Fission Product Yield Data for the Transmutation of Minor Actinide ...

8
(d) Prompt or delayed neutron emission:
[2.1.24, 2.1.32, 2.1.48, 2.1.75, 2.1.79, 2.1.82,
2.1.85, 2.1.110, 2.1.111];
(e) Emission of light charged particles:
[2.1.112–2.1.114].
(3) Deuteron induced fission:
(a) Mass distribution: [2.1.23, 2.1.45, 2.1.68,
2.1.115–2.1.117];
(b) Nuclear charge distribution: [2.1.45,
2.1.118, 2.1.119];
(c) Isomeric yields: [2.1.16];
(d) Prompt or delayed neutron emission:
[2.1.116];
(e) Emission of light charged particles: (no
references found).
(4) Helium-3 induced fission:
(a) Mass distribution: [2.1.20, 2.1.23, 2.1.38,
2.1.78, 2.1.120–2.1.122];
(b) Nuclear charge distribution: [2.1.123];
(c) Isomeric yields: (no references found);
(d) Prompt or delayed neutron emission: (no
references found);
(e) Emission of light charged particles: (no
references found).
(5) Alpha particle induced fission:
(a) Mass distribution: [2.1.2, 2.1.35–2.1.38,
2.1.45, 2.1.78, 2.1.122, 2.1.124–2.1.142];
(b) Nuclear charge distribution: [2.1.45,
2.1.123, 2.1.136, 2.1.143, 2.1.144];
(c) Isomeric yields: [2.1.15, 2.1.145–2.1.150];
(d) Prompt or delayed neutron emission:
[2.1.145];
(e) Emission of light charged particles:
[2.1.137].
(6) Fission induced by some other charged
particles:
(a) Mass distribution: [2.1.18, 2.1.23, 2.1.26,
2.1.39–2.1.42, 2.1.48, 2.1.49, 2.1.51–2.1.54,
2.1.63, 2.1.66, 2.1.79];
(b) Nuclear charge distribution: [2.1.18,
2.1.26, 2.1.49, 2.1.51–2.1.54, 2.1.79, 2.1.97,
2.1.100, 2.1.102];
(c) Isomeric yields: [2.1.108];
(d) Prompt or delayed neutron emission:
[2.1.48, 2.1.79];
(e) Emission of light charged particles:
[2.1.112, 2.1.113].
(7) Photon induced fission:
(a) Mass distribution: [2.1.151–2.1.161];
(b) Nuclear charge distribution: [2.1.151,
2.1.153–2.1.157, 2.1.162–2.1.168];
(c) Isomeric yields: [2.1.151, 2.1.152, 2.1.169–
2.1.171];
(d) Prompt or delayed neutron emission:
[2.1.159, 2.1.172];
(e) Emission of light charged particles:
[2.1.173, 2.1.174].
(8) Fission in inverse kinematics: [2.1.175–2.1.185]
REFERENCES TO SECTION 2.1
[2.1.1] ETHVIGNOT, T., et al., Intermediate energy
neutron-induced fission of uranium: Product
yields and isomer studies, personal communication,
2001.
[2.1.2] FORD, G.P., LEACHMAN, R.B., Fission mass
yield dependence on angular momentum, Phys.
Rev. 137 (1965) B826–B836.
[2.1.3] GINDLER, J.E., et al., Mass distributions in
monoenergetic-neutron-induced fission of 239Pu, Phys. Rev. C 27 (1983) 2058–2062.
[2.1.4] GLENDENIN, L.E., et al., Mass distributions in
monoenergetic-neutron-induced fission of 232 Th,
Phys. Rev. C 22 (1980) 152–159.
[2.1.5] GLENDENIN, L.E., et al., Mass distributions
for monoenergetic-neutron-induced fission of
235
U, Phys. Rev. C 24 (1981) 2600–2605.
[2.1.6] GOVERDOVSKII, A.A., et al., Temperature
effects in pre-scission-deformation spectra of
238Np fission fragments, Phys. At. Nucl. 60 (1997)
1441–1447.
[2.1.7] HAMELIN, C., Etude des Distributions en
Masse et en Charge Nucléaire dans la Fission
Induite par Neutrons de 3 MeV pour quelques
Noyeaux fissiles, PhD thesis, Université scientifique
et médicale de Grenoble, France (1983).
[2.1.8] NAGY, S., et al., Mass distribution in monoenergetic-neutron-induced
fission of 238U, Phys. Rev.
C 17 (1978) 163–171.
[2.1.9] YOUNES, W., et al., Transition from asymmetric
to symmetric fission in the 235U(n,f) reaction,
Phys. Rev. C 64 (2001) 054613–054635.
[2.1.10] ZÖLLER, C.M., Untersuchung der neutroneninduzierten
Spaltung von 238U im Energiebereich
von 1 MeV bis 500 MeV, PhD thesis,
Technische Hochschule Darmstadt, Germany
(1995).