Final-state interaction in electromagnetic response functions
References (37)
- et al.
Phys. Rev.
(1985) - et al.
Phys. Rev.
(1989) - et al.
Z. Phys.
(1988)et al.Nucl. Phys.
(1990) Phys. Rev. Lett.
(1981)Phys. Rev.
(1985)Nucl. Phys.
(1986)- et al.
Phys. Rev.
(1989) - et al.
Phys. Rev.
(1985)et al.Phys. Rev.
(1989) - et al.
Nucl. Phys.
(1981) - et al.
Nuovo Cim.
(1971) - et al.
Nucl. Phys.
(1969) - et al.
Ann. of Phys.
(1967)
Nucl. Phys.
Nucl. Phys.
Nucl. Phys.
Phys. Rev.
Phys. Rev.
Nucl. Phys.
Phys. Rev. Lett.
Phys. Rev. Lett.
Phys. Rev.
Phys. Rev.
Phys. Rev.
Phys. Lett.
Phys. Rev.
Phys. Rev.
Nucl. Phys.
Cited by (71)
Nucleon momentum distribution extracted from the experimental scaling function
2020, Nuclear Physics ACitation Excerpt :In the Relativistic Green's function (RGF) model FSI were originally developed within a nonrelativistic [44,45] and then within a fully relativistic framework [46,47] for the inclusive quasielastic (QE) electron scattering using complex energy-dependent optical potential. The model was successfully applied to electron scattering data [21,44–46,48,49] and later extended to neutrino-nucleus scattering [50–52]. The general structure of the paper is as follows.
NuSTEC White Paper: Status and challenges of neutrino–nucleus scattering
2018, Progress in Particle and Nuclear PhysicsEnergy levels of light nuclei A = 12
2017, Nuclear Physics ANeutrino–nucleus interactions and the determination of oscillation parameters
2017, Physics ReportsCitation Excerpt :In inclusive processes, however, there is no absorption, and FSI are usually described using a real optical potential. An alternative relativistic formalism employed for the description of inclusive processes is based on the expansion of the Green’s function entering the definition of the target response tensor in eigenfunctions of a non-hermitian optical potential [70]. It has to be pointed out that the NN cross section, driving the rescattering processes, is strongly influenced by the presence of the nuclear medium, which affects both the incoming flux and the available phase space.