AAMathNote

Operator Norm

Yun-Hao Lee, Cheng-Han Huang

Credit: Bhargava Marripati from Pexels


1. Introduction

The operator norm is a norm defined on the space of bounded linear operators between two given normed vector spaces.

2. Normed Vector Space and Linear Operator

Definition 2.1. A normed vector space (𝒱,||||) over a field 𝔽 is a vector space 𝒱 endowed with a function |||| : 𝒱 such that

  • ||v|| 0 for all v 𝒱.
  • ||v|| = 0 if and only if v = 0.
  • ||λv|| = |λ|||v|| for every v 𝒱 and every scalar λ 𝔽.
  • ||v1 + v2||||v1|| + ||v2|| for all v1,v2 𝒱.

Lemma 2.2. A linear operator between normed vector spaces is bounded if and only if it is continuous.

Proof. Let (A,||||a),(B,||||b) over a field 𝔽 be normed vector spaces and L : (A,||||a) (B,||||b) be a linear map, that is,

L(αa1) = αL(a1)andL(a1 + a2) = L(a1) + L(a2)fora1,a2 Awithα 𝔽

: Suppose L is bounded, then for all vectors a,h A with h0,

0 ||L(a + h) L(a)||b = ||L(h)||b M||h||afor some constant M

As h goes to 0,

lim h00 lim h0||L(a + h) L(a)||b = lim h0||L(h)||b lim h0M||h||a.

Since lim h0 = 0 and lim h0M||h||a = 0, applying squeeze theorem gives

lim h0||L(a + h) L(a)||b = 0

Hence L is continuous.

: By definition of continuous, for all 𝜀 > 0, there exists δ > 0 such that

||h 0||a < δimplies||L(h) L(0)||b < 𝜀

for all h A. Since L is a linear map, ||L(h) L(0)||b = ||L(h)||b. Now taking 𝜀 = 1, then for all nonzero α A, we have

||L(α)||b = ||2 δL(δ 2α)||b = ||2||α||a δ L(δ 2 α ||α||a)||b = 2||α||a δ ||L(δ 2 α ||α||a)||b < 2||α||a δ = 2 δ||α||a

Hence L is bounded.

3. Definition of Operator Norm

Given two normed vector space (X,||||X) and (Y,||||Y ) over the same field 𝔽, a linear operator A : (X,||||X) (Y,||||Y ) is continuous if and only if there exists a real number c 𝔽 such that

||Ax||Y c||x||Xfor allx X

Now we give the definition of operator norm.

Definition 3.1. The norm of a linear operator A is defined by

||A||op = inf {c 0 : ||Ax||Y c||x||Xfor allx X}

4. The Equivalence Definitions About Operator Norm

Theorem 4.1. If X{0}, then

||A||op = inf {c 0 : ||Ax||Y c||x||Xfor allx X} = sup {||Ax||Y : ||x||X 1andx X} = sup {||Ax||Y : ||x||X {0,1}andx X} = sup {||Ax||Y : ||x||X = 1andx X} = sup {||Ax||Y ||x||X : x0andx X}

Proof. Let

I = inf {c 0 : ||Ax||Y c||x||Xfor allx X} S1 = sup {||Ax||Y : ||x||X 1andx X} S2 = sup {||Ax||Y : ||x||X = 1andx X} S3 = sup {||Ax||Y ||x||X : x0andx X}

First, we show S1 = S2 = S3.
Notice that

{||Ax||Y : ||x||X = 1andx X}{||Ax||Y : ||x||X 1andx X}

The supremum of {||Ax||Y : ||x||X = 1andx X} must not be greater then the supremum of {||Ax||Y : ||x||X 1andx X}, that is

S2 S1

On the other hand, since A is a linear operator, the elements in {||Ax||Y ||x||X : x0andx X} can be written in the form

||Ax||Y ||x||X = ||A x ||x||X||Y ,and|| x ||x||X||X = 1

So

{||Ax||Y ||x||X : x0andx X}{||Ax||Y : ||x||X = 1andx X}

One may check that the two sets are actually identical, but for convenience only subset relation will be taken here and S3 S2 can be obtained by the relation.

Also, for all ||x||X 1, the inequality

||Ax||Y 1 ||x||X||Ax||Y

is sufficient to give S1 S3.
Hence we conclude S1 = S2 = S3.

Now, we show I = S3 and therefore S1 = S2 = S3 = I.
Since S3 = sup {||Ax||Y ||x||X : x0andx X}, for all x X the inequality ||Ax||Y S3||x||X must be satisfied, so I S3.
By definition of supremum, there is xn X with

I ||Axn||Y ||xn||X S3 1 nfor alln

this gives I S3.
Since I S3 and I S3, equality must hold and therefore I = S3.

Note that we have left the case sup {||Ax||Y : ||x||X {0,1}}. As ||Ax||Y must be nonnegative and

||x||X = 0x = 0Ax = 0||Ax||Y = 0

Therefore, sup {||Ax||Y : ||x||X {0,1}} is exactly the same as S2.

Note 4.2. If X = {0}, then the last two equivalence definitions can not be applied since ||0||X must be 0 and 0 cannot be the denominator.

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