scholarly journals The integral of the spin-dependent structure function g1p and the Ellis-Jaffe sum rule

1988 ◽  
Vol 212 (4) ◽  
pp. 511-514 ◽  
Author(s):  
V.W. Hughes ◽  
V. Papavassiliou ◽  
R. Piegaia ◽  
K.P. Schüler ◽  
G. Baum
Keyword(s):  
1996 ◽  
Vol 05 (01) ◽  
pp. 121-129
Author(s):  
YOSHINORI NISHINO

We calculate the second moment [Formula: see text] of the flavor-singlet structure function [Formula: see text] for the pion and the kaon in the framework of the QCD sum rule, and investigate how the results depend on their flavor structure (quark contents). Our calculations give similar values of [Formula: see text] for these two mesons as a result of the cancellation among several non-small factors.


2002 ◽  
Vol 549 (1-2) ◽  
pp. 109-114 ◽  
Author(s):  
Anke Knauf ◽  
Michael Meyer-Hermann ◽  
Gerhard Soff

1993 ◽  
Vol 391 (1-2) ◽  
pp. 69-99 ◽  
Author(s):  
S. Narison ◽  
G.M. Shore ◽  
G. Veneziano

2013 ◽  
Vol 28 (19) ◽  
pp. 1350086 ◽  
Author(s):  
AKBARI JAHAN ◽  
D. K. CHOUDHURY

Momentum sum rule can be used as an inequality to estimate the lower and upper bounds of the momentum fractions of quarks and gluons in a model of proton valid in a limited x range. We compute such bounds in a self-similarity based model of proton structure function valid in the range 6.2 × 10-7 ≤ x ≤ 10-2. The results conform to the asymptotic QCD expectations.


1997 ◽  
Vol 12 (05) ◽  
pp. 321-328
Author(s):  
Franco Buccella ◽  
Ofelia Pisanti ◽  
Pietro Santorelli

The combination [Formula: see text] is derived from SLAC data on polarized proton and deuteron targets, evaluated at Q2=10  GeV 2, and compared with the results of SMC experiment. The agreement is satisfactory except for the points at the three lowest x, which have an important role in the SMC evaluation on the L.H.S. of the Bjorken sum rule.


1997 ◽  
Vol 50 (1) ◽  
pp. 53
Author(s):  
Hiko Morita ◽  
Toru Suzuki

The structure function of 4He is calculated based on a realistic spectral function which is consistent with the momentum sum rule. The calculation reproduces the empirical suppression of the EMC ratio R(x) = F2(4He)/F2(D) at x < 1. At x~ 1 the quasielastic contribution produces a sizable effect in the ratio, but it becomes negligible around Q2 ~ 20 (GeV/c)2.


Sign in / Sign up

Export Citation Format

Share Document