High-Energy Quasielastic Proton-Proton Scattering and Final-State Interaction

1963 ◽  
Vol 131 (5) ◽  
pp. 2292-2304 ◽  
Author(s):  
M. M. Islam
1969 ◽  
Vol 136 (2) ◽  
pp. 337-352 ◽  
Author(s):  
C.C. Chang ◽  
E. Bar-Avraham ◽  
H.H. Forster ◽  
C.C. Kim ◽  
P. TomaŠ ◽  
...  

1977 ◽  
Vol 3 (1) ◽  
pp. 7-20 ◽  
Author(s):  
B S Aladashvili ◽  
J -F Germond ◽  
V V Glagolev ◽  
M S Nioradze ◽  
T Siemiarczuk ◽  
...  

1994 ◽  
Vol 579 (1-2) ◽  
pp. 13-44 ◽  
Author(s):  
L.J. de Bever ◽  
H.P. Blok ◽  
J. Blouw ◽  
M. Fujiwara ◽  
K. Hosono ◽  
...  

Universe ◽  
2019 ◽  
Vol 5 (6) ◽  
pp. 133 ◽  
Author(s):  
Máté Csanád ◽  
Sándor Lökös ◽  
Márton Nagy

Investigation of momentum space correlations of particles produced in high energy reactions requires taking final state interactions into account, a crucial point of any such analysis. Coulomb interaction between charged particles is the most important such effect. In small systems like those created in e + e - - or p + p collisions, the so-called Gamow factor (valid for a point-like particle source) gives an acceptable description of the Coulomb interaction. However, in larger systems such as central or mid-central heavy ion collisions, more involved approaches are needed. In this paper we investigate the Coulomb final state interaction for Lévy-type source functions that were recently shown to be of much interest for a refined description of the space-time picture of particle production in heavy-ion collisions.


1973 ◽  
Vol 8 (3) ◽  
pp. 863-869 ◽  
Author(s):  
J. C. Davis ◽  
J. D. Anderson ◽  
S. M. Grimes ◽  
C. Wong

1970 ◽  
Vol 156 (3) ◽  
pp. 616-628 ◽  
Author(s):  
M. Ivanovich ◽  
W. Von Witsch ◽  
E.V. Hungerford ◽  
Phillips G.C.

1968 ◽  
Vol 28 (3) ◽  
pp. 175-177 ◽  
Author(s):  
C.C. Chang ◽  
E. Bar-Avraham ◽  
H.H. Forster ◽  
C.C. Kim ◽  
J.R. Richardson ◽  
...  

1969 ◽  
Vol 30 (7) ◽  
pp. 460-462 ◽  
Author(s):  
H. Brückmann ◽  
W. Kluge ◽  
H. Matthäy ◽  
L. Schänzler ◽  
K. Wick

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