Final-state interactions and superscaling in the semi-relativistic approach to quasielastic electron and neutrino scattering
arXiv:nucl-th/0612056 · doi:10.1103/PhysRevC.75.034613
Abstract
The semi-relativistic approach to electron and neutrino quasielastic scattering from nuclei is extended to include final-state interactions. Starting with the usual non-relativistic continuum shell model, the problem is relativized by using the semi-relativistic expansion of the current in powers of the initial nucleon momentum and relativistic kinematics. Two different approaches are considered for the final-state interactions: the Smith-Wambach 2p-2h damping model and the Dirac-equation-based potential extracted from a relativistic mean-field plus the Darwin factor. Using the latter the scaling properties of and cross sections for intermediate momentum transfers are investigated.
36 pages, 17 figures
Cited by in corpus (13)
- Scaling and isospin effects in quasielastic lepton-nucleus scattering in the Relativistic Mean Field Approach
- Relativistic descriptions of inclusive quasielastic electron scattering: application to scaling and superscaling ideas
- Impact of nuclear effects on the determination of the nucleon axial mass
- Quasielastic Charged Current Neutrino-nucleus Scattering
- Superscaling and Charge-Changing Neutrino Scattering from Nuclei in the -Region beyond the Relativistic Fermi Gas Model
- Superscaling and Neutral Current Quasielastic Neutrino-Nucleus Scattering beyond the Relativistic Fermi Gas Model
- Charged current anti-neutrino reactions from C at MiniBooNE energies
- Quasi-elastic neutrino charged-current scattering off C-12
- Final-State Interactions in the Superscaling Analysis of Neutral-Current Quasielastic Neutrino Scattering
- Superscaling Predictions for Neutral Current Quasielastic Neutrino-Nucleus Scattering
- y-scaling in Quasielastic Electron Scattering from Nuclei
- Longitudinal and Transverse Scaling Functions within the Coherent Density Fluctuation Model
- Superscaling of non-quasielastic electron-nucleus scattering