Isospin effects in nucleon inelastic scattering from single-closed-shell nuclei: (I). The N = 50 isotones☆
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Cited by (53)
Symmetry energy III: Isovector skins
2017, Nuclear Physics ANuclear Data Sheets for A = 88
2014, Nuclear Data SheetsIsospin dependent global neutron-nucleus optical model potential
2012, Nuclear Physics ACalculation and analysis of n+<sup>90,91,92,94,96,nat</sup>Zr reactions in the E<inf>n</inf> ≤ 250 MeV energy range
2010, Annals of Nuclear EnergyCitation Excerpt :There are some experimental data of elastic scattering cross sections and elastic scattering angular distributions for natural zirconium and 90,91,92,94Zr below incident neutron energy 75.0 MeV. The experimental data of total cross sections taken from Finlay et al. (1993), Guenther et al. (1975) and Green and Mitchell (1973), all nonelastic cross sections (Ball et al., 1958; Beyster et al., 1955, 1956; Gregor et al., 1957, 1958; Kent et al., 1962; Walt and Beyster, 1955; Ibaraki et al., 2002) and elastic scattering angular distributions (Guenther et al., 1975; Daniel et al., 1974, 1977; Stooksberry et al., 1976; Bainum et al., 1978; Wang and Rapaport, 1990; Tanaka and Yamanouti, 1977; Walt and Barschall, 1954; Smith and Guenther, 1984; Anderson et al., 1959; Clarke and Cross, 1967; Chiba et al., 1992; Ibaraki et al., 2000) are used to obtain a set of neutron optical model potential parameters for n+90Zr reaction in incident neutron energy from 0.1 to 300 MeV. The adjustment of optical model potential parameters for 90Zr is performed to minimize a quantity called χ2, which represents the deviation of the theoretical calculated results from the experimental values.
Nuclear data sheets for A = 88
2005, Nuclear Data SheetsLocal and global nucleon optical models from 1 keV to 200 MeV
2003, Nuclear Physics A
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Supported in part by the National Science Foundation.
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