[1] Chen J P, Meziani Z E, Beck D, et al. Longitudinal and transverse response functions in 56Fe(e,e′) at momentum transfer near 1 GeV/c[J]. Phys Rev Lett, 1991, 66: 1 283-1 286. [2] Meziani Z E, Barreau P, Bernheim M, et al. Coulomb sum rule for 40Ca, 48Ca, and 56Fe for |q|≤500 MeV/c[J]. Phys Rev Lett, 1984, 52: 2 130-2 133. [3] Meziani Z E, Barreau P, Bernheim M, et al. Transverse response functions in deep-inelastic electron scattering for 40Ca, 48Ca, and 56Fe[J]. Phys Rev Lett, 1985, 54: 1 233-1 236. [4] Deady M, Williamson C F, Zimmerman P D, et al. Deep inelastic separated response functions from 40Ca and 48Ca[J]. Phys Rev C, 1986, 33: 1 897-1 904. [5] Blatchley C C, LeRose J J, Pruet O E, et al. Quasi-elastic electron scattering from 238U[J]. Phys Rev C, 1986, 34: 1 234-1 247. [6] De Forest Jr T. The relativistic Coulomb sum rule for electron scattering in the independent-particle model[J]. Nucl Phys A, 1984, 414(3): 347-358. [7] Grupen C. Particle Detectors[M]. Cambridge: Cambridge University Press, 1996: 193. [8] Liyanage N. A study of the 16O(e,e′p) reaction at deep missing energies[D]. Massachusetts Institute of Technology, Cambridge, Massachusetts, 1999. [9] Alcorn J, et al (JLab Collaboration). Basic instrumentaion for Hall A at Jefferson Lab[J]. Nuclear Instruments and Methods in Physics Research A, 2004,522:294-346. |