Infinite-dimensional vector function
Infinite–dimensional vector function refers to a function whose values lie in an infinite-dimensional topological vector space, such as a Hilbert space or a Banach space.
Such functions are applied in most sciences including physics.
Example
Set for every positive integer and every real number Then the function defined for real numbers by the formula takes values that lie in the infinite-dimensional vector space (or ) of real-valued sequences. For example,
As a number of different topologies can be defined on the space to talk about the derivative of it is first necessary to specify a topology on or the concept of a limit in
Moreover, for any set there exist infinite-dimensional vector spaces having the (Hamel) dimension of the cardinality of (for example, the space of functions with finitely-many nonzero elements, where is the desired field of scalars). Furthermore, the argument could lie in any set instead of the set of real numbers.
Integral and derivative
Most theorems on integration and differentiation of scalar functions can be generalized to vector-valued functions, often using essentially the same proofs. Perhaps the most important exception is that absolutely continuous functions need not equal the integrals of their (a.e.) derivatives (unless, for example, is a Hilbert space); see Radon–Nikodym theorem
Derivatives
If where is a Banach space or another topological vector space then the derivative of can be defined in the usual way:
Functions with values in a Hilbert space
If is a function of real numbers with values in a Hilbert space then the derivative of at a point can be defined as in the finite-dimensional case: Most results of the finite-dimensional case also hold in the infinite-dimensional case too, with some modifications. Differentiation can also be defined to functions of several variables (for example, or even where is an infinite-dimensional vector space).
N.B. If is a Hilbert space, then one can easily show that any derivative (and any other limit) can be computed componentwise: if (that is, where is an orthonormal basis of the space ), and exists, then However, the existence of a componentwise derivative does not guarantee the existence of a derivative, as componentwise convergence in a Hilbert space does not guarantee convergence with respect to the actual topology of the Hilbert space.
Most of the above hold for other topological vector spaces too. However, not as many classical results hold in the Banach space setting, for example, an absolutely continuous function with values in a suitable Banach space need not have a derivative anywhere. Moreover, in most Banach spaces setting there are no orthonormal bases.
Measurability
The measurability of can be defined by a number of ways, most important of which are Bochner measurability and weak measurability.
Integrals
The most important integrals of are called Bochner integral (when is a Banach space) and Pettis integral (when is a topological vector space). Both these integrals commute with linear functionals. Also spaces have been defined for such functions.
See also
- Differentiation in Fréchet spaces
- Differentiable vector–valued functions from Euclidean space – Differentiable function in functional analysis
References
- Einar Hille & Ralph Phillips: "Functional Analysis and Semi Groups", Amer. Math. Soc. Colloq. Publ. Vol. 31, Providence, R.I., 1957.
- Halmos, Paul R. (8 November 1982). A Hilbert Space Problem Book. Graduate Texts in Mathematics. Vol. 19 (2nd ed.). New York: Springer-Verlag. ISBN 978-0-387-90685-0. OCLC 8169781.