I. A. Qattan; J. Arrington; R. E. Segel; X. Zheng; K. Aniol; O. K. Baker; R. Beams; E. J. Brash; J. Calarco; A. Camsonne; J.-P. Chen; M. E. Christy; D. Dutta; R. Ent; S. Frullani; D. Gaskell; O. Gayou; R. Gilman; C. Glashausser; K. Hafidi; J.-O. Hansen; D. W. Higinbotham; W. Hinton; R. J. Holt; G. M. Huber; H. Ibrahim; L. Jisonna; M. K. Jones; C. E. Keppel; E. Kinney; G. J. Kumbartzki; A. Lung; D. J. Margaziotis; K. McCormick; D. Meekins; R. Michaels; P. Monaghan; P. Moussiegt; L. Pentchev; C. Perdrisat; V. Punjabi; R. Ransome; J. Reinhold; B. Reitz; A. Saha; A. Sarty; E. C. Schulte; K. Slifer; P. Solvignon; V. Sulkosky; K. Wijesooriya; B. Zeidman
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research ER (United States)2004
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research ER (United States)2004
AbstractAbstract
[en] We report the results of a new Rosenbluth measurement of the proton form factors at Q2 values of 2.64, 3.20 and 4.10 GeV2. Cross sections were determined by detecting the recoiling proton in contrast to previous measurements in which the scattered electron was detected. At each Q2, relative cross sections were determined to better than 1%. The measurement focused on the extraction of GE/GM which was determined to 4-8% and found to approximate form factor scaling, i.e. μpGE ∼ GM. These results are consistent with and much more precise than previous Rosenbluth extractions. However, they are inconsistent with recent polarization transfer measurements of comparable precision, implying a systematic difference between the two techniques
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Source
1 Oct 2004; 187 Kilobytes; DOE/ER--40150-2951; NUCL-EX--0410010; AC--05-84ER40150; Available from PURL: https://www.osti.gov/servlets/purl/834054-Bt1V0z/native/
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Miscellaneous
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K. Garrow; D. McKee; A. Ahmidouch; C. S. Armstrong; J. Arrington; R. Asaturyan; S. Avery; O. K. Baker; D. H. Beck; H. P. Blok; C. W. Bochna; W. Boeglin; P. Bosted; M. Bouwhuis; H. Breuer; D. S. Brown; A. Bruell; R. D. Carlini; N. S. Chant; A. Cochran; L. Cole; S. Danagoulian; D. B. Day; J. Dunne; D. Dutta; R. Ent; H. C. Fenker; B. Fox; L. Gan; D. Gaskell; A. Gasparian; H. Gao; D. F. Geesaman; R. Gilman; P. L. J. Gueye; M. Harvey; R. J. Holt; X. Jiang; C. E. Keppel; E. Kinney; Y. Liang; W. Lorenzon; A. Lung; D. J. Mack; P. Markowitz; J. W. Martin; K. McIlhany; D. Meekins; M. A. Miller; R. G. Milner; J. H. Mitchell; H. Mkrtchyan; B. A. Mueller; A. Nathan; G. Niculescu; I. Niculescu; T. G. O'Neill; V. Papavassiliou; S. Pate; R. B. Piercey; D. Potterveld; R. D. Ransome; J. Reinhold; E. Rollinde; P. Roos; A. J. Sarty; R. Sawafta; E. C. Schulte; E. Segbefia; C. Smith; S. Stepanyan; S. Strauch; V. Tadevosyan; L. Tang; R. Tieulent; A. Uzzle; W. F. Vulcan; S. A. Wood; F. Xiong; L. Yuan; M. Zeier; B. Zihlmann; V. Ziskin
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2002
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2002
AbstractAbstract
[en] The quasielastic (e,e[prime]p) reaction was studied on targets of deuterium, carbon, and iron up to a value of momentum transfer Q2 of 8.1 (GeV/c)2. A nuclear transparency was determined by comparing the data to calculations in the plane-wave impulse approximation. The dependence of the nuclear transparency on Q2 and the mass number A was investigated in a search for the onset of the color transparency phenomenon. We find no evidence for the onset of color transparency within our range of Q2. A fit to the world's nuclear transparency data reflects the energy dependence of the free-proton-nucleon cross section
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Source
JLAB-PHY--02-59; DOE/ER--40150-2395; AC--05-84ER40150
Record Type
Journal Article
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