Extra nodes and the phase shift of the scattering wave function for a nonlocal potential

1977 ◽  
Vol 15 (5) ◽  
pp. 1623-1635 ◽  
Author(s):  
B. Bagchi ◽  
T. O. Krause ◽  
B. Mulligan
2011 ◽  
Vol 84 (11) ◽  
Author(s):  
Shigeru Tsukamoto ◽  
Yoshiyuki Egami ◽  
Kikuji Hirose ◽  
Stefan Blügel

1976 ◽  
Vol 54 (22) ◽  
pp. 2225-2239 ◽  
Author(s):  
R. J. W. Hodgson ◽  
J. Tan

The fully off-shell T matrix is generated from a real symmetric function σ(k,k′) which in turn can be obtained from a knowledge of the two-body wave function in the interaction interior. The resulting T matrices are employed to compute the binding energies of 16O, 40Ca, and nuclear matter. Limiting the two-body wave function to physically acceptable forms limits the allowed σ functions. A 'difference integral' is defined in terms of the two-body scattering wave function, which seems to be strongly correlated with the binding energies.


1981 ◽  
Vol 23 (2) ◽  
pp. 926-927 ◽  
Author(s):  
M. S. Hussein ◽  
M. P. Pato ◽  
L. F. Canto ◽  
R. Donangelo
Keyword(s):  

1976 ◽  
Vol 54 (11) ◽  
pp. 1129-1133 ◽  
Author(s):  
B. Linet ◽  
P. Tourrenc

We calculate the phase shift of a quantum mechanics wave function and of an electromagnetic wave produced by any gravitational disturbance using the eikonal approximation. We examine the best conditions for detection of gravitational waves. In particular, we establish that any resonant effect has a linear time dependance.


2004 ◽  
Vol 19 (09) ◽  
pp. 693-702 ◽  
Author(s):  
MICHAEL CHESTERMAN ◽  
MARCELO B. SILKA

We reformulate the conditions of Liouville integrability in the language of Gozzi et al.'s quantum BRST–anti-BRST description of classical mechanics. The Das–Okubo geometrical Lax equation is particularly suited for this approach. We find that the Lax pair and inverse scattering wave function appear naturally in certain sectors of the quantum theory.


1996 ◽  
Vol 74 (7-8) ◽  
pp. 501-504 ◽  
Author(s):  
E. A. G. Armour ◽  
J. M. Carr

The Kohn variational method has recently been applied to the calculation of the addition to the Coulomb phase shift, in positron scattering, by the hydrogen molecular ion below the positronium-formation threshold at 9.45 eV. In this paper the wave function obtained for the lowest spheroidal partial wave of [Formula: see text] symmetry is used to calculate the contribution to Zeff from this symmetry. The results are significantly larger than those obtained using the Coulomb–Born approximation.


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