1989
DOI: 10.1007/bf02845910
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Light-charged particle emission in fission

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Cited by 9 publications
(6 citation statements)
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“…(23) with particle binding energies estimated using Eqs. (3)(4)(5)(6)(7)9) as discussed in section II (see table I or model I in table II). The model parameters are then adjusted to minimize the fitting metric defined in Eq.…”
Section: Comparison Of the Model With Experimentsmentioning
confidence: 99%
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“…(23) with particle binding energies estimated using Eqs. (3)(4)(5)(6)(7)9) as discussed in section II (see table I or model I in table II). The model parameters are then adjusted to minimize the fitting metric defined in Eq.…”
Section: Comparison Of the Model With Experimentsmentioning
confidence: 99%
“…The main ternary-fission observables include the probability per fission event of generating various isotopes, their energy spectra and angular distributions. Extensive measurements of these properties have been made and substantially documented in several review articles [3][4][5][6]. The dominant ternary-fission particles are α particles, which occur a few times per thousand thermal-neutron-induced or spontaneous fissions.…”
Section: Introductionmentioning
confidence: 99%
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“…Although there have been many studies on prescission α-particle emission in many heavy-ion-induced fusion-fission reactions [1,2,[5][6][7][8][9], a global systematics is yet to be developed. In low-energy fission (thermal neutron-induced, photo-, and spontaneous fission) NSE is a dominant channel [11][12][13] and exhibits characteristic energy and angular distributions corresponding to strong focusing of the particles by the Coulomb field of the fragments. The near-scission α-particle multiplicities are found to increase linearly with Z 2 /A of the fissioning nucleus [11,12].…”
mentioning
confidence: 99%
“…In low-energy fission (thermal neutron-induced, photo-, and spontaneous fission) NSE is a dominant channel [11][12][13] and exhibits characteristic energy and angular distributions corresponding to strong focusing of the particles by the Coulomb field of the fragments. The near-scission α-particle multiplicities are found to increase linearly with Z 2 /A of the fissioning nucleus [11,12]. The features of the NSE observed in low-energy fission have been understood qualitatively with the sudden neck collapse dynamic model suggested by Halpern [13].…”
mentioning
confidence: 99%