AxiomOfChoice
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I have started coming across square roots (H+kI)^{\frac 12} of slight modifications of Schrodinger operators H on L^2(\mathbb R^d); that is, operators that look like this:
<br /> H = -\Delta + V(x),<br />
where \Delta is the d-dimensional Laplacian and V corresponds to multiplication by some function. But how do we go about defining (H+kI)^{1/2}? My understanding was that we defined functions of self-adjoint operators by using the spectral theorem, but that only holds for bounded Borel functions, right? And f(x) = \sqrt x certainly isn't bounded. And because of the \Delta, the operator H isn't even bounded. So what do we do?
<br /> H = -\Delta + V(x),<br />
where \Delta is the d-dimensional Laplacian and V corresponds to multiplication by some function. But how do we go about defining (H+kI)^{1/2}? My understanding was that we defined functions of self-adjoint operators by using the spectral theorem, but that only holds for bounded Borel functions, right? And f(x) = \sqrt x certainly isn't bounded. And because of the \Delta, the operator H isn't even bounded. So what do we do?
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