ENTRY 14558 20190506 14531455800000001 SUBENT 14558001 20190506 14531455800100001 BIB 11 28 1455800100002 TITLE Neutron capture cross sections of 108,110Pd 1455800100003 AUTHOR (K.S.Krane) 1455800100004 INSTITUTE (1USAORU) 1455800100005 REFERENCE (J,PR/C,99,044313,2019) 1455800100006 FACILITY (REAC,1USAORU) Measurements were performed at the 1455800100007 Oregon State University TRIGA Reactor. 1455800100008 SAMPLE Natural Pd metal of thickness 0.025 mm was used as a 1455800100009 sample. Simultaneous irradiations of Au, Co, and Zr 1455800100010 were done to determine the neutron flux. 1455800100011 DETECTOR (HPGE) The gamma rays were observed with a high- 1455800100012 purity Ge detector with efficiency of 35% compared 1455800100013 with NaI at 1332 keV. The detector resolution was 1455800100014 typically 1.68 keV at 1332 keV. 1455800100015 METHOD (ACTIV) Activation method was used 1455800100016 INC-SOURCE (THCOL)Activation were performed in reactor thermal 1455800100017 column with nominal thermal and epithermal neutron 1455800100018 fluxes 7E+10 and 2E+8 n/cm2/s-1, respectively. Some 1455800100019 samples were irradiated using fast pneumatic transfer 1455800100020 facility with neutron fluxes 1E+13 and 3.5E+11 1455800100021 n/cm2/s-1, respectively 1455800100022 ERR-ANALYS (ERR-S,,1.0) Statistical uncertainty 1455800100023 (ERR-2,,1.0) Syst. uncertainty in detection efficiency 1455800100024 (ERR-3) Syst. uncertainty due to intercomparison of 1455800100025 different flux monitors 1455800100026 (ERR-4,3.0,8.0) Syst. uncertainty due to branching 1455800100027 ratios 1455800100028 (ERR-T) Total uncertainty 1455800100029 HISTORY (20190506C) Compiled by S.H. 1455800100030 ENDBIB 28 0 1455800100031 COMMON 1 3 1455800100032 ERR-3 1455800100033 PER-CENT 1455800100034 3. 1455800100035 ENDCOMMON 3 0 1455800100036 ENDSUBENT 35 0 1455800199999 SUBENT 14558002 20190506 14531455800200001 BIB 3 8 1455800200002 REACTION (46-PD-108(N,G)46-PD-109-G,,SIG,,MXW) 1455800200003 DECAY-DATA (46-PD-109-G,13.45HR,DG,88.0,0.0367, 1455800200004 DG,309.2,0.000380, 1455800200005 DG,636.3,0.000111, 1455800200006 DG,647.3,0.000260, 1455800200007 DG,781.4,0.000121) 1455800200008 Half-live measured by author 1455800200009 STATUS (TABLE) Data taken from tab. 2. of the reference 1455800200010 ENDBIB 8 0 1455800200011 NOCOMMON 0 0 1455800200012 DATA 3 1 1455800200013 EN-DUMMY DATA ERR-T 1455800200014 EV B B 1455800200015 0.0253 7.7 0.5 1455800200016 ENDDATA 3 0 1455800200017 ENDSUBENT 16 0 1455800299999 SUBENT 14558003 20190506 14531455800300001 BIB 4 13 1455800300002 REACTION (46-PD-108(N,G)46-PD-109-G,,RI) 1455800300003 DECAY-DATA (46-PD-109-G,13.45HR,DG,88.0,0.0367, 1455800300004 DG,309.2,0.000380, 1455800300005 DG,636.3,0.000111, 1455800300006 DG,647.3,0.000260, 1455800300007 DG,781.4,0.000121) 1455800300008 Half-live measured by author 1455800300009 STATUS (TABLE) Data taken from tab. 2. of the reference 1455800300010 COMMENT In the paper there are given no energy limits on 1455800300011 resonance integral. Since irradiations were performed 1455800300012 using Cd box with thickness of 1 mm and Cd cut-off 1455800300013 energy is approx. 0.5 eV, we used this value as 1455800300014 EN-MIN. 1455800300015 ENDBIB 13 0 1455800300016 NOCOMMON 0 0 1455800300017 DATA 3 1 1455800300018 EN-MIN DATA ERR-T 1455800300019 EV B B 1455800300020 0.5 138. 8. 1455800300021 ENDDATA 3 0 1455800300022 ENDSUBENT 21 0 1455800399999 SUBENT 14558004 20190506 14531455800400001 BIB 3 4 1455800400002 REACTION (46-PD-108(N,G)46-PD-109-M,,SIG,,MXW) 1455800400003 DECAY-DATA (46-PD-109-M,4.694MIN,DG,189.0,0.530) 1455800400004 Half-live measured by author 1455800400005 STATUS (TABLE) Data taken from tab. 2. of the reference 1455800400006 ENDBIB 4 0 1455800400007 NOCOMMON 0 0 1455800400008 DATA 3 1 1455800400009 EN-DUMMY DATA ERR-T 1455800400010 EV B B 1455800400011 0.0253 0.172 0.010 1455800400012 ENDDATA 3 0 1455800400013 ENDSUBENT 12 0 1455800499999 SUBENT 14558005 20190506 14531455800500001 BIB 4 9 1455800500002 REACTION (46-PD-108(N,G)46-PD-109-M,,RI) 1455800500003 DECAY-DATA (46-PD-109-M,4.694MIN,DG,189.0,0.530) 1455800500004 Half-live measured by author 1455800500005 STATUS (TABLE) Data taken from tab. 2. of the reference 1455800500006 COMMENT In the paper there are given no energy limits on 1455800500007 resonance integral. Since irradiations were performed 1455800500008 using Cd box with thickness of 1 mm and Cd cut-off 1455800500009 energy is approx. 0.5 eV, we used this value as 1455800500010 EN-MIN. 1455800500011 ENDBIB 9 0 1455800500012 NOCOMMON 0 0 1455800500013 DATA 3 1 1455800500014 EN-MIN DATA ERR-T 1455800500015 EV B B 1455800500016 0.5 3.07 0.15 1455800500017 ENDDATA 3 0 1455800500018 ENDSUBENT 17 0 1455800599999 SUBENT 14558006 20190506 14531455800600001 BIB 3 8 1455800600002 REACTION (46-PD-110(N,G)46-PD-111-G,,SIG,,MXW) 1455800600003 DECAY-DATA (46-PD-111-G,23.6MIN,DG,547.0,0.00332, 1455800600004 DG,580.0,0.00730, 1455800600005 DG,650.5,0.00481, 1455800600006 DG,835.8,0.00233, 1455800600007 DG,1388.4,0.00425) 1455800600008 Half-live measured by author 1455800600009 STATUS (TABLE) Data taken from tab. 2. of the reference 1455800600010 ENDBIB 8 0 1455800600011 NOCOMMON 0 0 1455800600012 DATA 3 1 1455800600013 EN-DUMMY DATA ERR-T 1455800600014 EV B B 1455800600015 0.0253 0.289 0.021 1455800600016 ENDDATA 3 0 1455800600017 ENDSUBENT 16 0 1455800699999 SUBENT 14558007 20190506 14531455800700001 BIB 4 13 1455800700002 REACTION (46-PD-110(N,G)46-PD-111-G,,RI) 1455800700003 DECAY-DATA (46-PD-111-G,23.6MIN,DG,547.0,0.00332, 1455800700004 DG,580.0,0.00730, 1455800700005 DG,650.5,0.00481, 1455800700006 DG,835.8,0.00233, 1455800700007 DG,1388.4,0.00425) 1455800700008 Half-live measured by author 1455800700009 STATUS (TABLE) Data taken from tab. 2. of the reference 1455800700010 COMMENT In the paper there are given no energy limits on 1455800700011 resonance integral. Since irradiations were performed 1455800700012 using Cd box with thickness of 1 mm and Cd cut-off 1455800700013 energy is approx. 0.5 eV, we used this value as 1455800700014 EN-MIN. 1455800700015 ENDBIB 13 0 1455800700016 NOCOMMON 0 0 1455800700017 DATA 3 1 1455800700018 EN-MIN DATA ERR-T 1455800700019 EV B B 1455800700020 0.5 3.33 0.23 1455800700021 ENDDATA 3 0 1455800700022 ENDSUBENT 21 0 1455800799999 SUBENT 14558008 20190506 14531455800800001 BIB 3 9 1455800800002 REACTION (46-PD-110(N,G)46-PD-111-M,,SIG,,MXW) 1455800800003 DECAY-DATA (46-PD-111-M,5.563HR,DG,172.2,0.354, 1455800800004 DG,391.3,0.0465, 1455800800005 DG,575.1,0.0279, 1455800800006 DG,632.6,0.0292, 1455800800007 DG,694.1,0.0171, 1455800800008 DG,762.0,0.0099) 1455800800009 Half-live measured by author 1455800800010 STATUS (TABLE) Data taken from tab. 2. of the reference 1455800800011 ENDBIB 9 0 1455800800012 NOCOMMON 0 0 1455800800013 DATA 3 1 1455800800014 EN-DUMMY DATA ERR-T 1455800800015 EV B B 1455800800016 0.0253 0.0116 0.0006 1455800800017 ENDDATA 3 0 1455800800018 ENDSUBENT 17 0 1455800899999 SUBENT 14558009 20190506 14531455800900001 BIB 4 14 1455800900002 REACTION (46-PD-110(N,G)46-PD-111-M,,RI) 1455800900003 DECAY-DATA (46-PD-111-M,5.563HR,DG,172.2,0.354, 1455800900004 DG,391.3,0.0465, 1455800900005 DG,575.1,0.0279, 1455800900006 DG,632.6,0.0292, 1455800900007 DG,694.1,0.0171, 1455800900008 DG,762.0,0.0099) 1455800900009 Half-live measured by author 1455800900010 STATUS (TABLE) Data taken from tab. 2. of the reference 1455800900011 COMMENT No energy limits on resonance integral are given 1455800900012 in the paper. Since irradiations were performed 1455800900013 using Cd box with thickness of 1 mm and Cd cut-off 1455800900014 energy is approx. 0.5 eV, we used this value as 1455800900015 EN-MIN. 1455800900016 ENDBIB 14 0 1455800900017 NOCOMMON 0 0 1455800900018 DATA 3 1 1455800900019 EN-MIN DATA ERR-T 1455800900020 EV B B 1455800900021 0.5 0.152 0.012 1455800900022 ENDDATA 3 0 1455800900023 ENDSUBENT 22 0 1455800999999 ENDENTRY 9 0 1455899999999