The constraint on the spin dependent structure function g1 at low Q2 through the sum rule corresponding to the moment at n = 0

2007 ◽  
Author(s):  
Susumu Koretune
1998 ◽  
Vol 210 (1) ◽  
pp. 199-228 ◽  
Author(s):  
M. Potthoff ◽  
T. Herrmann ◽  
T. Wegner ◽  
W. Nolting
Keyword(s):  
Sum Rule ◽  

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

1988 ◽  
Vol 212 (4) ◽  
pp. 511-514 ◽  
Author(s):  
V.W. Hughes ◽  
V. Papavassiliou ◽  
R. Piegaia ◽  
K.P. Schüler ◽  
G. Baum
Keyword(s):  

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

2002 ◽  
Vol 05 (04) ◽  
pp. 409-431 ◽  
Author(s):  
YANEER BAR-YAM

We derive a sum rule that constrains the scale based decomposition of the trajectories of finite systems of particles. The sum rule reflects a tradeoff between the finer and larger scale collective degrees of freedom. For short duration trajectories, where acceleration is irrelevant, the sum rule can be related to the moment of inertia and the kinetic energy (times a characteristic time squared). Thus, two nonequilibrium systems that have the same kinetic energy and moment of inertia can, when compared to each other, have different scales of behavior, but if one of them has larger scales of behavior than the other, it must compensate by also having smaller scales of behavior. In the context of coherence or correlation, the larger scale of behavior corresponds to the collective motion, while the smaller scales of behavior correspond to the relative motion of correlated particles. For longer duration trajectories, the sum rule includes the full effective moment of inertia of the system in space-time with respect to an external frame of reference, providing the possibility of relating the class of systems that can exist in the same space-time domain.


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.


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