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Determination of the pion charge form factor at Q2=1.60 and 2.45 (GeV/c)2
Authors:Horn T,Aniol K,Arrington J,Barrett B,Beise E J,Blok H P,Boeglin W,Brash E J,Breuer H,Chang C C,Christy M E,Ent R,Gaskell D,Gibson E,Holt R J,Huber G M,Jin S,Jones M K,Keppel C E,Kim W,King P M,Kovaltchouk V,Liu J,Lolos G J,Mack D J,Margaziotis D J,Markowitz P,Matsumura A,Meekins D,Miyoshi T,Mkrtchyan H,Niculescu I,Okayasu Y,Pentchev L,Perdrisat C,Potterveld D,Punjabi V,Reimer P,Reinhold J,Roche J,Roos P G,Sarty A,Smith G R,Tadevosyan V,Tang L G,Tvaskis V,Vidakovic S,Volmer J,Vulcan W,Warren G,Wood S A,Xu C,Zheng X  Jefferson Lab F Collaboration
Affiliation:Department of Physics, University of Maryland, College Park, MD 20742, USA.
Abstract:The 1H(e,e'pi+)n cross section was measured at four-momentum transfers of Q2=1.60 and 2.45 GeV2 at an invariant mass of the photon nucleon system of W=2.22 GeV. The charged pion form factor (F(pi)) was extracted from the data by comparing the separated longitudinal pion electroproduction cross section to a Regge model prediction in which F(pi) is a free parameter. The results indicate that the pion form factor deviates from the charge-radius constrained monopole form at these values of Q2 by one sigma, but is still far from its perturbative quantum chromodynamics prediction.
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