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