Cross sections of some reactions of Al, S, Mn, Fe, Ni, In AND I with 14.8 MeV neutrons
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Cited by (37)
A theoretical study for the production of <sup>32</sup>P radioisotope using neutrons from the <sup>68</sup>Zn(p,n)<sup>68</sup>Ga reaction in a medical cyclotron
2022, Applied Radiation and IsotopesCitation Excerpt :Other research has also been done to measure the cross section of 68Zn(p,n)68Ga reaction in different proton energy range (Barrandon et al., 1975; Johnson et al., 1964; Blosser and Handley, 1955; Blaser et al., 1951;; Mcgee et al., 1970; Howe, 1958; Hille et al., 1972). Activation cross section of 32P in neutron induced nuclear reactions on 32S at the energy of 14.8 MeV have been measured by various research groups (Robertson et al., 1973; Barrall et al., 1969; Levkovskii et al., 1969; Pasquarelli, 1967; Khurana and Govil, 1965). Paulsen and Liskien (Paulsen and Liskien, 1966) measured the cross section of 32S(n,p)32P reaction within the neutron energy range of 1.56–2.22 MeV.
Theoretical calculations and evaluations of n + <sup>32,33,34,36,nat.</sup>S reactions
2014, Annals of Nuclear EnergyCitation Excerpt :The experimental data may be too small, since the calculated inelastic scattering angular distributions around 14.1 MeV for the excited states are in agreement with the corresponding experimental data. The calculated results and the experimental data (Barrall et al., 1969; Barrall et al., 1969; Santry and Butler, 1963; Robertson et al., 1973; Pasquarelli, 1967; Paulsen and Liskien, 1966; Khurana and Hans, 1959; Khurana and Govil, 1965; Levkovskiy, 1963; Levkovskiy, 1968) for 32S (n, p) reaction cross sections are shown in Fig. 31. The calculated curves pass through some experimental data within error bars.
Cross-sections for (n,2n), and (n,α) reactions on <sup>55</sup>Mn isotope around neutron energy of 14MeV
2012, Radiation Physics and ChemistryCitation Excerpt :In this case, gamma rays emitted are at 834.848 keV, the self-absorption factor have been calculated to be 1.0416, coincidence summing to be 1, and the geometry to be 1.020. Fig. 5 and Table 2 show that cross section for 55Mn(n,2n)54Mn reaction along with previous results (Araminowicz and Dresler, 1973; Barrall et al., 1969; Bormann and Lammers, 1969; Bostan and Qaim, 1994; Csikai and Peto, 1967; Deak et al., 1975; Ercan et al., 1991; Granger and Longueve, 1963; Greenwood, 1987; Hanlin et al., 1980; Ikeda et al., 1988; Kayashima et al., 1979; Kobayashi and Kimura, 1988a,b; Maslov et al., 1972; Menlove et al., 1967; Murata et al., 2008; Paulsen and Liskien, 1965; Salnikov et al., 1971; Schwerer et al., 1976; Uwamino et al., 1992; Weigold, 1960; Wenusch and Vonach,1962). Below 15 MeV, cross section value increases as the neutron energy increases.
Cross-section measurements for the reactions of 14 MeV neutrons on indium isotopes
2006, Applied Radiation and IsotopesComparison of calculated and measured high energy neutron reaction rates at the manual Jr. Lujan Center Spallation Source
2005, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Work done under the auspices of the U.S. Atomic Energy Commission.