65 MeV polarized proton elastic scattering and the effective two-body interaction range
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Cited by (49)
Nuclear Structure and Decay Data for A=44 Isobars
2023, Nuclear Data SheetsNuclear Data Sheets for A=40
2017, Nuclear Data SheetsValidation of elastic cross section models for space radiation applications
2017, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :There is an abundance of elastic [56–70], reaction [56,71–129], and total cross section [56,58,69,70,130–146] data; therefore, these data have been used for validation of the model. An accurate representation of the available elastic differential cross section data [142,147–283] is also presented; however, there is a paucity of nucleus-nucleus differential cross section data for energies greater than a few hundred MeV/n. This manuscript proceeds as follows.
Nuclear Data Sheets for A = 54
2014, Nuclear Data SheetsCalculation and analysis for p + <sup>50,52,53,54,nat</sup>Cr reactions
2014, Annals of Nuclear EnergyCitation Excerpt :The spin–orbit potential is taken as a Thomas form. Based on the experimental data of non-elastic cross sections and elastic scattering angular distributions for p + 48Ti, p + 51V and p + 52Cr reactions (Lamba et al., 1968; Fulmer, 1962; Peterson, 1969; Shore et al., 1961; Lombardi et al., 1972; Fulmer and Goodman, 1960; Varner, 1986; Sakaguchi, 1982; Sakaguchi et al., 1979; Antropov et al., 1976, 1974; Demay et al., 1967; Comparat et al., 1974; Maripuu, 1970; Rao et al., 1994; Woo et al., 1984; Maripuu et al., 1970; Noro et al., 1981) at incident proton energies below 150 MeV, a set of optical potential parameters for p + 52Cr reaction is obtained using the code APMN (Shen, 2002), as shown in Table 1. The best optical potential parameters are reached by minimizing the quantity called χ2 which represents the deviation of the calculated results from the experiment data.
Nuclear Data Sheets for A = 89
2013, Nuclear Data Sheets