pomeron coupling
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2011 ◽  
Vol 695 (1-4) ◽  
pp. 162-164 ◽  
Author(s):  
E.G. de Oliveira ◽  
A.D. Martin ◽  
M.G. Ryskin


2010 ◽  
Vol 69 (1-2) ◽  
pp. 95-101 ◽  
Author(s):  
E. G. S. Luna ◽  
V. A. Khoze ◽  
A. D. Martin ◽  
M. G. Ryskin
Keyword(s):  




1998 ◽  
Vol 57 (11) ◽  
pp. R6585-R6589 ◽  
Author(s):  
A. Bialas ◽  
H. Navelet ◽  
R. Peschanski


1997 ◽  
Vol 12 (03) ◽  
pp. 173-181 ◽  
Author(s):  
S. V. Goloskokov

We analyze the diffractive [Formula: see text] production and final jet kinematics in polarized deep-inelastic lp scattering at [Formula: see text] GeV. We show that this reaction can be used in the new spectrometer of the COMPASS collaboration at CERN to study the quark–pomeron coupling structure.



1995 ◽  
Vol 65 (4) ◽  
pp. 657-666 ◽  
Author(s):  
B. A. Kniehl ◽  
H. -G. Kohrs ◽  
G. Kramer
Keyword(s):  


1995 ◽  
Vol 352 (2) ◽  
pp. 203-210 ◽  
Author(s):  
J. Klenner ◽  
A. Sch�fer ◽  
W. Greiner


1980 ◽  
Vol 58 (4) ◽  
pp. 455-462
Author(s):  
R. Migneron ◽  
J. L. Robinson

A characteristic rise in the cross section near x = 1 has been reported for the single particle inclusive reaction π−p → π−X at Fermilab energies. Factorizable Regge amplitudes are used with a well-established analysis of the pp → pX peak to construct a parametrization of the triple-Regge couplings with αP(0) > 1 and to give a triple-Regge description of the meson + proton → meson + X cross section. Good agreement with the π−p → π−X data at 147 GeV/c is obtained and the peak is dominated by the triple-Pomeron component. This approach provides a reliable method for obtaining an estimate of the non-diffractive component. The inelastic diffractive cross section rises with energy and is found to account for most of the observed rise in σtot(π±p). The procedure is extended to K±p → K±X.



1980 ◽  
Vol 21 (7) ◽  
pp. 2021-2026
Author(s):  
Ricardo E. Gomboa Saraví
Keyword(s):  


1979 ◽  
Vol 62 (6) ◽  
pp. 1783-1785
Author(s):  
J. Koike
Keyword(s):  


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