Vector-valued differential form: Difference between revisions
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With this operation the set of all Lie algebra-valued forms on a manifold ''M'' becomes a [[graded Lie superalgebra]]. |
With this operation the set of all Lie algebra-valued forms on a manifold ''M'' becomes a [[graded Lie superalgebra]]. |
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The operation <math>[\omega\wedge\eta]</math> can also be defined as the bilinear operation on <math>\Omega(M, \mathfrak g)</math> satisfying |
The operation <math>[\omega\wedge\eta]</math> can also be defined as the bilinear operation on <math>\Omega(M, \mathfrak g)</math> satisfying |
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:<math>[(g \otimes \alpha) \wedge (h \otimes \beta)] = [g, h] \otimes (\alpha \wedge \beta)</math> |
:<math>[(g \otimes \alpha) \wedge (h \otimes \beta)] = [g, h] \otimes (\alpha \wedge \beta)</math> |
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for all <math>g, h \in \mathfrak g</math> and <math>\alpha, \beta \in \Omega(M, \mathbb R)</math>. |
for all <math>g, h \in \mathfrak g</math> and <math>\alpha, \beta \in \Omega(M, \mathbb R)</math>. |
Revision as of 21:54, 28 March 2013
In mathematics, a vector-valued differential form on a manifold M is a differential form on M with values in a vector space V. More generally, it is a differential form with values in some vector bundle E over M. Ordinary differential forms can be viewed as R-valued differential forms. Vector-valued forms are natural objects in differential geometry and have numerous applications.
Formal definition
Let M be a smooth manifold and E → M be a smooth vector bundle over M. We denote the space of smooth sections of a bundle E by Γ(E). A E-valued differential form of degree p is a smooth section of the tensor product bundle of E with Λp(T*M), the p-th exterior power of the cotangent bundle of M. The space of such forms is denoted by
Because Γ is a monoidal functor, this can also be interpreted as
where the latter two tensor products are the tensor product of modules over the ring Ω0(M) of smooth R-valued functions on M (see the fifth example here). By convention, an E-valued 0-form is just a section of the bundle E. That is,
Equivalently, a E-valued differential form can be defined as a bundle morphism
which is totally skew-symmetric.
Let V be a fixed vector space. A V-valued differential form of degree p is a differential form of degree p with values in the trivial bundle M × V. The space of such forms is denoted Ωp(M, V). When V = R one recovers the definition of an ordinary differential form. If V is finite-dimensional, then one can show that the natural homomorphism
where the first tensor product is of vector spaces over R, is an isomorphism. One can verify this for p=0 by turning a basis for V into a set of constant functions to V, which allows the construction of an inverse to the above homomorphism. The general case can be proved by noting that
and that because is a sub-ring of Ω0(M) via the constant functions,
Operations on vector-valued forms
Pullback
One can define the pullback of vector-valued forms by smooth maps just as for ordinary forms. The pullback of an E-valued form on N by a smooth map φ : M → N is an (φ*E)-valued form on M, where φ*E is the pullback bundle of E by φ.
The formula is given just as in the ordinary case. For any E-valued p-form ω on N the pullback φ*ω is given by
Wedge product
Just as for ordinary differential forms, one can define a wedge product of vector-valued forms. The wedge product of a E1-valued p-form with a E2-valued q-form is naturally a (E1⊗E2)-valued (p+q)-form:
The definition is just as for ordinary forms with the exception that real multiplication is replaced with the tensor product:
In particular, the wedge product of an ordinary (R-valued) p-form with an E-valued q-form is naturally an E-valued (p+q)-form (since the tensor product of E with the trivial bundle M × R is naturally isomorphic to E). For ω ∈ Ωp(M) and η ∈ Ωq(M, E) one has the usual commutativity relation:
In general, the wedge product of two E-valued forms is not another E-valued form, but rather an (E⊗E)-valued form. However, if E is an algebra bundle (i.e. a bundle of algebras rather than just vector spaces) one can compose with multiplication in E to obtain an E-valued form. If E is a bundle of commutative, associative algebras then, with this modified wedge product, the set of all E-valued differential forms
becomes a graded-commutative associative algebra. If the fibers of E are not commutative then Ω(M,E) will not be graded-commutative.
Exterior derivative
For any vector space V there is a natural exterior derivative on the space of V-valued forms. This is just the ordinary exterior derivative acting component-wise relative to any basis of V. Explicitly, if {eα} is a basis for V then the differential of a V-valued p-form ω = ωαeα is given by
The exterior derivative on V-valued forms is completely characterized by the usual relations:
More generally, the above remarks apply to E-valued forms where E is any flat vector bundle over M (i.e. a vector bundle whose transition functions are constant). The exterior derivative is defined as above on any local trivialization of E.
If E is not flat then there is no natural notion of an exterior derivative acting on E-valued forms. What is needed is a choice of connection on E. A connection on E is a linear differential operator taking sections of E to E-valued one forms:
If E is equipped with a connection ∇ then there is a unique covariant exterior derivative
extending ∇. The covariant exterior derivative is characterized by linearity and the equation
where ω is a E-valued p-form and η is an ordinary q-form. In general, one need not have d∇2 = 0. In fact, this happens if and only if the connection ∇ is flat (i.e. has vanishing curvature).
Lie algebra-valued forms
An important case of vector-valued differential forms are Lie algebra-valued forms. These are -valued forms where is a Lie algebra. Such forms have important applications in the theory of connections on a principal bundle as well as in the theory of Cartan connections.
Since every Lie algebra has a bilinear Lie bracket operation, the wedge product of two Lie algebra-valued forms can be composed with the bracket operation to obtain another Lie algebra-valued form. This operation is denoted by to indicate both operations involved, or often just . For example, if and are Lie algebra-valued one forms, then one has
With this operation the set of all Lie algebra-valued forms on a manifold M becomes a graded Lie superalgebra.
The operation can also be defined as the bilinear operation on satisfying
for all and .
The alternative notation , which resembles a commutator, is justified by the fact that if the Lie algebra is a matrix algebra then is nothing but the graded commutator of and , i. e. if and then
where are wedge products formed using the matrix multiplication on .
Basic or tensorial forms on principal bundles
Let E → M be a smooth vector bundle of rank k over M and let π : F(E) → M be the (associated) frame bundle of E, which is a principal GLk(R) bundle over M. The pullback of E by π is isomorphic to the trivial bundle F(E) × Rk. Therefore, the pullback by π of an E-valued form on M determines an Rk-valued form on F(E). It is not hard to check that this pulled back form is right-equivariant with respect to the natural action of GLk(R) on F(E) × Rk and vanishes on vertical vectors (tangent vectors to F(E) which lie in the kernel of dπ). Such vector-valued forms on F(E) are important enough to warrant special terminology: they are called basic or tensorial forms on F(E).
Let π : P → M be a (smooth) principal G-bundle and let V be a fixed vector space together with a representation ρ : G → GL(V). A basic or tensorial form on P of type ρ is a V-valued form ω on P which is equivariant and horizontal in the sense that
- for all g ∈ G, and
- whenever at least one of the vi are vertical (i.e., dπ(vi) = 0).
Here Rg denotes the right action of G on P for some g ∈ G. Note that for 0-forms the second condition is vacuously true.
Given P and ρ as above one can construct the associated vector bundle E = P ×ρ V. Tensorial forms on P are in one-to-one correspondence with E-valued forms on M. As in the case of the principal bundle F(E) above, E-valued forms on M pull back to V-valued forms on P. These are precisely the basic or tensorial forms on P of type ρ. Conversely given any tensorial form on P of type ρ one can construct the associated E-valued form on M in a straightforward manner.