scholarly journals Sum rules for total cross sections of hadron photoproduction on pseudoscalar mesons

2006 ◽  
Vol 74 (3) ◽  
Author(s):  
S. Dubnička ◽  
A. Z. Dubničková ◽  
E. A. Kuraev
1968 ◽  
Vol 57 (2) ◽  
pp. 442-445 ◽  
Author(s):  
C. Ferro Fontán ◽  
M. Lusignoli ◽  
R. Odorico ◽  
M. Restignoli ◽  
G. Violini

1971 ◽  
Vol 4 (7) ◽  
pp. 2017-2020 ◽  
Author(s):  
P. B. James ◽  
John M. Rawls

1976 ◽  
Vol 55 (5) ◽  
pp. 1504-1513 ◽  
Author(s):  
T. Miyakoshi ◽  
A. Kanazawa ◽  
N. Hashimoto

2021 ◽  
Vol 2021 (7) ◽  
Author(s):  
Artur Amorim ◽  
Miguel S. Costa ◽  
Matti Järvinen

Abstract We initiate the study of Regge theory in a bottom-up holographic model for QCD in the Veneziano limit, where the backreaction of the quarks to the gluon dynamics is included. We determine the parameters of the model by carrying out a precise fit to the meson spectrum in QCD. The spectrum for spin-one and pseudoscalar mesons is well reproduced. We then generalise the model to incluce higher spin fields in the bulk trajectories dual to the Pomeron and meson Regge trajectories at the boundary. With this setting, we fit the masses of the mesons with spins J = 2, 3, and 4, as well as the experimental data of the total cross-sections σ(γγ → X), σ(γp → X) and σ(pp → X). For the cross sections we obtain a $$ {\chi}_{\mathrm{d}.\mathrm{o}.\mathrm{f}}^2 $$ χ d . o . f 2 of 0.74 for a total of 199 experimental points.


Author(s):  
S. Golladay

The theory of multiple scattering has been worked out by Groves and comparisons have been made between predicted and observed signals for thick specimens observed in a STEM under conditions where phase contrast effects are unimportant. Independent measurements of the collection efficiencies of the two STEM detectors, calculations of the ratio σe/σi = R, where σe, σi are the total cross sections for elastic and inelastic scattering respectively, and a model of the unknown mass distribution are needed for these comparisons. In this paper an extension of this work will be described which allows the determination of the required efficiencies, R, and the unknown mass distribution from the data without additional measurements or models. Essential to the analysis is the fact that in a STEM two or more signal measurements can be made simultaneously at each image point.


Sign in / Sign up

Export Citation Format

Share Document