ENTRY 23196 20130628 22352319600000001 SUBENT 23196001 20130628 22352319600100001 BIB 16 214 2319600100002 TITLE Evaluation of resonance parameters for neutron induced 2319600100003 reactions in cadmium. 2319600100004 AUTHOR (K.Volev, A.Borella,S.Kopecky, C.Lampoudis, C.Massimi, 2319600100005 A.Moens, M.Moxon, P.Schillebeeckx,P.Siegler, I.Sirakov,2319600100006 A.Trkov, R.Wynants) 2319600100007 INSTITUTE (2ZZZGEL) K.Volev, A.Borella,S.Kopecky, C.Lampoudis, 2319600100008 A.Moens,P.Schillebeeckx,P.Siegler, I.Sirakov,R.Wynants.2319600100009 (3BULBLA) K.Volev, I.Sirakov. 2319600100010 (2BLGMOL) A.Borella. 2319600100011 (2ITYUBO) C.Massimi. 2319600100012 (2UK UK) Hyde Copse, Marcham -M.Moxon 2319600100013 (3SLNIJS) A.Trkov 2319600100014 (3ZZZIAE) A.Trkov 2319600100015 REFERENCE (J,NIM/B,300,11,2013) Data Tables. 2319600100016 #doi:10.1016/j.nimb.2013.01.030 2319600100017 REL-REF (I,,D.Tronc+,J,NIM/A,228,217,1985) 2319600100018 Details of GELINA facility. 2319600100019 (M,,A.Borella+,J,NIM/A,577,626,2007) 2319600100020 PHWT method. 2319600100021 (R,23077001,S.Kopecky+,J,NIM/B,267,2345,2009) 2319600100022 (R,,R.C.Lloyd+,J,NT,79,82,1987) 2319600100023 FACILITY (LINAC,2ZZZGEL) Neutron TOF facility GELINA. 2319600100024 Transmission measurements at the 25-m station have been2319600100025 performed with the accelerator operating at 50, 400 and2319600100026 800 Hz. At capture measurement -at 50 Hz and 400 Hz. 2319600100027 INC-SOURCE Moderated neutron beam. 2319600100028 Transmission: 2319600100029 B-10 overlap filter, areal density 0.008 at/b, was used2319600100030 to eliminate neutrons from previous burst. Li-carbonate2319600100031 + resin, Pb and Cu-collimators were used to reduce the 2319600100032 neutron beam to a diameter of 35 mm at the sample 2319600100033 position. 15-mm diameter neutron beam at the sample 2319600100034 position. A 5-mm thick Pb filter was placed in front of2319600100035 the sample changer to reduce the intense gamma-ray 2319600100036 flash. 2319600100037 Capture: 2319600100038 Moderated neutron beam was collimated to about 75 mm 2319600100039 diameter at the sample position by Li-carbonate, Cu- 2319600100040 and Pb-collimators. 2319600100041 SAMPLE Samples at a constant temperature of about 20 deg C : 2319600100042 # Weight Size Thickness Areal density Cd-purity2319600100043 g mm at/b wt.% 2319600100044 1 1.281 80.40mm diam. 0.03 1.363E-4 99.9975 2319600100045 2 3.184 80.04mm diam. 0.08 3.390E-4 99.9975 2319600100046 3 87.460 80.00mm diam. 2.06 93.406E-4 99.9975 2319600100047 4 1.979 50.08mm diam. 0.12 5.382E-4 > 99.99 2319600100048 5 17.1120 50.00mm diam. 1.02 46.698E-4 99.999 2319600100049 6 414.646 50.00mm diam. 25.00 1.205E-1 99.999 2319600100050 7 447.216 100x100mm2 5.09 231.020E-4 99.99 2319600100051 Samples 1-6 as discs, sample 7 - foil. 2319600100052 Transmission, path 25m: samples 1,2 were used, 2319600100053 transmission, path 50m: samples 3,4,6,7, 2319600100054 capture, path 12.5m: samples 1,3, 2319600100055 capture, path 30m: sample 5 . 2319600100056 DETECTOR (PROPC) BaF3 proportional counters are used to monitor 2319600100057 the stability of the accelerator and to normalize 2319600100058 TOF-spectra to the same total neutron intensity. 2319600100059 Transmission: 2319600100060 (GLASD) 6.35-mm thick, 101.6-mm diameter NE912 Li-glass2319600100061 scintillator enriched to 95% in 6Li, coupled to a 2319600100062 boron-free quartz windowed EMI9823-QKB photomultiplier 2319600100063 The detector was placed at a distance of 49.34 m from 2319600100064 the exit face of the moderator. 2319600100065 Used to detect neutrons - at 50 m path. 2319600100066 NE905 Li-glass scintillator, enriched to 95% in 6Li, 2319600100067 110.0 mm diameter and 12.7 mm thick, placed in a 2319600100068 thin-walled Al can, viewed by two EMI9823-QKB PMTs. 2319600100069 Used to detect neutrons - at 25 m path. 2319600100070 Capture: 2319600100071 (SCIN) Gamma-rays were detected by a pair of C6D6 2319600100072 detectors, each positioned at an angle of 125deg with 2319600100073 respect to the direction of the neutron beam, 2319600100074 coupled to a boron-free quartz windowed PMT. 2319600100075 The linearity and resolution of the C6D6 detectors were2319600100076 monitored on a weekly basis by measurements of the 2319600100077 2.6 MeV gamma-ray from the 232Th decay chain. 2319600100078 (IOCH) The energy dependent neutron spectrum below 2319600100079 150 keV was measured in parallel with a 10B Frisch 2319600100080 gridded ionization chamber placed at about 80 cm before2319600100081 the sample. Cathode loaded with two back-to-back 2319600100082 layers of B-10 with an effective diameter of 84 mm 2319600100083 and areal density of about 40 microg/cm2, evaporated on2319600100084 30-microm thick Al backing; the entrance and exit 2319600100085 windows had a thickness of 40 microm. The chambers were2319600100086 operated with a continuous flow of a mixture of Ar(90%)2319600100087 and methane (10%) at atmospheric pressure. 2319600100088 METHOD (TRN,TOF) 2319600100089 Discrimination level of the capture detection systems 2319600100090 at 12.5 m and 30 m corresponded to 200 keV and 150 keV 2319600100091 deposited energy. The total energy detection principle 2319600100092 in combination with the pulse height weighting 2319600100093 technique (PHWT) was applied to arrive at a detection 2319600100094 efficiency for a capture event directly proportional 2319600100095 to the total gamma-ray energy liberated in the capture 2319600100096 event. Weighting functions were calculated by Monte 2319600100097 Carlo simulations and validated by experiment ( see 2319600100098 REL-REF of A.Borella+). 2319600100099 ANALYSIS (SHAPE) Resonance shape analysis RSA. 2319600100100 Capture: 2319600100101 Normalization accounts for energy independent factors- 2319600100102 the absolute neutron flux, the efficiency of the flux 2319600100103 detector and the solid angle subtended by the target 2319600100104 and the C6D6 detectors. The normalization constant was 2319600100105 considered as a free parameter in the RSA and was 2319600100106 defined by resonances for which the parameters were 2319600100107 determined from the transmission data. 2319600100108 Resonance parameters were extracted by a simultaneous 2319600100109 least squares adjustment of the capture and 2319600100110 transmission data using REFIT, taking into account 2319600100111 the Doppler broadening, self-shielding and scattering 2319600100112 in the sample, the attenuation of gamma-rays in sample,2319600100113 the response of the TOF-spectrometer and the neutron 2319600100114 sensitivity of the capture detection system, also 2319600100115 the target characteristics - inhomogeneities, isotopic 2319600100116 composition and impurities. 2319600100117 The flight path length of the 50 m transmission station2319600100118 at GELINA (determined from the transmission dip of the 2319600100119 6.673+-0.001 eV resonance in 238U+n) was used as a 2319600100120 reference to determine the resonance energies. 2319600100121 Resonance parameters files are the result of a combined2319600100122 analysis of available experimental data together with a2319600100123 RSA of transmission and capture data on nat-Cd at 2319600100124 GELINA. 2319600100125 ERR-ANALYS (ERR-1,,0.5) Uncertainty of normalization. 2319600100126 CORRECTION For backgrounds in transmission: 2319600100127 -contribution due to the 2.2 MeV gamma-ray resulting 2319600100128 from neutron capture in hydrogen dominates the 2319600100129 background for t < 100 micros at 25 m and 50 m flight 2319600100130 path lengths. 2319600100131 -due to neutrons scattered inside the detector station 2319600100132 and due to neutrons scattered at other flight paths. 2319600100133 The background level was continuously monitored by 2319600100134 performing all measurements with at least one fixed 2319600100135 black resonance filter in the beam. 2319600100136 For dead-time effects- for neutron energies below 2319600100137 500 eV was < 2% in transmission. 2319600100138 Capture: 2319600100139 - for gamma-ray attenuation in sample, in-exit window, 2319600100140 in air; 2319600100141 - maximum correction for the dead time was < 1% in flux2319600100142 measurement (dead time was 3500 ns); the dead time for 2319600100143 the capture measurement systems was 2800 ns; for the 2319600100144 measurements at 12.5 m and 30 m the maximum dead time 2319600100145 corrections were less than 20% and 5%, respectively. 2319600100146 Bias effects due to such dead time corrections are 2319600100147 <1.0%. 2319600100148 - for backgrounds : 2319600100149 - time independent component due to ambient radiation 2319600100150 and possible radioactivity in the sample and its 2319600100151 surroundings; estimated from measurements when the 2319600100152 accelerator was switched off; 2319600100153 - time dependent component independent of the sample; 2319600100154 deduced from measurements without a sample in the beam;2319600100155 - time dependent component depending on the sample 2319600100156 characteristics - due to neutrons and gamma-rays 2319600100157 scattered from the sample; smooth part of this 2319600100158 time-dependent background component (mainly due to 2319600100159 potential scattering in the sample) was determined from2319600100160 measurements with a 0.5-mm thick 208Pb sample. 2319600100161 ADD-RES The impact of the resonance parameter file on 2319600100162 theoretical estimates has been studied by comparing 2319600100163 F-Cd-factors using the Cd data from the present work 2319600100164 with those resulting from calculations with 2319600100165 ENDF/B-VII.0 and the IRDF-2002 file. In the 2319600100166 calculations a parallel beam was considered and the 2319600100167 effect of the scattering neglected. The F-Cd-factor was2319600100168 expressed as ratio of integral of T(E)*SIG(E)*f(E) from2319600100169 0 to E-max to integral of SIG(E)*f(E) from E-Cd to 2319600100170 E-max, where E-Cd=0.55 eV, E-max=2 MeV, 2319600100171 T(E) - exponential attenuation due to Cd-cover, 2319600100172 f(E) - neutron flux, 2319600100173 SIG(E) - capture cross-section. 2319600100174 The data are given in Table 8 of J,NIM/B,300,11,2013 2319600100175 when F-Cd based on IRDF-2002 differs by more than 1% 2319600100176 from the one based on ENDF/B-VII parameters and 2319600100177 the parameters derived in this work. 2319600100178 Nuclide IRDF-2002 ENDF/B-VII.0 This work 2319600100179 F-Cd Diff. (%) Diff. (%) 2319600100180 56-Ba-130 0.862 15.8 15.8 2319600100181 56-Ba-140 0.882 2.3 2.7 2319600100182 37-Rb-86 0.951 1.6 2.2 2319600100183 34-Se-78 0.952 2.1 2.0 2319600100184 46-Pd-107 0.958 1.8 2.0 2319600100185 54-Xe-132 0.960 1.3 1.8 2319600100186 90-Th-232 0.976 1.7 1.7 2319600100187 96-Cm-242 0.972 1.4 1.6 2319600100188 27-Co-58 1.504 <1 -1.5 2319600100189 58-Ce-144 0.972 1.1 1.2 2319600100190 58-Ce-136 0.937 <1 -1.1 2319600100191 91-Pa-231 1.425 1.0 1.1 2319600100192 63-Eu-151 1.798 <1 1.1 2319600100193 To study the effect of the resonance parameters 2319600100194 obtained in this work on the interpretation of the 2319600100195 integral experiments reported by R.C.Lloyd+, the 2319600100196 exercise performed by S.Kopecky+ was repeated. The 2319600100197 results are given in Table 9 of J,NIM/B,300,11,2013. 2319600100198 COMMENT Of compiler. Question was sent to author: 2319600100199 what values of 2319600100200 -EN-RES-MIN,-MAX for average res.parameters 2319600100201 ( Subents 010-017), 2319600100202 - EN-MIN,-MAX for radius (Subents 018-025) 2319600100203 for Cd isotopes did you use ? 2319600100204 Reply : 2319600100205 " We are only dealing with the resolved resonance 2319600100206 region. However, the parameters obtained are fully 2319600100207 related to the effective scattering radii that were 2319600100208 used and given in table 3 of the paper". 2319600100209 EN-RES-MAX values were taken from ENDF/B-VII.1 RRR; 2319600100210 URR in ENDF/B-VII.1 max.energy is 100.keV . 2319600100211 EN-MAX in Subents 018-025 was taken as maximal energy 2319600100212 limit presented on figures of the article - 10 keV. 2319600100213 HISTORY (20130628C) M.M. 2319600100214 Entry was sent 30.07.2013 to author P.Schillebeeckx to 2319600100215 approve. 2319600100216 ENDBIB 214 0 2319600100217 NOCOMMON 0 0 2319600100218 ENDSUBENT 217 0 2319600199999 SUBENT 23196002 20130628 22352319600200001 BIB 4 8 2319600200002 REACTION 1(48-CD-106(N,TOT),,SIG,,,EVAL) 2319600200003 2(48-CD-106(N,G)48-CD-107,,SIG,,,EVAL) 2319600200004 ANALYSIS The nuclear cross sections (at 0 K i.e. without Doppler2319600200005 broadening) are calculated at 2200 m/s using the 2319600200006 resonance parameters obtained in this work. 2319600200007 ERR-ANALYS No errors given. 2319600200008 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319600200009 (DEP,23196026) Res.parameters. 2319600200010 ENDBIB 8 0 2319600200011 NOCOMMON 0 0 2319600200012 DATA 3 1 2319600200013 EN DATA 1DATA 2 2319600200014 EV B B 2319600200015 0.0253 5.527 0.986 2319600200016 ENDDATA 3 0 2319600200017 ENDSUBENT 16 0 2319600299999 SUBENT 23196003 20130628 22352319600300001 BIB 4 8 2319600300002 REACTION 1(48-CD-108(N,TOT),,SIG,,,EVAL) 2319600300003 2(48-CD-108(N,G)48-CD-109,,SIG,,,EVAL) 2319600300004 ANALYSIS The nuclear cross sections (at 0 K i.e. without Doppler2319600300005 broadening) are calculated at 2200 m/s using the 2319600300006 resonance parameters obtained in this work. 2319600300007 ERR-ANALYS No errors given. 2319600300008 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319600300009 (DEP,23196027) Res.parameters. 2319600300010 ENDBIB 8 0 2319600300011 NOCOMMON 0 0 2319600300012 DATA 3 1 2319600300013 EN DATA 1DATA 2 2319600300014 EV B B 2319600300015 0.0253 4.236 0.906 2319600300016 ENDDATA 3 0 2319600300017 ENDSUBENT 16 0 2319600399999 SUBENT 23196004 20130628 22352319600400001 BIB 4 8 2319600400002 REACTION 1(48-CD-110(N,TOT),,SIG,,,EVAL) 2319600400003 2(48-CD-110(N,G)48-CD-111,,SIG,,,EVAL) 2319600400004 ANALYSIS The nuclear cross sections (at 0 K i.e. without Doppler2319600400005 broadening) are calculated at 2200 m/s using the 2319600400006 resonance parameters obtained in this work. 2319600400007 ERR-ANALYS No errors given. 2319600400008 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319600400009 (DEP,23196028) Res.parameters. 2319600400010 ENDBIB 8 0 2319600400011 NOCOMMON 0 0 2319600400012 DATA 3 1 2319600400013 EN DATA 1DATA 2 2319600400014 EV B B 2319600400015 0.0253 15.233 10.999 2319600400016 ENDDATA 3 0 2319600400017 ENDSUBENT 16 0 2319600499999 SUBENT 23196005 20130628 22352319600500001 BIB 4 8 2319600500002 REACTION 1(48-CD-111(N,TOT),,SIG,,,EVAL) 2319600500003 2(48-CD-111(N,G)48-CD-112,,SIG,,,EVAL) 2319600500004 ANALYSIS The nuclear cross sections (at 0 K i.e. without Doppler2319600500005 broadening) are calculated at 2200 m/s using the 2319600500006 resonance parameters obtained in this work. 2319600500007 ERR-ANALYS No errors given. 2319600500008 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319600500009 (DEP,23196029) Res.parameters. 2319600500010 ENDBIB 8 0 2319600500011 NOCOMMON 0 0 2319600500012 DATA 3 1 2319600500013 EN DATA 1DATA 2 2319600500014 EV B B 2319600500015 0.0253 12.457 6.870 2319600500016 ENDDATA 3 0 2319600500017 ENDSUBENT 16 0 2319600599999 SUBENT 23196006 20130628 22352319600600001 BIB 4 8 2319600600002 REACTION 1(48-CD-112(N,TOT),,SIG,,,EVAL) 2319600600003 2(48-CD-112(N,G)48-CD-113,,SIG,,,EVAL) 2319600600004 ANALYSIS The nuclear cross sections (at 0 K i.e. without Doppler2319600600005 broadening) are calculated at 2200 m/s using the 2319600600006 resonance parameters obtained in this work. 2319600600007 ERR-ANALYS No errors given. 2319600600008 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319600600009 (DEP,23196030) Res.parameters. 2319600600010 ENDBIB 8 0 2319600600011 NOCOMMON 0 0 2319600600012 DATA 3 1 2319600600013 EN DATA 1DATA 2 2319600600014 EV B B 2319600600015 0.0253 7.273 2.198 2319600600016 ENDDATA 3 0 2319600600017 ENDSUBENT 16 0 2319600699999 SUBENT 23196007 20130628 22352319600700001 BIB 4 8 2319600700002 REACTION 1(48-CD-113(N,TOT),,SIG,,,EVAL) 2319600700003 2(48-CD-113(N,G)48-CD-114,,SIG,,,EVAL) 2319600700004 ANALYSIS The nuclear cross sections (at 0 K i.e. without Doppler2319600700005 broadening) are calculated at 2200 m/s using the 2319600700006 resonance parameters obtained in this work. 2319600700007 ERR-ANALYS No errors given. 2319600700008 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319600700009 (DEP,23196031) Res.parameters. 2319600700010 ENDBIB 8 0 2319600700011 NOCOMMON 0 0 2319600700012 DATA 3 1 2319600700013 EN DATA 1DATA 2 2319600700014 EV B B 2319600700015 0.0253 20185.203 20163.670 2319600700016 ENDDATA 3 0 2319600700017 ENDSUBENT 16 0 2319600799999 SUBENT 23196008 20130628 22352319600800001 BIB 4 8 2319600800002 REACTION 1(48-CD-114(N,TOT),,SIG,,,EVAL) 2319600800003 2(48-CD-114(N,G)48-CD-115,,SIG,,,EVAL) 2319600800004 ANALYSIS The nuclear cross sections (at 0 K i.e. without Doppler2319600800005 broadening) are calculated at 2200 m/s using the 2319600800006 resonance parameters obtained in this work. 2319600800007 ERR-ANALYS No errors given. 2319600800008 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319600800009 (DEP,23196032) Res.parameters. 2319600800010 ENDBIB 8 0 2319600800011 NOCOMMON 0 0 2319600800012 DATA 3 1 2319600800013 EN DATA 1DATA 2 2319600800014 EV B B 2319600800015 0.0253 5.991 0.305 2319600800016 ENDDATA 3 0 2319600800017 ENDSUBENT 16 0 2319600899999 SUBENT 23196009 20130628 22352319600900001 BIB 4 8 2319600900002 REACTION 1(48-CD-116(N,TOT),,SIG,,,EVAL) 2319600900003 2(48-CD-116(N,G)48-CD-117,,SIG,,,EVAL) 2319600900004 ANALYSIS The nuclear cross sections (at 0 K i.e. without Doppler2319600900005 broadening) are calculated at 2200 m/s using the 2319600900006 resonance parameters obtained in this work. 2319600900007 ERR-ANALYS No errors given. 2319600900008 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319600900009 (DEP,23196033) Res.parameters. 2319600900010 ENDBIB 8 0 2319600900011 NOCOMMON 0 0 2319600900012 DATA 3 1 2319600900013 EN DATA 1DATA 2 2319600900014 EV B B 2319600900015 0.0253 5.019 0.076 2319600900016 ENDDATA 3 0 2319600900017 ENDSUBENT 16 0 2319600999999 SUBENT 23196010 20130628 22352319601000001 BIB 5 17 2319601000002 REACTION 1(48-CD-106(N,G),,WID,,AV,EVAL) 2319601000003 Average gamma width. 2319601000004 2(48-CD-106(N,EL),,WID/RED,,AV,EVAL) 2319601000005 Upper limit of p-wave reduced neutron width. 2319601000006 ANALYSIS Deduced from RSA. 2319601000007 The average radiation widths are mainly based on the 2319601000008 analysis of GELINA data and the results of 2319601000009 A.R. de L. Musgrove et al. 2319601000010 REL-REF (R,30453001,A.R.de L Musgrove+,J,JP/G,4,(5),771,1978) 2319601000011 ERR-ANALYS No errors given. 2319601000012 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319601000013 (DEP,23196002) Thermal c-s. 2319601000014 (DEP,23196018) Radius. 2319601000015 The parameters obtained are fully related to the 2319601000016 effective scattering radii that were used and given in 2319601000017 table 3 of the paper" (comment of P.Schillebeeckx). 2319601000018 RSA is explained in Subent 001, ANALYSIS . 2319601000019 ENDBIB 17 0 2319601000020 COMMON 1 3 2319601000021 EN-RES-MAX 2319601000022 KEV 2319601000023 6. 2319601000024 ENDCOMMON 3 0 2319601000025 DATA 3 2 2319601000026 MOMENTUM L DATA 1DATA-MAX 2 2319601000027 NO-DIM MILLI-EV MILLI-EV 2319601000028 0. 150.0 2319601000029 1. 172.5 190. 2319601000030 ENDDATA 4 0 2319601000031 ENDSUBENT 30 0 2319601099999 SUBENT 23196011 20130628 22352319601100001 BIB 5 17 2319601100002 REACTION 1(48-CD-108(N,G),,WID,,AV,EVAL) 2319601100003 Average gamma width. 2319601100004 2(48-CD-108(N,EL),,WID/RED,,AV,EVAL) 2319601100005 Upper limit of p-wave reduced neutron width. 2319601100006 ANALYSIS Deduced from RSA. 2319601100007 The average radiation widths are mainly based on the 2319601100008 analysis of GELINA data and the results of 2319601100009 A.R. de L. Musgrove et al. 2319601100010 REL-REF (R,30453001,A.R.de L Musgrove+,J,JP/G,4,(5),771,1978) 2319601100011 ERR-ANALYS No errors given. 2319601100012 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319601100013 (DEP,23196003) Thermal c-s. 2319601100014 (DEP,23196019) Radius. 2319601100015 The parameters obtained are fully related to the 2319601100016 effective scattering radii that were used and given in 2319601100017 table 3 of the paper" (comment of P.Schillebeeckx). 2319601100018 RSA is explained in Subent 001, ANALYSIS . 2319601100019 ENDBIB 17 0 2319601100020 COMMON 1 3 2319601100021 EN-RES-MAX 2319601100022 KEV 2319601100023 6. 2319601100024 ENDCOMMON 3 0 2319601100025 DATA 3 2 2319601100026 MOMENTUM L DATA 1DATA-MAX 2 2319601100027 NO-DIM MILLI-EV MILLI-EV 2319601100028 0. 103.0 2319601100029 1. 123.0 640. 2319601100030 ENDDATA 4 0 2319601100031 ENDSUBENT 30 0 2319601199999 SUBENT 23196012 20130628 22352319601200001 BIB 5 17 2319601200002 REACTION 1(48-CD-110(N,G),,WID,,AV,EVAL) 2319601200003 Average gamma width. 2319601200004 2(48-CD-110(N,EL),,WID/RED,,AV,EVAL) 2319601200005 Upper limit of p-wave reduced neutron width. 2319601200006 ANALYSIS Deduced from RSA. 2319601200007 The average radiation widths are mainly based on the 2319601200008 analysis of GELINA data and the results of 2319601200009 A.R. de L. Musgrove et al. 2319601200010 REL-REF (R,30453001,A.R.de L Musgrove+,J,JP/G,4,(5),771,1978) 2319601200011 ERR-ANALYS No errors given. 2319601200012 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319601200013 (DEP,23196004) Thermal c-s. 2319601200014 (DEP,23196020) Radius. 2319601200015 The parameters obtained are fully related to the 2319601200016 effective scattering radii that were used and given in 2319601200017 table 3 of the paper" (comment of P.Schillebeeckx). 2319601200018 RSA is explained in Subent 001, ANALYSIS . 2319601200019 ENDBIB 17 0 2319601200020 COMMON 1 3 2319601200021 EN-RES-MAX 2319601200022 KEV 2319601200023 7. 2319601200024 ENDCOMMON 3 0 2319601200025 DATA 3 2 2319601200026 MOMENTUM L DATA 1DATA-MAX 2 2319601200027 NO-DIM MILLI-EV MILLI-EV 2319601200028 0. 70.0 2319601200029 1. 79.0 300. 2319601200030 ENDDATA 4 0 2319601200031 ENDSUBENT 30 0 2319601299999 SUBENT 23196013 20130628 22352319601300001 BIB 4 13 2319601300002 REACTION 1(48-CD-111(N,G),,WID,,AV,EVAL) 2319601300003 Average gamma width. 2319601300004 2(48-CD-111(N,EL),,WID/RED,,AV,EVAL) 2319601300005 Upper limit of p-wave reduced neutron width. 2319601300006 ANALYSIS Deduced from RSA. 2319601300007 ERR-ANALYS No errors given. 2319601300008 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319601300009 (DEP,23196005) Thermal c-s. 2319601300010 (DEP,23196021) Radius. 2319601300011 The parameters obtained are fully related to the 2319601300012 effective scattering radii that were used and given in 2319601300013 table 3 of the paper" (comment of P.Schillebeeckx). 2319601300014 RSA is explained in Subent 001, ANALYSIS . 2319601300015 ENDBIB 13 0 2319601300016 COMMON 1 3 2319601300017 EN-RES-MAX 2319601300018 KEV 2319601300019 2.3 2319601300020 ENDCOMMON 3 0 2319601300021 DATA 3 2 2319601300022 MOMENTUM L DATA 1DATA-MAX 2 2319601300023 NO-DIM MILLI-EV MILLI-EV 2319601300024 0. 130.0 2319601300025 1. 165.0 56. 2319601300026 ENDDATA 4 0 2319601300027 ENDSUBENT 26 0 2319601399999 SUBENT 23196014 20130628 22352319601400001 BIB 5 17 2319601400002 REACTION 1(48-CD-112(N,G),,WID,,AV,EVAL) 2319601400003 Average gamma width. 2319601400004 2(48-CD-112(N,EL),,WID/RED,,AV,EVAL) 2319601400005 Upper limit of p-wave reduced neutron width. 2319601400006 ANALYSIS Deduced from RSA. 2319601400007 The average radiation widths are mainly based on the 2319601400008 analysis of GELINA data and the results of 2319601400009 A.R. de L. Musgrove et al. 2319601400010 REL-REF (R,30453001,A.R.de L Musgrove+,J,JP/G,4,(5),771,1978) 2319601400011 ERR-ANALYS No errors given. 2319601400012 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319601400013 (DEP,23196006) Thermal c-s. 2319601400014 (DEP,23196022) Radius. 2319601400015 The parameters obtained are fully related to the 2319601400016 effective scattering radii that were used and given in 2319601400017 table 3 of the paper" (comment of P.Schillebeeckx). 2319601400018 RSA is explained in Subent 001, ANALYSIS . 2319601400019 ENDBIB 17 0 2319601400020 COMMON 1 3 2319601400021 EN-RES-MAX 2319601400022 KEV 2319601400023 11.5 2319601400024 ENDCOMMON 3 0 2319601400025 DATA 3 2 2319601400026 MOMENTUM L DATA 1DATA-MAX 2 2319601400027 NO-DIM MILLI-EV MILLI-EV 2319601400028 0. 77.5 2319601400029 1. 90.5 280. 2319601400030 ENDDATA 4 0 2319601400031 ENDSUBENT 30 0 2319601499999 SUBENT 23196015 20130628 22352319601500001 BIB 4 13 2319601500002 REACTION 1(48-CD-113(N,G),,WID,,AV,EVAL) 2319601500003 Average gamma width. 2319601500004 2(48-CD-113(N,EL),,WID/RED,,AV,EVAL) 2319601500005 Upper limit of p-wave reduced neutron width. 2319601500006 ANALYSIS Deduced from RSA. 2319601500007 ERR-ANALYS No errors given. 2319601500008 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319601500009 (DEP,23196007) Thermal c-s. 2319601500010 (DEP,23196023) Radius. 2319601500011 The parameters obtained are fully related to the 2319601500012 effective scattering radii that were used and given in 2319601500013 table 3 of the paper" (comment of P.Schillebeeckx). 2319601500014 RSA is explained in Subent 001, ANALYSIS . 2319601500015 ENDBIB 13 0 2319601500016 COMMON 1 3 2319601500017 EN-RES-MAX 2319601500018 KEV 2319601500019 5. 2319601500020 ENDCOMMON 3 0 2319601500021 DATA 3 2 2319601500022 MOMENTUM L DATA 1DATA-MAX 2 2319601500023 NO-DIM MILLI-EV MILLI-EV 2319601500024 0. 113.5 2319601500025 1. 145.0 47. 2319601500026 ENDDATA 4 0 2319601500027 ENDSUBENT 26 0 2319601599999 SUBENT 23196016 20130628 22352319601600001 BIB 5 17 2319601600002 REACTION 1(48-CD-114(N,G),,WID,,AV,EVAL) 2319601600003 Average gamma width. 2319601600004 2(48-CD-114(N,EL),,WID/RED,,AV,EVAL) 2319601600005 Upper limit of p-wave reduced neutron width. 2319601600006 ANALYSIS Deduced from RSA. 2319601600007 The average radiation widths are mainly based on the 2319601600008 analysis of GELINA data and the results of 2319601600009 A.R. de L. Musgrove et al. 2319601600010 REL-REF (R,30453001,A.R.de L Musgrove+,J,JP/G,4,(5),771,1978) 2319601600011 ERR-ANALYS No errors given. 2319601600012 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319601600013 (DEP,23196008) Thermal c-s. 2319601600014 (DEP,23196024) Radius. 2319601600015 The parameters obtained are fully related to the 2319601600016 effective scattering radii that were used and given in 2319601600017 table 3 of the paper" (comment of P.Schillebeeckx). 2319601600018 RSA is explained in Subent 001, ANALYSIS . 2319601600019 ENDBIB 17 0 2319601600020 COMMON 1 3 2319601600021 EN-RES-MAX 2319601600022 KEV 2319601600023 8. 2319601600024 ENDCOMMON 3 0 2319601600025 DATA 3 2 2319601600026 MOMENTUM L DATA 1DATA-MAX 2 2319601600027 NO-DIM MILLI-EV MILLI-EV 2319601600028 0. 54.0 2319601600029 1. 71.5 430. 2319601600030 ENDDATA 4 0 2319601600031 ENDSUBENT 30 0 2319601699999 SUBENT 23196017 20130628 22352319601700001 BIB 5 17 2319601700002 REACTION 1(48-CD-116(N,G),,WID,,AV,EVAL) 2319601700003 Average gamma width. 2319601700004 2(48-CD-116(N,EL),,WID/RED,,AV,EVAL) 2319601700005 Upper limit of p-wave reduced neutron width. 2319601700006 ANALYSIS Deduced from RSA. 2319601700007 The average radiation widths are mainly based on the 2319601700008 analysis of GELINA data and the results of 2319601700009 A.R. de L. Musgrove et al. 2319601700010 REL-REF (R,30453001,A.R.de L Musgrove+,J,JP/G,4,(5),771,1978) 2319601700011 ERR-ANALYS No errors given. 2319601700012 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319601700013 (DEP,23196009) Thermal c-s. 2319601700014 (DEP,23196025) Radius. 2319601700015 The parameters obtained are fully related to the 2319601700016 effective scattering radii that were used and given in 2319601700017 table 3 of the paper" (comment of P.Schillebeeckx). 2319601700018 RSA is explained in Subent 001, ANALYSIS . 2319601700019 ENDBIB 17 0 2319601700020 COMMON 1 3 2319601700021 EN-RES-MAX 2319601700022 KEV 2319601700023 9.5 2319601700024 ENDCOMMON 3 0 2319601700025 DATA 3 2 2319601700026 MOMENTUM L DATA 1DATA-MAX 2 2319601700027 NO-DIM MILLI-EV MILLI-EV 2319601700028 0. 47.2 2319601700029 1. 70.0 560. 2319601700030 ENDDATA 4 0 2319601700031 ENDSUBENT 30 0 2319601799999 SUBENT 23196018 20130628 22352319601800001 BIB 4 4 2319601800002 REACTION (48-CD-106(N,EL)48-CD-106,,RAD,,,EVAL) 2319601800003 ANALYSIS Effective scattering radius deduced from RSA. 2319601800004 ERR-ANALYS No errors given. 2319601800005 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319601800006 ENDBIB 4 0 2319601800007 NOCOMMON 0 0 2319601800008 DATA 2 1 2319601800009 EN-MAX DATA 2319601800010 KEV FERMI 2319601800011 10. 6.0 2319601800012 ENDDATA 3 0 2319601800013 ENDSUBENT 12 0 2319601899999 SUBENT 23196019 20130628 22352319601900001 BIB 4 4 2319601900002 REACTION (48-CD-108(N,EL)48-CD-108,,RAD,,,EVAL) 2319601900003 ANALYSIS Effective scattering radius deduced from RSA. 2319601900004 ERR-ANALYS No errors given. 2319601900005 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319601900006 ENDBIB 4 0 2319601900007 NOCOMMON 0 0 2319601900008 DATA 2 1 2319601900009 EN-MAX DATA 2319601900010 KEV FERMI 2319601900011 10. 5.79 2319601900012 ENDDATA 3 0 2319601900013 ENDSUBENT 12 0 2319601999999 SUBENT 23196020 20130628 22352319602000001 BIB 4 4 2319602000002 REACTION (48-CD-110(N,EL)48-CD-110,,RAD,,,EVAL) 2319602000003 ANALYSIS Effective scattering radius deduced from RSA. 2319602000004 ERR-ANALYS No errors given. 2319602000005 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319602000006 ENDBIB 4 0 2319602000007 NOCOMMON 0 0 2319602000008 DATA 2 1 2319602000009 EN-MAX DATA 2319602000010 KEV FERMI 2319602000011 10. 5.80 2319602000012 ENDDATA 3 0 2319602000013 ENDSUBENT 12 0 2319602099999 SUBENT 23196021 20130628 22352319602100001 BIB 4 4 2319602100002 REACTION (48-CD-111(N,EL)48-CD-111,,RAD,,,EVAL) 2319602100003 ANALYSIS Effective scattering radius deduced from RSA. 2319602100004 ERR-ANALYS No errors given. 2319602100005 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319602100006 ENDBIB 4 0 2319602100007 NOCOMMON 0 0 2319602100008 DATA 2 1 2319602100009 EN-MAX DATA 2319602100010 KEV FERMI 2319602100011 10. 6.15 2319602100012 ENDDATA 3 0 2319602100013 ENDSUBENT 12 0 2319602199999 SUBENT 23196022 20130628 22352319602200001 BIB 4 4 2319602200002 REACTION (48-CD-112(N,EL)48-CD-112,,RAD,,,EVAL) 2319602200003 ANALYSIS Effective scattering radius deduced from RSA. 2319602200004 ERR-ANALYS No errors given. 2319602200005 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319602200006 ENDBIB 4 0 2319602200007 NOCOMMON 0 0 2319602200008 DATA 2 1 2319602200009 EN-MAX DATA 2319602200010 KEV FERMI 2319602200011 10. 6.6 2319602200012 ENDDATA 3 0 2319602200013 ENDSUBENT 12 0 2319602299999 SUBENT 23196023 20130628 22352319602300001 BIB 4 4 2319602300002 REACTION (48-CD-113(N,EL)48-CD-113,,RAD,,,EVAL) 2319602300003 ANALYSIS Effective scattering radius deduced from RSA. 2319602300004 ERR-ANALYS No errors given. 2319602300005 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319602300006 ENDBIB 4 0 2319602300007 NOCOMMON 0 0 2319602300008 DATA 2 1 2319602300009 EN-MAX DATA 2319602300010 KEV FERMI 2319602300011 10. 6.5 2319602300012 ENDDATA 3 0 2319602300013 ENDSUBENT 12 0 2319602399999 SUBENT 23196024 20130628 22352319602400001 BIB 4 4 2319602400002 REACTION (48-CD-114(N,EL)48-CD-114,,RAD,,,EVAL) 2319602400003 ANALYSIS Effective scattering radius deduced from RSA. 2319602400004 ERR-ANALYS No errors given. 2319602400005 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319602400006 ENDBIB 4 0 2319602400007 NOCOMMON 0 0 2319602400008 DATA 2 1 2319602400009 EN-MAX DATA 2319602400010 KEV FERMI 2319602400011 10. 6.9 2319602400012 ENDDATA 3 0 2319602400013 ENDSUBENT 12 0 2319602499999 SUBENT 23196025 20130628 22352319602500001 BIB 4 5 2319602500002 REACTION (48-CD-116(N,EL)48-CD-116,,RAD,,,EVAL) 2319602500003 ANALYSIS Effective scattering radius deduced from RSA for energy2319602500004 region covered in transmission data. 2319602500005 ERR-ANALYS No errors given. 2319602500006 STATUS (TABLE) Table 3 of J,NIM/B,300,11,2013. 2319602500007 ENDBIB 5 0 2319602500008 NOCOMMON 0 0 2319602500009 DATA 2 1 2319602500010 EN-MAX DATA 2319602500011 KEV FERMI 2319602500012 10. 6.24 2319602500013 ENDDATA 3 0 2319602500014 ENDSUBENT 13 0 2319602599999 SUBENT 23196026 20130628 22352319602600001 BIB 5 17 2319602600002 REACTION 1(48-CD-106(N,0),,EN) 2319602600003 2(48-CD-106(N,EL),,WID,,G) g*Gn 2319602600004 3(48-CD-106(N,G),,WID) G-gamma 2319602600005 4(48-CD-106(N,0),,J) Spin J 2319602600006 5(48-CD-106(N,0),,PTY) Parity 2319602600007 ANALYSIS Resonance energy and g*Gn have been determined from 2319602600008 the GELINA data. The radiation width was deduced and a 2319602600009 spin assignment was made based on a simultaneous 2319602600010 analysis of thin-thick transmission and/or capture 2319602600011 data. 2319602600012 REL-REF (R,,G.Audi+,J,NP/A,729,337,2003) 2319602600013 Neutron separation energy 7924.0+-8.0 keV and 2319602600014 atomic mass 105.906461 u from this REL-REF were used in2319602600015 analysis. 2319602600016 ERR-ANALYS (ERR-S) Uncorrelated component due to counting 2319602600017 statistics. 2319602600018 STATUS (TABLE) Table 4 of J,NIM/B,300,11,2013. 2319602600019 ENDBIB 17 0 2319602600020 NOCOMMON 0 0 2319602600021 DATA 8 2 2319602600022 DATA 1ERR-S 1DATA 2ERR-S 2DATA 3ERR-S 32319602600023 DATA 4DATA 5 2319602600024 EV EV MILLI-EV MILLI-EV MILLI-EV MILLI-EV 2319602600025 NO-DIM NO-DIM 2319602600026 456.657 0.017 102.0 5.1 2319602600027 2319602600028 635.087 0.014 794.0 15.0 110.0 5.0 2319602600029 0.5 +1. 2319602600030 ENDDATA 8 0 2319602600031 ENDSUBENT 30 0 2319602699999 SUBENT 23196027 20130628 22352319602700001 BIB 5 14 2319602700002 REACTION 1(48-CD-108(N,0),,EN) 2319602700003 2(48-CD-108(N,EL),,WID,,G) g*Gn 2319602700004 ANALYSIS Resonance energy and g*Gn have been determined from 2319602700005 the GELINA data. The radiation width was deduced and a 2319602700006 spin assignment was made based on a simultaneous 2319602700007 analysis of thin-thick transmission and/or capture 2319602700008 data. 2319602700009 REL-REF (R,,G.Audi+,J,NP/A,729,337,2003) 2319602700010 Neutron separation energy 7327.0+-6.0 keV and 2319602700011 atomic mass 107.904176 u from this REL-REF were used in2319602700012 analysis. 2319602700013 ERR-ANALYS (ERR-S) Uncorrelated component due to counting 2319602700014 statistics. 2319602700015 STATUS (TABLE) Table 4 of J,NIM/B,300,11,2013. 2319602700016 ENDBIB 14 0 2319602700017 NOCOMMON 0 0 2319602700018 DATA 4 2 2319602700019 DATA 1ERR-S 1DATA 2ERR-S 2 2319602700020 EV EV MILLI-EV MILLI-EV 2319602700021 233.704 0.010 349.0 6.0 2319602700022 311.653 0.007 539.0 7.0 2319602700023 ENDDATA 4 0 2319602700024 ENDSUBENT 23 0 2319602799999 SUBENT 23196028 20130628 22352319602800001 BIB 5 17 2319602800002 REACTION 1(48-CD-110(N,0),,EN) 2319602800003 2(48-CD-110(N,EL),,WID,,G) g*Gn 2319602800004 3(48-CD-110(N,G),,WID) G-gamma 2319602800005 4(48-CD-110(N,0),,J) Spin J 2319602800006 5(48-CD-110(N,0),,PTY) Parity 2319602800007 ANALYSIS Resonance energy and g*Gn have been determined from 2319602800008 the GELINA data. The radiation width was deduced and a 2319602800009 spin assignment was made based on a simultaneous 2319602800010 analysis of thin-thick transmission and/or capture 2319602800011 data. 2319602800012 REL-REF (R,,G.Audi+,J,NP/A,729,337,2003) 2319602800013 Neutron separation energy 6975.85+-0.19 keV and 2319602800014 atomic mass 109.903005 u from this REL-REF were used in2319602800015 analysis. 2319602800016 ERR-ANALYS (ERR-S) Uncorrelated component due to counting 2319602800017 statistics. 2319602800018 STATUS (TABLE) Table 4 of J,NIM/B,300,11,2013. 2319602800019 ENDBIB 17 0 2319602800020 NOCOMMON 0 0 2319602800021 DATA 8 15 2319602800022 DATA 1ERR-S 1DATA 2ERR-S 2DATA 3ERR-S 32319602800023 DATA 4DATA 5 2319602800024 EV EV MILLI-EV MILLI-EV MILLI-EV MILLI-EV 2319602800025 NO-DIM NO-DIM 2319602800026 89.549 0.001 162.7 0.4 73.2 0.5 2319602800027 0.5 +1. 2319602800028 231.026 0.006 6.7 0.1 2319602800029 2319602800030 369.684 0.005 19.60 0.21 89.0 1.5 2319602800031 0.5 +1. 2319602800032 800.145 0.007 452.0 4.6 69.0 1.0 2319602800033 0.5 +1. 2319602800034 824.575 0.300 2.89 0.28 2319602800035 2319602800036 917.598 0.018 17.08 0.34 2319602800037 2319602800038 921.180 0.011 66.8 1.5 83.0 6.0 2319602800039 0.5 +1. 2319602800040 1117.852 0.415 39.1 4.3 2319602800041 2319602800042 1347.109 0.013 962. 11. 2319602800043 0.5 +1. 2319602800044 1828.557 0.020 342.2 7.2 2319602800045 2319602800046 2067.150 0.023 1877. 26. 82.8 2.5 2319602800047 0.5 +1. 2319602800048 2377.926 0.031 1896. 34. 2319602800049 2319602800050 3956.386 0.062 1281. 48. 2319602800051 2319602800052 5987.225 0.154 1144. 68. 2319602800053 2319602800054 8832.493 0.211 3518. 121. 2319602800055 0.5 +1. 2319602800056 ENDDATA 34 0 2319602800057 ENDSUBENT 56 0 2319602899999 SUBENT 23196029 20130628 22352319602900001 BIB 5 17 2319602900002 REACTION 1(48-CD-111(N,0),,EN) 2319602900003 2(48-CD-111(N,EL),,WID,,G) g*Gn 2319602900004 3(48-CD-111(N,G),,WID) G-gamma 2319602900005 4(48-CD-111(N,0),,J) Spin J 2319602900006 5(48-CD-111(N,0),,PTY) Parity 2319602900007 ANALYSIS Resonance energy and g*Gn have been determined from 2319602900008 the GELINA data. The radiation width was deduced and a 2319602900009 spin assignment was made based on a simultaneous 2319602900010 analysis of thin-thick transmission and/or capture 2319602900011 data. 2319602900012 REL-REF (R,,G.Audi+,J,NP/A,729,337,2003) 2319602900013 Neutron separation energy 9394.32+-0.30 keV and 2319602900014 atomic mass 110.904182 u from this REL-REF were used in2319602900015 analysis. 2319602900016 ERR-ANALYS (ERR-S) Uncorrelated component due to counting 2319602900017 statistics. 2319602900018 STATUS (TABLE) Table 4 of J,NIM/B,300,11,2013. 2319602900019 ENDBIB 17 0 2319602900020 NOCOMMON 0 0 2319602900021 DATA 8 43 2319602900022 DATA 1ERR-S 1DATA 2ERR-S 2DATA 3ERR-S 32319602900023 DATA 4DATA 5 2319602900024 EV EV MILLI-EV MILLI-EV MILLI-EV MILLI-EV 2319602900025 NO-DIM NO-DIM 2319602900026 27.57000 0.00064 3.684 0.017 131.1 3.0 2319602900027 1. +1. 2319602900028 69.590 0.022 0.132 0.010 2319602900029 2319602900030 86.1850 0.0036 2.516 0.033 130.1 9.0 2319602900031 1. +1. 2319602900032 99.4910 0.0024 10.930 0.090 129.6 5.0 2319602900033 1. +1. 2319602900034 138.1660 0.0022 7.125 0.046 2319602900035 2319602900036 164.2450 0.0015 51.44 0.36 127.0 4.0 2319602900037 1. +1. 2319602900038 225.1460 0.0028 24.08 0.19 130.5 8.0 2319602900039 1. +1. 2319602900040 233.4660 0.0028 38.48 0.35 2319602900041 2319602900042 275.6938 0.0039 15.32 0.13 2319602900043 2319602900044 332.085 0.041 5.81 0.38 176. 20. 2319602900045 0. +1. 2319602900046 356.2102 0.0036 36.12 0.32 2319602900047 2319602900048 389.1695 0.0062 19.91 0.23 2319602900049 2319602900050 422.94 0.71 0.70 0.26 2319602900051 2319602900052 478.217 0.022 3.88 0.20 2319602900053 2319602900054 483.071 0.072 1.28 0.10 2319602900055 2319602900056 484.931 0.034 2.33 0.11 2319602900057 2319602900058 540.460 0.025 18.51 0.60 2319602900059 2319602900060 576.184 0.017 35.87 0.83 2319602900061 2319602900062 603.834 0.010 25.88 0.35 2319602900063 2319602900064 622.773 0.021 35.90 0.98 2319602900065 2319602900066 706.68 0.24 3.22 0.73 2319602900067 2319602900068 790.917 0.032 40.3 1.4 2319602900069 2319602900070 809.768 0.028 41.4 1.4 2319602900071 2319602900072 861.311 0.094 14.9 1.2 2319602900073 2319602900074 878.714 0.037 31.1 1.3 2319602900075 2319602900076 882.543 0.040 6.42 0.26 2319602900077 2319602900078 965.786 0.047 44.0 2.1 2319602900079 2319602900080 1042.354 0.064 46.7 2.2 2319602900081 2319602900082 1048.331 0.049 15.29 0.54 2319602900083 2319602900084 1068.41 0.12 5.28 0.28 2319602900085 2319602900086 1252.819 0.042 110.8 4.2 2319602900087 2319602900088 1261.862 0.027 27.15 0.71 2319602900089 2319602900090 1308.590 0.034 23.97 0.62 2319602900091 2319602900092 1449.166 0.052 15.65 0.52 2319602900093 2319602900094 1468.679 0.040 49.4 1.3 2319602900095 2319602900096 1523.315 0.062 17.60 0.68 2319602900097 2319602900098 1565.488 0.054 21.32 0.83 2319602900099 2319602900100 1582.349 0.042 161.4 4.7 2319602900101 1. +1. 2319602900102 1597.576 0.025 61.2 1.5 2319602900103 2319602900104 1618.290 0.055 172. 17. 152.0 6.0 2319602900105 0. +1. 2319602900106 1631.895 0.040 185.0 5.3 2319602900107 1. +1. 2319602900108 1743.411 0.041 372.0 9.8 121.0 4.0 2319602900109 1. +1. 2319602900110 1766.678 0.051 15.43 0.68 2319602900111 2319602900112 ENDDATA 90 0 2319602900113 ENDSUBENT 112 0 2319602999999 SUBENT 23196030 20130628 22352319603000001 BIB 5 17 2319603000002 REACTION 1(48-CD-112(N,0),,EN) 2319603000003 2(48-CD-112(N,EL),,WID,,G) g*Gn 2319603000004 3(48-CD-112(N,G),,WID) G-gamma 2319603000005 4(48-CD-112(N,0),,J) Spin J 2319603000006 5(48-CD-112(N,0),,PTY) Parity 2319603000007 ANALYSIS Resonance energy and g*Gn have been determined from 2319603000008 the GELINA data. The radiation width was deduced and a 2319603000009 spin assignment was made based on a simultaneous 2319603000010 analysis of thin-thick transmission and/or capture 2319603000011 data. 2319603000012 REL-REF (R,,G.Audi+,J,NP/A,729,337,2003) 2319603000013 Neutron separation energy 6540.10+-0.60 keV and 2319603000014 atomic mass 111.902757 u from this REL-REF were used in2319603000015 analysis. 2319603000016 ERR-ANALYS (ERR-S) Uncorrelated component due to counting 2319603000017 statistics. 2319603000018 STATUS (TABLE) Table 4 of J,NIM/B,300,11,2013. 2319603000019 ENDBIB 17 0 2319603000020 NOCOMMON 0 0 2319603000021 DATA 8 17 2319603000022 DATA 1ERR-S 1DATA 2ERR-S 2DATA 3ERR-S 32319603000023 DATA 4DATA 5 2319603000024 EV EV MILLI-EV MILLI-EV MILLI-EV MILLI-EV 2319603000025 NO-DIM NO-DIM 2319603000026 66.7800 0.0010 8.480 0.050 62.8 1.5 2319603000027 0.5 +1. 2319603000028 226.5090 0.0030 20.57 0.17 56.0 3.0 2319603000029 0.5 +1. 2319603000030 443.1000 0.0040 61.31 0.56 61.6 2.0 2319603000031 0.5 +1. 2319603000032 565.944 0.029 2.430 0.090 2319603000033 2319603000034 737.738 0.020 353.4 2.9 67.4 1.0 2319603000035 0.5 +1. 2319603000036 884.841 0.070 11.8 2.0 2319603000037 2319603000038 895.029 0.061 5.74 0.48 2319603000039 2319603000040 909.220 0.007 277.0 3.3 68.7 1.0 2319603000041 0.5 +1. 2319603000042 1052.936 0.039 8.65 0.32 2319603000043 2319603000044 1116.124 0.010 657.0 7.5 60.6 1.1 2319603000045 0.5 +1. 2319603000046 1208.097 0.088 18.8 1.4 2319603000047 2319603000048 1640.327 0.056 22.1 1.0 2319603000049 2319603000050 2036.695 0.020 1492. 17. 2319603000051 0.5 +1. 2319603000052 2338.535 0.019 679. 13. 2319603000053 2319603000054 2574.840 0.032 1525. 25. 2319603000055 0.5 +1. 2319603000056 4561.319 0.048 1588. 66. 83.5 3.2 2319603000057 0.5 +1. 2319603000058 5578.370 0.217 857. 51. 2319603000059 2319603000060 ENDDATA 38 0 2319603000061 ENDSUBENT 60 0 2319603099999 SUBENT 23196031 20130628 22352319603100001 BIB 5 17 2319603100002 REACTION 1(48-CD-113(N,0),,EN) 2319603100003 2(48-CD-113(N,EL),,WID,,G) g*Gn 2319603100004 3(48-CD-113(N,G),,WID) G-gamma 2319603100005 4(48-CD-113(N,0),,J) Spin J 2319603100006 5(48-CD-113(N,0),,PTY) Parity 2319603100007 ANALYSIS Resonance energy and g*Gn have been determined from 2319603100008 the GELINA data. The radiation width was deduced and a 2319603100009 spin assignment was made based on a simultaneous 2319603100010 analysis of thin-thick transmission and/or capture 2319603100011 data. 2319603100012 REL-REF (R,,G.Audi+,J,NP/A,729,337,2003) 2319603100013 Neutron separation energy 9042.98+-0.14 keV and 2319603100014 atomic mass 112.904400 u from this REL-REF were used in2319603100015 analysis. 2319603100016 ERR-ANALYS (ERR-S) Uncorrelated component due to counting 2319603100017 statistics. 2319603100018 STATUS (TABLE) Table 4 of J,NIM/B,300,11,2013. 2319603100019 ENDBIB 17 0 2319603100020 NOCOMMON 0 0 2319603100021 DATA 8 28 2319603100022 DATA 1ERR-S 1DATA 2ERR-S 2DATA 3ERR-S 32319603100023 DATA 4DATA 5 2319603100024 EV EV MILLI-EV MILLI-EV MILLI-EV MILLI-EV 2319603100025 NO-DIM NO-DIM 2319603100026 0.17870 0.00010 0.4800 0.0015 113.5 0.1 2319603100027 1. +1. 2319603100028 63.7091 0.0014 2.375 0.015 2319603100029 2319603100030 84.8740 0.0092 24.59 0.11 2319603100031 2319603100032 108.3320 0.0017 8.175 0.050 123.3 4.5 2319603100033 1. +1. 2319603100034 143.0974 0.0054 2.250 0.032 2319603100035 2319603100036 158.7720 0.0029 6.068 0.052 2319603100037 2319603100038 192.8711 0.0022 47.25 0.30 112.3 1.5 2319603100039 0. +1. 2319603100040 215.2592 0.0024 19.05 0.14 129.9 5.0 2319603100041 1. +1. 2319603100042 261.1192 0.0028 23.36 0.18 144.5 6.5 2319603100043 1. +1. 2319603100044 269.3491 0.0038 15.44 0.17 120.3 7.0 2319603100045 0. +1. 2319603100046 291.6503 0.0095 4.073 0.087 2319603100047 2319603100048 414.1187 0.0036 93.15 0.90 2319603100049 1. +1. 2319603100050 432.0578 0.0062 19.29 0.24 2319603100051 2319603100052 551.9610 0.0053 80.25 0.98 111.4 2.5 2319603100053 1. +1. 2319603100054 841.849 0.011 53.49 0.97 2319603100055 1. +1. 2319603100056 851.9014 0.0075 389.3 4.4 2319603100057 1. +1. 2319603100058 901.689 0.019 13.95 0.75 2319603100059 2319603100060 911.831 0.030 17.14 0.79 2319603100061 2319603100062 965.64 0.12 16.9 1.9 2319603100063 2319603100064 1051.52 0.37 13.8 0.9 2319603100065 2319603100066 1068.475 0.055 12.26 0.51 2319603100067 2319603100068 1120.405 0.016 93.1 2.3 2319603100069 1. +1. 2319603100070 1252.136 0.023 36.98 0.83 2319603100071 1. +1. 2319603100072 1267.632 0.031 139.5 3.5 129.5 4.0 2319603100073 1. +1. 2319603100074 1318.290 0.035 77.0 4.8 2319603100075 0. +1. 2319603100076 1364.75 0.15 102.6 1.0 103.0 5.0 2319603100077 1. +1. 2319603100078 1468.20 0.11 91.0 5.5 110.8 5.0 2319603100079 1. +1. 2319603100080 1628.34 0.12 65.0 6.0 2319603100081 0. +1. 2319603100082 ENDDATA 60 0 2319603100083 ENDSUBENT 82 0 2319603199999 SUBENT 23196032 20130628 22352319603200001 BIB 5 17 2319603200002 REACTION 1(48-CD-114(N,0),,EN) 2319603200003 2(48-CD-114(N,EL),,WID,,G) g*Gn 2319603200004 3(48-CD-114(N,G),,WID) G-gamma 2319603200005 4(48-CD-114(N,0),,J) Spin J 2319603200006 5(48-CD-114(N,0),,PTY) Parity 2319603200007 ANALYSIS Resonance energy and g*Gn have been determined from 2319603200008 the GELINA data. The radiation width was deduced and a 2319603200009 spin assignment was made based on a simultaneous 2319603200010 analysis of thin-thick transmission and/or capture 2319603200011 data. 2319603200012 REL-REF (R,,G.Audi+,J,NP/A,729,337,2003) 2319603200013 Neutron separation energy 6140.9+-0.6 keV and 2319603200014 atomic mass 113.903357 u from this REL-REF were used in2319603200015 analysis. 2319603200016 ERR-ANALYS (ERR-S) Uncorrelated component due to counting 2319603200017 statistics. 2319603200018 STATUS (TABLE) Table 4 of J,NIM/B,300,11,2013. 2319603200019 ENDBIB 17 0 2319603200020 NOCOMMON 0 0 2319603200021 DATA 8 16 2319603200022 DATA 1ERR-S 1DATA 2ERR-S 2DATA 3ERR-S 32319603200023 DATA 4DATA 5 2319603200024 EV EV MILLI-EV MILLI-EV MILLI-EV MILLI-EV 2319603200025 NO-DIM NO-DIM 2319603200026 120.1300 0.0010 60.81 0.48 50.0 0.5 2319603200027 0.5 +1. 2319603200028 392.550 0.010 936.2 5.6 55.2 0.4 2319603200029 0.5 +1. 2319603200030 671.190 0.010 402.3 5.3 56.4 1.0 2319603200031 0.5 +1. 2319603200032 752.4400 0.0060 367.5 2.9 53.7 1.0 2319603200033 0.5 +1. 2319603200034 962.388 0.067 11.03 0.68 2319603200035 2319603200036 1100.2340 0.0080 302.4 3.3 50.7 0.7 2319603200037 0.5 +1. 2319603200038 1327.484 0.055 37.3 1.5 2319603200039 2319603200040 1426.722 0.023 1812. 15. 48.0 1.1 2319603200041 0.5 +1. 2319603200042 1605.28 0.11 31.7 1.9 2319603200043 2319603200044 2134.030 0.039 279.4 7.8 2319603200045 2319603200046 3822.665 0.068 1200. 29. 2319603200047 2319603200048 5362.34 0.13 482. 26. 2319603200049 2319603200050 5517.404 0.081 783. 31. 2319603200051 2319603200052 6411.893 0.099 829. 44. 2319603200053 2319603200054 7845.02 0.22 1793. 94. 2319603200055 2319603200056 8376.25 0.20 1572. 79. 2319603200057 0.5 +1. 2319603200058 ENDDATA 36 0 2319603200059 ENDSUBENT 58 0 2319603299999 SUBENT 23196033 20130628 22352319603300001 BIB 5 17 2319603300002 REACTION 1(48-CD-116(N,0),,EN) 2319603300003 2(48-CD-116(N,EL),,WID,,G) g*Gn 2319603300004 3(48-CD-116(N,G),,WID) G-gamma 2319603300005 4(48-CD-116(N,0),,J) Spin J 2319603300006 5(48-CD-116(N,0),,PTY) Parity 2319603300007 ANALYSIS Resonance energy and g*Gn have been determined from 2319603300008 the GELINA data. The radiation width was deduced and a 2319603300009 spin assignment was made based on a simultaneous 2319603300010 analysis of thin-thick transmission and/or capture 2319603300011 data. 2319603300012 REL-REF (R,,G.Audi+,J,NP/A,729,337,2003) 2319603300013 Neutron separation energy 5777.2+-1.0 keV and 2319603300014 atomic mass 115.904755 u from this REL-REF were used in2319603300015 analysis. 2319603300016 ERR-ANALYS (ERR-S) Uncorrelated component due to counting 2319603300017 statistics. 2319603300018 STATUS (TABLE) Table 4 of J,NIM/B,300,11,2013. 2319603300019 ENDBIB 17 0 2319603300020 NOCOMMON 0 0 2319603300021 DATA 8 4 2319603300022 DATA 1ERR-S 1DATA 2ERR-S 2DATA 3ERR-S 32319603300023 DATA 4DATA 5 2319603300024 EV EV MILLI-EV MILLI-EV MILLI-EV MILLI-EV 2319603300025 NO-DIM NO-DIM 2319603300026 676.691 0.082 21.1 1.6 2319603300027 2319603300028 889.230 0.018 53.7 1.8 73. 10. 2319603300029 0.5 +1. 2319603300030 1048.800 0.017 511.7 8.0 2319603300031 0.5 +1. 2319603300032 1384.542 0.068 119.1 6.1 170. 16. 2319603300033 0.5 +1. 2319603300034 ENDDATA 12 0 2319603300035 ENDSUBENT 34 0 2319603399999 SUBENT 23196034 20130628 22352319603400001 BIB 5 14 2319603400002 REACTION (48-CD-0(N,TOT),,SIG) 2319603400003 SAMPLE (48-CD-106,NAT=0.0125) 2319603400004 (48-CD-108,NAT=0.0089) 2319603400005 (48-CD-110,NAT=0.1249) 2319603400006 (48-CD-111,NAT=0.1280) 2319603400007 (48-CD-112,NAT=0.2413) 2319603400008 (48-CD-113,NAT=0.1222) 2319603400009 (48-CD-114,NAT=0.2873) 2319603400010 (48-CD-116,NAT=0.0749) 2319603400011 ANALYSIS The Doppler broadened total cross section for natCd 2319603400012 + n at thermal energy (2200 m/s) and room temperature 2319603400013 (300 K) resulting from the total cross section. 2319603400014 ERR-ANALYS (DATA-ERR) Not specified 2319603400015 STATUS (TABLE) Table 5 of J,NIM/B,300,11,2013. 2319603400016 ENDBIB 14 0 2319603400017 NOCOMMON 0 0 2319603400018 DATA 3 1 2319603400019 EN DATA DATA-ERR 2319603400020 EV B B 2319603400021 0.0253 2450. 40. 2319603400022 ENDDATA 3 0 2319603400023 ENDSUBENT 22 0 2319603499999 SUBENT 23196035 20130628 22352319603500001 BIB 4 5 2319603500002 REACTION 1(48-CD-0(N,TOT),,SIG/TMP,,,EVAL) 2319603500003 2(48-CD-0(N,ABS),,SIG/TMP,,,EVAL) 2319603500004 ANALYSIS The value deduced from the resonance parameters. 2319603500005 ERR-ANALYS No errors given. 2319603500006 STATUS (TABLE) Table 5 of J,NIM/B,300,11,2013. 2319603500007 ENDBIB 5 0 2319603500008 COMMON 1 3 2319603500009 EN 2319603500010 EV 2319603500011 0.0253 2319603500012 ENDCOMMON 3 0 2319603500013 DATA 3 2 2319603500014 TEMP DATA 1DATA 2 2319603500015 K B B 2319603500016 0. 2474. 2467. 2319603500017 300. 2487. 2480. 2319603500018 ENDDATA 4 0 2319603500019 ENDSUBENT 18 0 2319603599999 SUBENT 23196036 20130628 22352319603600001 BIB 6 15 2319603600002 REACTION 1(48-CD-113(N,0),,EN,,,EVAL) 2319603600003 2(48-CD-113(N,EL),,WID,,G,EVAL) g*Gn 2319603600004 ANALYSIS Resonance parameters were adjusted or added as result 2319603600005 of a simultaneous analysis of GELINA and ORELA data. 2319603600006 The change in spin assignments of analyzed resonances 2319603600007 is with respect to those reported by C.Frankle. 2319603600008 REL-REF (R,13629001,C.M.Frankle+,J,PR/C,50,2774,1994) 2319603600009 Data from ORELA. 2319603600010 FLAG (1.) New resonance. 2319603600011 (2.) Spin change. 2319603600012 ERR-ANALYS (ERR-S) Uncorrelated component due to counting 2319603600013 statistics. 2319603600014 STATUS (TABLE) Table 7 of J,NIM/B,300,11,2013. 2319603600015 (DEP,13629004) ORELA data. 2319603600016 (DEP,23196031) Gelina data. 2319603600017 ENDBIB 15 0 2319603600018 NOCOMMON 0 0 2319603600019 DATA 7 414 2319603600020 DATA 1ERR-S 1DATA 2ERR-S 2SPIN J PARITY 2319603600021 FLAG 2319603600022 EV EV MILLI-EV MILLI-EV NO-DIM NO-DIM 2319603600023 NO-DIM 2319603600024 21.830 0.014 0.00662 0.00038 2. -1. 2319603600025 2319603600026 49.767 0.020 0.0144 0.0010 1. -1. 2319603600027 2319603600028 81.551 0.045 0.0138 0.0011 2. -1. 2319603600029 2319603600030 196.180 0.082 0.0599 0.0053 2. -1. 2319603600031 2319603600032 211.864 0.087 0.0670 0.0056 2. -1. 2319603600033 2319603600034 232.3042 0.0071 1.007 0.014 1. +1. 2319603600035 2319603600036 281.796 0.026 0.474 0.019 1. -1. 2319603600037 2. 2319603600038 376.767 0.015 0.827 0.018 1. -1. 2319603600039 2319603600040 446.9354 0.0085 2.110 0.026 0. +1. 2319603600041 2319603600042 457.612 0.012 1.529 0.027 1. +1. 2319603600043 2319603600044 495.027 0.027 0.873 0.030 2. -1. 2319603600045 2. 2319603600046 629.820 0.037 1.183 0.048 2. -1. 2319603600047 2. 2319603600048 677.0862 0.0035 14.655 0.071 1. +1. 2319603600049 2319603600050 758.942 0.019 3.560 0.076 1. +1. 2319603600051 2319603600052 760.844 0.080 1.007 0.064 2. -1. 2319603600053 1. 2319603600054 824.465 0.033 2.601 0.084 2. -1. 2319603600055 2. 2319603600056 870.523 0.098 0.976 0.069 2. -1. 2319603600057 2319603600058 919.586 0.094 1.210 0.081 2. -1. 2319603600059 2319603600060 936.39 0.24 0.470 0.044 2. -1. 2319603600061 1. 2319603600062 939.655 0.021 5.62 0.11 1. +1. 2319603600063 2319603600064 975.971 0.012 10.66 0.14 1. +1. 2319603600065 2319603600066 1063.19 0.47 0.279 0.027 2. -1. 2319603600067 2319603600068 1081.455 0.088 1.93 0.12 2. -1. 2319603600069 2319603600070 1089.0819 0.0049 40.41 0.28 0. +1. 2319603600071 2319603600072 1146.780 0.086 2.02 0.14 2. -1. 2319603600073 2319603600074 1169.546 0.045 4.61 0.17 1. +1. 2319603600075 2319603600076 1174.824 0.048 4.37 0.16 1. +1. 2319603600077 2319603600078 1288.98 0.12 0.404 0.039 2. -1. 2319603600079 2319603600080 1310.6460 0.0083 24.02 0.20 1. +1. 2319603600081 2319603600082 1356.926 0.039 5.49 0.17 1. +1. 2319603600083 2319603600084 1368.82 0.27 0.764 0.069 2. -1. 2319603600085 1. 2319603600086 1410.19 0.18 1.25 0.10 2. -1. 2319603600087 2319603600088 1423.530 0.024 9.59 0.18 1. +1. 2319603600089 1. 2319603600090 1461.051 0.029 8.87 0.20 1. +1. 2319603600091 2319603600092 1471.42 0.18 1.47 0.12 2. -1. 2319603600093 1. 2319603600094 1511.462 0.067 4.29 0.19 2. -1. 2319603600095 2. 2319603600096 1516.10 0.10 2.79 0.17 2. -1. 2319603600097 2319603600098 1563.49 0.13 2.24 0.15 2. -1. 2319603600099 1. 2319603600100 1567.214 0.081 40.98 0.31 1. +1. 2319603600101 2319603600102 1578.22 0.36 0.847 0.079 2. -1. 2319603600103 2319603600104 1602.30 0.24 1.34 0.12 2. -1. 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