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References - Bogoliubov Laboratory of Theoretical Physics - JINR

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cos 0φ<br />

LU,I<br />

A<br />

sin φ<br />

ALU,I<br />

sin 2φ<br />

LU,I<br />

A<br />

Res. frac<br />

0.4<br />

0.2<br />

0<br />

0<br />

−0.2<br />

−0.4<br />

−0.6<br />

0<br />

−0.2<br />

−0.4<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

overall<br />

4<br />

2<br />

0<br />

0<br />

.2<br />

.4<br />

.6<br />

0<br />

.2<br />

.4<br />

4<br />

HERMES PRELIMINARY 3.4 % scale uncertainty<br />

e±<br />

+ p → e±<br />

+ p + γ Accep & smear → sys error<br />

0 0.2 0.4 0.6<br />

4<br />

3<br />

2<br />

.1<br />

0<br />

0 0.2 0.4 0.6<br />

2<br />

−t[GeV ]<br />

2<br />

0<br />

0<br />

.2<br />

.4<br />

.6<br />

0<br />

.2<br />

.4<br />

4<br />

3<br />

2<br />

.1<br />

0<br />

0.1 0.2 0.3<br />

0.1 0.2 0.3<br />

xB<br />

4<br />

2<br />

0<br />

0<br />

.2<br />

.4<br />

.6<br />

0<br />

.2<br />

.4<br />

4<br />

3<br />

2<br />

.1<br />

0<br />

VGG Regge, D<br />

VGG Fact., D<br />

2 4 6 8 10<br />

2 4 6 8 10<br />

2 2<br />

Q [GeV ]<br />

Figure 3: The amplitudes <strong>of</strong> the beam-helicity asymmetry from the interference term on the unpolarized<br />

hydrogen target [4]. The error bars (bands) represent the statistical (systematic) uncertainties. The<br />

curves are predictions <strong>of</strong> a double-distribution GPD model [5, 6].<br />

)<br />

coh.<br />

(-t < -t<br />

φ<br />

cos<br />

C<br />

A<br />

)<br />

incoh.<br />

(-t > -t<br />

φ<br />

cos<br />

C<br />

A<br />

0.1<br />

0<br />

0.1<br />

0<br />

Coherent enriched<br />

(accep. & smearing → sys. error,<br />

coherent fraction ~ 65%)<br />

2<br />

2<br />

2<br />

〈 -t〉<br />

= 0.018 GeV , 〈 x 〉 = 0.065, 〈 Q 〉 = 1.70 GeV<br />

B<br />

HERMES PRELIMINARY<br />

0 20 40 60 80 100 120 140<br />

Incoherent enriched<br />

(accep. & smearing → sys. error,<br />

A<br />

elastic incoherent fraction ~ 60%)<br />

2<br />

2<br />

2<br />

〈 -t〉<br />

= 0.20 GeV , 〈 x 〉 = 0.11, 〈 Q 〉 = 2.85 GeV<br />

B<br />

0 20 40 60 80 100 120 140<br />

A<br />

)<br />

coh.<br />

(-t-t<br />

(I),sinφ<br />

LU<br />

A<br />

0<br />

-0.5<br />

0<br />

-0.5<br />

Coherent enriched<br />

(accep. & smearing → sys. error,<br />

coherent fraction ~ 65%,<br />

4<br />

except He~ 30% )<br />

2<br />

2<br />

2<br />

〈 -t〉<br />

= 0.018 GeV , 〈 x 〉 = 0.065, 〈 Q 〉 = 1.70 GeV<br />

B<br />

1 Incoherent enriched 10<br />

(accep. & smearing → sys. error,<br />

elastic incoherent fraction ~ 60%)<br />

2<br />

2<br />

2<br />

〈 -t〉<br />

= 0.20 GeV , 〈 x 〉 = 0.11, 〈 Q 〉 = 2.85 GeV<br />

B<br />

1 10<br />

(a) (b)<br />

HERMES PRELIMINARY<br />

Figure 4: Nuclear-mass dependence <strong>of</strong> the cos φ amplitude <strong>of</strong> the beam-charge asymmetry (a) and <strong>of</strong><br />

the sin φ amplitude <strong>of</strong> the beam-helicity asymmetry (b) for the coherent-enriched (upper panels) and<br />

incoherent-enriched (lower panels) data samples. The inner (full) errors bar represent the statistical<br />

(total) uncertainties.<br />

183<br />

2<br />

10<br />

A<br />

2<br />

10<br />

A

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