LECTURE 6: THE RIEMANN CURVATURE TENSOR. 1. The curvature tensor
|
|
- Bartholomew Ray
- 5 years ago
- Views:
Transcription
1 LECTURE 6: THE RIEMANN CURVATURE TENSOR 1. The curvature tensor Let M be any smooth manifod with inear connection, then we know that R(X, Y )Z := X Y Z + Y X Z + [X,Y ] Z. defines a (1, 3)-tensor fied on M, caed the curvature tensor of. Locay if we write R = Rijk dx i dx j dx k j, then the coefficients can be expressed via the Christoffe symbos of as R ijk = Γ s jkγ is + Γ s ikγ js i Γ jk + j Γ ik, Obviousy the curvature tensor for the standard connection on R n is identicay zero, since its Christoffe s symbos are a zero. Exampe. Consider M = S n. Last time we have seen that X Y = X Y X Y, n n. defines a (Levi-Civita) connection on S n, where is the standard connection on R n+1 : X i i (Y j j ) = X i i (Y j ) j. To cacuate its curvature tensor, we need rewrite it into a simper form. Since n = (x 1, x 2,, x n+1 ), one get X n = X i i (x j ) j = X. It foows X Y, n n = Y, X n n = X, Y n. So X Y = X Y + X, Y n. Thus Y X Z = Y X Z + Y, X Z n = Y ( X Z + X, Z n) + X Y, Z n X Y, Z n = Y X Z + Y ( X, Z ) n + X, Z Y + X( Y, Z ) n X Y, Z n. In view of the fact R = 0, we get R(X, Y )Z = X( Y, Z ) n Y, Z X Y ( X, Z ) n + Y X, Z n + Y ( X, Z ) n + X, Z Y + X( Y, Z ) n X Y, Z n + [X, Y ], Z n = X, Z Y Y, Z X. 1
2 2 LECTURE 6: THE RIEMANN CURVATURE TENSOR By definition one immediatey gets the foowing anti-symmetry: (1) R(X, Y )Z = R(Y, X)Z For the curvature tensor R, one has Proposition 1.1 (The First Bianchi identity). If is a torsion-free, then (2) R(X, Y )Z + R(Y, Z)X + R(Z, X)Y = 0. Proof. Reca that is torsion-free means X Y Y X [X, Y ] = 0. So we have R(X, Y )Z + R(Y, Z)X + R(Z, X)Y = X Y Z + Y X Z + [X,Y ] Z Y Z X + Z Y X + [Y,Z] X Z X Y + X Z Y + [Z,X] Y = X [Y, Z] Y [Z, X] Z [X, Y ] + [X,Y ] Z + [Y,Z] X + [Z,X] Y = [X, [Y, Z]] [Y, [Z, X]] [Z, [X, Y ]] = 0, where in the ast step we used the Jacobi identity for vector fieds. Obviousy one can then write (1) and (2) in oca coordinates as Rijk = R Rijk + Rjki + Rkij = 0. Reca that one can aways extend a inear connection on the tangent bunde to a inear connection on tensor bundes. In particuar, for the tensor fied R of type (1, 3), X R is aso a tensor fied of type (1, 3), given by ( X R)(Y, Z, W ) := X (R(Y, Z)W ) R( X Y, Z)W R(Y, X Z)W R(Y, Z) X W. Proposition 1.2 (The Second Bianchi Identity). Suppose is torsion free, then Proof. By definition, jik, ( X R)(Y, Z, W ) + ( Y R)(Z, X, W ) + ( Z R)(X, Y, W ) = 0. ( X R)(Y, Z, W ) + ( Y R)(Z, X, W ) + ( Z R)(X, Y, W ) = X (R(Y, Z)W ) R( X Y, Z)W R(Y, X Z)W R(Y, Z) X W + Y (R(Z, X)W ) R( Y Z, X)W R(Z, Y X)W R(Z, X) Y W + Z (R(X, Y )W ) R( Z X, Y )W R(X, Z Y )W R(X, Y ) Z W. Using the torsion-freeness and (1), one can simpify the midde two coumns to R([X, Z], Y )W + R([Y, X], Z)W + R([Y, X], Z)W.
3 LECTURE 6: THE RIEMANN CURVATURE TENSOR 3 Now expand each R using its definition, the whoe expression becomes a summation of 27 terms, the first 9 terms being X Y Z W + X Z Y W + X [Y,Z] W [X,Z] Y W + Y [X,Z] W + [[X,Z],Y ] W + Y Z X W Z Y X W [Y,Z] X W, the second and third 9 terms are simiar to the first 9 terms above: one just repace X, Y, Z by Y, Z, X and Z, X, Y respectivey. It is not hard to check that a those expressions containing three s (12 terms in tota) cance out triviay, a those expressions containing two s (aso 12 terms in tota) cance out by using the fact [X, Y ] = [Y, X], and the remaining three terms in view of the Jacobi identity. [[X,Z],Y ] W + [[Y,X],Z] W + [[Z,Y ],X] W = 0 In oca coordinates we can write n R = Rijk ;ndx i dx j dx k j, Then the second Bianchi identity can be written as Rijk ;n + Rjnk ;i + Rnik ;j = The Riemann curvature tensor Now suppose (M, g) be a Riemannian manifod and the Levi-Civita connection. As ast time, by using the Riemannian metric g one can convert the (1, 3)-tensor R to a (0, 4)-tensor Rm Γ( 4 T M): Rm(X, Y, Z, W ) = g(r(x, Y )Z, W ). We sha ca Rm the Riemann curvature tensor of (M, g). Locay if we write Rm = R ijk dx i dx j dx k dx, then R ijk = Rm( i, j, k, ) = g(rijk m m, ) = g m Rijk m. In other words, the Riemannian metric ower one of the the index. Obviousy one can rewrite the identities (1) and (2) using Rm as Rm(X, Y, Z, W ) + Rm(Y, X, Z, W ) = 0, Rm(X, Y, Z, W ) + Rm(Y, Z, X, W ) + Rm(Z, X, Y, W ) = 0, or in oca coordinates as R ijk = R jik, R ijk + R jki + R kij = 0. Simiary the second Bianchi identity can be written in terms of Rm as ( X Rm)(Y, Z, W, V ) + ( Y Rm)(Z, X, W, V ) + ( Z Rm)(X, Y, W, V ) = 0,
4 4 LECTURE 6: THE RIEMANN CURVATURE TENSOR and if we denote R ijk;n = ( n R)( i, j, k, ), then R ijk;n + R jnk;i + R nik;j = 0. Exampe. The Riemann curvature tensor for S n (equiped with the standard round metric) is Rm(X, Y, Z, W ) = X, Z Y, W Y, Z X, W. Note that this can be written as Rm = 1 2 g g where is the Kukarni-Nomizu product which takes 2 symmetric (0, 2)- tensor into one (0, 4)-tensor that has many nice symmetry properties: (T 1 T 2 )(X, Y, Z, W ) =T 1 (X, Z)T 2 (Y, W ) T 1 (Y, Z)T 2 (X, W ) T 1 (X, W )T 2 (Y, Z) + T 1 (Y, W )T 2 (X, Z).. By staring at the above exampe, one see that the Riemann curvature tensor Rm on the standard S n has even more (anti-)symmetries than the ones we have seen, e.g. one can exchange Z with W to get a negative sign, or even exchange X, Y with Z, W. In fact thest two (anti-)symmetries are consequneces of metric compatibiities, and thus hod in genera: Proposition 2.1. The Riemann curvature tensor Rm satisfies Rm(X, Y, Z, W ) = Rm(X, Y, W, Z), (3) Rm(X, Y, Z, W ) = Rm(Z, W, X, Y ). Proof. We first notice that if we denote f = Z, Z, then in other words, It foows So X Z, Z = Xf Z, X Z, X Z, Z = 1 2 Xf. X Y Z, Z = X Y Z, Z Y Z, X Z = 1 2 X(Y f) Y Z, X Z. Rm(X, Y, Z, Z) = R(X, Y )Z, Z = X Y Z + Y X Z + [X,Y ] Z, Z = 1 2 X(Y f) Y (Xf) + 1 [X, Y ]f = 0. 2 As a consequence, we get Rm(X, Y, Z, W ) + Rm(X, Y, W, Z) =Rm(X, Y, Z + W, Z + W ) Rm(X, Y, Z, Z) Rm(X, Y, W, W ) =0.
5 LECTURE 6: THE RIEMANN CURVATURE TENSOR 5 The second one is a consequence of the first one together with (1) and (2). In fact, by the first Bianchi identity (2) one has Rm(X, Y, Z, W ) + Rm(Y, Z, X, W ) + Rm(Z, X, Y, W ) = 0, Rm(Y, Z, W, X) + Rm(Z, W, Y, X) + Rm(W, Y, Z, X) = 0, Rm(Z, W, X, Y ) + Rm(W, X, Z, Y ) + Rm(X, Z, W, Y ) = 0, Rm(W, X, Y, Z) + Rm(X, Y, W, Z) + Rm(Y, W, X, Z) = 0, Summing the equations and using (1) as we as the first one in (3) that we just proved, the first two coumns cance out and we get Rm(Z, X, Y, W ) + Rm(W, Y, Z, X) = 0, which is equivaent to the second one in (3). Of course if one use oca coordinates, then the two identities in (3) can be rewritten as R ijk = R ijk, R ijk = R kij.
Riemannian geometry of noncommutative surfaces
JOURNAL OF MATHEMATICAL PHYSICS 49, 073511 2008 Riemannian geometry of noncommutative surfaces M. Chaichian, 1,a A. Tureanu, 1,b R. B. Zhang, 2,c and Xiao Zhang 3,d 1 Department of Physica Sciences, University
More informationLECTURE 8: THE SECTIONAL AND RICCI CURVATURES
LECTURE 8: THE SECTIONAL AND RICCI CURVATURES 1. The Sectional Curvature We start with some simple linear algebra. As usual we denote by ( V ) the set of 4-tensors that is anti-symmetric with respect to
More informationCompletion. is dense in H. If V is complete, then U(V) = H.
Competion Theorem 1 (Competion) If ( V V ) is any inner product space then there exists a Hibert space ( H H ) and a map U : V H such that (i) U is 1 1 (ii) U is inear (iii) UxUy H xy V for a xy V (iv)
More informationDifferential Complexes in Continuum Mechanics
Archive for Rationa Mechanics and Anaysis manuscript No. (wi be inserted by the editor) Arzhang Angoshtari Arash Yavari Differentia Compexes in Continuum Mechanics Abstract We study some differentia compexes
More informationON THE GEOMETRY OF TANGENT BUNDLE OF A (PSEUDO-) RIEMANNIAN MANIFOLD
ANALELE ŞTIINŢIFICE ALE UNIVERSITĂŢII AL.I.CUZA IAŞI Tomul XLIV, s.i.a, Matematică, 1998, f1 ON THE GEOMETRY OF TANGENT BUNDLE OF A (PSEUDO-) RIEMANNIAN MANIFOLD BY V. OPROIU and N. PAPAGHIUC 0. Introduction.
More information2M2. Fourier Series Prof Bill Lionheart
M. Fourier Series Prof Bi Lionheart 1. The Fourier series of the periodic function f(x) with period has the form f(x) = a 0 + ( a n cos πnx + b n sin πnx ). Here the rea numbers a n, b n are caed the Fourier
More informationSINGLE BASEPOINT SUBDIVISION SCHEMES FOR MANIFOLD-VALUED DATA: TIME-SYMMETRY WITHOUT SPACE-SYMMETRY
SINGLE BASEPOINT SUBDIVISION SCHEMES FOR MANIFOLD-VALUED DATA: TIME-SYMMETRY WITHOUT SPACE-SYMMETRY TOM DUCHAMP, GANG XIE, AND THOMAS YU Abstract. This paper estabishes smoothness resuts for a cass of
More informationFaculty of Engineering, Mathematics and Science School of Mathematics
Faculty of Engineering, Mathematics and Science School of Mathematics JS & SS Mathematics SS Theoretical Physics SS TSM Mathematics Module MA3429: Differential Geometry I Trinity Term 2018???, May??? SPORTS
More informationarxiv:math/ v1 [math.dg] 29 Sep 1998
Unknown Book Proceedings Series Volume 00, XXXX arxiv:math/9809167v1 [math.dg] 29 Sep 1998 A sequence of connections and a characterization of Kähler manifolds Mikhail Shubin Dedicated to Mel Rothenberg
More information1. Introduction In the same way like the Ricci solitons generate self-similar solutions to Ricci flow
Kragujevac Journal of Mathematics Volume 4) 018), Pages 9 37. ON GRADIENT η-einstein SOLITONS A. M. BLAGA 1 Abstract. If the potential vector field of an η-einstein soliton is of gradient type, using Bochner
More informationBASIC DIFFERENTIAL GEOMETRY: CONNECTIONS AND GEODESICS
BASIC DIFFERENTIAL GEOMETRY: CONNECTIONS AND GEODESICS WERNER BALLMANN Introduction I discuss basic features of connections on manifolds: torsion and curvature tensor, geodesics and exponential maps, and
More informationGravity theory on Poisson manifold with R-flux
Gravity theory on Poisson manifold with R-flux Hisayoshi MURAKI (University of Tsukuba) in collaboration with Tsuguhiko ASAKAWA (Maebashi Institute of Technology) Satoshi WATAMURA (Tohoku University) References
More informationIsometries, Local Isometries, Riemannian Coverings and Submersions, Killing Vector Fields
Chapter 16 Isometries, Local Isometries, Riemannian Coverings and Submersions, Killing Vector Fields 16.1 Isometries and Local Isometries Recall that a local isometry between two Riemannian manifolds M
More informationCHAPTER 1 PRELIMINARIES
CHAPTER 1 PRELIMINARIES 1.1 Introduction The aim of this chapter is to give basic concepts, preliminary notions and some results which we shall use in the subsequent chapters of the thesis. 1.2 Differentiable
More informationIsometries, Local Isometries, Riemannian Coverings and Submersions, Killing Vector Fields
Chapter 15 Isometries, Local Isometries, Riemannian Coverings and Submersions, Killing Vector Fields The goal of this chapter is to understand the behavior of isometries and local isometries, in particular
More informationIndex Notation for Vector Calculus
Index Notation for Vector Calculus by Ilan Ben-Yaacov and Francesc Roig Copyright c 2006 Index notation, also commonly known as subscript notation or tensor notation, is an extremely useful tool for performing
More informationConnections for noncommutative tori
Levi-Civita connections for noncommutative tori reference: SIGMA 9 (2013), 071 NCG Festival, TAMU, 2014 In honor of Henri, a long-time friend Connections One of the most basic notions in differential geometry
More informationarxiv:quant-ph/ v3 6 Jan 1995
arxiv:quant-ph/9501001v3 6 Jan 1995 Critique of proposed imit to space time measurement, based on Wigner s cocks and mirrors L. Diósi and B. Lukács KFKI Research Institute for Partice and Nucear Physics
More informationPHYS 110B - HW #1 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased
PHYS 110B - HW #1 Fa 2005, Soutions by David Pace Equations referenced as Eq. # are from Griffiths Probem statements are paraphrased [1.] Probem 6.8 from Griffiths A ong cyinder has radius R and a magnetization
More informationBERGMAN KERNEL ON COMPACT KÄHLER MANIFOLDS
BERGMAN KERNEL ON COMPACT KÄHLER MANIFOLDS SHOO SETO Abstract. These are the notes to an expository talk I plan to give at MGSC on Kähler Geometry aimed for beginning graduate students in hopes to motivate
More information$, (2.1) n="# #. (2.2)
Chapter. Eectrostatic II Notes: Most of the materia presented in this chapter is taken from Jackson, Chap.,, and 4, and Di Bartoo, Chap... Mathematica Considerations.. The Fourier series and the Fourier
More informationarxiv: v1 [math.qa] 31 Mar 2008
A Note on Fedosov Quantization arxiv:0803.4201v1 [math.qa] 31 Mar 2008 Kaus Bering 1 Institute for Theoretica Physics & Astrophysics Masaryk University Kotářská 2 CZ-611 37 Brno Czech Repubic October 25,
More informationFundamental Materials of Riemannian Geometry
Chapter 1 Fundamental aterials of Riemannian Geometry 1.1 Introduction In this chapter, we give fundamental materials in Riemannian geometry. In this book, we assume basic materials on manifolds. We give,
More informationCourse 2BA1, Section 11: Periodic Functions and Fourier Series
Course BA, 8 9 Section : Periodic Functions and Fourier Series David R. Wikins Copyright c David R. Wikins 9 Contents Periodic Functions and Fourier Series 74. Fourier Series of Even and Odd Functions...........
More informationIsometric Immersions into Hyperbolic 3-Space
Isometric Immersions into Hyperbolic 3-Space Andrew Gallatin 18 June 016 Mathematics Department California Polytechnic State University San Luis Obispo APPROVAL PAGE TITLE: AUTHOR: Isometric Immersions
More informationVI.G Exact free energy of the Square Lattice Ising model
VI.G Exact free energy of the Square Lattice Ising mode As indicated in eq.(vi.35), the Ising partition function is reated to a sum S, over coections of paths on the attice. The aowed graphs for a square
More informationSOME ALMOST COMPLEX STRUCTURES WITH NORDEN METRIC ON THE TANGENT BUNDLE OF A SPACE FORM
ANALELE ŞTIINŢIFICE ALE UNIVERSITĂŢII AL.I.CUZA IAŞI Tomul XLVI, s.i a, Matematică, 2000, f.1. SOME ALMOST COMPLEX STRUCTURES WITH NORDEN METRIC ON THE TANGENT BUNDLE OF A SPACE FORM BY N. PAPAGHIUC 1
More informationDifferential Geometry MTG 6257 Spring 2018 Problem Set 4 Due-date: Wednesday, 4/25/18
Differential Geometry MTG 6257 Spring 2018 Problem Set 4 Due-date: Wednesday, 4/25/18 Required problems (to be handed in): 2bc, 3, 5c, 5d(i). In doing any of these problems, you may assume the results
More informationMath 124B January 31, 2012
Math 124B January 31, 212 Viktor Grigoryan 7 Inhomogeneous boundary vaue probems Having studied the theory of Fourier series, with which we successfuy soved boundary vaue probems for the homogeneous heat
More informationarxiv: v2 [math.dg] 3 Sep 2014
HOLOMORPHIC HARMONIC MORPHISMS FROM COSYMPLECTIC ALMOST HERMITIAN MANIFOLDS arxiv:1409.0091v2 [math.dg] 3 Sep 2014 SIGMUNDUR GUDMUNDSSON version 2.017-3 September 2014 Abstract. We study 4-dimensional
More informationRepresentation theory and the X-ray transform
AMSI Summer School on Integral Geometry and Imaging at the University of New England, Lecture 1 p. 1/18 Representation theory and the X-ray transform Differential geometry on real and complex projective
More informationEECS 117 Homework Assignment 3 Spring ω ω. ω ω. ω ω. Using the values of the inductance and capacitance, the length of 2 cm corresponds 1.5π.
EES 7 Homework Assignment Sprg 4. Suppose the resonant frequency is equa to ( -.5. The oad impedance is If, is equa to ( ( The ast equaity hods because ( -.5. Furthermore, ( Usg the vaues of the ductance
More informationarxiv:gr-qc/ v1 12 Jul 1994
5 July 1994 gr-qc/9407012 PARAMETRIC MANIFOLDS II: Intrinsic Approach arxiv:gr-qc/9407012v1 12 Jul 1994 Stuart Boersma Department of Mathematics, Oregon State University, Corvallis, OR 97331, USA 1 boersma@math.orst.edu
More informationRiemannian Curvature Functionals: Lecture I
Riemannian Curvature Functionals: Lecture I Jeff Viaclovsky Park City athematics Institute July 16, 2013 Overview of lectures The goal of these lectures is to gain an understanding of critical points of
More information5.2 The Levi-Civita Connection on Surfaces. 1 Parallel transport of vector fields on a surface M
5.2 The Levi-Civita Connection on Surfaces In this section, we define the parallel transport of vector fields on a surface M, and then we introduce the concept of the Levi-Civita connection, which is also
More informationPHYS 4390: GENERAL RELATIVITY NON-COORDINATE BASIS APPROACH
PHYS 4390: GENERAL RELATIVITY NON-COORDINATE BASIS APPROACH 1. Differential Forms To start our discussion, we will define a special class of type (0,r) tensors: Definition 1.1. A differential form of order
More information1.3 LECTURE 3. Vector Product
12 CHAPTER 1. VECTOR ALGEBRA Example. Let L be a line x x 1 a = y y 1 b = z z 1 c passing through a point P 1 and parallel to the vector N = a i +b j +c k. The equation of the plane passing through the
More informationArgument shift method and sectional operators: applications to differential geometry
Loughborough University Institutional Repository Argument shift method and sectional operators: applications to differential geometry This item was submitted to Loughborough University's Institutional
More information1 Curvature of submanifolds of Euclidean space
Curvature of submanifolds of Euclidean space by Min Ru, University of Houston 1 Curvature of submanifolds of Euclidean space Submanifold in R N : A C k submanifold M of dimension n in R N means that for
More informationRiemannian Manifolds
Chapter 25 Riemannian Manifolds Our ultimate goal is to study abstract surfaces that is 2-dimensional manifolds which have a notion of metric compatible with their manifold structure see Definition 2521
More informationt, H = 0, E = H E = 4πρ, H df = 0, δf = 4πJ.
Lecture 3 Cohomologies, curvatures Maxwell equations The Maxwell equations for electromagnetic fields are expressed as E = H t, H = 0, E = 4πρ, H E t = 4π j. These equations can be simplified if we use
More informationDIFFERENTIAL GEOMETRY. LECTURE 12-13,
DIFFERENTIAL GEOMETRY. LECTURE 12-13, 3.07.08 5. Riemannian metrics. Examples. Connections 5.1. Length of a curve. Let γ : [a, b] R n be a parametried curve. Its length can be calculated as the limit of
More information1.4 LECTURE 4. Tensors and Vector Identities
16 CHAPTER 1. VECTOR ALGEBRA 1.3.2 Triple Product The triple product of three vectors A, B and C is defined by In tensor notation it is A ( B C ) = [ A, B, C ] = A ( B C ) i, j,k=1 ε i jk A i B j C k =
More informationLESSON 7.1 FACTORING POLYNOMIALS I
LESSON 7.1 FACTORING POLYNOMIALS I LESSON 7.1 FACTORING POLYNOMIALS I 293 OVERVIEW Here s what you ll learn in this lesson: Greatest Common Factor a. Finding the greatest common factor (GCF) of a set of
More informationPerelman s Dilaton. Annibale Magni (TU-Dortmund) April 26, joint work with M. Caldarelli, G. Catino, Z. Djadly and C.
Annibale Magni (TU-Dortmund) April 26, 2010 joint work with M. Caldarelli, G. Catino, Z. Djadly and C. Mantegazza Topics. Topics. Fundamentals of the Ricci flow. Topics. Fundamentals of the Ricci flow.
More informationSpacetime Geometry. Beijing International Mathematics Research Center 2007 Summer School
Spacetime Geometry Beijing International Mathematics Research Center 2007 Summer School Gregory J. Galloway Department of Mathematics University of Miami October 29, 2007 1 Contents 1 Pseudo-Riemannian
More informationWEAK CONTINUITY OF THE GAUSS-CODAZZI-RICCI SYSTEM FOR ISOMETRIC EMBEDDING
WEAK CONTINUITY OF THE GAUSS-CODAZZI-RICCI SYSTEM FOR ISOMETRIC EMBEDDING GUI-QIANG CHEN, MARSHALL SLEMROD, AND DEHUA WANG Abstract. We estabish the wea continuity of the Gauss-Coddazi-Ricci system for
More informationCurvature homogeneity of type (1, 3) in pseudo-riemannian manifolds
Curvature homogeneity of type (1, 3) in pseudo-riemannian manifolds Cullen McDonald August, 013 Abstract We construct two new families of pseudo-riemannian manifolds which are curvature homegeneous of
More informationRiemannian Manifolds
Riemannian Manifolds Joost van Geffen Supervisor: Gil Cavalcanti June 12, 2017 Bachelor thesis for Mathematics and Physics Contents 1 Introduction 2 2 Riemannian manifolds 4 2.1 Preliminary Definitions.....................................
More information7 Curvature of a connection
[under construction] 7 Curvature of a connection 7.1 Theorema Egregium Consider the derivation equations for a hypersurface in R n+1. We are mostly interested in the case n = 2, but shall start from the
More informationChapter 12. Connections on Manifolds
Chapter 12 Connections on Manifolds 12.1 Connections on Manifolds Given a manifold, M, in general, for any two points, p, q 2 M, thereisno natural isomorphismbetween the tangent spaces T p M and T q M.
More informationLECTURE NOTES 8 THE TRACELESS SYMMETRIC TENSOR EXPANSION AND STANDARD SPHERICAL HARMONICS
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Physics 8.07: Eectromagnetism II October, 202 Prof. Aan Guth LECTURE NOTES 8 THE TRACELESS SYMMETRIC TENSOR EXPANSION AND STANDARD SPHERICAL HARMONICS
More informationLecture Notes 4: Fourier Series and PDE s
Lecture Notes 4: Fourier Series and PDE s 1. Periodic Functions A function fx defined on R is caed a periodic function if there exists a number T > such that fx + T = fx, x R. 1.1 The smaest number T for
More informationarxiv: v1 [math.dg] 19 Apr 2016
ON THREE DIMENSIONAL AFFINE SZABÓ MANIFOLDS arxiv:1604.05422v1 [math.dg] 19 Apr 2016 ABDOUL SALAM DIALLO*, SILAS LONGWAP**, FORTUNÉ MASSAMBA*** ABSTRACT. In this paper, we consider the cyclic parallel
More informationINTEGRALSATSER VEKTORANALYS. (indexräkning) Kursvecka 4. and CARTESIAN TENSORS. Kapitel 8 9. Sidor NABLA OPERATOR,
VEKTORANALYS Kursvecka 4 NABLA OPERATOR, INTEGRALSATSER and CARTESIAN TENSORS (indexräkning) Kapitel 8 9 Sidor 83 98 TARGET PROBLEM In the plasma there are many particles (10 19, 10 20 per m 3 ), strong
More informationNOISE-INDUCED STABILIZATION OF STOCHASTIC DIFFERENTIAL EQUATIONS
NOISE-INDUCED STABILIZATION OF STOCHASTIC DIFFERENTIAL EQUATIONS TONY ALLEN, EMILY GEBHARDT, AND ADAM KLUBALL 3 ADVISOR: DR. TIFFANY KOLBA 4 Abstract. The phenomenon of noise-induced stabiization occurs
More informationNIELINIOWA OPTYKA MOLEKULARNA
NIELINIOWA OPTYKA MOLEKULARNA chapter 1 by Stanisław Kielich translated by:tadeusz Bancewicz http://zon8.physd.amu.edu.pl/~tbancewi Poznan,luty 2008 ELEMENTS OF THE VECTOR AND TENSOR ANALYSIS Reference
More informationLECTURE 9: MOVING FRAMES IN THE NONHOMOGENOUS CASE: FRAME BUNDLES. 1. Introduction
LECTURE 9: MOVING FRAMES IN THE NONHOMOGENOUS CASE: FRAME BUNDLES 1. Introduction Until now we have been considering homogenous spaces G/H where G is a Lie group and H is a closed subgroup. The natural
More informationDIFFERENTIAL GEOMETRY, LECTURE 16-17, JULY 14-17
DIFFERENTIAL GEOMETRY, LECTURE 16-17, JULY 14-17 6. Geodesics A parametrized line γ : [a, b] R n in R n is straight (and the parametrization is uniform) if the vector γ (t) does not depend on t. Thus,
More informationLeibniz cohomology and the calculus of variations
Differential Geometry and its Applications 21 24 113 126 www.elsevier.com/locate/difgeo Leibniz cohomology and the calculus of variations Jerry M. Lodder 1 Mathematical Sciences, Department 3MB, New Mexico
More informationMATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES
MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES Separation of variabes is a method to sove certain PDEs which have a warped product structure. First, on R n, a inear PDE of order m is
More informationRiemannian geometry of the twistor space of a symplectic manifold
Riemannian geometry of the twistor space of a symplectic manifold R. Albuquerque rpa@uevora.pt Departamento de Matemática, Universidade de Évora Évora, Portugal September 004 0.1 The metric In this short
More informationON THE GEOMETRY OF CONFORMAL FOLIATIONS WITH MINIMAL LEAVES
ON THE GEOMETRY OF CONFORMAL FOLIATIONS WITH MINIMAL LEAVES JOE OLIVER Master s thesis 015:E39 Faculty of Science Centre for Mathematical Sciences Mathematics CENTRUM SCIENTIARUM MATHEMATICARUM Abstract
More informationJune 21, Peking University. Dual Connections. Zhengchao Wan. Overview. Duality of connections. Divergence: general contrast functions
Dual Peking University June 21, 2016 Divergences: Riemannian connection Let M be a manifold on which there is given a Riemannian metric g =,. A connection satisfying Z X, Y = Z X, Y + X, Z Y (1) for all
More information1 First and second variational formulas for area
1 First and second variational formulas for area In this chapter, we will derive the first and second variational formulas for the area of a submanifold. This will be useful in our later discussion on
More informationGauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law
Gauss Law 1. Review on 1) Couomb s Law (charge and force) 2) Eectric Fied (fied and force) 2. Gauss s Law: connects charge and fied 3. Appications of Gauss s Law Couomb s Law and Eectric Fied Couomb s
More informationJackson 4.10 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell
Jackson 4.10 Homework Probem Soution Dr. Christopher S. Baird University of Massachusetts Lowe PROBLEM: Two concentric conducting spheres of inner and outer radii a and b, respectivey, carry charges ±.
More informationHilbert s Metric and Gromov Hyperbolicity
Hilbert s Metric and Gromov Hyperbolicity Andrew Altman May 13, 2014 1 1 HILBERT METRIC 2 1 Hilbert Metric The Hilbert metric is a distance function defined on a convex bounded subset of the n-dimensional
More informationIntrinsic Differential Geometry with Geometric Calculus
MM Research Preprints, 196 205 MMRC, AMSS, Academia Sinica No. 23, December 2004 Intrinsic Differential Geometry with Geometric Calculus Hongbo Li and Lina Cao Mathematics Mechanization Key Laboratory
More informationCHAPTER 7 DIV, GRAD, AND CURL
CHAPTER 7 DIV, GRAD, AND CURL 1 The operator and the gradient: Recall that the gradient of a differentiable scalar field ϕ on an open set D in R n is given by the formula: (1 ϕ = ( ϕ, ϕ,, ϕ x 1 x 2 x n
More informationMat 1501 lecture notes, penultimate installment
Mat 1501 ecture notes, penutimate instament 1. bounded variation: functions of a singe variabe optiona) I beieve that we wi not actuay use the materia in this section the point is mainy to motivate the
More information6 Wave Equation on an Interval: Separation of Variables
6 Wave Equation on an Interva: Separation of Variabes 6.1 Dirichet Boundary Conditions Ref: Strauss, Chapter 4 We now use the separation of variabes technique to study the wave equation on a finite interva.
More informationSection 2. Basic formulas and identities in Riemannian geometry
Section 2. Basic formulas and identities in Riemannian geometry Weimin Sheng and 1. Bianchi identities The first and second Bianchi identities are R ijkl + R iklj + R iljk = 0 R ijkl,m + R ijlm,k + R ijmk,l
More informationPattern Frequency Sequences and Internal Zeros
Advances in Appied Mathematics 28, 395 420 (2002 doi:10.1006/aama.2001.0789, avaiabe onine at http://www.ideaibrary.com on Pattern Frequency Sequences and Interna Zeros Mikós Bóna Department of Mathematics,
More informationUNIVERSITY OF DUBLIN
UNIVERSITY OF DUBLIN TRINITY COLLEGE JS & SS Mathematics SS Theoretical Physics SS TSM Mathematics Faculty of Engineering, Mathematics and Science school of mathematics Trinity Term 2015 Module MA3429
More informationORTHOGONAL MULTI-WAVELETS FROM MATRIX FACTORIZATION
J. Korean Math. Soc. 46 2009, No. 2, pp. 281 294 ORHOGONAL MLI-WAVELES FROM MARIX FACORIZAION Hongying Xiao Abstract. Accuracy of the scaing function is very crucia in waveet theory, or correspondingy,
More informationLINEAR CONNECTIONS ON NORMAL ALMOST CONTACT MANIFOLDS WITH NORDEN METRIC 1
LINEAR CONNECTIONS ON NORMAL ALMOST CONTACT MANIFOLDS WITH NORDEN METRIC 1 Marta Teofilova Abstract. Families of linear connections are constructed on almost contact manifolds with Norden metric. An analogous
More informationSUPPLEMENTARY MATERIAL TO INNOVATED SCALABLE EFFICIENT ESTIMATION IN ULTRA-LARGE GAUSSIAN GRAPHICAL MODELS
ISEE 1 SUPPLEMENTARY MATERIAL TO INNOVATED SCALABLE EFFICIENT ESTIMATION IN ULTRA-LARGE GAUSSIAN GRAPHICAL MODELS By Yingying Fan and Jinchi Lv University of Southern Caifornia This Suppementary Materia
More informationContact Metric Manifold Admitting Semi-Symmetric Metric Connection
International Journal of Mathematics Research. ISSN 0976-5840 Volume 6, Number 1 (2014), pp. 37-43 International Research Publication House http://www.irphouse.com Contact Metric Manifold Admitting Semi-Symmetric
More informationA NOTE ON QUASI-STATIONARY DISTRIBUTIONS OF BIRTH-DEATH PROCESSES AND THE SIS LOGISTIC EPIDEMIC
(January 8, 2003) A NOTE ON QUASI-STATIONARY DISTRIBUTIONS OF BIRTH-DEATH PROCESSES AND THE SIS LOGISTIC EPIDEMIC DAMIAN CLANCY, University of Liverpoo PHILIP K. POLLETT, University of Queensand Abstract
More informationCarleman estimates for anisotropic hyperbolic systems in Riemannian manifolds and applications
Lecture Notes in Mathematical Sciences The University of Tokyo Carleman estimates for anisotropic hyperbolic systems in Riemannian manifolds and applications Mourad Bellassoued and Masahiro Yamamoto Graduate
More information338 Jin Suk Pak and Yang Jae Shin 2. Preliminaries Let M be a( + )-dimensional almost contact metric manifold with an almost contact metric structure
Comm. Korean Math. Soc. 3(998), No. 2, pp. 337-343 A NOTE ON CONTACT CONFORMAL CURVATURE TENSOR Jin Suk Pak* and Yang Jae Shin Abstract. In this paper we show that every contact metric manifold with vanishing
More informationTENSORS AND DIFFERENTIAL FORMS
TENSORS AND DIFFERENTIAL FORMS SVANTE JANSON UPPSALA UNIVERSITY Introduction The purpose of these notes is to give a quick course on tensors in general differentiable manifolds, as a complement to standard
More informationb n n=1 a n cos nx (3) n=1
Fourier Anaysis The Fourier series First some terminoogy: a function f(x) is periodic if f(x ) = f(x) for a x for some, if is the smaest such number, it is caed the period of f(x). It is even if f( x)
More informationNotes: Most of the material presented in this chapter is taken from Jackson, Chap. 2, 3, and 4, and Di Bartolo, Chap. 2. 2π nx i a. ( ) = G n.
Chapter. Eectrostatic II Notes: Most of the materia presented in this chapter is taken from Jackson, Chap.,, and 4, and Di Bartoo, Chap... Mathematica Considerations.. The Fourier series and the Fourier
More informationζ-determinants of Laplacians with Neumann and Dirichlet boundary conditions
INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL AND GENERAL J. Phys. A: Math. Gen. 38 (25) 8967 8977 doi:1.188/35-447/38/41/9 ζ-determinants of Lapacians with Neumann and Dirichet boundary
More informationTHINKING IN PYRAMIDS
ECS 178 Course Notes THINKING IN PYRAMIDS Kenneth I. Joy Institute for Data Anaysis and Visuaization Department of Computer Science University of Caifornia, Davis Overview It is frequenty usefu to think
More informationCS229 Lecture notes. Andrew Ng
CS229 Lecture notes Andrew Ng Part IX The EM agorithm In the previous set of notes, we taked about the EM agorithm as appied to fitting a mixture of Gaussians. In this set of notes, we give a broader view
More informationCovariant Derivative Lengths in Curvature Homogeneous Manifolds
Covariant Derivative Lengths in Curvature Homogeneous Manifolds Gabrielle Konyndyk August 7, 208 Abstract This research finds new families of pseudo-riemannian manifolds that are curvature homogeneous
More informationTwo-Stage Least Squares as Minimum Distance
Two-Stage Least Squares as Minimum Distance Frank Windmeijer Discussion Paper 17 / 683 7 June 2017 Department of Economics University of Bristo Priory Road Compex Bristo BS8 1TU United Kingdom Two-Stage
More information221B Lecture Notes Notes on Spherical Bessel Functions
Definitions B Lecture Notes Notes on Spherica Besse Functions We woud ike to sove the free Schrödinger equation [ h d r R(r) = h k R(r). () m r dr r m R(r) is the radia wave function ψ( x) = R(r)Y m (θ,
More informationMATH Topics in Applied Mathematics Lecture 12: Evaluation of determinants. Cross product.
MATH 311-504 Topics in Applied Mathematics Lecture 12: Evaluation of determinants. Cross product. Determinant is a scalar assigned to each square matrix. Notation. The determinant of a matrix A = (a ij
More information(f) is called a nearly holomorphic modular form of weight k + 2r as in [5].
PRODUCTS OF NEARLY HOLOMORPHIC EIGENFORMS JEFFREY BEYERL, KEVIN JAMES, CATHERINE TRENTACOSTE, AND HUI XUE Abstract. We prove that the product of two neary hoomorphic Hece eigenforms is again a Hece eigenform
More informationFRIEZE GROUPS IN R 2
FRIEZE GROUPS IN R 2 MAXWELL STOLARSKI Abstract. Focusing on the Eucidean pane under the Pythagorean Metric, our goa is to cassify the frieze groups, discrete subgroups of the set of isometries of the
More information5 Constructions of connections
[under construction] 5 Constructions of connections 5.1 Connections on manifolds and the Levi-Civita theorem We start with a bit of terminology. A connection on the tangent bundle T M M of a manifold M
More informationPartial permutation decoding for MacDonald codes
Partia permutation decoding for MacDonad codes J.D. Key Department of Mathematics and Appied Mathematics University of the Western Cape 7535 Bevie, South Africa P. Seneviratne Department of Mathematics
More informationTurbo Codes. Coding and Communication Laboratory. Dept. of Electrical Engineering, National Chung Hsing University
Turbo Codes Coding and Communication Laboratory Dept. of Eectrica Engineering, Nationa Chung Hsing University Turbo codes 1 Chapter 12: Turbo Codes 1. Introduction 2. Turbo code encoder 3. Design of intereaver
More informationThe Einstein Field Equations
The Einstein Field Equations on semi-riemannian manifolds, and the Schwarzschild solution Rasmus Leijon VT 2012 Examensarbete, 15hp Kandidatexamen i tillämpad matematik, 180hp Institutionen för matematik
More informationEinstein Field Equations (EFE)
Einstein Field Equations (EFE) 1 - General Relativity Origins In the 1910s, Einstein studied gravity. Following the reasoning of Faraday and Maxwell, he thought that if two objects are attracted to each
More informationAn H 2 type Riemannian metric on the space of planar curves
An H 2 type Riemannian metric on the space of panar curves Jayant hah Mathematics Department, Northeastern University, Boston MA emai: shah@neu.edu Abstract An H 2 type metric on the space of panar curves
More information