Infinite-dimensional vector function explained

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 formulaf(t) = (f_1(t), f_2(t), f_3(t), \ldots)\,,takes values that lie in the infinite-dimensional vector space

X

(or

\R\N

) of real-valued sequences. For example,f(2) = \left(2, \frac, \frac, \frac, \frac, \ldots\right).

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

A\toK

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]\toX,

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) = \lim_\frac.

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)=\lim_ \frac.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,

t\inRn

or even

t\inY,

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: iff = (f_1,f_2,f_3,\ldots)(that is,

f=f1e1+f2e2+f3e3+ … ,

where

e1,e2,e3,\ldots

is an orthonormal basis of the space

X

), and

f'(t)

exists, thenf'(t) = (f_1'(t),f_2'(t),f_3'(t),\ldots).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

See main article: 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]

. 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. 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. 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:\beginf :\;&& [0, 1] &&\;\to \;& L^2(0, 1) \\[0.3ex] && t &&\;\mapsto\;& \mathbb_ \\\endwhere

1[0,t]:(0,1)\to\{0,1\}

is the indicator function defined byx \;\mapsto\; \begin1 & \text x \in [0, t]\\ 0 & \text \endA 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).

A crinkled arc

f:[0,1]\toX

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.

If

h:[0,1]\to[0,1]

is an increasing homeomorphism then

f\circh

is called a reparameterization of the curve

f:[0,1]\toX.

Two curves

f

and

g

in an inner product space

X

are unitarily equivalent if there exists a unitary operator

L:X\toX

(which is an isometric linear bijection) such that

g=L\circf

(or equivalently,

f=L-1\circg

).

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.

References