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The QCD Quark Propagator in Coulomb Gauge and - Institut für Physik

The QCD Quark Propagator in Coulomb Gauge and - Institut für Physik

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Chapter 6. Nucleon Form Factors <strong>in</strong> a Covariant Diquark-<strong>Quark</strong> model 79<br />

1<br />

G E<br />

p<br />

0.8<br />

0.6<br />

0.4<br />

fit F.W.<br />

set A ; χ 1<br />

=1<br />

set A ; χ 1<br />

=0<br />

set A ; χ 1<br />

=2<br />

set B ; χ 1<br />

=1<br />

set B ; χ 1<br />

=0<br />

set B ; χ 1<br />

=2<br />

G M<br />

p<br />

4<br />

3<br />

2<br />

0.2<br />

1<br />

0<br />

0 1 2 3 4 5 6<br />

Q 2 [GeV 2 ]<br />

0<br />

0 1 2 3 4 5 6<br />

Q 2 [GeV 2 ]<br />

0.06<br />

0.0<br />

-0.5<br />

0.04<br />

-1.0<br />

G E<br />

n<br />

G M<br />

n<br />

0.02<br />

-1.5<br />

-2.0<br />

0<br />

0 1 2 3 4 5 6<br />

Q 2 [GeV 2 ]<br />

0 1 2 3 4 5 6<br />

Q 2 [GeV 2 ]<br />

Figure 6.3: Response of nucleon form factors to variations <strong>in</strong> the electric quadrupole moment<br />

of the axial-vector diquark, cf. [AHK + 05]: χ 1 + = 0, 1, 2; with µ 1 + = 2, κ T = 2. <strong>The</strong> other<br />

features are described <strong>in</strong> the caption of figure6.2.

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