hamburgminicourse2017:classes_of_static_potentials
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| hamburgminicourse2017:classes_of_static_potentials [2017/04/02 15:44] – markus | hamburgminicourse2017:classes_of_static_potentials [2017/04/04 09:27] (current) – markus | ||
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| **Theorem (Kato--Rellich).** For $A$ self-adjoint, | **Theorem (Kato--Rellich).** For $A$ self-adjoint, | ||
| - | With tools of Fourier analysis one shows that for $A=-\Delta$ this indeed holds for $B=v \in L^2(\mathbb{R}^3)+L^\infty(\mathbb{R}^3)$ which includes the usual singular Coulomb potential and also for finite sums $B=V=\sum_i v(x_i) + \sum_{i< | + | With tools of Fourier analysis one shows that for $A=-\Delta$ this indeed holds for $B=v \in L^2(\mathbb{R}^3)+L^\infty(\mathbb{R}^3)$, which includes the usual singular Coulomb potential, and it also holds for finite sums $B=V=\sum_i v(x_i) + \sum_{i< |
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| \|V\psi\|_{L^2} \leq \|V\|_K \|\psi\|_{H^2}. | \|V\psi\|_{L^2} \leq \|V\|_K \|\psi\|_{H^2}. | ||
| \] | \] | ||
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| + | One could ask if the Kato perturbations are the maximal class for the Kato--Rellich theorem to hold, but this is not the case. An almost maximal class is given by the so-called Stummel class potentials that are closely related to the Kato class (again something different than the Kato perturbations) of the form version of the Kato--Rellich theorem, called KLMN theorem. | ||
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hamburgminicourse2017/classes_of_static_potentials.1491140666.txt.gz · Last modified: 2017/04/02 15:44 by markus