COHOMOLOGY OF FOLIATED FINSLER MANIFOLDS. Adelina MANEA 1
|
|
- Georgiana Franklin
- 5 years ago
- Views:
Transcription
1 Bulletin of the Transilvania University of Braşov Vol 4(53), No Series III: Mathematics, Informatics, Physics, COHOMOLOGY OF FOLIATED FINSLER MANIFOLDS Adelina MANEA 1 Communicated to: Finsler Extensions of Relativity Theory, August 29 - September 4, 2011, Braşov, Romania Abstract We consider a foliation F of a Finsler manifold M. Its tangent manifold T M is Riemannian with respect to the Sasaki-Finsler metric and admits a natural foliation as a fibered manifold, called vertical foliation. Foliation on M determines a foliation F T on T M. The bundle T T M has two decompositions with respect to vertical foliation and to F T, respectively. We define the vertical-tangent, the horizontal-tangent, the vertical-transversal and the horizontal-transversal vector fields on T M. We also define a new type of differential forms on T M. The exterior derivative on T M admits a decomposition into some operators, one of them satisfies a Poincare type lemma, and we established a de Rham theorem for this particular one Mathematics Subject Classification: 53C12, 53C60. Key words: Finsler manifold, foliation, cohomology. 1 Preliminaries Finding new topological invariants of differentiable manifolds is still an open problem for geometries. The cohomology groups are such invariants. The Finsler manifolds are interesting models for some physical phenomena, so their properties are also useful to investigate, [1], [2], [3], [5]. The cohomology groups of manifolds, related sometimes to some foliations on the manifolds, have been studied in the last decades, [8], [9]. A study of foliations on a Lagrangian manifolds could be found in [7]. Our present work intends to develop the study of the Finsler manifolds and the foliated structures on the tangent bundle of such a manifold. For the beginning, we present the verical foliation on the tangent manifold T M of a n-dimensional Finsler manifold (M, F ), following [1]. In this paper the indices take the values i, j, i 1, j 1,... = 1, n. Let (M, F ) be a n-dimensional Finsler manifold and G be the Sasaki-Finsler metric on its tangent manifold T M. The vertical bundle V T M of T M is the tangent (structural) bundle to vertical foliation F V determined by the fibers of π : T M M. If (x i, y i ) i=1,n are local coordinates on T M, then V T M is locally spanned 1 Faculty of Mathematics and Informatics, Transilvania University of Braşov, Romania, amanea28@yahoo.com
2 24 Adelina Manea by { y i } i. A canonical transversal (also called horizontal) distribution is constructed in [1] as follows. We denote by (g ij (x, y)) i,j the inverse matrix of g = (g ij (x, y)) i,j, where g ij (x, y) = 1 2 F 2 2 y i (x, y), (1.1) yj and F is the fundamental function of the Finsler manifold. Obviously, we have the equalities g ij = g y k ik = g jk. y j y i We locally define the functions G i = 1 ( 2 F 2 4 gik y k x h yh F 2 ) x k, G j i = Gj y i. There exists on T M a n distribution HT M locally spanned by the vector fields x i = x i Gj i The Riemannian metric G on T M is satisfying, ( )i = 1, n. (1.2) yj G( x i, x j ) = G( y i, y j ) = g ij, G( x i, ) = 0, ( )i, j. (1.3) yj The local basis { decomposition x i, y i } i is called adapted to vertical foliation F V and we have the 2 Vertical cohomology of T M T T M = HT M V T M. (1.4) Corresponding to decomposition (1.4) we have the decomposition of module of vector fields on T M into horizontal vector fiels X h (T M) locally spanned by { } and vertical vector x i fiels X v (T M) locally spanned by { }. We also have two distributions, the vertical one y i being integrable. The Poisson braket of two horizontal vector fields depends on [ ] x i, x j = Rij k y k, Rk ij = Gi j x k Gi k x j. (2.1) The horizontal distribution is integrable iff Rij k = 0 for all indices. We apply theory of differential forms on foliated manifolds, [9], to the Riemannian foliated manifold (T M, G, F V ) and we consider the (p, q)-forms on T M being (p + q)- forms on T M which are non-zero only for p-arguments in X h (T M) and q-arguments in X v (T M). The module of (p, q)- forms is denoted by Ω p,q (T M) and we have the following decomposition of module of r-forms on T M: Ω r (T M) = p+q=r Ω p,q (T M).
3 Cohomology of foliated Finsler manifolds 25 Local cobasis adapted to vertical foliation is {dx i, y i = dy i + G i j dxj }. Locally, ω Ω p,q (T M) has the following expression: ω = α i1 i 2...i pj 1...j q dx i 1... dx ip y j 1... y jq. We compute dy i = k<j Ri jk dxk dx j + G i j k,j y k dx j, hence the exterior derivative on T M admits a decomposition into three y k operators: locally given by: d 10 : Ω p,q (T M) Ω p+1,q (T M); d = d 10 + d 2, 1 + d 01, d 2, 1 : Ω p,q (T M) Ω p+2,q 1 (T M); d 01 : Ω p,q (T M) Ω p,q+1 (T M), d 10 ω = α i 1 i 2...i pj 1...j q x i dx i dx i 1... dx ip y j 1... y jq + G j k +α i i1 i 2...i pj 1...j q y l y l dx i dx i 1... dx ip y j 1... where the symbol ˆ y j k means that this element is missing. y ˆj k... y j q, d 2, 1 ω = α i1 i 2...i pj 1...j q R j k il dx l dx i dx i 1... dx ip y j 1... y ˆj k... y j q, d 01 ω = α i 1 i 2...i pj 1...j q y i y i dx i 1... dx ip y j 1... y jq. From d 2 = 0 it follows d 2 01 = 0, this operator being exactly the foliated derivative of (T M, F V ) from [9]. It is known that the foliated derivative satisfies a Poincare type lemma. Let us denote by Φ v the sheaf of germs of basic functions on T M, that means f Ω 0 (T M) such that d 01 f = 0. The de Rham cohomology groups of foliated manifold (T M, F V ) are the quotient groups of the following semiexact sequence Φ v (T M) Ω 0 (T M) d 01 Ω 0,1 (T M) d 01 Ω 0,2 (T M) d 01..., H q v(t M) = Kerd 01 d 01 (Ω 0,q 1 (T M)), and these groups are so called v-cohomology of T M. Here Kerd 01 = {ω Ω 0,q (T M),d 01 ω = 0} is the set of d 01 -closed (0, q)-forms which is usually denoted by Z 0,q (T M). The set d 01 (Ω 0,q 1 (T M)) is usually denoted by B 0,q (T M) and it is called the set of d 01 -exact (0, q)-forms. The sheaves sequence 0 Φ v Ω 0 d 01 Ω 0,1 d 01 Ω 0,2 d 01..., is a fine resolution of Φ v. A de Rham theorem is also true, H q v(t M) is isomorphic with the q-dimensional Cech cohomology group of T M with coefficients in Φ v. All these results come from the theory of foliated manifolds applied to (T M, F V ).
4 26 Adelina Manea 3 Foliated Finsler manifold In this section we consider the Finsler manifold (M, F ) from the previous sections endowed with a m-codimensional foliation F. It follows that there is a partition of M into n m -dimensional submanifolds, called leaves. In the following, the indices take the values u, v, u 1, v 1,... = m + 1, n and a, b, a 1, b 1,...= 1, m. There is an atlas on M adapted to this foliation with local adapted charts (U, (x a, x u )) such that the leaves are locally defined by x a = constant, for all a = 1, m. The local coordinates on the tangent manifold T M are (x a, x u, y a, y u ). Generally, for two local charts (U, (x i )) and Ũ, ( xi 1 )), whose domains overlap, on T M, in U Ũ we have ỹ i 1 = xi 1 x i yi. Now, the above relations give the following changing coordinates rules on T M: x a 1 = x a 1 (x a ); x u 1 = x u 1 (x a, x u ), ỹ a 1 = xa 1 x a ya ; ỹ u 1 = xu1 x a ya + xu1 x u yu. Foliation F on M determine a 2m-codimensional foliation F T locally defined by x a = constant, y a = constant. on T M, whose leaves are Taking into account decomposition (1.4) of T T M, the local base { x a, x u, y a, y u } adapted to vertical foliation satisfies the following relations in U Ũ: x a 1 = xa x a 1 x a + xu x a 1 x u, ỹ a 1 = xa x a 1 x u 1 ỹ u 1 y a + xu x a 1 = xu x u 1 x u, = xu x u 1 y u, y u, Returning now to the foliation F T, the tangent bundle T F T to leaves, also called the structural bundle of this foliation, is locally spanned by { x, u y } and it is a subbundle u of T T M. Definition 3.1. We say that the foliation F of M is compatible with the Finsler structure F on M if, in every local chart around a point (x, y) T M, the matrix (g uv ) u,v, g uv (x, y) = 1 2 F 2 2 y u (x, y), yv
5 Cohomology of foliated Finsler manifolds 27 is nondegenerate and the functions G a are satisfying the relation for all a = 1, m, u = m + 1, n. G a y u = 0, Remark 3.1. The condition that a foliation is compatible to F has geometrical meaning. Indeed, in U Ũ we have and the matix ( xu x u 1 ) u,u 1 g u1,v 1 = g uv x u x u 1 x v x v 1, is obviously nondegenerate in every local chart. Proposition 3.1. If the foliation F of M is compatible with the Finsler structure F on M, then the vector fields on T M locally given by ξ a = x a tu a x u, ζ a = y a tu a y u, (3.1) are orthogonal to { x }, { u y }, with respect to Sasaki-Finsler metric G from (1.3), where u {t u a} are solutions of the system g av t u ag uv = 0. Proof. The compatibility between foliation on M and the Finsler structure of this manifold assures the solvability of the system g av t u ag uv = 0. Moreover, computing G(ξ a, x u ) = g au t a vg vu, G(ζ a, y u ) = g au t a vg vu, it results that these vector fields are orthogonal. As a consequence of the above Proposition, for a vector X T M we have the followig decomposition: X = X i x i + Y i y i = The basis = X a x a + Xu x u + Y a y a + Y u y u = = X a ξ a + (X u + t u ax a ) x u + Y a ζ a + (Y u + t u ay a ) y u. {ξ a, x u, ζ a, y u } (3.2) is adapted to F T and to vertical foliation, too. We denote by T F T the orthogonal bundle to T F T with respect to Sasaki-Finsler metric on T M.
6 28 Adelina Manea Definition 3.2. The vertical component of a section of T F T is called a verticaltangent vector field on T M. Their collection is denoted by V F T. The horizontal component of a section of T F T is called a horizontal-tangent vector field on T M. Their collection is denoted by HF T. The vertical component of a section of T F T is called a vertical-transversal vector field on T M. Their collection is denoted by V F T. The horizontal component of a section of T F T is called a horizontal-transversal vector field on T M. Their collection is denoted by H F T. From the above definition we have the decomposition of module of vector fields on T M into H F T HF T V F T V F T. Locally, H F T, HF T, V F T, V F T are spanned by {ξ a }, { x }, {ζ u a }, { y }, respectively. u The cobasis dual to basis (3.2) is {dx a, θ u, y a, η u }, where θ u = dx u + t u adx a, η u = y u + t u ay a. Definition 3.3. A (0, q)-form ω on T M is called a (0, s, t)-form if s + t = q and if it is nonzero only for s-arguments in V F T and t-arguments in V F T. We denote the space of (0, s, t)-forms by Ω 0,s,t (T M) and we have Ω 0,q (T M) = s+t=q Ω 0,s,t (T M). The foliated derivative d 01 acts on a (0, s, t)-form locally given by as it follows: ω = α a1,a 2,...,a s,u 1,..,u t y a 1... y as η u 1... η ut d 01 ω = ζ a (α a1,a 2,...,a s,u 1,..,u t )y a y a 1... y as η u 1... η ut + +( 1) s α a 1,a 2,...,a s,u 1,..,u t y u y a 1... y as η u η u 1... η ut. Hence there are two operators d 0,1,0 : Ω 0,s,t (T M) Ω 0,s+1,t (T M), d 0,0,1 : Ω 0,s,t (T M) Ω 0,s,t+1 (T M), with and d 01 = d 0,1,0 + d 0,0,1, d 0,0,1 ω = ( 1) s α a 1,a 2,...,a s,u 1,..,u t y u y a 1... y as η u η u 1... η ut. The equality d 2 01 = 0 implies d2 0,0,1 = 0. A function f Ω0 (T M) is called vertical basic if d 0,0,1 f = 0. We denote by Φ 0,0 the sheaf of germs of vertical basic functions. The following sequence
7 Cohomology of foliated Finsler manifolds 29 Φ 0,0 (T M) Ω 0 (T M) d 0,0,1 Ω 0,0,1 (T M) d 0,0,1 Ω 0,0,2 (T M) d 0,0,1..., is semiexact and we call the quotient group H q v,t (T M) = Z0,0,q (T M) B 0,0,q (T M), the v,t-cohomology of T M. Here Z 0,0,q (T M) = {ω Ω 0,0,q (T M), d 0,0,1 ω = 0} is the set of d 0,0,1 -closed (0, 0, q)-forms. The set B 0,q (T M) = d 0,0,1 (Ω 0,0,q 1 (T M)) is called the set of d 0,0,1 -exact (0, 0, q)-forms. Remark 3.2. We have the following strict inclusions: Z 0,q (T M) Ω 0,0,q (T M) Z 0,0,q (T M), B 0,q (T M) Ω 0,0,q (T M) B 0,0,q (T M). Another property of the operator d 0,0,1 is a Poincare type lemma, namely Theorem 3.1. Let ω be a d 0,0,1 -closed (0, 0, t)-form. For every open domain U T M there is γ Ω 0,0,t 1 (U) such that in U we have the equality ω = d 0,0,1 γ. Proof. Since ω is a (0, 0, t)-form, its local expression is ω = α u1,u 2,...,u t η u 1... η ut. From d 0,0,1 ω = 0 it follows d 01 ω = ζ a (α u1,u 2,...,u t )y a η u 1... η ut, so d 01 ω = 0 (modulo y 1, y 2,..., y m n ) But the operator d 01 satisfies a Poincare type lemma, hence in space y a = 0 we have that for every open domain U of T M there is a (0, t 1)-form ϕ such that in U ω = d 0,0,1 ϕ (modulo y 1, y 2,..., y m n ). Let γ be the (0, 0, t 1)-component of ϕ. Then we have the following equality in U: ω = d 0,0,1 γ + µ a y a, with µ a (0, t 1)-forms on U. By equalizing the terms of the same type in the above equality we obtain ω = d 0,0,1 γ, so every d 0,0,1 -closed form is locally d 0,0,1 -exact. Let Ω 0,0,q the sheaf of germs of (0, 0, q)-forms and i : Φ 0,0 Ω 0 the natural inclusion. The shaves Ω 0,0,q are fins, so the shaves sequence 0 Φ 0,0 Ω 0 d 0,0,1 Ω 0,0,1 d 0,0,1 Ω 0,0,2 d 0,0,1..., is a fine resolution of the sheaf Φ 0,0. Applying now a well-known theorem of algebraic topology it results a de Rham type theorem for the v, t-cohomology of T M: Theorem 3.2. H q v,t (T M) is isomorphic with the q-dimensional Cech cohomology group of T M with coefficients in Φ 0,0.
8 30 Adelina Manea References [1] Bejancu, A., Farran, H.R., Finsler geomerty and natural foliations on the tangent bundle, Reports on Mathematical Phisics, 58 (2006), [2] Bidabad, B., Complete Finsler manifolds and adapted coordinates, Balkan Journal of Geometry and Its Applications, 14 (2009), [3] Miron, R., Anastasiei, M., Vector bundles, Lagrange spaces. Applications to the theory of relativity, Balkan Press, Bucharest, [4] Miron, R., Pop, I., Topologie algebrică. Omologie, omotopie, spaţii de acoperire., Ed. Acad. RSR, Bucharest [5] Munteanu, Gh., Purcaru, M., On R-complex Finsler spaces, Balkan Journal of Geometry and Its Applications, 14 (2009), [6] Pitis, Gh., Munteanu, Gh., V-Cohomology of complex Finsler manifolds, Studia Univ. Babeş-Bolyai, Mathematica, 43 (1998), [7] Popescu, M., Popescu, P., Projectable non-linear connections and foliations, Proc. Summer School on Diff. Geometry, Universidade de Coimbra, (1999), [8] Tondeur, Ph., Foliations on Riemannian manifolds, Universitext, Springer-Verlag, New-York, [9] Vaisman, I., Cohomology and differential forms, Marcel Dekker Inc., New York, 1973.
Some Remarks about Mastrogiacomo Cohomolgy
General Mathematics Vol. 13, No. 4 (2005), 19 32 Some Remarks about Mastrogiacomo Cohomolgy Adelina Manea Dedicated to Professor Dumitru Acu on his 60th anniversary Abstract We prove the isomorphism between
More informationBulletin of the Transilvania University of Braşov Vol 8(57), No Series III: Mathematics, Informatics, Physics, 43-56
Bulletin of the Transilvania University of Braşov Vol 857, No. 1-2015 Series III: Mathematics, Informatics, Physics, 43-56 FIRST ORDER JETS OF BUNDLES OVER A MANIFOLD ENDOWED WITH A SUBFOLIATION Adelina
More information1 Introduction and preliminaries notions
Bulletin of the Transilvania University of Braşov Vol 2(51) - 2009 Series III: Mathematics, Informatics, Physics, 193-198 A NOTE ON LOCALLY CONFORMAL COMPLEX LAGRANGE SPACES Cristian IDA 1 Abstract In
More informationA V -COHOMOLOGY WITH RESPECT TO COMPLEX LIOUVILLE DISTRIBUTION
International Electronic Journal of Geometry Volume 5 No. 1 pp. 151-162 (2012) c IEJG A V -COHOMOLOGY WITH RESPECT TO COMPLEX LIOUVILLE DISTRIBUTION ADELINA MANEA AND CRISTIAN IDA (Communicated by Murat
More informationSOME PROPERTIES OF COMPLEX BERWALD SPACES. Cristian IDA 1
ulletin of the Transilvania University of raşov Vol 3(52) - 2010 Series III: Mathematics, Informatics, Physics, 33-40 SOME PROPERTIES OF COMPLEX ERWALD SPACES Cristian IDA 1 Abstract The notions of complex
More informationarxiv: v1 [math.dg] 5 Jan 2016
arxiv:60.00750v [math.dg] 5 Jan 06 On the k-semispray of Nonlinear Connections in k-tangent Bundle Geometry Florian Munteanu Department of Applied Mathematics, University of Craiova, Romania munteanufm@gmail.com
More informationDirac Structures on Banach Lie Algebroids
DOI: 10.2478/auom-2014-0060 An. Şt. Univ. Ovidius Constanţa Vol. 22(3),2014, 219 228 Dirac Structures on Banach Lie Algebroids Vlad-Augustin VULCU Abstract In the original definition due to A. Weinstein
More informationNEW LIFTS OF SASAKI TYPE OF THE RIEMANNIAN METRICS
NEW LIFTS OF SASAKI TYPE OF THE RIEMANNIAN METRICS Radu Miron Abstract One defines new elliptic and hyperbolic lifts to tangent bundle T M of a Riemann metric g given on the base manifold M. They are homogeneous
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 informationActa Mathematica Academiae Paedagogicae Nyíregyháziensis 24 (2008), ISSN
Acta Mathematica Academiae Paedagogicae Nyíregyháziensis 24 2008, 115 123 wwwemisde/journals ISSN 1786-0091 ON NONLINEAR CONNECTIONS IN HIGHER ORDER LAGRANGE SPACES MARCEL ROMAN Abstract Considering a
More informationOn the geometry of higher order Lagrange spaces.
On the geometry of higher order Lagrange spaces. By Radu Miron, Mihai Anastasiei and Ioan Bucataru Abstract A Lagrange space of order k 1 is the space of accelerations of order k endowed with a regular
More informationarxiv:alg-geom/ v1 29 Jul 1993
Hyperkähler embeddings and holomorphic symplectic geometry. Mikhail Verbitsky, verbit@math.harvard.edu arxiv:alg-geom/9307009v1 29 Jul 1993 0. ntroduction. n this paper we are studying complex analytic
More informationGENERALIZED QUATERNIONIC STRUCTURES ON THE TOTAL SPACE OF A COMPLEX FINSLER SPACE
Bulletin of the Transilvania University of Braşov Vol 554, No. 1-2012 Series III: Mathematics, Informatics, Physics, 85-96 GENERALIZED QUATERNIONIC STRUCTURES ON THE TOTAL SPACE OF A COMPLEX FINSLER SPACE
More informationLECTURE 28: VECTOR BUNDLES AND FIBER BUNDLES
LECTURE 28: VECTOR BUNDLES AND FIBER BUNDLES 1. Vector Bundles In general, smooth manifolds are very non-linear. However, there exist many smooth manifolds which admit very nice partial linear structures.
More informationNONLINEAR CONNECTION FOR NONCONSERVATIVE MECHANICAL SYSTEMS
NONLINEAR CONNECTION FOR NONCONSERVATIVE MECHANICAL SYSTEMS IOAN BUCATARU, RADU MIRON Abstract. The geometry of a nonconservative mechanical system is determined by its associated semispray and the corresponding
More informationLie algebra cohomology
Lie algebra cohomology Relation to the de Rham cohomology of Lie groups Presented by: Gazmend Mavraj (Master Mathematics and Diploma Physics) Supervisor: J-Prof. Dr. Christoph Wockel (Section Algebra and
More informationReminder on basic differential geometry
Reminder on basic differential geometry for the mastermath course of 2013 Charts Manifolds will be denoted by M, N etc. One should think of a manifold as made out of points (while the elements of a vector
More informationLinear connections induced by a nonlinear connection in the geometry of order two
Linear connections induced by a nonlinear connection in the geometry of order two by Ioan Bucataru 1 and Marcel Roman Pour une variété différentiable, n-dimensionelle M, nous considerons Osc 2 M l éspace
More informationMath 550 / David Dumas / Fall Problems
Math 550 / David Dumas / Fall 2014 Problems Please note: This list was last updated on November 30, 2014. Problems marked with * are challenge problems. Some problems are adapted from the course texts;
More informationINTRO TO SUBRIEMANNIAN GEOMETRY
INTRO TO SUBRIEMANNIAN GEOMETRY 1. Introduction to subriemannian geometry A lot of this tal is inspired by the paper by Ines Kath and Oliver Ungermann on the arxiv, see [3] as well as [1]. Let M be a smooth
More informationLagrange Spaces with β-change
Int. J. Contemp. Math. Sciences, Vol. 7, 2012, no. 48, 2363-2371 Lagrange Spaces with β-change T. N. Pandey and V. K. Chaubey Department of Mathematics and Statistics D. D. U. Gorakhpur University Gorakhpur
More informationHARMONIC COHOMOLOGY OF SYMPLECTIC FIBER BUNDLES
HARMONIC COHOMOLOGY OF SYMPLECTIC FIBER BUNDLES OLIVER EBNER AND STEFAN HALLER Abstract. We show that every de Rham cohomology class on the total space of a symplectic fiber bundle with closed Lefschetz
More informationFormality of Kähler manifolds
Formality of Kähler manifolds Aron Heleodoro February 24, 2015 In this talk of the seminar we like to understand the proof of Deligne, Griffiths, Morgan and Sullivan [DGMS75] of the formality of Kähler
More informationGEOMETRIC QUANTIZATION
GEOMETRIC QUANTIZATION 1. The basic idea The setting of the Hamiltonian version of classical (Newtonian) mechanics is the phase space (position and momentum), which is a symplectic manifold. The typical
More informationThis article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research and
This article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research and education use, including for instruction at the authors institution
More informationLECTURE 1: LINEAR SYMPLECTIC GEOMETRY
LECTURE 1: LINEAR SYMPLECTIC GEOMETRY Contents 1. Linear symplectic structure 3 2. Distinguished subspaces 5 3. Linear complex structure 7 4. The symplectic group 10 *********************************************************************************
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 informationLECTURE 5: COMPLEX AND KÄHLER MANIFOLDS
LECTURE 5: COMPLEX AND KÄHLER MANIFOLDS Contents 1. Almost complex manifolds 1. Complex manifolds 5 3. Kähler manifolds 9 4. Dolbeault cohomology 11 1. Almost complex manifolds Almost complex structures.
More informationAdiabatic limits of co-associative Kovalev-Lefschetz fibrations
Adiabatic limits of co-associative Kovalev-Lefschetz fibrations Simon Donaldson February 3, 2016 To Maxim Kontsevich, on his 50th. birthday 1 Introduction This article makes the first steps in what we
More informationRIEMANN S INEQUALITY AND RIEMANN-ROCH
RIEMANN S INEQUALITY AND RIEMANN-ROCH DONU ARAPURA Fix a compact connected Riemann surface X of genus g. Riemann s inequality gives a sufficient condition to construct meromorphic functions with prescribed
More informationLAGRANGE GEOMETRY VIA COMPLEX LAGRANGE GEOMETRY
Novi Sad J. Math. Vol. 32, No. 2, 2002, 141-154 141 AGANGE GEOMETY VIA COMPEX AGANGE GEOMETY Gheorghe Munteanu 1 Abstract. Asking that the metric of a complex Finsler space should be strong convex, Abate
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 informationChapter 3. Riemannian Manifolds - I. The subject of this thesis is to extend the combinatorial curve reconstruction approach to curves
Chapter 3 Riemannian Manifolds - I The subject of this thesis is to extend the combinatorial curve reconstruction approach to curves embedded in Riemannian manifolds. A Riemannian manifold is an abstraction
More informationA First Lecture on Sheaf Cohomology
A First Lecture on Sheaf Cohomology Elizabeth Gasparim Departamento de Matemática, Universidade Federal de Pernambuco Cidade Universitária, Recife, PE, BRASIL, 50670-901 gasparim@dmat.ufpe.br I. THE DEFINITION
More informationThe Strominger Yau Zaslow conjecture
The Strominger Yau Zaslow conjecture Paul Hacking 10/16/09 1 Background 1.1 Kähler metrics Let X be a complex manifold of dimension n, and M the underlying smooth manifold with (integrable) almost complex
More informationHard Lefschetz Theorem for Vaisman manifolds
Hard Lefschetz Theorem for Vaisman manifolds Antonio De Nicola CMUC, University of Coimbra, Portugal joint work with B. Cappelletti-Montano (Univ. Cagliari), J.C. Marrero (Univ. La Laguna) and I. Yudin
More informationSYMPLECTIC MANIFOLDS, GEOMETRIC QUANTIZATION, AND UNITARY REPRESENTATIONS OF LIE GROUPS. 1. Introduction
SYMPLECTIC MANIFOLDS, GEOMETRIC QUANTIZATION, AND UNITARY REPRESENTATIONS OF LIE GROUPS CRAIG JACKSON 1. Introduction Generally speaking, geometric quantization is a scheme for associating Hilbert spaces
More informationLinearized geometric dynamics of Tobin-Benhabib-Miyao economic flow
Linearized geometric dynamics of Tobin-Benhabib-Miyao economic flow Constantin Udrişte and Armando Ciancio Abstract The aim of this paper is to study the influence of the Euclidean-Lagrangian structure
More informationLECTURE: KOBORDISMENTHEORIE, WINTER TERM 2011/12; SUMMARY AND LITERATURE
LECTURE: KOBORDISMENTHEORIE, WINTER TERM 2011/12; SUMMARY AND LITERATURE JOHANNES EBERT 1.1. October 11th. 1. Recapitulation from differential topology Definition 1.1. Let M m, N n, be two smooth manifolds
More information30 Surfaces and nondegenerate symmetric bilinear forms
80 CHAPTER 3. COHOMOLOGY AND DUALITY This calculation is useful! Corollary 29.4. Let p, q > 0. Any map S p+q S p S q induces the zero map in H p+q ( ). Proof. Let f : S p+q S p S q be such a map. It induces
More informationAction-angle coordinates and geometric quantization. Eva Miranda. Barcelona (EPSEB,UPC) STS Integrable Systems
Action-angle coordinates and geometric quantization Eva Miranda Barcelona (EPSEB,UPC) STS Integrable Systems Eva Miranda (UPC) 6ecm July 3, 2012 1 / 30 Outline 1 Quantization: The general picture 2 Bohr-Sommerfeld
More informationLECTURE 16: LIE GROUPS AND THEIR LIE ALGEBRAS. 1. Lie groups
LECTURE 16: LIE GROUPS AND THEIR LIE ALGEBRAS 1. Lie groups A Lie group is a special smooth manifold on which there is a group structure, and moreover, the two structures are compatible. Lie groups are
More informationCohomology and Vector Bundles
Cohomology and Vector Bundles Corrin Clarkson REU 2008 September 28, 2008 Abstract Vector bundles are a generalization of the cross product of a topological space with a vector space. Characteristic classes
More informationThe Canonical Sheaf. Stefano Filipazzi. September 14, 2015
The Canonical Sheaf Stefano Filipazzi September 14, 015 These notes are supposed to be a handout for the student seminar in algebraic geometry at the University of Utah. In this seminar, we will go over
More informationStable bundles with small c 2 over 2-dimensional complex tori
Stable bundles with small c 2 over 2-dimensional complex tori Matei Toma Universität Osnabrück, Fachbereich Mathematik/Informatik, 49069 Osnabrück, Germany and Institute of Mathematics of the Romanian
More informationON THE SINGULAR DECOMPOSITION OF MATRICES
An. Şt. Univ. Ovidius Constanţa Vol. 8, 00, 55 6 ON THE SINGULAR DECOMPOSITION OF MATRICES Alina PETRESCU-NIŢǍ Abstract This paper is an original presentation of the algorithm of the singular decomposition
More informationSUBTANGENT-LIKE STATISTICAL MANIFOLDS. 1. Introduction
SUBTANGENT-LIKE STATISTICAL MANIFOLDS A. M. BLAGA Abstract. Subtangent-like statistical manifolds are introduced and characterization theorems for them are given. The special case when the conjugate connections
More informationDIFFERENTIAL FORMS AND COHOMOLOGY
DIFFERENIAL FORMS AND COHOMOLOGY ONY PERKINS Goals 1. Differential forms We want to be able to integrate (holomorphic functions) on manifolds. Obtain a version of Stokes heorem - a generalization of the
More informationarxiv: v3 [math.ag] 21 Nov 2013
THE FRÖLICHER SPECTRAL SEQUENCE CAN BE ARBITRARILY NON DEGENERATE LAURA BIGALKE AND SÖNKE ROLLENSKE arxiv:0709.0481v3 [math.ag] 21 Nov 2013 Abstract. The Frölicher spectral sequence of a compact complex
More informationReduction of Homogeneous Riemannian structures
Geometric Structures in Mathematical Physics, 2011 Reduction of Homogeneous Riemannian structures M. Castrillón López 1 Ignacio Luján 2 1 ICMAT (CSIC-UAM-UC3M-UCM) Universidad Complutense de Madrid 2 Universidad
More informationOn Berwald Spaces which Satisfy the Relation Γ k ij = p k g ij for Some Functions p k on TM
International Mathematical Forum, 2, 2007, no. 67, 3331-3338 On Berwald Spaces which Satisfy the Relation Γ k ij = p k g ij for Some Functions p k on TM Dariush Latifi and Asadollah Razavi Faculty of Mathematics
More informationSome brief notes on the Kodaira Vanishing Theorem
Some brief notes on the Kodaira Vanishing Theorem 1 Divisors and Line Bundles, according to Scott Nollet This is a huge topic, because there is a difference between looking at an abstract variety and local
More informationOrientation transport
Orientation transport Liviu I. Nicolaescu Dept. of Mathematics University of Notre Dame Notre Dame, IN 46556-4618 nicolaescu.1@nd.edu June 2004 1 S 1 -bundles over 3-manifolds: homological properties Let
More informationA Crash Course of Floer Homology for Lagrangian Intersections
A Crash Course of Floer Homology for Lagrangian Intersections Manabu AKAHO Department of Mathematics Tokyo Metropolitan University akaho@math.metro-u.ac.jp 1 Introduction There are several kinds of Floer
More informationComplex manifolds, Kahler metrics, differential and harmonic forms
Complex manifolds, Kahler metrics, differential and harmonic forms Cattani June 16, 2010 1 Lecture 1 Definition 1.1 (Complex Manifold). A complex manifold is a manifold with coordinates holomorphic on
More informationA DANILOV-TYPE FORMULA FOR TORIC ORIGAMI MANIFOLDS VIA LOCALIZATION OF INDEX
A DANILOV-TYPE FORMULA FOR TORIC ORIGAMI MANIFOLDS VIA LOCALIZATION OF INDEX HAJIME FUJITA Abstract. We give a direct geometric proof of a Danilov-type formula for toric origami manifolds by using the
More informationTwisted Poisson manifolds and their almost symplectically complete isotropic realizations
Twisted Poisson manifolds and their almost symplectically complete isotropic realizations Chi-Kwong Fok National Center for Theoretical Sciences Math Division National Tsing Hua University (Joint work
More informationOn some special vector fields
On some special vector fields Iulia Hirică Abstract We introduce the notion of F -distinguished vector fields in a deformation algebra, where F is a (1, 1)-tensor field. The aim of this paper is to study
More informationConification of Kähler and hyper-kähler manifolds and supergr
Conification of Kähler and hyper-kähler manifolds and supergravity c-map Masaryk University, Brno, Czech Republic and Institute for Information Transmission Problems, Moscow, Russia Villasimius, September
More informationLIE ALGEBRA PREDERIVATIONS AND STRONGLY NILPOTENT LIE ALGEBRAS
LIE ALGEBRA PREDERIVATIONS AND STRONGLY NILPOTENT LIE ALGEBRAS DIETRICH BURDE Abstract. We study Lie algebra prederivations. A Lie algebra admitting a non-singular prederivation is nilpotent. We classify
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 informationThe geometry of hydrodynamic integrability
1 The geometry of hydrodynamic integrability David M. J. Calderbank University of Bath October 2017 2 What is hydrodynamic integrability? A test for integrability of dispersionless systems of PDEs. Introduced
More informationDeformations of coisotropic submanifolds in symplectic geometry
Deformations of coisotropic submanifolds in symplectic geometry Marco Zambon IAP annual meeting 2015 Symplectic manifolds Definition Let M be a manifold. A symplectic form is a two-form ω Ω 2 (M) which
More informationSYMPLECTIC GEOMETRY: LECTURE 1
SYMPLECTIC GEOMETRY: LECTURE 1 LIAT KESSLER 1. Symplectic Linear Algebra Symplectic vector spaces. Let V be a finite dimensional real vector space and ω 2 V, i.e., ω is a bilinear antisymmetric 2-form:
More informationON SOME INVARIANT SUBMANIFOLDS IN A RIEMANNIAN MANIFOLD WITH GOLDEN STRUCTURE
ANALELE ŞTIINŢIFICE ALE UNIVERSITĂŢII AL.I. CUZA DIN IAŞI (S.N.) MATEMATICĂ, Tomul LIII, 2007, Supliment ON SOME INVARIANT SUBMANIFOLDS IN A RIEMANNIAN MANIFOLD WITH GOLDEN STRUCTURE BY C.-E. HREŢCANU
More informationAdvanced Course: Transversal Dirac operators on distributions, foliations, and G-manifolds. Ken Richardson and coauthors
Advanced Course: Transversal Dirac operators on distributions, foliations, and G-manifolds Ken Richardson and coauthors Universitat Autònoma de Barcelona May 3-7, 2010 Universitat Autònoma de Barcelona
More informationLIE ALGEBROIDS AND POISSON GEOMETRY, OLIVETTI SEMINAR NOTES
LIE ALGEBROIDS AND POISSON GEOMETRY, OLIVETTI SEMINAR NOTES BENJAMIN HOFFMAN 1. Outline Lie algebroids are the infinitesimal counterpart of Lie groupoids, which generalize how we can talk about symmetries
More informationComplex line bundles. Chapter Connections of line bundle. Consider a complex line bundle L M. For any integer k N, let
Chapter 1 Complex line bundles 1.1 Connections of line bundle Consider a complex line bundle L M. For any integer k N, let be the space of k-forms with values in L. Ω k (M, L) = C (M, L k (T M)) Definition
More informationReduction of Symplectic Lie Algebroids by a Lie Subalgebroid and a Symmetry Lie Group
Symmetry, Integrability and Geometry: Methods and Applications SIGMA 3 (2007), 049, 28 pages Reduction of Symplectic Lie Algebroids by a Lie Subalgebroid and a Symmetry Lie Group David IGLESIAS, Juan Carlos
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 informationA MARSDEN WEINSTEIN REDUCTION THEOREM FOR PRESYMPLECTIC MANIFOLDS
A MARSDEN WEINSTEIN REDUCTION THEOREM FOR PRESYMPLECTIC MANIFOLDS FRANCESCO BOTTACIN Abstract. In this paper we prove an analogue of the Marsden Weinstein reduction theorem for presymplectic actions of
More informationLecture 6: Classifying spaces
Lecture 6: Classifying spaces A vector bundle E M is a family of vector spaces parametrized by a smooth manifold M. We ask: Is there a universal such family? In other words, is there a vector bundle E
More informationSmooth Dynamics 2. Problem Set Nr. 1. Instructor: Submitted by: Prof. Wilkinson Clark Butler. University of Chicago Winter 2013
Smooth Dynamics 2 Problem Set Nr. 1 University of Chicago Winter 2013 Instructor: Submitted by: Prof. Wilkinson Clark Butler Problem 1 Let M be a Riemannian manifold with metric, and Levi-Civita connection.
More informationExercises in Geometry II University of Bonn, Summer semester 2015 Professor: Prof. Christian Blohmann Assistant: Saskia Voss Sheet 1
Assistant: Saskia Voss Sheet 1 1. Conformal change of Riemannian metrics [3 points] Let (M, g) be a Riemannian manifold. A conformal change is a nonnegative function λ : M (0, ). Such a function defines
More information1. 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 consider (M, g) an n-dimensional smooth manifold endowed with a Riemannian metric g. 1.1. Notations
More informationINTRODUCTION TO ALGEBRAIC GEOMETRY
INTRODUCTION TO ALGEBRAIC GEOMETRY WEI-PING LI 1 Preliminary of Calculus on Manifolds 11 Tangent Vectors What are tangent vectors we encounter in Calculus? (1) Given a parametrised curve α(t) = ( x(t),
More informationKlaus Janich. Vector Analysis. Translated by Leslie Kay. With 108 Illustrations. Springer
Klaus Janich Vector Analysis Translated by Leslie Kay With 108 Illustrations Springer Preface to the English Edition Preface to the First German Edition Differentiable Manifolds 1 1.1 The Concept of a
More informationHyperkähler geometry lecture 3
Hyperkähler geometry lecture 3 Misha Verbitsky Cohomology in Mathematics and Physics Euler Institute, September 25, 2013, St. Petersburg 1 Broom Bridge Here as he walked by on the 16th of October 1843
More informationTransverse geometry. consisting of finite sums of monomials of the form
Transverse geometry The space of leaves of a foliation (V, F) can be described in terms of (M, Γ), with M = complete transversal and Γ = holonomy pseudogroup. The natural transverse coordinates form the
More informationLecture 8: More characteristic classes and the Thom isomorphism
Lecture 8: More characteristic classes and the Thom isomorphism We begin this lecture by carrying out a few of the exercises in Lecture 1. We take advantage of the fact that the Chern classes are stable
More information3. Signatures Problem 27. Show that if K` and K differ by a crossing change, then σpk`q
1. Introduction Problem 1. Prove that H 1 ps 3 zk; Zq Z and H 2 ps 3 zk; Zq 0 without using the Alexander duality. Problem 2. Compute the knot group of the trefoil. Show that it is not trivial. Problem
More informationNon-Classical Lagrangian Dynamics and Potential Maps
Non-Classical Lagrangian Dynamics and Potential Maps CONSTANTIN UDRISTE University Politehnica of Bucharest Faculty of Applied Sciences Department of Mathematics Splaiul Independentei 313 060042 BUCHAREST,
More informationGroup Actions and Cohomology in the Calculus of Variations
Group Actions and Cohomology in the Calculus of Variations JUHA POHJANPELTO Oregon State and Aalto Universities Focused Research Workshop on Exterior Differential Systems and Lie Theory Fields Institute,
More informationChapter 17 Computation of Some Hodge Numbers
Chapter 17 Computation of Some Hodge Numbers The Hodge numbers of a smooth projective algebraic variety are very useful invariants. By Hodge theory, these determine the Betti numbers. In this chapter,
More informationDIRAC STRUCTURES FROM LIE INTEGRABILITY
International Journal of Geometric Methods in Modern Physics Vol. 9, No. 4 (01) 10005 (7 pages) c World Scientific Publishing Company DOI: 10.114/S0198878100058 DIRAC STRUCTURES FROM LIE INTEGRABILITY
More informationTHE HODGE DECOMPOSITION
THE HODGE DECOMPOSITION KELLER VANDEBOGERT 1. The Musical Isomorphisms and induced metrics Given a smooth Riemannian manifold (X, g), T X will denote the tangent bundle; T X the cotangent bundle. The additional
More informationAcceleration bundles on Banach and Fréchet manifolds
Acceleration bundles on Banach and JGP Editorial Board Scientific Meeting In commemoration of André Lichnerowicz 27-29 June 2006, International School for Advanced Studies, Miramare, Trieste Italy C.T.J.
More informationSCREEN TRANSVERSAL LIGHTLIKE SUBMANIFOLDS OF INDEFINITE KENMOTSU MANIFOLDS
SARAJEVO JOURNAL OF MATHEMATICS Vol.7 (19) (2011), 103 113 SCREEN TRANSVERSAL LIGHTLIKE SUBMANIFOLDS OF INDEFINITE KENMOTSU MANIFOLDS RAM SHANKAR GUPTA AND A. SHARFUDDIN Abstract. In this paper, we introduce
More informationQuaternionic Complexes
Quaternionic Complexes Andreas Čap University of Vienna Berlin, March 2007 Andreas Čap (University of Vienna) Quaternionic Complexes Berlin, March 2007 1 / 19 based on the joint article math.dg/0508534
More informationRIEMANN SURFACES: TALK V: DOLBEAULT COHOMOLOGY
RIEMANN SURFACES: TALK V: DOLBEAULT COHOMOLOGY NICK MCCLEEREY 0. Complex Differential Forms Consider a complex manifold X n (of complex dimension n) 1, and consider its complexified tangent bundle T C
More informationSome aspects of the Geodesic flow
Some aspects of the Geodesic flow Pablo C. Abstract This is a presentation for Yael s course on Symplectic Geometry. We discuss here the context in which the geodesic flow can be understood using techniques
More informationTopic: First Chern classes of Kähler manifolds Mitchell Faulk Last updated: April 23, 2016
Topic: First Chern classes of Kähler manifolds itchell Faulk Last updated: April 23, 2016 We study the first Chern class of various Kähler manifolds. We only consider two sources of examples: Riemann surfaces
More informationOn para-norden metric connections
On para-norden metric connections C. Ida, A. Manea Dedicated to Professor Constantin Udrişte at his 75-th anniversary Abstract. The aim of this paper is the construction of some para-norden metric connections
More informationHamilton-Jacobi theory on Lie algebroids: Applications to nonholonomic mechanics. Manuel de León Institute of Mathematical Sciences CSIC, Spain
Hamilton-Jacobi theory on Lie algebroids: Applications to nonholonomic mechanics Manuel de León Institute of Mathematical Sciences CSIC, Spain joint work with J.C. Marrero (University of La Laguna) D.
More informationPart III- Hodge Theory Lecture Notes
Part III- Hodge Theory Lecture Notes Anne-Sophie KALOGHIROS These lecture notes will aim at presenting and explaining some special structures that exist on the cohomology of Kähler manifolds and to discuss
More informationNOTES ON FIBER BUNDLES
NOTES ON FIBER BUNDLES DANNY CALEGARI Abstract. These are notes on fiber bundles and principal bundles, especially over CW complexes and spaces homotopy equivalent to them. They are meant to supplement
More informationTHE NEWLANDER-NIRENBERG THEOREM. GL. The frame bundle F GL is given by x M Fx
THE NEWLANDER-NIRENBERG THEOREM BEN MCMILLAN Abstract. For any kind of geometry on smooth manifolds (Riemannian, Complex, foliation,...) it is of fundamental importance to be able to determine when two
More informationCONNECTIONS ON PRINCIPAL BUNDLES AND CLASSICAL ELECTROMAGNETISM
CONNECTIONS ON PRINCIPAL BUNDLES AND CLASSICAL ELECTROMAGNETISM APURV NAKADE Abstract. The goal is to understand how Maxwell s equations can be formulated using the language of connections. There will
More informationChern numbers and Hilbert Modular Varieties
Chern numbers and Hilbert Modular Varieties Dylan Attwell-Duval Department of Mathematics and Statistics McGill University Montreal, Quebec attwellduval@math.mcgill.ca April 9, 2011 A Topological Point
More informationFrom action-angle coordinates to geometric quantization: a 30-minute round-trip. Eva Miranda
From action-angle coordinates to geometric quantization: a 30-minute round-trip Eva Miranda Barcelona (UPC) Geometric Quantization in the non-compact setting Eva Miranda (UPC) MFO, 2011 18 February, 2011
More information