ENTRY C1924 20120529 C118C192400000001 SUBENT C1924001 20120529 C118C192400100001 BIB 7 16 C192400100002 TITLE Search for inverse fission of uranium C192400100003 AUTHOR (R.Yanez,W.Loveland,J.Beckerman,M.Leonard,C.J.Gross, C192400100004 D.Shapira,J.F.Liang,Z.Kohley,R.L.Varner) C192400100005 INSTITUTE (1USAORU,1USAORL) C192400100006 REFERENCE (J,PR/C,85,044620,2012) C192400100007 FACILITY (VDGT,1USAORL) Measurements were carried out at the C192400100008 Holifield Radioactive Ion Beam Facility (HRIBF) at C192400100009 the Oak Ridge National Laboratory. C192400100010 SAMPLE (42-MO-100,ENR=0.97) Enriched Mo target with C192400100011 thickness of 0.976mg/cm2.The beam passed through a C192400100012 0.286 mg/cm2 C degrader foil before striking the C192400100013 tilted (45deg) 100Mo target. All recoils formed were C192400100014 implanted in a single Al catcher foil of thickness C192400100015 8.1 mg/cm2 tilted an angle of 45deg with respect to C192400100016 the beam direction C192400100017 HISTORY (20120529C) Compiled by S.H. C192400100018 ENDBIB 16 0 C192400100019 NOCOMMON 0 0 C192400100020 ENDSUBENT 19 0 C192400199999 SUBENT C1924002 20120529 C118C192400200001 BIB 3 6 C192400200002 REACTION (42-MO-100(50-SN-124,FUS),,SIG,ER) C192400200003 STATUS (TABLE) Data taken from text p. 4 of the reference C192400200004 DETECTOR (MCPLT) Two microchannel plates in front of the target C192400200005 were used to determine time of ion arrival C192400200006 (IOCH)Ionization chamber was used to determine energy C192400200007 loss of detected particles. C192400200008 ENDBIB 6 0 C192400200009 NOCOMMON 0 0 C192400200010 DATA 2 2 C192400200011 EN-CM DATA-MAX C192400200012 MEV MB C192400200013 258.0 0.2 C192400200014 273.0 0.5 C192400200015 ENDDATA 4 0 C192400200016 ENDSUBENT 15 0 C192400299999 SUBENT C1924003 20120529 C118C192400300001 BIB 3 5 C192400300002 REACTION (42-MO-100(50-SN-132,2N)92-U-230,,SIG) C192400300003 STATUS (TABLE) Data taken from text p. 4 of the reference C192400300004 DETECTOR Alpha spectrometer with solid angle of 2pi was used C192400300005 to detect alpha particles emitted from evaporation C192400300006 residues with energy between 6 and 8 MeV C192400300007 ENDBIB 5 0 C192400300008 NOCOMMON 0 0 C192400300009 DATA 2 1 C192400300010 EN-CM DATA-MAX C192400300011 MEV MICRO-B C192400300012 220.0 550.0 C192400300013 ENDDATA 3 0 C192400300014 ENDSUBENT 13 0 C192400399999 SUBENT C1924004 20120529 C118C192400400001 BIB 5 13 C192400400002 REACTION 1(42-MO-100(50-SN-124,2N)92-U-222,,SIG) C192400400003 2(42-MO-100(50-SN-124,2N)92-U-222,,SIG) C192400400004 STATUS (TABLE) Data taken from text p. 4,5 of the reference C192400400005 METHOD 1In beam alpha spectroscopy during 10 s beam-off period C192400400006 2Using post irradiation alpha spectroscopy in attempt C192400400007 to identify 206Po in decay chain 222U C192400400008 DETECTOR 1(MCPLT) Two microchannel plates in front of target C192400400009 were used to determine time of ion arrival C192400400010 (IOCH)Ionization chamber was used to determine energy C192400400011 loss of detected particles. C192400400012 2Alpha spectrometer with solid angle of 2pi was used C192400400013 to detect alpha particles emitted from 206Po C192400400014 ERR-ANALYS (DATA-ERR) No information given C192400400015 ENDBIB 13 0 C192400400016 NOCOMMON 0 0 C192400400017 DATA 5 2 C192400400018 EN-CM DATA 1+DATA-ERR 1-DATA-ERR 1DATA-MAX 2 C192400400019 MEV NB NB NB NB C192400400020 225.0 21.0 38.0 21.0 C192400400021 225.0 270.0 C192400400022 ENDDATA 4 0 C192400400023 ENDSUBENT 22 0 C192400499999 ENDENTRY 4 0 C192499999999