cwf:space-analyticity_of_wave_function:coulomb_potential
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| cwf:space-analyticity_of_wave_function:coulomb_potential [2016/11/25 19:07] – markus | cwf:space-analyticity_of_wave_function:coulomb_potential [2017/01/24 14:42] (current) – markus | ||
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| + | ====== Space-analyticity of wave function under evolution with Coulomb potential ====== | ||
| + | Free evolution [[free evolution|conserves analyticity]] but what if the initial state $\Psi_0$ is real-analytic but the acting Hamiltonian includes a non-analytic or even singular potential, like the Coulomb central potential $V(x) = -1/|x|$? One would suppose that in this case, analyticity gets destroyed, at least for almost all times $t \neq 0$. | ||
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| + | If one scans the literature a positive analyticity result can be found in [(: | ||
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| + | > On the other hand, if $V$ is not smooth, e.g., if $V$ is the Coulomb potential in dimension three, the singularities of $V$ create those of the FDS and $E(t, x, y)$ [the fundamental solution] is not smooth everywhere. However, the strong dissipation property of the free propagator $\mathrm{e}^{-\mathrm{itH_0}}$ moderates the singularities and we expect that $E(t, x, y)$ is bounded and continuous for $t\neq 0$ if $V$ is bounded at infinity in a suitable norm and is not too singular locally (see Simon [14] [ref. [(: | ||
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| + | The author goes on and shows boundedness and continuity for the fundamental solution for a class that includes the Coulomb potential in dimension three. Finally one should note that for a Hamiltonian with Coulomb potentials and even including Coulomb interactions between multiple particles, it is known that an eigenstate is analytic away from the potential sigularities and has $|x|$-formed cusps at the location of the singularities [(: | ||
