Nuclear EMC Effect in a Statistical Model
arXiv:0909.0454 · doi:10.1016/j.nuclphysa.2009.07.006
Abstract
A simple statistical model in terms of light-front kinematic variables is used to explain the nuclear EMC effect in the range , which was constructed by us previously to calculate the parton distribution functions (PDFs) of the nucleon. Here, we treat the temperature as a parameter of the atomic number , and get reasonable results in agreement with the experimental data. Our results show that the larger , the lower thus the bigger volume , and these features are consistent with other models. Moreover, we give the predictions of the quark distribution ratios, \emph{i.e.}, , , and , and also the gluon ratio for iron as an example. The predictions are different from those by other models, thus experiments aiming at measuring the parton ratios of antiquarks, strange quarks, and gluons can provide a discrimination of different models.
26 latex pages, 3 figures
References in corpus (3)
Cited by in corpus (10)
- Light flavor asymmetry of nucleon sea
- Quark sea asymmetries of the octet baryons
- Nucleon structure functions and longitudinal spin asymmetries in the chiral quark constituent model
- Dynamical and thermal descriptions in parton distribution functions
- The European Muon Collaboration effect from short-range correlated nucleons in a -rescaling model
- Flavor-dependent EMC effect from a nucleon swelling model
- Quark flavor distribution functions for the octet baryons in the chiral quark constituent model
- Electromagnetic and Axial-Vector Form Factors of the Quarks and Nucleon
- Octet Quark Contents from SU(3) Flavor Symmetry
- Parton distribution functions and nuclear EMC effect in a statistical model