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References - Bogoliubov Laboratory of Theoretical Physics - JINR

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kinematic range to low values <strong>of</strong> Bjorken x, alow0.1 GeV 2 threshold is used for Q 2 .The<br />

structure function F2(x, Q 2 ) <strong>of</strong> the proton is presented in Fig. 1. The overall normalization<br />

uncertainty, which is mainly due to the luminosity normalization, is estimated to be 6.4%.<br />

Results <strong>of</strong> other experiments performed at DESY, CERN, and SLAC are presented as well<br />

for comparison. A previously unexplored region in the plane x-Q 2 is covered by this new<br />

measurement. At the same time there is a good agreement with world data in the overlap<br />

region. The structure function F2(x) <strong>of</strong> the deuteron is measured as well but not shown.<br />

p F2 ⋅ c<br />

10 7<br />

10 6<br />

10 5<br />

10 4<br />

10 3<br />

10 2<br />

SLAC<br />

JLAB<br />

HERMES<br />

PRELIMINARY<br />

GD07 fit<br />

SMC fit<br />

BCDMS<br />

NMC<br />

E665<br />

H1<br />

ZEUS<br />

1 10<br />

〈x〉 c<br />

0.008 1.6 36<br />

0.011 1.6 35<br />

0.015 1.6 34<br />

0.019 1.6 33<br />

0.025 1.6 32<br />

0.134 1.6 24<br />

0.108 1.6 25<br />

0.089 1.6 26<br />

0.073 1.6 27<br />

0.060 1.6 28<br />

0.049 1.6 29<br />

0.040 1.6 30<br />

0.033 1.6 31<br />

0.166 1.6 23<br />

0.211 1.6 22<br />

0.273 1.6 21<br />

0.366 1.6 20<br />

0.509 1.6 19<br />

0.679 1.6 18<br />

Q 2 [GeV 2 ]<br />

Figure 1: Structure function F2(x, Q 2 ) <strong>of</strong> the proton as a function <strong>of</strong> Q 2 , for different bins in x. Inner<br />

error bars are total minus the normalization uncertainty, shown as an outer error bar. The HERMES data<br />

are compared to measurements from NMC, BCDMS, JLab, HERA and SLAC. The phenomenological parameterizations<br />

<strong>of</strong> world data by the SMC [4] and GD07 [5] are shown by curves. Both parameterizations<br />

do not include the HERMES data points.<br />

Structure function g2(x). The spin-dependent nucleon structure function g2(x) has<br />

no probabilistic interpretation in simple quark parton model. It has contributions from<br />

quark-gluon correlations and can be written as a sum <strong>of</strong> two terms, g2(x, Q2 )=gWW 2 (x, Q2 )<br />

+¯g2(x, Q2 ), where gWW 2 (x, Q2 )=−g1(x, Q2 )+ � 1<br />

x g1(y, Q2 )dy/y is the twist-2 Wandzura-<br />

Wilczek part, while ¯g2(x, Q2 ) is the unknown twist-3 part. A measurement <strong>of</strong> the structure<br />

function g2(x) requires a longitudinally polarized beam and a transversely polarized<br />

target. The polarization-dependent part <strong>of</strong> the cross-section is given by:<br />

222

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