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Name: | ||||||||||||
Miloslav Znojil | ||||||||||||
Reviewer number: | ||||||||||||
9689 | ||||||||||||
Email: | ||||||||||||
znojil@ujf.cas.cz | ||||||||||||
Item's zbl-Number: | ||||||||||||
DE 017 587 319 | ||||||||||||
Author(s): | ||||||||||||
Andrianov, A. Yu. | ||||||||||||
Shorttitle: | ||||||||||||
A spectral theorem for Sturm Liouville operators | ||||||||||||
Source: | ||||||||||||
Differ. Equ. 37, No. 8, 1074 - 1087 (2001); translation from Russian: Differ. Uravn. 37, No. 8, 1028 - 1040 (2001). | ||||||||||||
Classification: | ||||||||||||
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Primary Classification: | ||||||||||||
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Keywords:
| Schroedinger equation; potentials that are finite sums of exponentials; | Review: | A finite sum of exponentials exp(igx) (over some K positive g's) defines a potential V(x) and Hamiltonian H which is not self-adjoint. The author proves that the set of the related (right) Hilbert-space eigenfunctions may still be understood as playing the same eigenfunction expansion role as their standard Sturm-Liouville analogs do in the self-adjoint cases. The precise meaning of this observation is formulated and proved as a theorem giving the expansion of a function f in terms of the eigenstates of H in the form of the Fourier-type pricipal-value integral over the spectrum. The author adds a remark which recommends an alternative arrangement of the eigenfunction expansion in the form with separates the contribution of the continuous spectrum from that of the isolated spectral singularities. Marginally, it is also worth noting that on the certain modified domains specified by the so called PT symmetry requirement in quantum mechanics, the Hamiltonians H in question may still possess the pure point spectrum [cf. F. Cannata et al, Phys. Lett. A 246 (1998) 219 where K = 1 and M. Znojil, Phys. Lett. A 264 (1999) 108 where K = 2] and could attract a further study motivated by the physics of bound states. Remarks to the editors: |
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