Single-step and coupled-channels calculations of pion inelastic scattering

1992 ◽  
Vol 45 (3) ◽  
pp. 1351-1355 ◽  
Author(s):  
M. A. Kagarlis ◽  
H. T. Fortune
1989 ◽  
Vol 39 (5) ◽  
pp. 1935-1943 ◽  
Author(s):  
C. S. Whisnant ◽  
G. S. Adams ◽  
J. A. Escalante ◽  
C. S. Mishra ◽  
M. Al-Solami ◽  
...  

1980 ◽  
Vol 97 (1) ◽  
pp. 37-40 ◽  
Author(s):  
C.-A. Wiedner ◽  
K.R. Cordell ◽  
W. Saathoff ◽  
S.T. Thornton ◽  
J. Bolger ◽  
...  

1982 ◽  
Vol 116 (4) ◽  
pp. 215-218 ◽  
Author(s):  
C. Glashausser ◽  
R. de Swiniarski ◽  
K. Jones ◽  
S. Nanda ◽  
F.T. Baker ◽  
...  

1975 ◽  
Vol 253 (2) ◽  
pp. 461-468 ◽  
Author(s):  
F.Todd Bake ◽  
C. Glashausser ◽  
A.B. Robbins ◽  
E. Ventura

1973 ◽  
Vol 51 (12) ◽  
pp. 1293-1299 ◽  
Author(s):  
R. de Swiniarski ◽  
H. E. Conzett ◽  
C. R. Lamontagne ◽  
B. Frois ◽  
R. J. Slobodrian

Angular distributions of the analyzing power and cross sections have been measured for the elastic and inelastic scattering of 25.25 MeV protons exciting the K = 0+ ground-state band in 28Si. Good agreement with experiment is obtained in the coupled-channels formalism on the basis of the rotational model with a quadrupole deformation β2 = −0.40 (oblate) and a hexadecapole deformation β4 = +0.15. The calculations show the great sensitivity of the experimental results to both the magnitude and sign of the quadrupole and hexadecapole deformations. Equivalent fits of the data were obtained either by keeping the deformation length of the various deformed terms of the optical potential constant (δ0 = β0R0 = βIRI = βLSRLS) or by increasing the deformation of the spin–orbit optical potential relative to the central potential by a factor of 1.5 (βLS = 1.5βcent).


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