all norms on finite-dimensional vector spaces are equivalent

Theorem.

All norms on finite-dimensional vector spaces over $\mathrm{R}$ or $\mathrm{C}$ are equivalent (http://planetmath.org/EquivalentNorms).

A consequence of this is that there is only one norm induced topology on a finite dimensional vector space. This means that on such a vector space, we need not worry about what norm we use when we talk about convergence of a sequence of vectors in norm. So a standard use of this theorem is in continuity arguments over finite dimensional vector spaces, and it allows you to pick the most convenient norm for your argument (the Euclidean norm is not always very convenient).

This obviously is not true for infinite dimensional spaces, for example see the different $L^p$ spaces (http://planetmath.org/LpSpace). Note that the reason all this works is because a unit sphere is compact in a finite dimensional vector space, while that is not true in an infinite dimensional one.

Proof.

Any such finite-dimensional space is really just the same as ${ℝ}^n$ so we can talk about just those spaces. That is, any finite-dimensional vector space over $ℝ$ or $ℂ$ is isomorphic to ${ℝ}^n$ for some $n$ (note that $ℂ$ is just isomorphic to ${ℝ}^2$ as a vector space over $ℝ$). To see this, just write any element of the space in of the basis and then define the isomorphism to take that basis to the standard basis in ${ℝ}^n$ and then extend linearly.

First let’s show that if two norms are equivalent on the unit sphere (all $\overrightarrow{x}$ such that $\parallel \overrightarrow{x}\parallel =1$ with respect to some norm, for example the standard Euclidean norm) then they are equivalent everywhere. We can write any $\overrightarrow{x}\in {ℝ}^n$ as a multiple of some scalar $\gamma \ge 0$ and a vector on the unit sphere, say $\overrightarrow{x_0}$, that is $\overrightarrow{x}=\gamma \overrightarrow{x_0}$. Then when suppose we have two equivalent norms, say $\parallel \cdot {\parallel }_a$ and $\parallel \cdot {\parallel }_b$, on the unit sphere

$$\alpha {\parallel \overrightarrow{x_0}\parallel }_a\le {\parallel \overrightarrow{x_0}\parallel }_b\le \beta {\parallel \overrightarrow{x_0}\parallel }_a$$

$$\gamma \alpha {\parallel \overrightarrow{x_0}\parallel }_a\le \gamma {\parallel \overrightarrow{x_0}\parallel }_b\le \gamma \beta {\parallel \overrightarrow{x_0}\parallel }_a$$

$$\alpha {\parallel \gamma \overrightarrow{x_0}\parallel }_a\le {\parallel \gamma \overrightarrow{x_0}\parallel }_b\le \beta {\parallel \gamma \overrightarrow{x_0}\parallel }_a$$

$$\alpha {\parallel \overrightarrow{x}\parallel }_a\le {\parallel \overrightarrow{x}\parallel }_b\le \beta {\parallel \overrightarrow{x}\parallel }_a.$$

So the norms are equivalent everywhere.

Suppose we are working with the 2-norm. Now we want to show that any other norm is a continuous function with respect to the 2-norm. Take an arbitrary finite-dimensional space $X$ and an arbitrary norm $\parallel \cdot \parallel$. Also suppose that ${\{\overrightarrow{b_i}\}}_1^n$ is a basis of $X$ and so an element $\overrightarrow{x}\in X$ may be written as $\overrightarrow{x}={\sum }_1^n{x}_i\overrightarrow{b_i}$. Now given an $ϵ>0$, choose $\delta >0$ such that (the Euclidean distance is less then $\delta$) implies that

In fact we can just choose $\delta$ to be the right side of the above inequality. Now we note that the triangle inequality immediately also yields the inequality $|\parallel \overrightarrow{x}\parallel -\parallel \overrightarrow{y}\parallel |\le \parallel \overrightarrow{x}-\overrightarrow{y}\parallel$. So

And so $\parallel \cdot \parallel$ is a continuous function.

Suppose we are given two norms $\parallel \cdot {\parallel }_a$ and $\parallel \cdot {\parallel }_b$, we know that they are both continuous functions with respect to the 2-norm. And so the function defined as

$$f(\overrightarrow{x}):=\frac{{\parallel \overrightarrow{x}\parallel }_a}{{\parallel \overrightarrow{x}\parallel }_b}$$

is a continuous function on the unit sphere (with respect to the 2-norm). This function is continuous except perhaps at 0, but we don’t care about the value at zero. On the unit sphere however $f(\overrightarrow{x})$ is continuous and thus achieves a maximum and a minimum since the unit sphere is compact. Let’s call the minimum and maximum, $\alpha$ and $\beta$ respectively. Then for any $\overrightarrow{x}$ on the unit sphere we have

$$\alpha \le f(\overrightarrow{x})\le \beta$$

$$\alpha \le \frac{{\parallel \overrightarrow{x}\parallel }_a}{{\parallel \overrightarrow{x}\parallel }_b}\le \beta$$

$$\alpha {\parallel \overrightarrow{x}\parallel }_b\le {\parallel \overrightarrow{x}\parallel }_a\le \beta {\parallel \overrightarrow{x}\parallel }_b.$$

And so the norms are equivalent on the unit sphere and thus as we shown above, everywhere. ∎

Title	all norms on finite-dimensional vector spaces are equivalent
Canonical name	AllNormsOnFinitedimensionalVectorSpacesAreEquivalent
Date of creation	2013-03-22 14:08:54
Last modified on	2013-03-22 14:08:54
Owner	jirka (4157)
Last modified by	jirka (4157)
Numerical id	15
Author	jirka (4157)
Entry type	Theorem
Classification	msc 46B99