformations 6 Raster Methods for Geometric Transformations 7 OpenGL Raster Transformations 8 Transformations between Two-Dimensional Coordinate Systems 9 OpenGL Functions for Two-Dimensional Geometric Transformations 10 OpenGL Geometric-Transformation o far, we have seen how we can describe a scene in Programming Examples S 11 Summary terms of graphics primitives, such as line segments and fill areas, and the attributes associated with these primitives. Also, we have explored the scan-line algorithms for displaying output primitives on a raster device. Now, we take a look at transformation operations that we can apply to objects to reposition or resize them. These operations are also used in the viewing routines that convert a world-coordinate scene description to a display for an output device. In addition, they are used in a variety of other applications, such as computer-aided design (CAD) and computer animation. An architect, for example, creates a layout by arranging the orientation and size of the component parts of a design, and a computer animator develops a video sequence by moving the “camera” position or the objects in a scene along specified paths. Operations that are applied to the geometric description of an object to change its position, orientation, or size are called geometric transformations. Sometimes geometric transformations are also referred to as modeling transformations, but some graphics packages make a From Chapter 7 of Computer Graphics with OpenGL®, Fourth Edition, Donald Hearn, M. -
Feature Matching and Heat Flow in Centro-Affine Geometry
Symmetry, Integrability and Geometry: Methods and Applications SIGMA 16 (2020), 093, 22 pages Feature Matching and Heat Flow in Centro-Affine Geometry Peter J. OLVER y, Changzheng QU z and Yun YANG x y School of Mathematics, University of Minnesota, Minneapolis, MN 55455, USA E-mail: [email protected] URL: http://www.math.umn.edu/~olver/ z School of Mathematics and Statistics, Ningbo University, Ningbo 315211, P.R. China E-mail: [email protected] x Department of Mathematics, Northeastern University, Shenyang, 110819, P.R. China E-mail: [email protected] Received April 02, 2020, in final form September 14, 2020; Published online September 29, 2020 https://doi.org/10.3842/SIGMA.2020.093 Abstract. In this paper, we study the differential invariants and the invariant heat flow in centro-affine geometry, proving that the latter is equivalent to the inviscid Burgers' equa- tion. Furthermore, we apply the centro-affine invariants to develop an invariant algorithm to match features of objects appearing in images. We show that the resulting algorithm com- pares favorably with the widely applied scale-invariant feature transform (SIFT), speeded up robust features (SURF), and affine-SIFT (ASIFT) methods. Key words: centro-affine geometry; equivariant moving frames; heat flow; inviscid Burgers' equation; differential invariant; edge matching 2020 Mathematics Subject Classification: 53A15; 53A55 1 Introduction The main objective in this paper is to study differential invariants and invariant curve flows { in particular the heat flow { in centro-affine geometry. In addition, we will present some basic applications to feature matching in camera images of three-dimensional objects, comparing our method with other popular algorithms. -
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. -
Math 704: Part 1: Principal Bundles and Connections
MATH 704: PART 1: PRINCIPAL BUNDLES AND CONNECTIONS WEIMIN CHEN Contents 1. Lie Groups 1 2. Principal Bundles 3 3. Connections and curvature 6 4. Covariant derivatives 12 References 13 1. Lie Groups A Lie group G is a smooth manifold such that the multiplication map G × G ! G, (g; h) 7! gh, and the inverse map G ! G, g 7! g−1, are smooth maps. A Lie subgroup H of G is a subgroup of G which is at the same time an embedded submanifold. A Lie group homomorphism is a group homomorphism which is a smooth map between the Lie groups. The Lie algebra, denoted by Lie(G), of a Lie group G consists of the set of left-invariant vector fields on G, i.e., Lie(G) = fX 2 X (G)j(Lg)∗X = Xg, where Lg : G ! G is the left translation Lg(h) = gh. As a vector space, Lie(G) is naturally identified with the tangent space TeG via X 7! X(e). A Lie group homomorphism naturally induces a Lie algebra homomorphism between the associated Lie algebras. Finally, the universal cover of a connected Lie group is naturally a Lie group, which is in one to one correspondence with the corresponding Lie algebras. Example 1.1. Here are some important Lie groups in geometry and topology. • GL(n; R), GL(n; C), where GL(n; C) can be naturally identified as a Lie sub- group of GL(2n; R). • SL(n; R), O(n), SO(n) = O(n) \ SL(n; R), Lie subgroups of GL(n; R). -
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]. -
Geometric Transformation Techniques for Digital I~Iages: a Survey
GEOMETRIC TRANSFORMATION TECHNIQUES FOR DIGITAL I~IAGES: A SURVEY George Walberg Department of Computer Science Columbia University New York, NY 10027 [email protected] December 1988 Technical Report CUCS-390-88 ABSTRACT This survey presents a wide collection of algorithms for the geometric transformation of digital images. Efficient image transformation algorithms are critically important to the remote sensing, medical imaging, computer vision, and computer graphics communities. We review the growth of this field and compare all the described algorithms. Since this subject is interdisci plinary, emphasis is placed on the unification of the terminology, motivation, and contributions of each technique to yield a single coherent framework. This paper attempts to serve a dual role as a survey and a tutorial. It is comprehensive in scope and detailed in style. The primary focus centers on the three components that comprise all geometric transformations: spatial transformations, resampling, and antialiasing. In addition, considerable attention is directed to the dramatic progress made in the development of separable algorithms. The text is supplemented with numerous examples and an extensive bibliography. This work was supponed in part by NSF grant CDR-84-21402. 6.5.1 Pyramids 68 6.5.2 Summed-Area Tables 70 6.6 FREQUENCY CLAMPING 71 6.7 ANTIALIASED LINES AND TEXT 71 6.8 DISCUSSION 72 SECTION 7 SEPARABLE GEOMETRIC TRANSFORMATION ALGORITHMS 7.1 INTRODUCTION 73 7.1.1 Forward Mapping 73 7.1.2 Inverse Mapping 73 7.1.3 Separable Mapping 74 7.2 2-PASS TRANSFORMS 75 7.2.1 Catmull and Smith, 1980 75 7.2.1.1 First Pass 75 7.2.1.2 Second Pass 75 7.2.1.3 2-Pass Algorithm 77 7.2.1.4 An Example: Rotation 77 7.2.1.5 Bottleneck Problem 78 7.2.1.6 Foldover Problem 79 7.2.2 Fraser, Schowengerdt, and Briggs, 1985 80 7.2.3 Fant, 1986 81 7.2.4 Smith, 1987 82 7.3 ROTATION 83 7.3.1 Braccini and Marino, 1980 83 7.3.2 Weiman, 1980 84 7.3.3 Paeth, 1986/ Tanaka. -
Transformation Groups in Non-Riemannian Geometry Charles Frances
Transformation groups in non-Riemannian geometry Charles Frances To cite this version: Charles Frances. Transformation groups in non-Riemannian geometry. Sophus Lie and Felix Klein: The Erlangen Program and Its Impact in Mathematics and Physics, European Mathematical Society Publishing House, pp.191-216, 2015, 10.4171/148-1/7. hal-03195050 HAL Id: hal-03195050 https://hal.archives-ouvertes.fr/hal-03195050 Submitted on 10 Apr 2021 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Transformation groups in non-Riemannian geometry Charles Frances Laboratoire de Math´ematiques,Universit´eParis-Sud 91405 ORSAY Cedex, France email: [email protected] 2000 Mathematics Subject Classification: 22F50, 53C05, 53C10, 53C50. Keywords: Transformation groups, rigid geometric structures, Cartan geometries. Contents 1 Introduction . 2 2 Rigid geometric structures . 5 2.1 Cartan geometries . 5 2.1.1 Classical examples of Cartan geometries . 7 2.1.2 Rigidity of Cartan geometries . 8 2.2 G-structures . 9 3 The conformal group of a Riemannian manifold . 12 3.1 The theorem of Obata and Ferrand . 12 3.2 Ideas of the proof of the Ferrand-Obata theorem . 13 3.3 Generalizations to rank one parabolic geometries . -
WHAT IS a CONNECTION, and WHAT IS IT GOOD FOR? Contents 1. Introduction 2 2. the Search for a Good Directional Derivative 3 3. F
WHAT IS A CONNECTION, AND WHAT IS IT GOOD FOR? TIMOTHY E. GOLDBERG Abstract. In the study of differentiable manifolds, there are several different objects that go by the name of \connection". I will describe some of these objects, and show how they are related to each other. The motivation for many notions of a connection is the search for a sufficiently nice directional derivative, and this will be my starting point as well. The story will by necessity include many supporting characters from differential geometry, all of whom will receive a brief but hopefully sufficient introduction. I apologize for my ungrammatical title. Contents 1. Introduction 2 2. The search for a good directional derivative 3 3. Fiber bundles and Ehresmann connections 7 4. A quick word about curvature 10 5. Principal bundles and principal bundle connections 11 6. Associated bundles 14 7. Vector bundles and Koszul connections 15 8. The tangent bundle 18 References 19 Date: 26 March 2008. 1 1. Introduction In the study of differentiable manifolds, there are several different objects that go by the name of \connection", and this has been confusing me for some time now. One solution to this dilemma was to promise myself that I would some day present a talk about connections in the Olivetti Club at Cornell University. That day has come, and this document contains my notes for this talk. In the interests of brevity, I do not include too many technical details, and instead refer the reader to some lovely references. My main references were [2], [4], and [5]. -
Geometric Transformation of Finite Element Methods: Theory and Applications
GEOMETRIC TRANSFORMATION OF FINITE ELEMENT METHODS: THEORY AND APPLICATIONS MICHAEL HOLST AND MARTIN LICHT Abstract. We present a new technique to apply finite element methods to partial differential equations over curved domains. A change of variables along a coordinate transformation satisfying only low regularity assumptions can translate a Poisson problem over a curved physical domain to a Poisson prob- lem over a polyhedral parametric domain. This greatly simplifies both the geo- metric setting and the practical implementation, at the cost of having globally rough non-trivial coefficients and data in the parametric Poisson problem. Our main result is that a recently developed broken Bramble-Hilbert lemma is key in harnessing regularity in the physical problem to prove higher-order finite el- ement convergence rates for the parametric problem. Numerical experiments are given which confirm the predictions of our theory. 1. Introduction The computational theory of partial differential equations has been in a paradoxi- cal situation from its very inception: partial differential equations over domains with curved boundaries are of theoretical and practical interest, but numerical methods are generally conceived only for polyhedral domains. Overcoming this geomet- ric gap continues to inspire much ongoing research in computational mathematics for treating partial differential equations with geometric features. Computational methods for partial differential equations over curved domains commonly adhere to the philosophy of approximating the physical domain of the partial differential equation by a parametric domain. We mention isoparametric finite element meth- ods [2], surface finite element methods [10, 8, 3], or isogeometric analysis [14] as examples, which describe the parametric domain by a polyhedral mesh whose cells are piecewise distorted to approximate the physical domain closely or exactly.