Graduate

GraduateReal AnalysisFunctional Analysis


Operators on Spaces


In the vast field of functional analysis, a key concept is that of operators on spaces. Understanding these operators involves figuring out how functions can be transformed, represented, and manipulated within various types of spaces. These spaces typically form complete vector spaces with additional structures such as norms. The study of operators connects these concepts, playing a key role in practical applications ranging from quantum mechanics to differential equations.

To take a deeper look at this topic, let's first explore the basic building blocks - vector spaces and the different types of operators. Then, we'll explore how operators work in these spaces, including specific types of operators and practical examples.

Vector space

A vector space is a collection of objects, known as vectors, that can be added together and multiplied by scalars (numbers), usually real or complex numbers. The concept of a vector space is quite broad and includes infinite-dimensional spaces of functions and sequences.

For example, consider the 2-dimensional vector space ℝ². This space contains all ordered pairs (x, y) where x and y are real numbers. The 3-dimensional vector space ℝ³ contains all ordered triples (x, y, z).

Operators: An overview

An operator is essentially a function that maps elements from one vector space to another (or the same) vector space. Formally, if V and W are vector spaces, then the operator can be a mapping:

T : V → W

Usually, the operators we encounter in functional analysis are called linear operators, which means that they satisfy two criteria:

  1. Additivity: T(u v) = T(u) T(v) u, v ∈ V
  2. Symmetry: T(cu) = cT(u) where u ∈ V and scalar c

These conditions ensure that operators preserve vector space structure, such as addition and scalar multiplication.

Examples of linear operators

Some classic examples of linear operators include:

  • Matrix Multiplication: Consider a matrix A representing an operator on ℝ². If x is a vector in ℝ², then the product Ax is another vector in ℝ².
  • Differential Operator: Defined as (D(f))(x) = f'(x), where D maps a differentiable function to its derivative.
  • Integral Operator: Maps a function to its integral over a certain interval.

Visual example: Matrix multiplication

To see this, consider the matrix A = [[2, 1], [1, 2]] and the vector x = [3, 5]. The operator A transforms x into:

a * x = [[2, 1], 
         [1, 2]] * [3, 5] = [2*3   1*5, 1*3   2*5] = [11, 13]

[3, 5] [11, 13]

Here, the blue line represents the original vector, and the green line represents the transformed vector. This transformation characterizes how operators act within a vector space.

Functional analysis: A broader perspective

Functional analysis extends these concepts further by investigating operators on spaces of functions, often in infinite-dimensional settings. These spaces are equipped with additional structures, such as norms or inner products, which allow us to explore an array of topics such as continuity, limits, and compactness.

Normed spaces and Banach spaces

A normed space adds a function called the norm, which provides a measure of vector length. If V is a vector space, then the norm is a function || · ||: V → ℝ that satisfies certain properties:

  • ||v|| ≥ 0 for all v ∈ V (non-negativity)
  • ||v|| = 0 if and only if v = 0 (definiteness)
  • ||cv|| = |c| ||v|| for a scalar c (homogeneity)
  • ||u v|| ≤ ||u|| ||v|| (Triangle Inequality)

When a vector space with a norm is complete, meaning that all Cauchy sequences converge within the space, it becomes a Banach space.

Example: Continuity of operators

An operator T is continuous if, for every positive number ε, there exists δ > 0 such that:

||u - v|| < δ ⇒ ||T(u) - T(v)|| < ε

An important result in functional analysis is that linear operators from one normed space to another normed space are continuous if and only if they are bounded. A bounded operator T satisfies:

||T(v)|| ≤ C ||v|| for all v in V

Where C is a constant.

Visual example: Bounded operators

Consider an operator that scales vectors by a certain magnitude. If the original vector is represented as:

Original

And the operator measures it like this:

Flaky

This scaling is constant across all vectors, making the operator bounded.

Hilbert spaces

A Hilbert space is a vector space equipped with an inner product, which is a generalization of the dot product. This inner product allows us to define the concepts of angle and orthogonality, which are not possible in general Banach spaces.

Hilbert spaces are complete with respect to the norm induced by the inner product. The inner product on a space H is a function:

⟨ , · ⟩: H × H → ℂ

satisfying properties such as linearity, conjugate isomorphism and positivity. If u, v are elements in H, then ⟨u, v⟩ provides a measure of similarity or projection.

Types of operators on a Hilbert space

  • Self-adjoint operator: an operator T for which ⟨T(u), v⟩ = ⟨u, T(v)⟩ for all u, v in the space.
  • Unitary operator: preserves norms and distances, such that ⟨T(u), T(v)⟩ = ⟨u, v⟩.
  • Normal operator: commutes with its adjoint, i.e. if T* is adjoint, then TT* = T*T.

Example: Fourier transform as operator

The Fourier transform is a powerful operator in Hilbert space, important in signal processing. It decomposes a function into its frequency components, thereby aiding in the analysis and solution of differential equations.

Formally, for a function f(x), the Fourier integral is given by:

f(k) = ∫ f(x) e^(-2πikx) dx

It integrates the function against complex sinusoids, and provides insight into its behavior in frequency space.

Conclusion

Operators on spaces in functional analysis provide a rich framework for understanding transformations and interactions within vector spaces. These are essential not only from a theoretical mathematical point of view but also for practical applications in science and engineering. By studying different types of operators – linear, bounded, self-adjoint and unitary – within different spaces, we can visualise and handle many complex phenomena theoretically.

While this explanation covers many concepts, operators on space have even more depth and breadth that can be explored in more advanced contexts. Addressing this promising area of mathematics allows mathematicians and scientists to effectively model and solve real-world problems.


Graduate → 1.6.3


U
username
0%
completed in Graduate


Comments