Large order dimensional perturbation theory for complex energy eigenvalues

1993 ◽  
Vol 99 (10) ◽  
pp. 7739-7747 ◽  
Author(s):  
Timothy C. Germann ◽  
Sabre Kais
1998 ◽  
Vol 58 (1) ◽  
pp. 250-257 ◽  
Author(s):  
Shi-Wei Huang ◽  
David Z. Goodson ◽  
Mario López-Cabrera ◽  
Timothy C. Germann

1992 ◽  
Vol 68 (13) ◽  
pp. 1992-1995 ◽  
Author(s):  
M. López-Cabrera ◽  
D. Z. Goodson ◽  
D. R. Herschbach ◽  
J. D. Morgani

1992 ◽  
Vol 97 (11) ◽  
pp. 8481-8496 ◽  
Author(s):  
D. Z. Goodson ◽  
M. López‐Cabrera ◽  
D. R. Herschbach ◽  
John D. Morgan

1969 ◽  
Vol 24 (3) ◽  
pp. 344-349
Author(s):  
A. D. Jannussis

AbstractIn this paper the Dirac equation for a rectilinear onedimensional periodic potential is treated. It is shown that the energy eigenvalues are periodic functions of the wave number Kϰ and the continuous spectrum is split into energy bands. The end points of the energy bands are the points where the Bragg reflection takes place. These results are obtained by perturbation theory, as well as by the method of determinants, since the resulting eigenvalue equation has the form of a determinant which is similar to the Hill determinant.


1979 ◽  
Vol 49 (2) ◽  
pp. 205-213 ◽  
Author(s):  
J. Zinn-Justin

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