Confinement, form factors, and deep-inelastic scattering in two-dimensional quantum chromodynamics

1976 ◽  
Vol 14 (12) ◽  
pp. 3451-3471 ◽  
Author(s):  
Martin B. Einhorn
Keyword(s):  
Inelastic Scattering ◽  
Quantum Chromodynamics ◽  
Deep Inelastic Scattering ◽  
Form Factors ◽  
Two Dimensional

Non-leading mass effects in the effective weak Hamiltonian for Δc = 1 decays

1982 ◽  
Vol 60 (8) ◽  
pp. 1163-1167
Author(s):  
Gerry McKeon
Keyword(s):  
Inelastic Scattering ◽  
Quantum Chromodynamics ◽  
Deep Inelastic Scattering ◽  
Heavy Quarks ◽  
Second Order ◽  
Leading Order ◽  
Mass Effects ◽  
Quark Masses ◽  
B Quarks

Recently Altarelli, Curci, Martinelli, and Petrarca have calculated the second order corrections induced by quantum chromodynamics to the effective weak Hamiltonian in Δc = 1 processes. We extend their analysis by including the effects of the heavy t and b quarks. The technique used is that first introduced by Witten to study the effects of heavy quarks in deep inelastic scattering and used by Gilman and Wise and Guberina and Peccei to discuss how quark masses alter the effective weak Hamiltonian to leading order in [Formula: see text] processes.

QCD TEST OF THE TRIPLE VERTEX IN DEEP INELASTIC SCATTERING FOR DIFFERENT R=τL/σT PARAMETRIZATIONS

1989 ◽  
Vol 04 (21) ◽  
pp. 2017-2029
Author(s):  
A.V. KOTIKOV
Keyword(s):  
Inelastic Scattering ◽  
Quantum Chromodynamics ◽  
Deep Inelastic Scattering ◽  
Cross Sections ◽  
Gluon Distribution ◽  
Transverse Photon ◽  
Made In

Fit of gluon self-coupling suggested by E. Reya1 is made in Quantum Chromodynamics for three (n=3, 4, 5) moments of the gluon distribution in the region of Q2~ 50–1000 GeV 2. The result depends strongly on the parametrization of the ratio R(x, Q2) =σL/σT, where σL and σT are cross sections of the longitudinal and transverse photon on a nucleon. We show the necessity of the logarithmic rather than power violation of the Callan-Gross correlation.2

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