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N. C. R. Makins, R. Ent, M. S. Chapman, J.-O. Hansen, K. Lee, R. G. Milner, and J. Nelson
Laboratory for Nuclear Science, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139
R. G. Arnold, P. E. Bosted, C. E. Keppel, A. Lung, S. E. Rock, M. Spengos, Z. M. Szalata, L. H. Tao, and J. L. White
The American University, Washington, D.C. 20016
K. P. Coulter, D. F. Geesaman, R. J. Holt, H. E. Jackson, V. Papavassiliou, D. H. Potterveld, and B. Zeidman
Argonne National Laboratory, Argonne, Illinois 60439
J. Arrington, E. J. Beise, E. Belz, B. W. Filippone, H. Gao, W. Lorenzon, B. Mueller, R. D. McKeown, and T. G. O’Neill
W. K. Kellogg Radiation Laboratory, California Institute of Technology, Pasadena, California 91125
M. Epstein and D. J. Margaziotis
California State University, Los Angeles, California 90032
J. Napolitano
Rensselaer Polytechnic Institute, Troy, New York 12180
E. Kinney
University of Colorado, Boulder, Colorado 80309
P. L. Anthony, K. van Bibber, and F. S. Dietrich
Lawrence Livermore National Laboratory, Livermore, California 94550
R. A. Gearhart and G. G. Patratos
Stanford Linear Accelerator Center, Stanford, California 94309
S. E. Kuhn
Stanford University, Stanford, California 94305
J. F. J. van den Brand, H.-J. Bulten, and C. E. Jones
University of Wisconsin–Madison, Madison, Wisconsin 53706
The cross section for quasielastic 12C(e,e’p) scattering has been measured at momentum transfer Q2=1, 3, 5, and 6.8 (GeV/c)2. The results are consistent with scattering from a single nucleon as the dominant process. The nuclear transparency is obtained and compared with theoretical calculations that incorporate color transparency effects. No significant rise of the transparency with Q2 is observed.
URL:
http://link.aps.org/doi/10.1103/PhysRevLett.72.1986
DOI:
10.1103/PhysRevLett.72.1986