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

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78 6.5. Nucleon electromagnetic form factors: results<br />

1<br />

G E<br />

p<br />

0.8<br />

0.6<br />

0.4<br />

fit F.W.<br />

set A ; µ 1<br />

=2<br />

set A ; µ 1<br />

=1<br />

set A ; µ 1<br />

=3<br />

set B ; µ 1<br />

=2<br />

set B ; µ 1<br />

=1<br />

set B ; µ 1<br />

=3<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 6.2: Response of nucleon form factors to variations <strong>in</strong> the magnetic moment of the<br />

axial-vector diquark, cf. [AHK + 05]: µ 1 + = 1, 2, 3; with χ 1 + = 1, κ T = 2. <strong>The</strong> legend <strong>in</strong><br />

the top-left panel applies to all; the dashed-l<strong>in</strong>e marked by “∗” is a fit to experimental data<br />

[FW03] <strong>and</strong> the dashed-l<strong>in</strong>e marked by “+” <strong>in</strong> the lower-left panel is the fit to G n E (Q2 ) of<br />

reference[G + 71]; <strong>and</strong> the horizontal l<strong>in</strong>es <strong>in</strong> the right panels mark the experimental value of<br />

the nucleon’s magnetic moment.

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