A Spectrally Accurate Calculus of Forms
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Arxiv:2009.07259V1 [Math.AP] 15 Sep 2020
A GEOMETRIC TRAPPING APPROACH TO GLOBAL REGULARITY FOR 2D NAVIER-STOKES ON MANIFOLDS AYNUR BULUT AND KHANG MANH HUYNH Abstract. In this paper, we use frequency decomposition techniques to give a direct proof of global existence and regularity for the Navier-Stokes equations on two-dimensional Riemannian manifolds without boundary. Our techniques are inspired by an approach of Mattingly and Sinai [15] which was developed in the context of periodic boundary conditions on a flat background, and which is based on a maximum principle for Fourier coefficients. The extension to general manifolds requires several new ideas, connected to the less favorable spectral localization properties in our setting. Our argu- ments make use of frequency projection operators, multilinear estimates that originated in the study of the non-linear Schr¨odingerequation, and ideas from microlocal analysis. 1. Introduction Let (M; g) be a closed, oriented, connected, compact smooth two-dimensional Riemannian manifold, and let X(M) denote the space of smooth vector fields on M. We consider the incompressible Navier-Stokes equations on M, with viscosity coefficient ν > 0, @ U + div (U ⊗ U) − ν∆ U = − grad p in M t M ; (1) div U = 0 in M with initial data U0 2 X(M); where I ⊂ R is an open interval, and where U : I ! X(M) and p : I × M ! R represent the velocity and pressure of the fluid, respectively. Here, the operator ∆M is any choice of Laplacian defined on vector fields on M, discussed below. arXiv:2009.07259v1 [math.AP] 15 Sep 2020 The theory of two-dimensional fluid flows on flat spaces is well-developed, and a variety of global regularity results are well-known. -
Lecture Notes in Mathematics
Lecture Notes in Mathematics Edited by A. Dold and B. Eckmann Subseries: Mathematisches Institut der Universit~it und Max-Planck-lnstitut for Mathematik, Bonn - voL 5 Adviser: E Hirzebruch 1111 Arbeitstagung Bonn 1984 Proceedings of the meeting held by the Max-Planck-lnstitut fur Mathematik, Bonn June 15-22, 1984 Edited by E Hirzebruch, J. Schwermer and S. Suter I IIII Springer-Verlag Berlin Heidelberg New York Tokyo Herausgeber Friedrich Hirzebruch Joachim Schwermer Silke Suter Max-Planck-lnstitut fLir Mathematik Gottfried-Claren-Str. 26 5300 Bonn 3, Federal Republic of Germany AMS-Subject Classification (1980): 10D15, 10D21, 10F99, 12D30, 14H10, 14H40, 14K22, 17B65, 20G35, 22E47, 22E65, 32G15, 53C20, 57 N13, 58F19 ISBN 3-54045195-8 Springer-Verlag Berlin Heidelberg New York Tokyo ISBN 0-387-15195-8 Springer-Verlag New York Heidelberg Berlin Tokyo CIP-Kurztitelaufnahme der Deutschen Bibliothek. Mathematische Arbeitstagung <25. 1984. Bonn>: Arbeitstagung Bonn: 1984; proceedings of the meeting, held in Bonn, June 15-22, 1984 / [25. Math. Arbeitstagung]. Ed. by E Hirzebruch ... - Berlin; Heidelberg; NewYork; Tokyo: Springer, 1985. (Lecture notes in mathematics; Vol. 1t11: Subseries: Mathematisches I nstitut der U niversit~it und Max-Planck-lnstitut for Mathematik Bonn; VoL 5) ISBN 3-540-t5195-8 (Berlin...) ISBN 0-387q5195-8 (NewYork ...) NE: Hirzebruch, Friedrich [Hrsg.]; Lecture notes in mathematics / Subseries: Mathematischee Institut der UniversitAt und Max-Planck-lnstitut fur Mathematik Bonn; HST This work ts subject to copyright. All rights are reserved, whether the whole or part of the material is concerned, specifically those of translation, reprinting, re~use of illustrations, broadcasting, reproduction by photocopying machine or similar means, and storage in data banks. -
Differential Forms Diff Geom II, WS 2015/16
J.M. Sullivan, TU Berlin B: Differential Forms Diff Geom II, WS 2015/16 B. DIFFERENTIAL FORMS instance, if S has k elements this gives a k-dimensional vector space with S as basis. We have already seen one-forms (covector fields) on a Given vector spaces V and W, let F be the free vector space over the set V × W. (This consists of formal sums manifold. In general, a k-form is a field of alternating k- P linear forms on the tangent spaces of a manifold. Forms ai(vi, wi) but ignores all the structure we have on the set are the natural objects for integration: a k-form can be in- V × W.) Now let R ⊂ F be the linear subspace spanned by tegrated over an oriented k-submanifold. We start with ten- all elements of the form: sor products and the exterior algebra of multivectors. (v + v0, w) − (v, w) − (v0, w), (v, w + w0) − (v, w) − (v, w0), (av, w) − a(v, w), (v, aw) − a(v, w). B1. Tensor products These correspond of course to the bilinearity conditions Recall that, if V, W and X are vector spaces, then a map we started with. The quotient vector space F/R will be the b: V × W → X is called bilinear if tensor product V ⊗ W. We have started with all possible v ⊗ w as generators and thrown in just enough relations to b(v + v0, w) = b(v, w) + b(v0, w), make the map (v, w) 7→ v ⊗ w be bilinear. b(v, w + w0) = b(v, w) + b(v, w0), The tensor product is commutative: there is a natural linear isomorphism V⊗W → W⊗V such that v⊗w 7→ w⊗v. -
Applications of the Hodge Decomposition to Biological Structure and Function Modeling
Applications of the Hodge Decomposition to Biological Structure and Function Modeling Andrew Gillette joint work with Chandrajit Bajaj and John Luecke Department of Mathematics, Institute of Computational Engineering and Sciences University of Texas at Austin, Austin, Texas 78712, USA http://www.math.utexas.edu/users/agillette university-logo Computational Visualization Center , I C E S ( DepartmentThe University of Mathematics, of Texas atInstitute Austin of Computational EngineeringDec2008 and Sciences 1/32 University Introduction Molecular dynamics are governed by electrostatic forces of attraction and repulsion. These forces are described as the solutions of a PDE over the molecular surfaces. Molecular surfaces may have complicated topological features affecting the solution. The Hodge Decomposition relates topological properties of the surface to solution spaces of PDEs over the surface. ∼ (space of forms) = (solutions to ∆u = f 6≡ 0) ⊕ (non-trivial deRham classes)university-logo Computational Visualization Center , I C E S ( DepartmentThe University of Mathematics, of Texas atInstitute Austin of Computational EngineeringDec2008 and Sciences 2/32 University Outline 1 The Hodge Decomposition for smooth differential forms 2 The Hodge Decomposition for discrete differential forms 3 Applications of the Hodge Decomposition to biological modeling university-logo Computational Visualization Center , I C E S ( DepartmentThe University of Mathematics, of Texas atInstitute Austin of Computational EngineeringDec2008 and Sciences 3/32 University Outline 1 The Hodge Decomposition for smooth differential forms 2 The Hodge Decomposition for discrete differential forms 3 Applications of the Hodge Decomposition to biological modeling university-logo Computational Visualization Center , I C E S ( DepartmentThe University of Mathematics, of Texas atInstitute Austin of Computational EngineeringDec2008 and Sciences 4/32 University Differential Forms Let Ω denote a smooth n-manifold and Tx (Ω) the tangent space of Ω at x. -
[Math.GT] 7 Mar 2013 Ae Stems Ftetinuaintnst Zero
GEOMETRIC STRUCTURES ON THE COCHAINS OF A MANIFOLD SCOTT O. WILSON Abstract. In this paper we develop several algebraic structures on the sim- plicial cochains of a triangulated manifold that are analogues of objects in differential geometry. We study a cochain product and prove several state- ments about its convergence to the wedge product on differential forms. Also, for cochains with an inner product, we define a combinatorial Hodge star oper- ator, and describe some applications, including a combinatorial period matrix for surfaces. We show that for a particularly nice cochain inner product, these combinatorial structures converge to their continuum analogues as the mesh of a triangulation tends to zero. 1. Introduction In this paper we develop combinatorial analogues of several objects in differential and complex geometry, including the Hodge star operator and the period matrix of a Riemann surface. We define these structures on the appropriate combinatorial analogue of differential forms, namely simplicial cochains. As we recall in section 3, the two essential ingredients to the smooth Hodge star operator are Poincar´eDuality and a metric, or inner product. We’ll define the combinatorial star operator in much the same way, using both an inner product and Poincar´eDuality, expressed on cochains in the form of a (graded) commutative product. Using the inner product introduced in [6], we prove the following: Theorem 1.1. The combinatorial star operator, defined on the simplicial cochains of a triangulated Riemannian manifold, converges to the smooth Hodge star operator as the mesh of the triangulation tends to zero. We show in section 7 that, on a closed surface, this combinatorial star operator gives rise to a combinatorial period matrix and prove: arXiv:math/0505227v4 [math.GT] 7 Mar 2013 Theorem 1.2. -
Linearization Via the Lie Derivative ∗
Electron. J. Diff. Eqns., Monograph 02, 2000 http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu or ejde.math.unt.edu (login: ftp) Linearization via the Lie Derivative ∗ Carmen Chicone & Richard Swanson Abstract The standard proof of the Grobman–Hartman linearization theorem for a flow at a hyperbolic rest point proceeds by first establishing the analogous result for hyperbolic fixed points of local diffeomorphisms. In this exposition we present a simple direct proof that avoids the discrete case altogether. We give new proofs for Hartman’s smoothness results: A 2 flow is 1 linearizable at a hyperbolic sink, and a 2 flow in the C C C plane is 1 linearizable at a hyperbolic rest point. Also, we formulate C and prove some new results on smooth linearization for special classes of quasi-linear vector fields where either the nonlinear part is restricted or additional conditions on the spectrum of the linear part (not related to resonance conditions) are imposed. Contents 1 Introduction 2 2 Continuous Conjugacy 4 3 Smooth Conjugacy 7 3.1 Hyperbolic Sinks . 10 3.1.1 Smooth Linearization on the Line . 32 3.2 Hyperbolic Saddles . 34 4 Linearization of Special Vector Fields 45 4.1 Special Vector Fields . 46 4.2 Saddles . 50 4.3 Infinitesimal Conjugacy and Fiber Contractions . 50 4.4 Sources and Sinks . 51 ∗Mathematics Subject Classifications: 34-02, 34C20, 37D05, 37G10. Key words: Smooth linearization, Lie derivative, Hartman, Grobman, hyperbolic rest point, fiber contraction, Dorroh smoothing. c 2000 Southwest Texas State University. Submitted November 14, 2000. -
Operator-Valued Tensors on Manifolds: a Framework for Field
Operator-Valued Tensors on Manifolds: A Framework for Field Quantization 1 2 H. Feizabadi , N. Boroojerdian ∗ 1,2Department of pure Mathematics, Faculty of Mathematics and Computer Science, Amirkabir University of Technology, No. 424, Hafez Ave., Tehran, Iran. Abstract In this paper we try to prepare a framework for field quantization. To this end, we aim to replace the field of scalars R by self-adjoint elements of a commu- tative C⋆-algebra, and reach an appropriate generalization of geometrical concepts on manifolds. First, we put forward the concept of operator-valued tensors and extend semi-Riemannian metrics to operator valued metrics. Then, in this new geometry, some essential concepts of Riemannian geometry such as curvature ten- sor, Levi-Civita connection, Hodge star operator, exterior derivative, divergence,... will be considered. Keywords: Operator-valued tensors, Operator-Valued Semi-Riemannian Met- rics, Levi-Civita Connection, Curvature, Hodge star operator MSC(2010): Primary: 65F05; Secondary: 46L05, 11Y50. 0 Introduction arXiv:1501.05065v2 [math-ph] 27 Jan 2015 The aim of the present paper is to extend the theory of semi-Riemannian metrics to operator-valued semi-Riemannian metrics, which may be used as a framework for field quantization. Spaces of linear operators are directly related to C∗-algebras, so C∗- algebras are considered as a basic concept in this article. This paper has its roots in Hilbert C⋆-modules, which are frequently used in the theory of operator algebras, allowing one to obtain information about C⋆-algebras by studying Hilbert C⋆-modules over them. Hilbert C⋆-modules provide a natural generalization of Hilbert spaces arising when the field of scalars C is replaced by an arbitrary C⋆-algebra. -
Hamilton's Ricci Flow
The University of Melbourne, Department of Mathematics and Statistics Hamilton's Ricci Flow Nick Sheridan Supervisor: Associate Professor Craig Hodgson Second Reader: Professor Hyam Rubinstein Honours Thesis, November 2006. Abstract The aim of this project is to introduce the basics of Hamilton's Ricci Flow. The Ricci flow is a pde for evolving the metric tensor in a Riemannian manifold to make it \rounder", in the hope that one may draw topological conclusions from the existence of such \round" metrics. Indeed, the Ricci flow has recently been used to prove two very deep theorems in topology, namely the Geometrization and Poincar´eConjectures. We begin with a brief survey of the differential geometry that is needed in the Ricci flow, then proceed to introduce its basic properties and the basic techniques used to understand it, for example, proving existence and uniqueness and bounds on derivatives of curvature under the Ricci flow using the maximum principle. We use these results to prove the \original" Ricci flow theorem { the 1982 theorem of Richard Hamilton that closed 3-manifolds which admit metrics of strictly positive Ricci curvature are diffeomorphic to quotients of the round 3-sphere by finite groups of isometries acting freely. We conclude with a qualitative discussion of the ideas behind the proof of the Geometrization Conjecture using the Ricci flow. Most of the project is based on the book by Chow and Knopf [6], the notes by Peter Topping [28] (which have recently been made into a book, see [29]), the papers of Richard Hamilton (in particular [9]) and the lecture course on Geometric Evolution Equations presented by Ben Andrews at the 2006 ICE-EM Graduate School held at the University of Queensland. -
Hodge Theory
HODGE THEORY PETER S. PARK Abstract. This exposition of Hodge theory is a slightly retooled version of the author's Harvard minor thesis, advised by Professor Joe Harris. Contents 1. Introduction 1 2. Hodge Theory of Compact Oriented Riemannian Manifolds 2 2.1. Hodge star operator 2 2.2. The main theorem 3 2.3. Sobolev spaces 5 2.4. Elliptic theory 11 2.5. Proof of the main theorem 14 3. Hodge Theory of Compact K¨ahlerManifolds 17 3.1. Differential operators on complex manifolds 17 3.2. Differential operators on K¨ahlermanifolds 20 3.3. Bott{Chern cohomology and the @@-Lemma 25 3.4. Lefschetz decomposition and the Hodge index theorem 26 Acknowledgments 30 References 30 1. Introduction Our objective in this exposition is to state and prove the main theorems of Hodge theory. In Section 2, we first describe a key motivation behind the Hodge theory for compact, closed, oriented Riemannian manifolds: the observation that the differential forms that satisfy certain par- tial differential equations depending on the choice of Riemannian metric (forms in the kernel of the associated Laplacian operator, or harmonic forms) turn out to be precisely the norm-minimizing representatives of the de Rham cohomology classes. This naturally leads to the statement our first main theorem, the Hodge decomposition|for a given compact, closed, oriented Riemannian manifold|of the space of smooth k-forms into the image of the Laplacian and its kernel, the sub- space of harmonic forms. We then develop the analytic machinery|specifically, Sobolev spaces and the theory of elliptic differential operators|that we use to prove the aforementioned decom- position, which immediately yields as a corollary the phenomenon of Poincar´eduality. -
On Lie Derivation of Spinors Against Arbitrary Tangent Vector Fields
On Lie derivation of spinors against arbitrary tangent vector fields Andras´ LASZL´ O´ [email protected] Wigner RCP, Budapest, Hungary (joint work with L.Andersson and I.Rácz) CERS8 Workshop Brno, 17th February 2018 On Lie derivation of spinors against arbitrary tangent vector fields – p. 1 Preliminaries Ordinary Lie derivation. Take a one-parameter group (φt)t∈R of diffeomorphisms over a manifold M. Lie derivation against that is defined on the smooth sections χ of the mixed tensor algebra of T (M) and T ∗(M), with the formula: L φ∗ χ := ∂t φ∗ −t χ t=0 It has explicit formula: on T (M) : Lu(χ)=[u,χ] , a on F (M) := M× R : Lu(χ)= u da (χ) , ∗ a a on T (M) : Lu(χ)= u da (χ) + d(u χa), where u is the unique tangent vector field underlying (φt)t∈R. The map u 7→ Lu is faithful Lie algebra representation. On Lie derivation of spinors against arbitrary tangent vector fields – p. 2 Lie derivation on a vector bundle. Take a vector bundle V (M) over M. Take a one-parameter group of diffeomorphisms of the total space of V (M), which preserves the vector bundle structure. The ∂t() against the flows of these are vector bundle Lie derivations. t=0 (I.Kolár,P.Michor,K.Slovák:ˇ Natural operations in differential geometry; Springer 1993) Explicit expression: take a preferred covariant derivation ∇, then over the sections χ of V (M) one can express these as ∇ A a A A B L χ = u ∇a χ − CB χ (u,C) That is: Lie derivations on a vector bundle are uniquely characterized by their horizontal a A part u ∇a and vertical part CB . -
Intrinsic Differential Geometry with Geometric Calculus
MM Research Preprints, 196{205 MMRC, AMSS, Academia Sinica No. 23, December 2004 Intrinsic Di®erential Geometry with Geometric Calculus Hongbo Li and Lina Cao Mathematics Mechanization Key Laboratory Academy of Mathematics and Systems Science Chinese Academy of Sciences Beijing 100080, China Abstract. Setting up a symbolic algebraic system is the ¯rst step in mathematics mechanization of any branch of mathematics. In this paper, we establish a compact symbolic algebraic framework for local geometric computing in intrinsic di®erential ge- ometry, by choosing only the Lie derivative and the covariant derivative as basic local di®erential operators. In this framework, not only geometric entities such as the curva- ture and torsion of an a±ne connection have elegant representations, but their involved local geometric computing can be simpli¯ed. Keywords: Intrinsic di®erential geometry, Cli®ord algebra, Mathematics mecha- nization, Symbolic geometric computing. 1. Introduction Mathematics mechanization focuses on solving mathematical problems with symbolic computation techniques, particularly on mathematical reasoning by algebraic manipulation of mathematical symbols. In di®erential geometry, the mechanization viz. mechanical the- orem proving, is initiated by [7] using local coordinate representation. On the other hand, in modern di®erential geometry the dominant algebraic framework is moving frames and di®erential forms [1], which are independent of local coordinates. For mechanical theorem proving in spatial surface theory, [3], [4], [5] proposed to use di®erential forms and moving frames as basic algebraic tools. It appears that di®erential geometry bene¯ts from both local coordinates and global invariants [6]. For extrinsic di®erential geometry, [2] proposed to use Cli®ord algebra and vector deriva- tive viz. -
3. Algebra of Vector Fields. Lie Derivatives
INTRODUCTION TO MANIFOLDS | III Algebra of vector fields. Lie derivative(s). 1. Notations. The space of all C1-smooth vector ¯elds on a manifold M is n denoted by X(M). If v 2 X(M) is a vector ¯eld, then v(x) 2 TxM ' R is its value at a point x 2 M. The flow of a vector ¯eld v is denoted by vt: 8t 2 R vt : M ! M is a smooth map (automorphism) of M taking a point x 2 M into the point vt(x) 2 M which is the t-endpoint of an integral trajectory for the ¯eld v, starting at the point x. | Problem 1. Prove that the flow maps for a ¯eld v on a compact manifold M form a one-parameter group: 8t; s 2 R vt+s = vt ± vs = vs ± vt; and all vt are di®eomorphisms of M. | Problem 2. What means the formula ¯ ¯ d ¯ s ¯ v = v ds s=0 and is it true? 2. Star conventions. The space of all C1-smooth functions is denoted by C1(M). If F : M ! M is a smooth map (not necessary a di®eomorphism), then there appears a contravariant map F ¤ : C1(M) ! C1(M);F ¤ : f 7! F ¤f; F ¤(x) = f(F (x)): If F : M ! N is a smooth map between two di®erent manifolds, then F ¤ : C1(N) ! C1(M): Note that the direction of the arrows is reversed! | Problem 3. Prove that C1(M) is a commutative associative algebra over R with respect to pointwise addition, subtraction and multiplication of functions.