I tried to look this up on Wikipedia, but I couldn't find anything.

I am reading Barry Simon's book "Schrödinger Operators", where he brings up the concept of a form domain $Q(A)$ of a self-adjoint operator $A$. I looked in his mathematical physics series, but couldn't pinpoint a definition.

In parallel to stating some perturbation theorems about form domains, he also states theorems about operator domains, which are quite self-explanatory. I've never heard of form domains however.

What are they? How and where do they come up in operator theory? Why are they important, generally speaking?

  • $\begingroup$ I believe it might have something to do with quadratic forms... $\endgroup$
    – r.g.
    Commented Jul 11, 2011 at 7:37
  • $\begingroup$ Well, this is all discussed in detail in Reed and Simon vol. I. Section VIII.6 (also, Simon gives a reference...) $\endgroup$
    – t.b.
    Commented Jul 11, 2011 at 10:33
  • $\begingroup$ Thanks Theo. I was looking in the second volume, because in the book I was reading the chapter on Self-Adjointness, and the second volume of Reed-Simon series is about Fourier Analysis and Self-Adjointness. $\endgroup$
    – r.g.
    Commented Jul 11, 2011 at 11:26

1 Answer 1


The definition is given in Reed & Simon, Methods of Mathematical Physics, volume 1, page 276; see also example 2 on page 277.

Essentially the form domain is the "largest domain" on which a self-adjoint operator can "make sense" in a weak way. Formally speaking given an unbounded self-adjoint operator $A$ on some Hilbert space $\mathcal{H}$, you can consider the quadratic form $\psi \mapsto (\psi,A\psi)$. The largest dense subspace of $\mathcal{H}$ which we denote by $Q(A)$ on which this quadratic form makes sense is called the form domain of $A$.

As an example, let $\mathcal{H}$ be $L^2(\mathbb{R})$. We known that the Laplacian does not makes sense on all of $L^2$, it's domain $D(A)$ is roughly speaking the Sobolev space $H^2(\mathbb{R})$ of functions in $L^2$ whose second derivative is also in $L^2$. But if you consider the quadratic form $(\psi,\triangle\psi) = (\nabla\psi,\nabla\psi)$ (a formal integration by parts; this can be made more precise using the spectral representation of $A$), we see that the form domain $Q(A)$ is more like $H^1$; we just require the first derivative now to be in $L^2$.

Note that $Q(A)$ necessarily contains $D(A)$. But it is often possible to extend the quadratic form to a larger domain.

(For why and how this is used, you should see that section of Reed and Simon, as well as vol 2, Chapter X, the section on quadratic forms.)


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