E99-107 CLAS experiment for generalized form factor near threshold
- Spokespersons
- V. D. Burkert, R. Minehart
- Year
- 2005
- Abstract
- We report the first extraction of the pion-nucleon multipoles near the production threshold for the $n\pi^+$ channel at relatively high momentum transfer ($Q^2$ up to 4.2 $\rm{GeV^2}$). The dominance of the $s$-wave transverse multipole ($E_{0+}$), expected in this region, allowed us to access the generalized form factor $G_1$ within the light-cone sum rule (LCSR) framework as well as the axial form factor $G_A$. The data analyzed in this work were collected by the nearly $4\pi$ CEBAF Large Acceptance Spectrometer (CLAS) using a 5.754 $\rm{GeV}$ electron beam on a proton target. The differential cross section and the $\pi-N$-multipole $E_{0+}/G_D$ were measured using two different methods, the LCSR and a direct multipole fit. The results from the two methods are found to be consistent and almost $Q^2$ independent.
- Publication
-
- K.Park, R.W.Gothe, and CLAS Collaboration Measurement of the generalized form factors near threshold via γ* p -> nπ+ at high Q2 // Phys. Rev. C 85, 035208 (2012); arXiv:1201.0903v1
- Quantities
- dσ/dΩ
Measurements
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ID | Quantity | Beam | Target | Final state |
Q2min, GeV2 |
Q2max, GeV2 |
Wmin, GeV |
Wmax, GeV |
---|---|---|---|---|---|---|---|---|
E41M1 | dσ/dΩ | e | p | π+n | 2.0 | 2.23 | 1.1 | 1.12 |
E41M2 | dσ/dΩ | e | p | π+n | 2.23 | 2.66 | 1.1 | 1.12 |
E41M3 | dσ/dΩ | e | p | π+n | 2.66 | 3.17 | 1.1 | 1.12 |
E41M4 | dσ/dΩ | e | p | π+n | 3.17 | 3.79 | 1.1 | 1.12 |
E41M5 | dσ/dΩ | e | p | π+n | 3.79 | 4.52 | 1.1 | 1.12 |
E41M6 | dσ/dΩ | e | p | π+n | 2.0 | 2.23 | 1.12 | 1.14 |
E41M7 | dσ/dΩ | e | p | π+n | 2.23 | 2.66 | 1.12 | 1.14 |
E41M8 | dσ/dΩ | e | p | π+n | 2.66 | 3.17 | 1.12 | 1.14 |
E41M9 | dσ/dΩ | e | p | π+n | 3.17 | 3.79 | 1.12 | 1.14 |
E41M10 | dσ/dΩ | e | p | π+n | 3.79 | 4.52 | 1.12 | 1.14 |
E41M11 | dσ/dΩ | e | p | π+n | 2.0 | 2.23 | 1.14 | 1.16 |
E41M12 | dσ/dΩ | e | p | π+n | 2.23 | 2.66 | 1.14 | 1.16 |
E41M13 | dσ/dΩ | e | p | π+n | 2.66 | 3.17 | 1.14 | 1.16 |
E41M14 | dσ/dΩ | e | p | π+n | 3.17 | 3.79 | 1.14 | 1.16 |
E41M15 | dσ/dΩ | e | p | π+n | 3.79 | 4.52 | 1.14 | 1.16 |
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