Geometry

Elements of geometry FS25

Elements of geometry FS25


F. L.
This flashcard set covers advanced geometry concepts at the university level, focusing on manifolds, vector spaces, and differential forms. It delves into topics like Riemannian metrics, connections, curvature, and orientations, exploring their properties and applications. Ideal for students and researchers in mathematics, this set provides a comprehensive overview of geometric structures and their roles in modern geometry, offering insights into the fundamental theories and theorems that shape the field.
Karten
89
Lernende
2
Sprache
Englisch
Kategorie
Mathematik
Stufe
Universität
Erstellt / Aktualisiert
03.06.2025 / 14.06.2025

Lernkarten

tangent bundle

Let M be a smooth manifold. The tangent bundle of M, denoted by TM is defined as: \(TM = T_pM\). p∈M So it is the disjoint union of all the tangent spaces of M. We represent an element of TM as a pair (p,v) where p ∈ M and \(v ∈ T_pM\). There is an obvious map \(π : TM →M\) given by \(π(p,v) = p\).

vector bundle

Let M be a smooth manifold. A vector bundle of rank r on M is a smooth manifold E together with a smooth map \(π : E → M\) and a structure of a real vector space of rank r on each fiber \(π^{−1}(p)\) of \(π\) such that the following condition is satisfied; Every point of M admits an open neighborhood U and a smooth diffeomorphism \(ϕ : π^{−1}(U) \xrightarrow{\sim} U × \mathbb{R}^r\) compatible with the projections to U and such taht for every p ∈ U, the map \( ϕ_p : π^{−1}(p) → \mathbb{R}^r\) is a vector space isomorphism.

smooth section

Let M a smooth manifold and \(π : E → M\) a vector bundle on M. We denote by \(C^\infty(M;E) \) the set of all smooth sections of \(π\), i.e., of smooth maps \(s : M → E\) such that \(π ◦s = Id_M\). An element of \(C^\infty(M;E)\) is simply called a section of E.

vector field

Let M be a smooth manifold. A vector field on M is a smooth section of the tangent bundle on M, i.e., an element of the \(C^\infty(M)\)-module \(C^\infty(M;TM)\). Often, vector fields are denoted by X,Y,Z, etc. So they are smooth maps \(X :M →TM, p \mapsto X|_p ∈ TpM\). When we do not insist that the section X is smooth, we say that X is a rough vector field on M.

cotangent bundle

Let M be a smooth manifold. The cotangent bundle of M, denoted by \(T^∗M\), is defined to be the dual of the tangent bundle TM. Thus, the fiber at \(p ∈ M\) is the vector space \(T^*_ p M = Hom(T_pM,\mathbb{R})\)  of linear forms on \(T_pM\). The elements of \(T^∗_ pM\) are called the tangent covectors at p or simply covector at p.

differential form

Let M be a smooth manifold. A smooth section of the cotangent bundle is called a differential form on M. The \(C^\infty(M)\)-module of differential forms is denoted by \(Ω^1(M) = C^\infty(M;T^*M).\)

pullback

Let \(F : M → N\) be a smooth map. If \(ω ∈ Ω^1(N)\) is a smooth form, then \(F^∗(ω) ∈ Ω^1(M)\) is also smooth. In particular, we have an R-linear map: \(F^∗ : Ω^1(N) → Ω^1(M)\) which is \(C^\infty(N)\)-linear in the following sense \(F^∗(g · ω) = (g ◦F)·F^∗(ω)\) bzw. \(F^*\omega(X) =\omega(F_*X)\) for \(X \in T_pM\).

Diffeomorphism invariance of the integral

Let ω be a smooth differential form on the compact interval \([a,b] ⊆ \mathbb{R}\). Let \(φ : [c,d] → [a,b]\) be an increasing diffeomorphism (i.e., if \( t_1 ≤ t_2\), then \(φ(t_1) ≤ φ(t_2)\)). Then we have \(\int_{[c,d]}φ^∗ω = \int_{[a,b]}\omega\) 

line integral

Given a differential form \(\omega\) on M, \(\int_\gamma \omega = \int_{[a,b]} \gamma^*\omega\) is the line integral over \(\gamma\).

reparametrization

 If \(γ : [a,b] → M\) and \(\tilde{ γ} : [c,d] → M\) are curve segments, we say that \(\tilde{ γ}\) is a reparametrization of \(\gamma\) if there exists an increasing diffeomorphism \(φ : [c,d] → [a,b] \)such that \(γ ◦φ = \tilde{ γ}\).

Fundamental theorem for line integrals

Let M be a smooth manifold. Let \( f ∈ C^\infty(M)\) and \(γ : [a,b] → M\) a curve segment. Then \(\int_{\gamma}df = f(γ(b)) −f(γ(a))\).

differential k-form

 Let M be a manifold. A differential k-form on M is a smooth section of the vector bundle \(\wedge^k T^∗M\). If we don’t require smoothness, we speak of rough k-forms. The \(C^\infty(M)\)-module of differential k-forms is denoted by \( Ω^k(M) := C^\infty(M;\wedge^k T^∗M.)\)

Existence and uniqueness of exterior differential

Let M be a smooth manifold. There are unique operators \(d : Ω^∗(M) → Ω^{∗+1}(M)\), called exterior differentiation, satisfying the following properties:

(i) d is linear over R.

(ii) If \(ω ∈ Ω^k(M)\) and \(η ∈ Ω^l(M)\), then \(d(ω ∧η) = dω ∧η +(−1)^kω ∧dη.\)

(iii) \(d ◦ d = 0\).

(iv) For \(f ∈ Ω^0(M) = C^\infty(M)\), df is the 1-form defined in the previous chapter.

complex

A complex (of vector spaces) is a graded vector space \(K^• = {K^n}_{n∈Z}\) to gether with a degree-1 linear map \(K^• \xrightarrow{d}K^{•+1}\), such that \(d^2 = 0\).

cohomology

The n-th cohomology of a complex \(K^•\) is defined by \(H^n(K) := ker(d : K^n → K^{n+1})/Im(d : K^{n−1} → K^{n})\) For this to make sense we need that \(d^2 = 0\).

de rham complex

Let M be a smooth manifold. The de Rham complex of M is the complex \((Ω^•(M),d)\) of smooth differential forms with the exterior derivative.

de rham cohomology

The de Rham cohomology of M is the cohomology of the de Rham complex. It is denoted by: \(H^n _{dR}(M) := H^n(Ω^•(M)) = ker(d : Ω(M)^n → Ω(M)^{n+1})/Im(d : Ω(M)^{n−1} → Ω(M)^n)\)

morphism of complexes

Let \(K^•\) and \(L^•\) be two complexes of vector spaces. A morphism of complexes is a graded morphism \(f^• : K^• → L^• \) commuting with the differentials i.e. \(d^n _L◦f^n = f^{n+1}◦d^n _K\) for all \(n ∈ \mathbb{Z}\). 

 homotopy operator 

 Let \(K^•\) and \(L^•\) be two complexes of vector spaces. A homotopy operator from \(K^•\) to \(L^•\) is a sequence of maps \( h_n : K^n → L^{n−1}\). The associated morphism of complexes is: \(\{d^{n−1}_ L ◦h_n+h_{n+1}◦d^n _K\}_{n∈Z}\).

homotopy

Let \(f^•,g^• : K^• → L^•\) be two morphisms of complexes. A homotopy from \(f^•\) to \(g^•\) is a homotopy operator \( \{h_n\}_{n∈\mathbb{Z}}\) such that \( f^n −g^n =d^{n−1}_ L ◦h_n+h_{n+1}◦d^n_ K\) for all \(n ∈ \mathbb{Z}\). 

theorem homotopy invariance

Let M be a smooth manifold. Then the obvious projection \([0,1] × M \xrightarrow{p} M\) induces an isomorphism \(H^n _{dR}(M) \xrightarrow{p^*} H^n _{dR}([0,1] × M)\) for all \(n ∈ \mathbb{Z}\).

mayer vietoris theorem

Let M be a smooth manifold and assume that \(U,V ⊂ M\) are open subsets such that \(M = U ∪V\). Then we have a short exact sequence of de Rham complexes \(0 → Ω^•(M) → Ω^•(U)⊕Ω^•(V) → Ω^•(U ∩V) → 0\). It induces a long exact sequence in de Rham cohomology \(... → H^{n−1}_{ dR} (U ∩V)→H^n _{dR}(M) →H^n _{dR}(U)⊕H^n_{ dR}(V) → H^n _{dR}(U ∩V) → ...\)

star-shaped

 A subset \(U ⊂ \mathbb{R}^n\) is said to be star-shaped if there exists a point \(x_0 ∈ U\) such that for every \(y ∈ U\), the segment \([x_0,y]\) is contained in U.

poincaré lemma

Let M be a smooth manifold, and \(\omega\) a closed differential n-form, with n ≥ 1. Then \(\omega\) is locally exact, i.e., can be written locally as \(dη\), for \(η\) an n−1-form.

same orientation

Let V be a finite dimensional vector space over \(\mathbb{R}\). Let \((e_1,...e_n)\) and \((e′ _1, ..., e′ _n)\) be two bases of V. We say that these two bases have the same orientation if \(\frac{e′ _1∧...∧e′_n} {e_1∧...∧e_n} \in \mathbb{R} \backslash \{0\}\)  is positive. Equivalently, if we write \(e_i'=\sum_{j=1}^n a_{ij}e_j\) then \(det(a_{ij}) > 0\).

Remark on orientation

On every finite dimenional vector space V over \( \mathbb{R}\) there are exactly two equivalence classes of bases for the relation of having the same orientation. An orientation of V is a choice of one of these classes.

oriented vector space

An oriented vector space is a finite dimensional vector space V together with an orientation. A basis of V is said to be positively oriented if it belongs to the chosen orientation.

orientation

Let M be a smooth manifold of dimension n. An orientation of M is the choice of positive bases of \(∧^nT^∗M.\) More precisely, we consider the set of nowhere top degree forms \(\omega\) on M and we say that \( \omega ∼ \omega′ \) if there exists a positive smooth function f such that \(w′ = f\cdot\omega\) . An orientation is an equivalence class for this relation.

orientable

A smooth manifold M is said to be orientable if \(∧^{top}T^∗ M\) is trivial. An oriented smooth manifold is a pair consisting of smooth manifold together with an orientation.

oriented, preserves orientation

Let M and N be two oriented smooth manifolds, and F : M → N a local diffeomorphism. We say that F is oriented if for every positive top degree form on N, \(F^∗(\omega)\) is positive on M.

measure zero

A subset \( X ⊂ \mathbb{R}^n\) is said to have measure zero if for every \(δ > 0\), there exists a countable cover of X by rectangles \((C_i)_{i≥0}\), such that \(\sum_{i\geq0}Vol(C_i) ≤ δ\).

Lebesgues integrability criterion

Let \(A ⊂ \mathbb{R}^n\) be a closed rectangle and let \(f : A → \mathbb{R}\) be a bounded function. Assume that S = {x ∈ A|f not continuous at x} has measure zero. Then f is integrable.

domain of integration

 A subset \(D ⊂ \mathbb{R}^n\) is called a domain of integration if D is closed bounded and its boundary ∂D has measure zero.

integral of f on D

Let D be a domain of integration and A a closed rectangle containing A. Let \( f : D → \mathbb{R}\) be a continuous function. Let \(\tilde{ f }: A → \mathbb{R}\) be the extension by zero. Then \(S( \tilde{f}) ⊂ ∂A\) has measure zero and we can set \(\int_Df := \int_A \tilde{ f}\). It is easy to see that this is independent of the choice of A. This is called the integral of f on D.

theorem change of varibles

Let D and E be domains of integrations in Rn and let \(F : D → E\) be a smooth map inducing a diffeomorphism on the interior \(D^0 \xrightarrow{\sim} E^0\). Let \(g : E →\mathbb{R}\) be a continuous function. Then \(\int_E g = \int_D |det(DF)|\cdot g\circ F\) where DF is the Jacobian matrix.

manifold with boundary

A topoolgical manifold with boundary is a topological space which is locally homeomorphic to \(\mathbb{R}_+×\mathbb{R}^{n−1} = \mathbb{H}^n\). If M is a topological manifold with boundary, its boundary \(∂M\) is defined as the union of \(φ^{−1}({0}×\mathbb{R}^{n−1}∩φ(U))\) for all the charts \((U,φ)\) of M. A smooth manifold with boundary is a topological manifold with boundary endowed with a smooth atlas. If M is a smooth manifold with boundary, \(∂M\) is a smooth manifold.

stokes theorem

Let M be a smooth oriented n-manifold with boundary. Let \(\omega\) be a compactly supported (n − 1)-form on M. Then \(\int_Md \omega= \int_{\partial M} \omega|_{∂M}\).

inner product

Let V be a finite dimensional vector space over \(\mathbb{R}\). An inner product on V is a symmetric bilinear form \(<.,. >: V ×V →\mathbb{R}\) which is definite-positive, i.e.m such that \(< v,v >> 0\), for every nonzero v ∈ V .

angle

Let (V,<,>) be an inner product space. Given v ∈ V, we set \(∥v∥ = \sqrt{\langle v,v\rangle}\), which is called the length of v. Given two nonzero vectors \(v,w ∈ V\), the angle between v,w is defined as the unique \(θ ∈ [0,π]\) such that \(cosθ = \frac{\langle v,w \rangle}{∥v∥ · ∥w∥}\) . The right hand side belongs to [−1,1].

symmetric bilinear form

Let M be a smooth manifold and p : E → M a vector bundle on M. A symmetric bilinear form on E is a smooth section of B of \((E^V)^{⊗2} → M\), the bundle of bilinear forms on E, such that, for every p ∈ M, the bilinear fomr Bp : Ep × Ep → R is symmetric. 

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