Differential Geometry Andrzej Derdzinski
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Characterization of Exact Lumpability for Vector Fields on Smooth Manifolds
Preprint. Final version in: Differ.Geom.Appl. 48 (2016) 46-60 doi: 10.1016/j.difgeo.2016.06.001 Characterization of Exact Lumpability for Vector Fields on Smooth Manifolds Leonhard Horstmeyer∗ † Fatihcan M. Atay‡ Abstract We characterize the exact lumpability of smooth vector fields on smooth man- ifolds. We derive necessary and sufficient conditions for lumpability and express them from four different perspectives, thus simplifying and generalizing various re- sults from the literature that exist for Euclidean spaces. We introduce a partial connection on the pullback bundle that is related to the Bott connection and be- haves like a Lie derivative. The lumping conditions are formulated in terms of the differential of the lumping map, its covariant derivative with respect to the con- nection and their respective kernels. Some examples are discussed to illustrate the theory. PACS numbers: 02.40.-k, 02.30.Hq, 02.40.Hw AMS classification scheme numbers: 37C10, 34C40, 58A30, 53B05, 34A05 Keywords: lumping, aggregation, dimensional reduction, Bott connection 1 Introduction Dimensional reduction is an important aspect in the study of smooth dynamical systems and in particular in modeling with ordinary differential equations (ODEs). Often a reduction can elucidate key mechanisms, find decoupled subsystems, reveal conserved quantities, make the problem computationally tractable, or rid it from redundancies. A dimensional reduction by which micro state variables are aggregated into macro state variables also goes by the name of lumping. Starting from a micro state dynamics, this arXiv:1607.01237v2 [math.DG] 6 Jul 2016 aggregation induces a lumped dynamics on the macro state space. Whenever a non- trivial lumping, one that is neither the identity nor maps to a single point, confers the ∗Max Planck Institute for Mathematics in the Sciences, Inselstraße 22, 04103 Leipzig, Germany. -
Lorentzian Cobordisms, Compact Horizons and the Generic Condition
Lorentzian Cobordisms, Compact Horizons and the Generic Condition Eric Larsson Master of Science Thesis Stockholm, Sweden 2014 Lorentzian Cobordisms, Compact Horizons and the Generic Condition Eric Larsson Master’s Thesis in Mathematics (30 ECTS credits) Degree programme in Engineering Physics (300 credits) Royal Institute of Technology year 2014 Supervisor at KTH was Mattias Dahl Examiner was Mattias Dahl TRITA-MAT-E 2014:29 ISRN-KTH/MAT/E--14/29--SE Royal Institute of Technology School of Engineering Sciences KTH SCI SE-100 44 Stockholm, Sweden URL: www.kth.se/sci iii Abstract We consider the problem of determining which conditions are necessary for cobordisms to admit Lorentzian metrics with certain properties. In particu- lar, we prove a result originally due to Tipler without a smoothness hypothe- sis necessary in the original proof. In doing this, we prove that compact hori- zons in a smooth spacetime satisfying the null energy condition are smooth. We also prove that the ”generic condition” is indeed generic in the set of Lorentzian metrics on a given manifold. Acknowledgements I would like to thank my advisor Mattias Dahl for invaluable advice and en- couragement. Thanks also to Hans Ringström. Special thanks to Marc Nardmann for feedback on Chapter 2. Contents Contents iv 1 Lorentzian cobordisms 1 1.1 Existence of Lorentzian cobordisms . 2 1.2 Lorentzian cobordisms and causality . 4 1.3 Lorentzian cobordisms and energy conditions . 8 1.3.1 C 2 null hypersurfaces . 9 1.3.1.1 The null Weingarten map . 9 1.3.1.2 Generator flow on C 2 null hypersurfaces . -
The Holomorphic Φ-Sectional Curvature of Tangent Sphere Bundles with Sasakian Structures
ANALELE S¸TIINT¸IFICE ALE UNIVERSITAT¸II˘ \AL.I. CUZA" DIN IAS¸I (S.N.) MATEMATICA,˘ Tomul LVII, 2011, Supliment DOI: 10.2478/v10157-011-0004-5 THE HOLOMORPHIC '-SECTIONAL CURVATURE OF TANGENT SPHERE BUNDLES WITH SASAKIAN STRUCTURES BY S. L. DRUT¸ A-ROMANIUC˘ and V. OPROIU Abstract. We study the holomorphic '-sectional curvature of the natural diagonal tangent sphere bundles with Sasakian structures, determined by Drut¸a-Romaniuc˘ and Oproiu. After finding the explicit expressions for the components of the curvature tensor field and of the curvature tensor field corresponding to the Sasakian space forms, we find that there are no tangent sphere bundles of natural diagonal lift type of constant holomorphic '-sectional curvature. Mathematics Subject Classification 2000: 53C05, 53C15, 53C55. Key words: natural lift, tangent sphere bundle, Sasakian structure, holomorphic '-sectional curvature. 1. Introduction The geometry of the tangent sphere bundles of constant radius r, endowed with the metrics induced by some Riemannian metrics from the ambi- ent tangent bundle, was studied by authors like Abbassi, Boeckx, Cal- varuso, Kowalski, Munteanu, Park, Sekigawa, Sekizawa (see [1], [2], [4]-[7], [9], [12]-[14], [16]). In the most part of the papers, such as [4], [5] and [16], the metric considered on the tangent bundle TM was the Sasaki metric, but Boeckx noticed that the unit tangent bundle equipped with the induced Cheeger-Gromoll metric is isometric to the tangent sphere bun- dle T p1 M with the induced Sasaki metric. Then, in 2000, Kowalski and 2 Sekizawa showed how the geometry of the tangent sphere bundles depends on the radius (see [10]). -
Ricci Measure for Some Singular Riemannian Metrics
Math. Ann. (2016) 365:449–471 DOI 10.1007/s00208-015-1288-7 Mathematische Annalen Ricci measure for some singular Riemannian metrics John Lott1 Received: 10 April 2015 / Revised: 14 August 2015 / Published online: 4 September 2015 © Springer-Verlag Berlin Heidelberg 2015 Abstract We define the Ricci curvature, as a measure, for certain singular torsion- free connections on the tangent bundle of a manifold. The definition uses an integral formula and vector-valued half-densities. We give relevant examples in which the Ricci measure can be computed. In the time dependent setting, we give a weak notion of a Ricci flow solution on a manifold. 1 Introduction There has been much recent work about metric measure spaces with lower Ricci bounds, particularly the Ricci limit spaces that arise as measured Gromov–Hausdorff limits of smooth manifolds with a uniform lower Ricci bound. In this paper we address the question of whether one can make sense of the Ricci curvature itself on singular spaces. From one’s intuition about a two dimensional cone with total cone angle less than 2π, the Ricci curvature should exist at best as a measure. One natural approach toward a weak notion of Ricci curvature is to use an integral formula, such as the Bochner formula. The Bochner identity says that if ω1 and ω2 are smooth compactly supported 1-forms on a smooth Riemannian manifold M then ∗ ∗ ω1, Ric(ω2) = dω1, dω2+d ω1, d ω2−∇ω1, ∇ω2 dvol . (1.1) M B John Lott [email protected] 1 Department of Mathematics, University of California - Berkeley, Berkeley, CA 94720-3840, USA 123 450 J. -
On Manifolds of Negative Curvature, Geodesic Flow, and Ergodicity
ON MANIFOLDS OF NEGATIVE CURVATURE, GEODESIC FLOW, AND ERGODICITY CLAIRE VALVA Abstract. We discuss geodesic flow on manifolds of negative sectional curva- ture. We find that geodesic flow is ergodic on the tangent bundle of a manifold, and present the proof for both n = 2 on surfaces and general n. Contents 1. Introduction 1 2. Riemannian Manifolds 1 2.1. Geodesic Flow 2 2.2. Horospheres and Horocycle Flows 3 2.3. Curvature 4 2.4. Jacobi Fields 4 3. Anosov Flows 4 4. Ergodicity 5 5. Surfaces of Negative Curvature 6 5.1. Fuchsian Groups and Hyperbolic Surfaces 6 6. Geodesic Flow on Hyperbolic Surfaces 7 7. The Ergodicity of Geodesic Flow on Compact Manifolds of Negative Sectional Curvature 8 7.1. Foliations and Absolute Continuity 9 7.2. Proof of Ergodicity 12 Acknowledgments 14 References 14 1. Introduction We want to understand the behavior of geodesic flow on a manifold M of constant negative curvature. If we consider a vector in the unit tangent bundle of M, where does that vector go (or not go) when translated along its unique geodesic path. In a sense, we will show that the vector goes \everywhere," or that the vector visits a full measure subset of T 1M. 2. Riemannian Manifolds We first introduce some of the initial definitions and concepts that allow us to understand Riemannian manifolds. Date: August 2019. 1 2 CLAIRE VALVA Definition 2.1. If M is a differentiable manifold and α :(−, ) ! M is a dif- ferentiable curve, where α(0) = p 2 M, then the tangent vector to the curve α at t = 0 is a function α0(0) : D ! R, where d(f ◦ α) α0(0)f = j dt t=0 for f 2 D, where D is the set of functions on M that are differentiable at p. -
Thurston's Eight Model Geometries
Thurston's Eight Model Geometries Nachiketa Adhikari May 2016 Abstract Just like the distance in Euclidean space, we can assign to a manifold a no- tion of distance. Two manifolds with notions of distances can be topologically homoemorphic, but geometrically very different. The question then arises: are there any \standard" or \building block" manifolds such that any manifold is either a quotient of these manifolds or somehow \made up" of such quotients? If so, how do we define such standard manifolds, and how do we discover how many of them there are? In this project, we ask, and partially answer, these questions in three di- mensions. We go over the material necessary for understanding the proof of the existence and sufficiency of Thurston's eight three-dimensional geometries, study a part of the proof, and look at some examples of manifolds modeled on these geometries. On the way we try to throw light on some of the basic ideas of differential and Riemannian geometry. Done as part of the course Low Dimensional Geometry and Topology, under the supervision of Dr Vijay Ravikumar. The main sources used are [7] and [6]. Contents 1 Preliminaries 2 1.1 Basics . .2 1.2 Foliations . .3 1.3 Bundles . .4 2 Model Geometries 8 2.1 What is a model geometry? . .8 2.2 Holonomy and the developing map . .9 2.3 Compact point stabilizers . 11 3 Thurston's Theorem 14 3.1 In two dimensions . 14 3.2 In three dimensions . 14 3.2.1 Group discussion . 15 3.2.2 The theorem . -
Research Article Slant Curves in the Unit Tangent Bundles of Surfaces
Hindawi Publishing Corporation ISRN Geometry Volume 2013, Article ID 821429, 5 pages http://dx.doi.org/10.1155/2013/821429 Research Article Slant Curves in the Unit Tangent Bundles of Surfaces Zhong Hua Hou and Lei Sun Institute of Mathematics, Dalian University of Technology, Dalian, Liaoning 116024, China Correspondence should be addressed to Lei Sun; [email protected] Received 26 September 2013; Accepted 25 October 2013 Academic Editors: T. Friedrich and M. Pontecorvo Copyright © 2013 Z. H. Hou and L. Sun. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Let (, ) be a surface and let ((), ) be the unit tangent bundle of endowed with the Sasaki metric. We know that any curve Γ() in () consistofacurve() in and as unit vector field () along (). In this paper we study the geometric properties () and () satisfying when Γ() is a slant geodesic. 1. Introduction Theorem 1. Let Γ() = ((), ()) be a Legendrian geodesic parameterized by arc length in () with domain ∈[,]. (,,,,) Let be a 3-dimensional contact metric mani- If the set consisting of points ∈[,]such that () = 1 fold.Theslantcurvesin are generalization of Legendrian is discrete, then () is a geodesic of velocity 2 and () is the curves which form a constant angle with the Reeb vector field normal direction of in . .Choetal.[1] studied Lancret type problem for curves in Sasakian 3-manifold. They showed that a curve () ⊂ Theorem 2. Let Γ() = ((), ()) be a slant geodesic param- is slant if and only if ( ± 1)/ is constant where and eterized by arc length in () which is not Legendrian. -
Lectures on Mechanics Second Edition
Lectures on Mechanics Second Edition Jerrold E. Marsden March 24, 1997 Contents Preface iv 1 Introduction 1 1.1 The Classical Water Molecule and the Ozone Molecule ........ 1 1.2 Lagrangian and Hamiltonian Formulation ............... 3 1.3 The Rigid Body .............................. 4 1.4 Geometry, Symmetry and Reduction .................. 11 1.5 Stability .................................. 13 1.6 Geometric Phases ............................. 17 1.7 The Rotation Group and the Poincare Sphere ............. 23 2 A Crash Course in Geometric Mechanics 26 2.1 Symplectic and Poisson Manifolds ................... 26 2.2 The Flow of a Hamiltonian Vector Field ................ 28 2.3 Cotangent Bundles ............................ 28 2.4 Lagrangian Mechanics .......................... 29 2.5 Lie-Poisson Structures and the Rigid Body .............. 30 2.6 The Euler-Poincare Equations ...................... 33 2.7 Momentum Maps ............................. 35 2.8 Symplectic and Poisson Reduction ................... 37 2.9 Singularities and Symmetry ....................... 40 2.10 A Particle in a Magnetic Field ..................... 41 3 Tangent and Cotangent Bundle Reduction 44 3.1 Mechanical G-systems .......................... 44 3.2 The Classical Water Molecule ...................... 47 3.3 The Mechanical Connection ....................... 50 3.4 The Geometry and Dynamics of Cotangent Bundle Reduction .... 55 3.5 Examples ................................. 59 3.6 Lagrangian Reduction and the Routhian ................ 65 3.7 The Reduced Euler-Lagrange -
1. Geometry of the Unit Tangent Bundle
1 1. Geometry of the unit tangent bundle The main reference for this section is [8]. In the following, we consi- der (M, g) an n-dimensional smooth manifold endowed with a Riemannian metric g. 1.1. Notations Given a local chart (U, φ) on M, we will denote by (xi)16i6n the local coordinates and we write in these coordinates n X i j g = gijdx dx , i,j=1 ∂ ∂ ij where gij(x) = g , . We denote by (g ) the coefficient of the ∂xi ∂xj inverse matrix. Given x ∈ M, the norm of v ∈ TxM is given by |v|x = 1/2 1/2 gx(v, v) , which will sometimes be denoted hv, vix . In the following, we will often drop the index x. Note that if we are given other coordinates (yj), then one can check that in these new coordinates : n X ∂xi ∂xj k l (1.1) g = gij dy dy ∂yk ∂yl i,j,k,l=1 We define the musical isomorphism at x ∈ M by ∗ TxM → Tx M [ : v 7→ v[ = g(v, ·) This is an isomorphism between the two vector bundles TM and T ∗M since they are equidimensional and g is symmetric definite positive, thus non-degenerate. Given an orthonormal basis (ei) of TxM, we will denote i ∗ by (e ) the dual basis of Tx M which is, in other words, the image of the basis (ei) by the musical isomorphism. If E is a vector bundle over M, then the projection will be denoted π : E → M. We denote by Γ(M, E) the set of smooth sections of E. -
Measures on Differentiable Stacks
MEASURES ON DIFFERENTIABLE STACKS MARIUS CRAINIC AND JOAO˜ NUNO MESTRE Abstract. We introduce and study measures and densities (geometric mea- sures) on differentiable stacks, using a rather straightforward generalization of Haefliger’s approach to leaf spaces and to transverse measures for foliations. In general we prove Morita invariance, a Stokes formula which provides rein- terpretations in terms of (Ruelle-Sullivan type) algebroid currents, and a Van Est isomorphism. In the proper case we reduce the theory to classical (Radon) measures on the underlying space, we provide explicit (Weyl-type) formulas that shed light on Weinstein’s notion of volumes of differentiable stacks; in particular, in the symplectic case, we prove the conjecture left open in Wein- stein’s “The volume of a differentiable stack” [33]. We also revisit the notion of Haar systems (and the existence of cut-off functions). Our original moti- vation comes from the study of Poisson manifolds of compact types [9, 10, 8], which provide two important examples of such measures: the affine and the Duistermaat-Heckman measures. Mathematics Subject Classification (2010). 58H05; 22A22. Keywords: Lie groupoids, differentiable stacks, transverse measures. Contents 1. Introduction 1 2. Measures on manifolds 5 3. Transverse measures 10 4. Geometric transversemeasures(transversedensities) 18 5. Intermezzo:thecaseofproperLiegroupoids 21 6. Intermezzo:thecaseofregularLiegroupoids 26 7. Intermezzo:thecaseofsymplecticgroupoids 28 8. Stokes formula and (Ruelle-Sullivan) currents 33 9. Cohomological insight and the Van Est isomorphism 36 10. Appendix: Haarsystemsandcut-offfunctions,revisited 44 arXiv:1603.01673v2 [math.DG] 13 Apr 2020 References 51 1. Introduction In this paper we study measures on differentiable stacks or, equivalently, trans- verse measures on Lie groupoids. -
A Beginner's Guide to Holomorphic Manifolds
This is page Printer: Opaque this A Beginner’s Guide to Holomorphic Manifolds Andrew D. Hwang This is page i Printer: Opaque this Preface This book constitutes notes from a one-semester graduate course called “Complex Manifolds and Hermitian Differential Geometry” given during the Spring Term, 1997, at the University of Toronto. Its aim is not to give a thorough treatment of the algebraic and differential geometry of holomorphic manifolds, but to introduce material of current interest as quickly and concretely as possible with a minimum of prerequisites. There are several excellent references available for the reader who wishes to see subjects in more depth. The coverage includes standard introductory analytic material on holo- morphic manifolds, sheaf cohomology and deformation theory, differential geometry of vector bundles (Hodge theory, and Chern classes via curva- ture), and some applications to the topology and projective embeddability of K¨ahlerian manifolds. The final chapter is a short survey of extremal K¨ahler metrics and related topics, emphasizing the geometric and “soft” analytic aspects. There is a large number of exercises, particularly for a book at this level. The exercises introduce several specific but colorful ex- amples scattered through “folklore” and “the literature.” Because there are recurrent themes and varying viewpoints in the subject, some of the exercises overlap considerably. The course attendees were mostly advanced graduate students in math- ematics, but it is hoped that these notes will reach a wider audience, in- cluding theoretical physicists. The “ideal” reader would be familiar with smooth manifolds (charts, forms, flows, Lie groups, vector bundles), differ- ential geometry (metrics, connections, and curvature), and basic algebraic topology (simplicial and singular cohomology, the long exact sequence, and ii the fundamental group), but in reality the prerequisites are less strenuous, though a good reference for each subject should be kept at hand. -
Scl Danny Calegari
scl Danny Calegari 1991 Mathematics Subject Classification. Primary 20J05, 57M07; Secondary 20F12, 20F65, 20F67, 37E45, 37J05, 90C05 Key words and phrases. stable commutator length, bounded cohomology, rationality, Bavard’s Duality Theorem, hyperbolic groups, free groups, Thurston norm, Bavard’s Conjecture, rigidity, immersions, causality, group dynamics, Markov chains, central limit theorem, combable groups, finite state automata Supported in part by NSF Grants DMS-0405491 and DMS-0707130. Abstract. This book is a comprehensive introduction to the theory of sta- ble commutator length, an important subfield of quantitative topology, with substantial connections to 2-manifolds, dynamics, geometric group theory, bounded cohomology, symplectic topology, and many other subjects. We use constructive methods whenever possible, and focus on fundamental and ex- plicit examples. We give a self-contained presentation of several foundational results in the theory, including Bavard’s Duality Theorem, the Spectral Gap Theorem, the Rationality Theorem, and the Central Limit Theorem. The con- tents should be accessible to any mathematician interested in these subjects, and are presented with a minimal number of prerequisites, but with a view to applications in many areas of mathematics. Preface The historical roots of the theory of bounded cohomology stretch back at least as far as Poincar´e[167] who introduced rotation numbers in his study of circle diffeomorphisms. The Milnor–Wood inequality [154, 204] as generalized by Sul- livan [193], and the theorem of Hirsch–Thurston [109] on foliated bundles with amenable holonomy groups were also landmark developments. But it was not until the appearance of Gromov’s seminal paper [97] that a number of previously distinct and isolated phenomena crystallized into a coherent subject.