Quasielastic K-nucleus scattering
arXiv:nucl-th/9608012 · doi:10.1103/PhysRevC.55.1394
Abstract
Quasielastic K^+ - nucleus scattering data at q=290, 390 and 480 MeV/c are analyzed in a finite nucleus continuum random phase approximation framework, using a density-dependent particle-hole interaction. The reaction mechanism is consistently treated according to Glauber theory, keeping up to two-step inelastic processes. A good description of the data is achieved, also providing a useful constraint on the strength of the effective particle-hole interaction in the scalar-isoscalar channel at intermediate momentum transfers. We find no evidence for the increase in the effective number of nucleons participating in the reaction which has been reported in the literature.
21 pages, uses REVTeX and epsfig, 9 postscript figures; replaced version corrects a few minor errors in the text
References in corpus (8)
- Parity violation in quasielastic electron scattering from closed-shell nuclei
- Pion Cloud Contribution to K+ Nucleus Scattering
- The Pion in Electromagnetic and Weak Neutral Current Nuclear Response Functions
- CHIRAL SYMMETRY CONSTRAINTS ON THE INTERACTION WITH THE NUCLEAR PION CLOUD
- K-nucleus quasielastic scattering
- The Quasi-Elastic Nuclear Response
- Glauber isovector spin responses for (p,n) reactions at 494 MeV
- Comparison of and Quasielastic Scattering
Cited by in corpus (5)
- Antisymmetrized random phase approximation for quasielastic scattering in nuclear matter: Non-relativistic potentials
- Linear Response Theory with finite-range interactions
- Nuclear response functions with finite range Gogny force: tensor terms and instabilities
- Quasielastic K+ scattering in nuclei
- Delta excitation in K^+-nucleus collisions