2006
DOI: 10.1134/s0020441206060030
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A method and setup for studying the energy dependence of delayed neutron characteristics in nuclear fission induced by neutrons from the T(p, n), D(d, n), and T(d, n) reactions

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Cited by 7 publications
(14 citation statements)
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“…Because the pre-fission neutron spectra of second and third chance fissions are not provided in JENDL-4.0, we simply approximate ǫ ′ n = ǫ ′′ n = 0 to calculate Eq. (8). The effect of finite ǫ ′ n and ǫ ′′ n is discussed in sec.…”
Section: Second and Third Chance Fissionmentioning
confidence: 99%
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“…Because the pre-fission neutron spectra of second and third chance fissions are not provided in JENDL-4.0, we simply approximate ǫ ′ n = ǫ ′′ n = 0 to calculate Eq. (8). The effect of finite ǫ ′ n and ǫ ′′ n is discussed in sec.…”
Section: Second and Third Chance Fissionmentioning
confidence: 99%
“…In order to estimate the effect of finite pre-fission neutron energy, we calculate the delayed neutron yields of 238 U and 241 Pu varying ǫ ′ n and ǫ ′′ n in Eq. (8). We simply approximate…”
Section: B Energy Removal By Pre-fission Neutronmentioning
confidence: 99%
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“…The number of delayed neutrons per fission d of 233 U was determined on the basis of experimental data. The d value of 0.0067 at the thermal energy was obtained from the experimental data of Borzakov et al, 84) Conant and Palmedo, 85) and Keepin et al 56) In the energy region from 10 keV to 7 MeV, the d value was based on the data of Piksaykin et al, 86) Krick and Evans, 87) and Evans et al 88) As shown in Fig. 8, the present result is largely different from that in JENDL/AC-2008, which was determined by normalizing the data of Krick and Evans to 0.0067 at 0.0253 eV.…”
Section: )mentioning
confidence: 99%