On the origin of the leading-particle effect in high-energy hadronic processes

1981 ◽  
Vol 62 (3) ◽  
pp. 238-252 ◽  
Author(s):  
M. Giffon ◽  
E. Predazzi
1976 ◽  
Vol 103 (1) ◽  
pp. 123-144 ◽  
Author(s):  
X. Artru ◽  
Siv-Britt Ljung

1998 ◽  
Vol 2 (4) ◽  
pp. 733-740 ◽  
Author(s):  
Tsutomu Tashiro ◽  
Hujio Noda ◽  
Shin-ichi Nakariki ◽  
Kazuo Ishii ◽  
Kisei Kinoshita

2002 ◽  
Vol 89 (12) ◽  
Author(s):  
Eric Braaten ◽  
Yu Jia ◽  
Thomas Mehen

2007 ◽  
Vol 16 (07n08) ◽  
pp. 2344-2349
Author(s):  
TSUTOMU TASHIRO ◽  
HUJIO NODA ◽  
SHIN-ICHI NAKARIKI ◽  
KAZUMI FUKUMA

We relate the hyperon polarizations in proton-proton and proton-nucleus collisions to the leading particle effect and use the constituent quark-diquark cascade model with SU(6) wave function. We assume that the quantization axis is characterized by the production normal of the leading baryon of the most massive cascade chain and the incident valence diquark tends to pick up a spin down sea quark or conversely a sea diquark preferentially combines with the spin up incident valence quark to form a leading baryon as compared with the spin down valence quark.


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