Solved – Eigenfunctions and eigenvalues of the exponential kernel

kernel trick

What are the eigenfunctions and the eigenvalues of the exponential kernel?

The exponential kernel is defined as $$k(x,x')=\sigma^2\exp\left(\frac{||x-x'||}{l}\right)$$ where both $\sigma>0$ and $l>0$.

Mercers theorem tell us that for every kernel function $k(x,x')$ there exists a decomposition in eigenfunctions $\phi_i(x)$ and corresponding eigenvalues $\lambda_i$ such that

$$k(x,x')=\sum_{i=1}^\infty \lambda_i \phi_i(x)\phi_i(x)$$

The Fourier transform $$\mathcal{F}(k)(\omega)=\frac{1}{\sqrt{2 \pi}} \int_{-\infty}^{\infty} k(r) e^{i\omega r}dr$$ of the function $$k(r)=\sigma^2 \exp\left(\frac{||r||}{l}\right)$$ with $r=x-x'$ is $$\mathcal{F}(k)(\omega)=\frac{\sqrt{\frac{2}{\pi }} \sigma^2 l}{l^2 \omega ^2+1}.$$ How to proceed from here?

Best Answer

First of all, your question is not quite well-posed. The reason is that Mercer's theorem only applies for the case of a kernel defined on a finite measure space. Practically, this means that in order to apply the theorem, the eigenfunctions $\phi_i$ are in fact taken with respect to the operator $$K_{\mu}(f)= \left( x\mapsto \int_{\mathbb{R}} K(x,y)f(y)\mu(dy)\right)$$ where $\mu(dy)=p(y)dy$ is a probability measure. The $\phi_i$ are then orthonormal wrt to the inner product defined by $<f,g>=\int f(x)g(x)\mu(dx)$.

It is simple to see that the condition $\mu(\mathbb{R})<\infty$ is necessary for Mercer's theorem to hold. Consider the identity:

$$\int_{\mathbb{R}} e^{-(x-y)^2}xdx=\sqrt{\pi}y$$

This shows that the function $f(x)=x$ is an eigfunction of the operator $\int K(x,y)f(y)dy$. But evidently $\int_{\mathbb{R}} f(x)^2dx=\infty$, which shows that it is not possible to construct an orthonormal basis of $K$, without introducing a weighting function $p(y)$.

Secondly, I am assuming there should be a minus sign in the definition of the kernel $e^{-|x-y|}$, otherwise the resulting kernel fails to be positive definite.

Related Question