Frobenius theorem (differential topology)

Frobenius theorem (differential topology) En mathématiques, Frobenius' theorem gives necessary and sufficient conditions for finding a maximal set of independent solutions of an overdetermined system of first-order homogeneous linear partial differential equations. In modern geometric terms, given a family of vector fields, the theorem gives necessary and sufficient integrability conditions for the existence of a foliation by maximal integral manifolds whose tangent bundles are spanned by the given vector fields. The theorem generalizes the existence theorem for ordinary differential equations, which guarantees that a single vector field always gives rise to integral curves; Frobenius gives compatibility conditions under which the integral curves of r vector fields mesh into coordinate grids on r-dimensional integral manifolds. The theorem is foundational in differential topology and calculus on manifolds.

Contenu 1 Introduction 1.1 From analysis to geometry 2 Frobenius' theorem in modern language 2.1 Formulation using vector fields 2.2 Differential forms formulation 3 Généralisations 3.1 Infinite dimensions 3.1.1 Banach manifolds 3.2 Holomorphic forms 3.3 Higher degree forms 4 Histoire 5 Applications 6 Voir également 7 Remarques 8 References Introduction In its most elementary form, the theorem addresses the problem of finding a maximal set of independent solutions of a regular system of first-order linear homogeneous partial differential equations. Laisser {style d'affichage à gauche{F_{k}^{je}:mathbf {R} ^{n}to mathbf {R} : 1leq ileq n,1leq kleq rright}} be a collection of C1 functions, with r < n, and such that the matrix ( f i k ) has rank r. Consider the following system of partial differential equations for a C2 function u : Rn → R: {displaystyle (1)quad {begin{cases}L_{1}u {stackrel {mathrm {def} }{=}} sum _{i}f_{1}^{i}(x){frac {partial u}{partial x^{i}}}=0\L_{2}u {stackrel {mathrm {def} }{=}} sum _{i}f_{2}^{i}(x){frac {partial u}{partial x^{i}}}=0\qquad cdots \L_{r}u {stackrel {mathrm {def} }{=}} sum _{i}f_{r}^{i}(x){frac {partial u}{partial x^{i}}}=0end{cases}}} One seeks conditions on the existence of a collection of solutions u1, ..., un−r such that the gradients ∇u1, ..., ∇un−r are linearly independent. The Frobenius theorem asserts that this problem admits a solution locally[1] if, and only if, the operators Lk satisfy a certain integrability condition known as involutivity. Specifically, they must satisfy relations of the form {displaystyle L_{i}L_{j}u(x)-L_{j}L_{i}u(x)=sum _{k}c_{ij}^{k}(x)L_{k}u(x)} for 1 ≤ i, j ≤ r, and all C2 functions u, and for some coefficients ckij(x) that are allowed to depend on x. In other words, the commutators [Li, Lj] must lie in the linear span of the Lk at every point. The involutivity condition is a generalization of the commutativity of partial derivatives. In fact, the strategy of proof of the Frobenius theorem is to form linear combinations among the operators Li so that the resulting operators do commute, and then to show that there is a coordinate system yi for which these are precisely the partial derivatives with respect to y1, ..., yr. From analysis to geometry Even though the system is overdetermined there are typically infinitely many solutions. For example, the system of differential equations {displaystyle {begin{cases}{frac {partial f}{partial x}}+{frac {partial f}{partial y}}=0\{frac {partial f}{partial y}}+{frac {partial f}{partial z}}=0end{cases}}} clearly permits multiple solutions. Nevertheless, these solutions still have enough structure that they may be completely described. The first observation is that, even if f1 and f2 are two different solutions, the level surfaces of f1 and f2 must overlap. In fact, the level surfaces for this system are all planes in R3 of the form x − y + z = C, for C a constant. The second observation is that, once the level surfaces are known, all solutions can then be given in terms of an arbitrary function. Since the value of a solution f on a level surface is constant by definition, define a function C(t) by: {displaystyle f(x,y,z)=C(t){text{ whenever }}x-y+z=t.} Conversely, if a function C(t) is given, then each function f given by this expression is a solution of the original equation. Thus, because of the existence of a family of level surfaces, solutions of the original equation are in a one-to-one correspondence with arbitrary functions of one variable. Frobenius' theorem allows one to establish a similar such correspondence for the more general case of solutions of (1). Suppose that u1, ..., un−r are solutions of the problem (1) satisfying the independence condition on the gradients. Consider the level sets[2] of (u1, ..., un−r) as functions with values in Rn−r. If v1, ..., vn−r is another such collection of solutions, one can show (using some linear algebra and the mean value theorem) that this has the same family of level sets but with a possibly different choice of constants for each set. Thus, even though the independent solutions of (1) are not unique, the equation (1) nonetheless determines a unique family of level sets. Just as in the case of the example, general solutions u of (1) are in a one-to-one correspondence with (continuously differentiable) functions on the family of level sets.[3] The level sets corresponding to the maximal independent solution sets of (1) are called the integral manifolds because functions on the collection of all integral manifolds correspond in some sense to constants of integration. Once one of these constants of integration is known, then the corresponding solution is also known. Frobenius' theorem in modern language The Frobenius theorem can be restated more economically in modern language. Frobenius' original version of the theorem was stated in terms of Pfaffian systems, which today can be translated into the language of differential forms. An alternative formulation, which is somewhat more intuitive, uses vector fields. Formulation using vector fields In the vector field formulation, the theorem states that a subbundle of the tangent bundle of a manifold is integrable (or involutive) if and only if it arises from a regular foliation. In this context, the Frobenius theorem relates integrability to foliation; to state the theorem, both concepts must be clearly defined. One begins by noting that an arbitrary smooth vector field {displaystyle X} on a manifold {displaystyle M} defines a family of curves, its integral curves {displaystyle u:Ito M} (for intervals {displaystyle I} ). These are the solutions of {displaystyle {dot {u}}(t)=X_{u(t)}} , which is a system of first-order ordinary differential equations, whose solvability is guaranteed by the Picard–Lindelöf theorem. If the vector field {displaystyle X} is nowhere zero then it defines a one-dimensional subbundle of the tangent bundle of {displaystyle M} , and the integral curves form a regular foliation of {displaystyle M} . Thus, one-dimensional subbundles are always integrable. If the subbundle has dimension greater than one, a condition needs to be imposed. One says that a subbundle {displaystyle Esubset TM} of the tangent bundle {displaystyle TM} is integrable (or involutive), if, for any two vector fields {displaystyle X} and {displaystyle Y} taking values in {displaystyle E} , the Lie bracket {displaystyle [X,Y]} takes values in {displaystyle E} as well. This notion of integrability need only be defined locally; that is, the existence of the vector fields {displaystyle X} and {displaystyle Y} and their integrability need only be defined on subsets of {displaystyle M} . Several definitions of foliation exist. Here we use the following: Definition. A p-dimensional, class Cr foliation of an n-dimensional manifold M is a decomposition of M into a union of disjoint connected submanifolds {Lα}α∈A, called the leaves of the foliation, with the following property: Every point in M has a neighborhood U and a system of local, class Cr coordinates x=(x1, ⋅⋅⋅, xn) : U→Rn such that for each leaf Lα, the components of U ∩ Lα are described by the equations xp+1=constant, ⋅⋅⋅, xn=constant. A foliation is denoted by {displaystyle {mathcal {F}}} ={Lα}α∈A.[4] Trivially, any foliation of {displaystyle M} defines an integrable subbundle, since if {displaystyle pin M} and {displaystyle Nsubset M} is the leaf of the foliation passing through {displaystyle p} then {displaystyle E_{p}=T_{p}N} is integrable. Frobenius' theorem states that the converse is also true: Given the above definitions, Frobenius' theorem states that a subbundle {displaystyle E} is integrable if and only if the subbundle {displaystyle E} arises from a regular foliation of {displaystyle M} . Differential forms formulation Let U be an open set in a manifold M, Ω1(U) be the space of smooth, differentiable 1-forms on U, and F be a submodule of Ω1(U) of rank r, the rank being constant in value over U. The Frobenius theorem states that F is integrable if and only if for every p in U the stalk Fp is generated by r exact differential forms. Geometrically, the theorem states that an integrable module of 1-forms of rank r is the same thing as a codimension-r foliation. The correspondence to the definition in terms of vector fields given in the introduction follows from the close relationship between differential forms and Lie derivatives. Frobenius' theorem is one of the basic tools for the study of vector fields and foliations. There are thus two forms of the theorem: one which operates with distributions, that is smooth subbundles D of the tangent bundle TM; and the other which operates with subbundles of the graded ring Ω(M) of all forms on M. These two forms are related by duality. If D is a smooth tangent distribution on M, then the annihilator of D, I(D) consists of all forms {displaystyle alpha in Omega ^{k}(M)} (for any {displaystyle kin {1,dots ,operatorname {dim} M}} ) such that {displaystyle alpha (v_{1},dots ,v_{k})=0} for all {displaystyle v_{1},dots ,v_{k}in D} . The set I(D) forms a subring and, in fact, an ideal in Ω(M). Furthermore, using the definition of the exterior derivative, it can be shown that I(D) is closed under exterior differentiation (it is a differential ideal) if and only if D is involutive. Consequently, the Frobenius theorem takes on the equivalent form that I(D) is closed under exterior differentiation if and only if D is integrable. Generalizations The theorem may be generalized in a variety of ways. Infinite dimensions One infinite-dimensional generalization is as follows.[5] Let X and Y be Banach spaces, and A ⊂ X, B ⊂ Y a pair of open sets. Let {displaystyle F:Atimes Bto L(X,Y)} be a continuously differentiable function of the Cartesian product (which inherits a differentiable structure from its inclusion into X × Y) into the space L(X,Y) of continuous linear transformations of X into Y. A differentiable mapping u : A → B is a solution of the differential equation {displaystyle (1)quad y'=F(x,y)} if {displaystyle forall xin A:quad u'(x)=F(x,u(x)).} The equation (1) is completely integrable if for each {displaystyle (x_{0},y_{0})in Atimes B} , there is a neighborhood U of x0 such that (1) has a unique solution u(x) defined on U such that u(x0)=y0. The conditions of the Frobenius theorem depend on whether the underlying field is R or C. If it is R, then assume F is continuously differentiable. If it is C, then assume F is twice continuously differentiable. Then (1) is completely integrable at each point of A × B if and only if {displaystyle D_{1}F(x,y)cdot (s_{1},s_{2})+D_{2}F(x,y)cdot (F(x,y)cdot s_{1},s_{2})=D_{1}F(x,y)cdot (s_{2},s_{1})+D_{2}F(x,y)cdot (F(x,y)cdot s_{2},s_{1})} for all s1, s2 ∈ X. Here D1 (resp. D2) denotes the partial derivative with respect to the first (resp. second) variable; the dot product denotes the action of the linear operator F(x, y) ∈ L(X, Y), as well as the actions of the operators D1F(x, y) ∈ L(X, L(X, Y)) and D2F(x, y) ∈ L(Y, L(X, Y)). Banach manifolds The infinite-dimensional version of the Frobenius theorem also holds on Banach manifolds.[6] The statement is essentially the same as the finite-dimensional version. Let M be a Banach manifold of class at least C2. Let E be a subbundle of the tangent bundle of M. The bundle E is involutive if, for each point p ∈ M and pair of sections X and Y of E defined in a neighborhood of p, the Lie bracket of X and Y evaluated at p, lies in Ep: {displaystyle [X,Y]_{p}in E_{p}} On the other hand, E is integrable if, for each p ∈ M, there is an immersed submanifold φ : N → M whose image contains p, such that the differential of φ is an isomorphism of TN with φ−1E. The Frobenius theorem states that a subbundle E is integrable if and only if it is involutive. Holomorphic forms The statement of the theorem remains true for holomorphic 1-forms on complex manifolds — manifolds over C with biholomorphic transition functions.[7] Specifically, if {displaystyle omega ^{1},dots ,omega ^{r}} are r linearly independent holomorphic 1-forms on an open set in Cn such that {displaystyle domega ^{j}=sum _{i=1}^{r}psi _{i}^{j}wedge omega ^{i}} for some system of holomorphic 1-forms ψ j i, 1 ≤ i, j ≤ r, then there exist holomorphic functions fij and gi such that, on a possibly smaller domain, {displaystyle omega ^{j}=sum _{i=1}^{r}f_{i}^{j}dg^{i}.} This result holds locally in the same sense as the other versions of the Frobenius theorem. In particular, the fact that it has been stated for domains in Cn is not restrictive. Higher degree forms The statement does not generalize to higher degree forms, although there is a number of partial results such as Darboux's theorem and the Cartan-Kähler theorem. History Despite being named for Ferdinand Georg Frobenius, the theorem was first proven by Alfred Clebsch and Feodor Deahna. Deahna was the first to establish the sufficient conditions for the theorem, and Clebsch developed the necessary conditions. Frobenius is responsible for applying the theorem to Pfaffian systems, thus paving the way for its usage in differential topology. Applications In classical mechanics, the integrability of a system's constraint equations determines whether the system is holonomic or nonholonomic. See also Integrability conditions for differential systems Domain-straightening theorem Newlander-Nirenberg Theorem Notes ^ Here locally means inside small enough open subsets of Rn. Henceforth, when we speak of a solution, we mean a local solution. ^ A level set is a subset of Rn corresponding to the locus of: (u1, ..., un−r) = (c1, ..., cn−r), for some constants ci. ^ The notion of a continuously differentiable function on a family of level sets can be made rigorous by means of the implicit function theorem. ^ Lawson, H. Blaine (1974), "Foliations", Bulletin of the American Mathematical Society, 80 (3): 369–418, ISSN 0040-9383, Zbl 0293.57014 ^ Dieudonné, J (1969). "Ch. 10.9". Foundations of modern analysis. Academic Press. ISBN 9780122155307. ^ Lang, S. (1995). "Ch. VI: The theorem of Frobenius". Differential and Riemannian manifolds. Springer-Verlag. ISBN 978-0-387-94338-1. ^ Kobayashi, S.; Nomizu, K. (2009) [1969]. "Appendix 8". Foundations of Differential Geometry. Wiley Classics Library. Vol. 2. Wiley. ISBN 978-0-471-15732-8. Zbl 0175.48504. References Lawson, H.B. (1977). The Qualitative Theory of Foliations. American Mathematical Society CBMS Series. Vol. 27. AMS. Abraham, Ralph.; Marsden, Jerrold E. (2008) [1978]. "2.2.26 Frobenius' Theorem". Foundations of Mechanics (2nd ed.). American Mathematical Society. p. 93. ISBN 9780821844380. Clebsch, A. (1866). "Ueber die simultane Integration linearer partieller Differentialgleichungen". J. Reine. Angew. Math. (Crelle). 65: 257–268. doi:10.1515/crll.1866.65.257. Deahna, F. (1840). "Über die Bedingungen der Integrabilitat ...". J. Reine Angew. Math. 20: 340–350. doi:10.1515/crll.1840.20.340. Frobenius, G. (1877). "Über das Pfaffsche Problem". J. für Reine und Agnew. Math. 82: 230–315. doi:10.1515/crll.1877.82.230. Categories: Theorems in differential geometryTheorems in differential topologyDifferential systemsFoliations

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