Determination of the Charged Pion Form Factor at Q2=1.60 and 2.45 (GeV/c)2
| dc.creator | Fpi2 collaboration | |
| dc.creator | Horn, T. | |
| dc.creator | Aniol, K. | |
| dc.creator | Arrington, J. | |
| dc.creator | Barrett, B. | |
| dc.creator | Beise, E. J. | |
| dc.creator | Blok, H. P. | |
| dc.creator | Boeglin, W. | |
| dc.creator | Brash, E. J. | |
| dc.creator | Breuer, H. | |
| dc.creator | Chang, C. C. | |
| dc.creator | Christy, M. E. | |
| dc.creator | Ent, R. | |
| dc.creator | Gaskell, D. | |
| dc.creator | Gibson, E. | |
| dc.creator | Holt, R. J. | |
| dc.creator | Huber, G. M. | |
| dc.creator | Jin, S. | |
| dc.creator | Jones, M. K. | |
| dc.creator | Keppel, C. E. | |
| dc.creator | Kim, W. | |
| dc.creator | King, P. M. | |
| dc.creator | Kovaltchouk, V. | |
| dc.creator | Liu, J. | |
| dc.creator | Lolos, G. J. | |
| dc.creator | Mack, D. J. | |
| dc.creator | Margaziotis, D. J. | |
| dc.creator | Markowitz, P. | |
| dc.creator | Matsumura, A. | |
| dc.creator | Meekins, D. | |
| dc.creator | Miyoshi, T. | |
| dc.creator | Mkrtchyan, H. | |
| dc.creator | Niculescu, I. | |
| dc.creator | Okayasu, Y. | |
| dc.creator | Pentchev, L. | |
| dc.creator | Perdrisat, C. | |
| dc.creator | Potterveld, D. | |
| dc.creator | Punjabi, V. | |
| dc.creator | Reimer, P. | |
| dc.creator | Reinhold, J. | |
| dc.creator | Roche, J. | |
| dc.creator | Roos, P. G. | |
| dc.creator | Sarty, A. | |
| dc.creator | Smith, G. R. | |
| dc.creator | Tadevosyan, V. | |
| dc.creator | Tang, L. G. | |
| dc.creator | Tvaskis, V. | |
| dc.creator | Vidakovic, S. | |
| dc.creator | Volmer, J. | |
| dc.creator | Vulcan, W. | |
| dc.creator | Warren, G. | |
| dc.creator | Wood, S. A. | |
| dc.creator | Xu, C. | |
| dc.creator | Zheng, X. | |
| dc.date | 2006-07-07 | |
| dc.date.accessioned | 2026-07-07T11:59:58Z | |
| dc.date.available | 2026-07-07T11:59:58Z | |
| dc.description | The H(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 Chromo-Dynamics prediction. | |
| dc.description | 4 pages, 3 figures, submitted to Physical Review Letters | |
| dc.identifier | https://arxiv.org/abs/nucl-ex/0607005 | |
| dc.identifier | http://arxiv.org/abs/nucl-ex/0607005 | |
| dc.identifier | Phys.Rev.Lett.97:192001,2006 | |
| dc.identifier | doi:10.1103/PhysRevLett.97.192001 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/206753 | |
| dc.subject | Nuclear Experiment | |
| dc.title | Determination of the Charged Pion Form Factor at Q2=1.60 and 2.45 (GeV/c)2 | |
| dc.type | text |