Asymptotic (semiclassical) equivalence for Schrödinger equations with singular potentials and for related systems of two first‐order equations

1993 ◽  
Vol 34 (8) ◽  
pp. 3351-3377 ◽  
Author(s):  
Vincenzo Aquilanti ◽  
Simonetta Cavalli ◽  
Mikhail B. Sevryuk
Symmetry ◽  
2021 ◽  
Vol 13 (8) ◽  
pp. 1527
Author(s):  
Alexey Anatolievich Magazev ◽  
Maria Nikolaevna Boldyreva

We study symmetry properties and the possibility of exact integration of the time-independent Schrödinger equation in an external electromagnetic field. We present an algorithm for constructing the first-order symmetry algebra and describe its structure in terms of Lie algebra central extensions. Based on the well-known classification of the subalgebras of the algebra e(3), we classify all electromagnetic fields for which the corresponding time-independent Schrödinger equations admit first-order symmetry algebras. Moreover, we select the integrable cases, and for physically interesting electromagnetic fields, we reduced the original Schrödinger equation to an ordinary differential equation using the noncommutative integration method developed by Shapovalov and Shirokov.


10.14311/1366 ◽  
2011 ◽  
Vol 51 (2) ◽  
Author(s):  
A. Schulze-Halberg

We construct an explicit relation between propagators of generalized Schrödinger equations that are linked by a first-order supersymmetric transformation. Our findings extend and complement recent results on the conventional case [1].


2008 ◽  
Vol 23 (03n04) ◽  
pp. 537-546 ◽  
Author(s):  
AXEL SCHULZE-HALBERG

We construct first-order Darboux transformations for stationary Schrödinger equations with position-dependent (effective) mass and energy-dependent potential. We point out characteristic differences to the corresponding Darboux transformation for constant mass.14


Author(s):  
Andrii Khrabustovskyi ◽  
Imen Rassas ◽  
Éric Soccorsi

We consider the inverse problem of determining the coupling coefficients in a two-state Schrödinger system. We prove a Lipschitz stability inequality for the zeroth- and first-order coupling terms by finitely many partial lateral measurements of the solution to the coupled Schrödinger equations.


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