References quoted in the XUNDL dataset: 136SB U(P,F):%B-N:XUNDL-4
6 references found.
Clicking on a keynumber will list datasets that reference the given article.
J.Inorg.Nucl.Chem. 39, 753 (1977)
W.Rudolph, K.-L.Kratz, G.Herrmann
Half-Lives, Fission Yields and Neutron Emission Probabilities of Neutron-Rich Antimony Isotopes
RADIOACTIVITY 134,135,136Sb, 136Te; measured T1/2, delayed neutrons.
NUCLEAR REACTIONS 235U(n, F), E=th; measured fission yields, yields for 134,135Sb. 134,135,136Sb, 136Te deduced neutron emission probabilities.
doi: 10.1016/0022-1902(77)80148-6
Z.Phys. A287, 45 (1978)
J.Crancon, C.Ristori, H.Ohm, W.Rudolph, K.-L.Kratz, M.Asghar
Half-Lives and P(n) Values of Delayed-Neutron Precursors in the Mass Chains 85-87, 92, 135, 136 and 145
RADIOACTIVITY 85,86,87As, 92Br, 135,136Sb, 136Te, 145Cs; measured T1/2, neutron emission probability.
At.Data Nucl.Data Tables 53, 1 (1993)
G.Rudstam, K.Aleklett, L.Sihver
Delayed- Neutron Branching Ratios of Precursors in the Fission Product Region
COMPILATION A=75-150; compiled β--decay T1/2, neutron emission probability; deduced average delayed-neutron branching ratios.
RADIOACTIVITY 80,81,83,79,82Ga, 84Ge, 84,85,86,87As, 88,89,91,87Se, 100,99,98mY, 100,98Sr, 99,98,97,96,95,94,93,92Rb, 91,90,89,88,87Br, 129m,129,130m,131,128m,128,132In, 150,149,148,147La, 149,148,147,146Ba, 148,147,146,145,144,143,142,141Cs, 139,138,137I, 137,136Te, 136,135,134Sb, 134,133Sn(β-n); measured β-, neutron activity simultaneously; deduced revised neutron emission probability, T1/2, delayed neutron branching ratios.
Prog.Nucl.Energy 41, 39 (2002)
B.Pfeiffer, K.Kratz, P.Moller
Status of delayed-Neutron Precursor Data: Half-Lives and Neutron Emission Probabilities
COMPILATION Z=27-63; compiled, analyzed β-decay T1/2, neutron emission probabilities, model predictions.
University of Chicago (2015)
S.Caldwell
A trapped-ion technique for beta-delayed neutron studies
RADIOACTIVITY 135,136Sb, 137I(β-), (β-n)[from CARIBU-ANL facility]; measured γ, β, neutron spectra, βγ-coin, (recoil)β-coin, β(ce)-coin, delayed-neutron emission probabilities (Pn) using Beta-Decay Paul Trap (BPT) and Canadian Penning Trap Mass spectrometer (CPTMS) systems. Comparison with previous experimental values.
Phys.Rev. C 98, 034310 (2018)
R.Caballero-Folch, I.Dillmann, J.Agramunt, J.L.Tain, A.Algora, J.Aysto, F.Calvino, L.Canete, G.Cortes, C.Domingo-Pardo, T.Eronen, E.Ganioglu, W.Gelletly, D.Gorelov, V.Guadilla, J.Hakala, A.Jokinen, A.Kankainen, V.Kolhinen, J.Koponen, M.Marta, E.Mendoza, A.Montaner-Piza, I.Moore, C.R.Nobs, S.E.A.Orrigo, H.Penttila, I.Pohjalainen, J.Reinikainen, A.Riego, S.Rinta-Antila, B.Rubio, P.Salvador-Castineira, V.Simutkin, A.Tarifeno-Saldivia, A.Tolosa-Delgado, A.Voss
First determination of β-delayed multiple neutron emission beyond A-100 through direct neutron measurement: The P2n value of 136Sb
RADIOACTIVITY 136Sb(β-), (β-n), (β-2n), 136Te(β-), (β-n)[from U(p, F), E=25 MeV]; measured Eβ-, Iβ-, E(n), I(n), β- and neutron time correlated events, %β-n (or P1n) for decays of 136Sb and 136Te, and %β-2n (or P2n) for decay of 136Sb using JYFLTRAP Penning trap for isotope separation, plastic scintillator for β detection, and BELEN array of 3He counter tubes for neutron detection at the University of Jyvaskyla accelerator facility. Comparison with previous experimental values, evaluated data, and with several theoretical predictions.
doi: 10.1103/PhysRevC.98.034310