Impact-parameter-selected two-proton intensity interferometry forAr36+45Sc atE/A=80 MeV

1993 ◽  
Vol 70 (24) ◽  
pp. 3709-3712 ◽  
Author(s):  
M. A. Lisa ◽  
C. K. Gelbke ◽  
W. Bauer ◽  
P. Decowski ◽  
W. G. Gong ◽  
...  
1991 ◽  
Vol 43 (4) ◽  
pp. 1804-1820 ◽  
Author(s):  
W. G. Gong ◽  
C. K. Gelbke ◽  
W. Bauer ◽  
N. Carlin ◽  
R. T. de Souza ◽  
...  

2019 ◽  
Vol 34 (32) ◽  
pp. 1950259 ◽  
Author(s):  
S. M. Troshin ◽  
N. E. Tyurin

We comment briefly on relations between the elastic and inelastic cross-sections valid for the shadow and reflective modes of the elastic scattering. Those are based on the unitarity arguments. It is shown that the redistribution of the probabilities of the elastic and inelastic interactions (the form of the inelastic overlap function becomes peripheral) under the reflective scattering mode can lead to increasing ratio of [Formula: see text] at the LHC energies. In the shadow scattering mode, the mechanism of this increase is a different one, since the impact parameter dependence of the inelastic interactions probability is central in this mode. A short notice is also given on the slope parameter and the leading contributions to its energy dependence in both modes.


1999 ◽  
Vol 59 (4) ◽  
pp. R1844-R1845 ◽  
Author(s):  
M. Bleicher ◽  
M. Reiter ◽  
A. Dumitru ◽  
J. Brachmann ◽  
C. Spieles ◽  
...  

2021 ◽  
Vol 103 (9) ◽  
Author(s):  
Neelkamal Mallick ◽  
Sushanta Tripathy ◽  
Aditya Nath Mishra ◽  
Suman Deb ◽  
Raghunath Sahoo

2021 ◽  
Vol 424 ◽  
pp. 168346
Author(s):  
Jordan Cotler ◽  
Frank Wilczek ◽  
Victoria Borish

1982 ◽  
Vol 304 (2) ◽  
pp. 177-183 ◽  
Author(s):  
H. Schmidt-B�cking ◽  
H. Baumann ◽  
K. Bethge ◽  
A. Gruppe ◽  
W. Schadt ◽  
...  

2011 ◽  
Vol 20 (08) ◽  
pp. 1735-1754 ◽  
Author(s):  
M. MOHERY ◽  
M. ARAFA

The present paper deals with the interactions of 22 Ne and 28 Si nuclei at (4.1–4.5)A GeV /c with emulsion. Some characteristics of the compound multiplicity nc given by the sum of the number of shower particles ns and grey particles ng have been investigated. The present experimental data are compared with the corresponding ones calculated according to modified cascade evaporation model (MCEM). The results reveal that the compound multiplicity distributions for these two reactions are consistent with the corresponding ones of MCEM data. It can also be seen that the peak of these distributions shifts towards a higher value of nc with increasing projectile mass. It may further be seen that the compound multiplicity distributions becomes broader with increasing target size and its width increases with the size of the projectile nucleus. In addition, it has been found that the MCEM can describe the compound multiplicity characteristics of the different projectile, target and the correlation between different emitted particles. The values of average compound multiplicity increase with increasing mass of the projectile. Furthermore, it is observed that while the value of 〈nc〉 depends on the mass number of the projectile Ap and the target mass number At, the value of the ratio 〈nc〉/D(nc) seems to be independent of Ap and At. The impact parameter is found to affect the shape of the compound multiplicity distribution. Finally, the dependence of the average compound multiplicity on the numbers of grey and black particles, and the sum of them, is obvious. The values of the slope have been found to be independent of the projectile nucleus.


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