Proton-nucleus elastic scattering at 156 MeV
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Cited by (102)
Nuclear Data Sheets for A=40
2017, 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 SheetsThe cross sections and energy spectra of the particle emission in proton induced reactions on <sup>209</sup>Bi
2012, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :The theoretical calculated results of total reaction cross sections are in good agreement with the experimental data [26–31] of p+208Pb reaction as shown in Fig. 1. The comparison of the calculated results of elastic scattering angular distributions with the experimental data [32–34] for p+209Bi reaction shows that the calculated results are in good agreement with the experimental data. The calculated results of proton inelastic scattering angular distributions for different discrete levels at 61.7 MeV are compared with the experimental data [32,35].
Calculation and analysis of p + <sup>40,42,43,44,46,48,nat</sup>Ca reaction cross sections at incident energies from threshold to 250 MeV
2011, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :The calculated results of elastic scattering angular distributions at the incident proton energies from 9.86 to 201.4 MeV and elastic scattering angular distributions in the Rutherford ratio at the incident proton energies from 13.98 to 160.0 MeV are in good agreement with experimental data [38–61] for p + 40Ca reaction. Figs. 4–8 show respectively the comparison of the calculated results with experimental data [38,41,47–61]. The calculated results of elastic scattering angular distributions at the incident proton energies of 9.0, 12.0, 21.0, 25.0, 30.0, 35.0, 40.0, 45.0 and 48.4 MeV, and elastic scattering angular distributions in the Rutherford ratio at the incident proton energies of 22.85, 49.35 and 65.0 MeV are in good agreement with experimental data [47,60,62–64] for p + 42Ca reaction as shown in Figs. 9 and 10.
Calculation and analysis of cross-sections for p+ <sup>90,91,92,94,96,nat</sup>Zr reactions up to 200 MeV
2011, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :The calculated results reproduce the experimental data for p+90Zr reaction up to near 200 MeV well. The theoretical results of elastic scattering angular distributions for p+90Zr reaction are compared with experimental data at Ep = 9.7 MeV measured by Greenlees et al. [23], 14.71 MeV by Makofske et al. [24], 16 MeV by Varner et al. [25], 22.5 MeV by Ball et al. [26], 30 MeV by Swiniarski et al. [27], 40 MeV by Blumberg et al. [28], 65 MeV by Sakaguchi et al. [29], 80, 135 and 160 MeV by Nadasen et al. [30], 156 MeV by Comparat et al. [31] and 185 MeV by Hagberg et al. [32] in Fig. 2a. The calculated results of elastic scattering angular distributions in the Rutherford ratio for p+90Zr reaction are compared with experimental data measured by Gurbich et al. [33] at Ep = 5.574–9.018 MeV, Dickens et al. [34] at 12.7 MeV, Gray et al. [35] at 18.8 MeV, Glashausser et al. [36] at 20.25 MeV, Fricke et al. [37] at 40 MeV, Mani et al. [38] at 49.35 MeV, Fulmer et al. [39] at 61.4 MeV and Kwiatkowski et al. [40] at 100.4 MeV in Fig. 2b.