Infinite–dimensional vector function

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An infinite–dimensional vector function is 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 fk(t)=t/k2 for every positive integer k and every real number t. Then the function f defined by the formula f(t)=(f1(t),f2(t),f3(t),), takes values that lie in the infinite-dimensional vector space X (or ) of real-valued sequences. For example, f(2)=(2,24,29,216,225,).

As a number of different topologies can be defined on the space X, to talk about the derivative of f, it is first necessary to specify a topology on X or the concept of a limit in X.

Moreover, for any set A, there exist infinite-dimensional vector spaces having the (Hamel) dimension of the cardinality of A (for example, the space of functions AK with finitely-many nonzero elements, where K is the desired field of scalars). Furthermore, the argument t 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, X is a Hilbert space); see Radon–Nikodym theorem

A curve is a continuous map of the unit interval (or more generally, of a non−degenerate closed interval of real numbers) into a topological space. An arc is a curve that is also a topological embedding. A curve valued in a Hausdorff space is an arc if and only if it is injective.

Derivatives

If f:[0,1]X, where X is a Banach space or another topological vector space then the derivative of f can be defined in the usual way: f(t)=limh0f(t+h)f(t)h.

Functions with values in a Hilbert space

If f is a function of real numbers with values in a Hilbert space X, then the derivative of f at a point t can be defined as in the finite-dimensional case: f(t)=limh0f(t+h)f(t)h. 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, tRn or even tY, where Y is an infinite-dimensional vector space).

If X is a Hilbert space then any derivative (and any other limit) can be computed componentwise: if f=(f1,f2,f3,) (that is, f=f1e1+f2e2+f3e3+, where e1,e2,e3, is an orthonormal basis of the space X), and f(t) exists, then f(t)=(f1(t),f2(t),f3(t),). 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 X 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.

Crinkled arcs

Main page: Crinkled arc

If [a,b] is an interval contained in the domain of a curve f that is valued in a topological vector space then the vector f(b)f(a) is called the chord of f determined by [a,b].[1] If [c,d] is another interval in its domain then the two chords are said to be non−overlapping chords if [a,b] and [c,d] have at most one end−point in common.[1] Intuitively, two non−overlapping chords of a curve valued in an inner product space are orthogonal vectors if the curve makes a right angle turn somewhere along its path between its starting point and its ending point. If every pair of non−overlapping chords are orthogonal then such a right turn happens at every point of the curve; such a curve can not be differentiable at any point.[1] A crinkled arc is an injective continuous curve with the property that any two non−overlapping chords are orthogonal vectors. An example of a crinkled arc in the Hilbert L2 space L2(0,1) is:[2] f:[0,1]L2(0,1)t𝟙[0,t] where 𝟙[0,t]:(0,1){0,1} is the indicator function defined by x{1 if x[0,t]0 otherwise  A crinkled arc can be found in every infinite−dimensional Hilbert space because any such space contains a closed vector subspace that is isomorphic to L2(0,1).[2] A crinkled arc f:[0,1]X is said to be normalized if f(0)=0, f(1)=1, and the span of its image f([0,1]) is a dense subset of X.[2]

Proposition[2] — Given any two normalized crinkled arcs in a Hilbert space, each is unitarily equivalent to a reparameterization of the other.

If h:[0,1][0,1] is an increasing homeomorphism then fh is called a reparameterization of the curve f:[0,1]X.[1] Two curves f and g in an inner product space X are unitarily equivalent if there exists a unitary operator L:XX (which is an isometric linear bijection) such that g=Lf (or equivalently, f=L1g).

Measurability

The measurability of f can be defined by a number of ways, most important of which are Bochner measurability and weak measurability.

Integrals

The most important integrals of f are called Bochner integral (when X is a Banach space) and Pettis integral (when X is a topological vector space). Both these integrals commute with linear functionals. Also Lp spaces have been defined for such functions.

See also

References

  1. 1.0 1.1 1.2 1.3 Halmos 1982, pp. 5−7.
  2. 2.0 2.1 2.2 2.3 Halmos 1982, pp. 5−7,168−170.