ENTRY 23463 20190111 227623463 0 1 SUBENT 23463001 20190111 227623463 1 1 BIB 7 28 23463 1 2 TITLE New accurate measurements of neutron emission 23463 1 3 probabilities for relevant fission products 23463 1 4 AUTHOR (J.Agramunt,J.L.Tain,F.Albiol,A.Algora, 23463 1 5 R.Caballero-Folch,F.Calvino,G.Cortes,I.Dillmann, 23463 1 6 T.Eronen,A.R.Garcia,E.Ganioglu,W.Gelletly,D.Gorelov, 23463 1 7 V.Guadilla,H.Hakala,A.Jokinen,A.Kankainen, 23463 1 8 A.Montaner,M.Marta,E.Mendoza,I.Moore,C.Nobs,S.Orrigo, 23463 1 9 H.Penttila,M.Reponen,S.Rinta-Antila, A.Riego,B.Rubio, 23463 1 10 A.Saastamoinen,P.Salvador-Castineira, 23463 1 11 A.Tarifeno-Saldivia,A.Tolosa,E.Valencia) 23463 1 12 INSTITUTE (2SPNVAL,2SPNUPC,1CANTMF,2SF JYV,2GERGSI,2UK SUR, 23463 1 13 2TUKSTU,2SPNPCM,3HUNDEB) 23463 1 14 REFERENCE (J,EPJ/CS,146,01004,2017) 23463 1 15 #doi:10.1051/epjconf/201714601004 23463 1 16 FACILITY (OLMS,2SF JYV) IGISOL-IV mass separator at the 23463 1 17 Cyclotron Laboratory of the University of Jyvaskyla. 23463 1 18 The isotope of interest produced by proton-induced 23463 1 19 Ep = 25 MeV fission of a U target inside the ion source23463 1 20 and separated by means of a double Penning trap system.23463 1 21 DETECTOR (SCIN) 3 mm thick plastic scintillation detector 23463 1 22 placed 6 mm from the tape for counting of the 23463 1 23 beta-particles emitted by the implanted ion. 23463 1 24 (PROPC,HE3SP) The neutron counter BELEN used in this 23463 1 25 measurement consists of forty eight 3He proportional 23463 1 26 tubes arranged in three concentric rings inside a large23463 1 27 polyethylene block. 23463 1 28 (HPGE) HPGe detector for gamma-ray counting. 23463 1 29 HISTORY (20190111C) VS 23463 1 30 ENDBIB 28 0 23463 1 31 NOCOMMON 0 0 23463 1 32 ENDSUBENT 31 0 23463 199999 SUBENT 23463002 20190111 227623463 2 1 BIB 4 9 23463 2 2 REACTION (51-SB-135(0,B-)52-TE-135,,PN) 23463 2 3 ANALYSIS (DECAY) The time evolution of the neutron and beta 23463 2 4 fitted by the Bateman equation to disentangle the 23463 2 5 contributions of the precursor and its descendants. 23463 2 6 - The ratio of the beta-particles and neutron detection23463 2 7 efficiencies determined by Pn measurement of 95Rb. 23463 2 8 ERR-ANALYS (DATA-ERR) Uncertainty analysis not given. 23463 2 9 (ERR-S) Relative statistical uncertainty is about 4% 23463 2 10 STATUS (TABLE) Table 1, EPJ Web of Conferences 146(2017)01004.23463 2 11 ENDBIB 9 0 23463 2 12 NOCOMMON 0 0 23463 2 13 DATA 3 1 23463 2 14 DATA DATA-ERR ERR-S 23463 2 15 NO-DIM NO-DIM PER-CENT 23463 2 16 0.245 0.010 4. 23463 2 17 ENDDATA 3 0 23463 2 18 ENDSUBENT 17 0 23463 299999 SUBENT 23463003 20190111 227623463 3 1 BIB 4 9 23463 3 2 REACTION (53-I-138(0,B-)54-XE-138,,PN) 23463 3 3 ANALYSIS (DECAY) The time evolution of the neutron and beta 23463 3 4 fitted by the Bateman equation to disentangle the 23463 3 5 contributions of the precursor and its descendants. 23463 3 6 - The ratio of the beta-particles and neutron detection23463 3 7 efficiencies determined by Pn measurement of 95Rb. 23463 3 8 ERR-ANALYS (DATA-ERR) Uncertainty analysis not given. 23463 3 9 (ERR-S) Relative statistical uncertainty is about 4% 23463 3 10 STATUS (TABLE) Table 1, EPJ Web of Conferences 146(2017)01004.23463 3 11 ENDBIB 9 0 23463 3 12 NOCOMMON 0 0 23463 3 13 DATA 3 1 23463 3 14 DATA DATA-ERR ERR-S 23463 3 15 NO-DIM NO-DIM PER-CENT 23463 3 16 0.0498 0.0018 4. 23463 3 17 ENDDATA 3 0 23463 3 18 ENDSUBENT 17 0 23463 399999 SUBENT 23463004 20190111 227623463 4 1 BIB 4 9 23463 4 2 REACTION (53-I-139(0,B-)54-XE-139,,PN) 23463 4 3 ANALYSIS (DECAY) The time evolution of the neutron and beta 23463 4 4 fitted by the Bateman equation to disentangle the 23463 4 5 contributions of the precursor and its descendants. 23463 4 6 - The ratio of the beta-particles and neutron detection23463 4 7 efficiencies determined by Pn measurement of 95Rb. 23463 4 8 ERR-ANALYS (DATA-ERR) Uncertainty analysis not given. 23463 4 9 (ERR-S) Relative statistical uncertainty is about 4% 23463 4 10 STATUS (TABLE) Table 1, EPJ Web of Conferences 146(2017)01004.23463 4 11 ENDBIB 9 0 23463 4 12 NOCOMMON 0 0 23463 4 13 DATA 3 1 23463 4 14 DATA DATA-ERR ERR-S 23463 4 15 NO-DIM NO-DIM PER-CENT 23463 4 16 0.0927 0.0033 4. 23463 4 17 ENDDATA 3 0 23463 4 18 ENDSUBENT 17 0 23463 499999 SUBENT 23463005 20190111 227623463 5 1 BIB 4 9 23463 5 2 REACTION (53-I-140(0,B-)54-XE-140,,PN) 23463 5 3 ANALYSIS (DECAY) The time evolution of the neutron and beta 23463 5 4 fitted by the Bateman equation to disentangle the 23463 5 5 contributions of the precursor and its descendants. 23463 5 6 - The ratio of the beta-particles and neutron detection23463 5 7 efficiencies determined by Pn measurement of 95Rb. 23463 5 8 ERR-ANALYS (DATA-ERR) Uncertainty analysis not given. 23463 5 9 (ERR-S) Relative statistical uncertainty is about 4% 23463 5 10 STATUS (TABLE) Table 1, EPJ Web of Conferences 146(2017)01004.23463 5 11 ENDBIB 9 0 23463 5 12 NOCOMMON 0 0 23463 5 13 DATA 3 1 23463 5 14 DATA DATA-ERR ERR-S 23463 5 15 NO-DIM NO-DIM PER-CENT 23463 5 16 0.0760 0.0028 4. 23463 5 17 ENDDATA 3 0 23463 5 18 ENDSUBENT 17 0 23463 599999 SUBENT 23463006 20190111 227623463 6 1 BIB 4 5 23463 6 2 REACTION (52-TE-137(0,B-)53-I-137,,PN) 23463 6 3 METHOD (COINC) Beta- neutron coincidences determined from 23463 6 4 the time correlation distribution. 23463 6 5 ERR-ANALYS (DATA-ERR) Uncertainty analysis not given. 23463 6 6 STATUS (TABLE) Table 1, EPJ Web of Conferences 146(2017)01004.23463 6 7 ENDBIB 5 0 23463 6 8 NOCOMMON 0 0 23463 6 9 DATA 2 1 23463 6 10 DATA DATA-ERR 23463 6 11 NO-DIM NO-DIM 23463 6 12 0.0260 0.0030 23463 6 13 ENDDATA 3 0 23463 6 14 ENDSUBENT 13 0 23463 699999 SUBENT 23463007 20190111 227623463 7 1 BIB 4 6 23463 7 2 REACTION (52-TE-138(0,B-)53-I-138,,PN) 23463 7 3 METHOD (COINC) Beta- neutron coincidences determined from 23463 7 4 the time correlation distribution. 23463 7 5 ERR-ANALYS (DATA-ERR) Uncertainty analysis not given. 23463 7 6 (ERR-S) Relative statistical uncertainty is about 5% 23463 7 7 STATUS (TABLE) Table 1, EPJ Web of Conferences 146(2017)01004.23463 7 8 ENDBIB 6 0 23463 7 9 NOCOMMON 0 0 23463 7 10 DATA 3 1 23463 7 11 DATA DATA-ERR ERR-S 23463 7 12 NO-DIM NO-DIM PER-CENT 23463 7 13 0.0480 0.0023 5. 23463 7 14 ENDDATA 3 0 23463 7 15 ENDSUBENT 14 0 23463 799999 ENDENTRY 7 0 2346399999999