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Longitudinal Structure Function at Intermediate x and the Gluon Density
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CERN-TH 6785/93
ANL-HEP-PR-93-7
January, 1993
Longitudinal Structure Function
at Intermediate x and the Gluon Density
Edmond L. Berger1,2 and Ruibin Meng2
1CERN-Geneva
2High Energy Physics Division?
Argonne National Laboratory
Argonne, IL 60439
Abstract
Calculations are presented of the longitudinal structure function FL(x,Q
2). We use
next-to-leading order expressions in QCD (O(α2s)) plus parton densities determined
previously from global fits to data on deep inelastic lepton scattering, prompt photon
production, and bottom quark production. Anticipated data from the DESY ep collider
HERA should provide discriminating information on the gluon density, particularly for
values of x 0.05.
?Work supported by the U.S. Department of Energy, Division of High Energy Physics, Contract
W-31-109-ENG-38.
In perturbative quantum chromodynamics(QCD), the longitudinal structure function
FL(x,Q
2), measured in deep inelastic lepton scattering, may be expressed to leading order
as a sum of integrals over the gluon and quark densities of the nucleon[1]. As usual Q2 is
the square of the four-vector momentum exchange, and x is the Bjorken scaling variable. At
small values of x, the gluon contribution dominates, and, to fair approximation,
FL(x,Q
2) ~= 2αs(Q
2)
3π
1
1.77
x
a
G(
x
a
,Q2). (1)
Here G(x,Q2) is the gluon density, αs(Q
2) is the QCD coupling strength, and a is a parameter
whose value is about 0.4 for FL[2]. Correspondingly, measurement of FL has long been
advocated as perhaps the most direct probe of the gluon density at small x. Studies indicate
that precise measurements of FL should be feasible at the HERA ep collider at DESY for
values of x of order 10?2, or less, and values of Q2 in the range 10 to 100 GeV2[3].
Recently a full next-to-leading order calculation (O(α2s)) in QCD has been published
for the deep inelastic structure functions F2 and FL[4]. These analytic expressions allow us
to extend the exp
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