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Electric form factor of the neutron from theH2(e→,e’n→)1H reaction atQ2=0.255 (GeV/c)2

Authors :
K. Beard
W. ‐D. Jiang
P. E. Ulmer
R. W. Lourie
T. Payerle
B. S. Flanders
M. Farkhondeh
Larry Weinstein
D. Barkhuff
William Bertozzi
S. Kowalski
Pete Markowitz
T. Eden
C. E. Hyde-Wright
James J. Kelly
P. M. Rutt
R. R. Whitney
B. D. Anderson
J.M. Cameron
C. C. Chang
D. R. Tieger
Hartmuth Arenhövel
D. M. Manley
M. Spraker
B. Ni
T. Reichelt
G. W. Dodson
W. M. Zhang
John M. Finn
K. A. Dow
W. Turchinetz
P.J. Pella
Van Verst S
Richard Madey
J. Y. Mougey
Wolfgang Korsch
J. W. Watson
A. R. Baldwin
D. Keane
Source :
Physical Review C. 50:R1749-R1753
Publication Year :
1994
Publisher :
American Physical Society (APS), 1994.

Abstract

We determined the electric form factor [ital G][sup [ital n]][sub [ital E]] of the neutron from the quasielastic [sup 2]H([ital [rvec e]],[ital e][sup [prime]][ital [rvec n]])[sup 1]H reaction at a central squared four-momentum transfer [ital Q][sup 2]=0.255 (GeV/[ital c])[sup 2] with a longitudinally polarized electron beam of 868 MeV and a low ([similar to]0.8%) duty factor. A neutron polarimeter designed and constructed specifically for this experiment was used to measure the sideways polarization of the recoil neutron, which was detected in coincidence with the scattered electron. Theoretical calculations have established that this polarization-transfer technique for quasielastic scattering produces a value of [ital G][sup [ital n]][sub [ital E]] that shows little sensitivity to the influence of final-state interactions, meson-exchange currents, isobar configurations, and deuteron structure. The value for [ital G][sup [ital n]][sub [ital E]] from this measurement is 0.066[plus minus]0.036[plus minus]0.009.

Details

ISSN :
1089490X and 05562813
Volume :
50
Database :
OpenAIRE
Journal :
Physical Review C
Accession number :
edsair.doi...........9fe8b561e598697bd7302be620e9498a