Exactly solvable Schrödinger equations with a position-dependent mass: Null potential

2007 ◽  
Vol 107 (15) ◽  
pp. 3039-3045 ◽  
Author(s):  
J. J. Peña ◽  
G. Ovando ◽  
J. Morales ◽  
J. García-Ravelo ◽  
C. Pacheco-García
2010 ◽  
Vol 25 (34) ◽  
pp. 2915-2922
Author(s):  
T. K. JANA ◽  
P. ROY

It is shown that Hamiltonians of the form H(s) = (1 - s)H- + sH+, 0 ≤ s ≤ 1 where H± are supersymmetric partner Hamiltonians corresponding to position-dependent mass Schrödinger equations are exactly solvable for a number of deformed shape-invariant potentials. The method has also been extended to a system with broken supersymmetry.


2008 ◽  
Vol 108 (15) ◽  
pp. 2906-2913 ◽  
Author(s):  
J. J. Peña ◽  
G. Ovando ◽  
J. Morales ◽  
J. GarcÍa-Ravelo ◽  
C. Pacheco-García

2006 ◽  
Vol 21 (06) ◽  
pp. 1359-1377 ◽  
Author(s):  
AXEL SCHULZE-HALBERG

The formalism of Darboux transformations is established for time-dependent Schrödinger equations with an effective (position-dependent) mass. Explicit formulas are obtained for the transformed wave function and the difference between the original and the transformed potential. It is shown that for a noneffective mass our Darboux transformation reduces correctly to the well-known Darboux transformation.


2009 ◽  
Vol 18 (09) ◽  
pp. 1831-1844 ◽  
Author(s):  
AXEL SCHULZE-HALBERG ◽  
JESÚS GARCÍA-RAVELO ◽  
JOSÉ JUAN PEÑA GIL

We generalize the semiclassical Bohr–Sommerfeld quantization rule to an exact, implicit spectral formula for linear, generalized Schrödinger equations admitting a discrete spectrum. Special cases include the position-dependent mass Schrödinger equation or the Schrödinger equation for weighted energy. Requiring knowledge of the potential and the solution associated with the lowest spectral value, our formula predicts the complete spectrum in its exact form.


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