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 SIGMA 3 (2007), 110, 12 pages      arXiv:0711.3544     
https://doi.org/10.3842/SIGMA.2007.110 
Contribution to the Proceedings of the Seventh International Conference Symmetry in Nonlinear Mathematical Physics 
Alternative Method for Determining the Feynman Propagator of a Non-Relativistic Quantum Mechanical Problem
Marcos Moshinsky a, Emerson Sadurní a and Adolfo del Campo b
 a) Instituto de Física
 Universidad Nacional Autónoma de México,  Apartado Postal  20-364, 01000 México D.F., México
 b) Departamento de Química-Física, Universidad del País Vasco, Apdo. 644, Bilbao, Spain
 
 
Received August 21, 2007, in final form November 13, 2007; Published online November 22, 2007; Misprints are corrected December 06, 2007
 
Abstract
 
A direct procedure for determining the propagator
associated with a
 quantum mechanical problem was given by the Path
Integration Procedure of Feynman. The Green function, which is the
Fourier Transform with respect to the time variable of the
propagator, can be derived later. In our approach, with the help of
a Laplace transform, a direct way to get the energy dependent Green
function is presented, and the propagator can be obtained later with
an inverse Laplace transform. The method is illustrated through
simple one dimensional examples and for time independent potentials,
though it can be generalized to the derivation of more complicated
propagators.
  
 Key words:
propagator; Green functions; harmonic oscillator. 
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References
 
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- Jaeger J.C., An introduction to Laplace transform, Methuen,
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Table of integrals, series and products, Academic Press, 1965.
 
- Sakurai J.J.,
Modern quantum mechanics, Addison-Wesley, 1994.
 
-  Holstein  B.R., The linear potential propagator, Amer. J. Phys. 65 (1997), 414-418.
 
Holstein  B.R., The harmonic oscillator propagator, Amer. J. Phys.  66 (1998), 583-589. 
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Amer. J. Phys. 66 (1998), 537-540.
 
 
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