ENTRY 22813 20121231 22342281300000001 SUBENT 22813001 20121231 22342281300100001 BIB 11 47 2281300100002 TITLE .Neutron capture cross sections for stellar cadmium 2281300100003 production 2281300100004 AUTHOR (K.Wisshak,F.Voss,F.Kaeppeler,L.Kazakov) 2281300100005 INSTITUTE (2GERKFK) Wisshak, Voss, Kaeppeler 2281300100006 (4RUSFEI) Kazakov 2281300100007 REFERENCE (J,PR/C,66,(2),025801,2002) Main reference 2281300100008 (R,FZKA-6619,2001) Detailed analysis of 2281300100009 measurements and experimental details 2281300100010 REL-REF (I,22816001,K.Wisshak,R,FZKA-6694,2001) Experim.details2281300100011 (M,22374001,K.Wisshak+,J,PR/C,48,(3),1401,1993) - 2281300100012 experimental details, data analysis, method of total 2281300100013 cross section and relative errors calculation 2281300100014 Determination of statist. and system. uncertainties 2281300100015 in measurements with the 4PiBaF2 detector has been 2281300100016 described in all refs above. 2281300100017 (I,,K.Wisshak+,J,NIM/A,292,595,1990) - Detector 2281300100018 description 2281300100019 (I,22372001,K.Wisshak+,J,PR/C,45,(5),2470,199205) 2281300100020 experimental details 2281300100021 (I,22195001,K.Wisshak+,J,PR/C,42,(4),1731,199010) 2281300100022 experimental details 2281300100023 (I,,F.Voss+,R,FZKA-6104,1998) Experimental and analysis2281300100024 details 2281300100025 FACILITY (VDG,2GERKFK) 3.75 MV Van de Graaff accelerator 2281300100026 pulse width is less than 1 ns, repetition rate 2281300100027 250 kHz, average beam current 2.2 microAmp 2281300100028 INC-SOURCE (P-LI7) Metallic Li target of about 1 mg/cm2 2281300100029 INC-SPECT .Proton beam energy adjusted so to be 30 and 100 keV 2281300100030 above the 7-Li(p,n)7-Be reaction threshold 1.881 MeV 2281300100031 giving neutrons in energy ranges 3-100, 3-225 keV 2281300100032 experimental energy resolution 0.5 ns 2281300100033 SAMPLE .Standard sample Au-197, 15 mm diameter, 0.4 mm = 2281300100034 2.2470E-3 atoms/b thickness,weight 1.2987 gram, 2281300100035 enclosing aluminium canning 0.2662 gr 2281300100036 .Graphite sample 15 mm diameter, 1.5 mm = 1.3364E-2 2281300100037 atoms/b thickness, 0.4710 gram weight, enclosing 2281300100038 aluminium canning 0.3058 g 2281300100039 .Empty aluminium canning 0.2422 gram 2281300100040 CORRECTION .Corrections were made for multiple scattering, 2281300100041 for isotopic impurities, for neutron self-absorption, 2281300100042 for undetected events, for signal/background ratio - 2281300100043 all for different neutron energies 2281300100044 HISTORY (20031229C) + + J.O.S. 2281300100045 (20031229U) Last checking has been done. 2281300100046 (20121231A) SD: BIB update in all Subents. In Subents 2281300100047 014 - 019: Col. EN-MEAN -> KT; values were changed. 2281300100048 ERR-ANALYS moved to Subents 2-27. EN-RSL deleted. 2281300100049 ENDBIB 47 0 2281300100050 NOCOMMON 0 0 2281300100051 ENDSUBENT 50 0 2281300199999 SUBENT 22813002 20121231 22342281300200001 BIB 8 30 2281300200002 REACTION ((48-CD-110(N,G)48-CD-111,,SIG,,AV)/ 2281300200003 (79-AU-197(N,G)79-AU-198,,SIG,,AV)) Averaged over 2281300200004 energy interval given in data section 2281300200005 MONITOR .Absolute measurement 2281300200006 METHOD (TOF) Flight path is 78.8 cm, resolution 1.2 ns/m 2281300200007 (GSPEC) 2281300200008 DETECTOR (SCIN,D4PI) Karlsruhe 4pi-Ba-F2 detector consisting of 2281300200009 42 hexagonal and pentagonal crystals forming 2281300200010 a spherical Ba-F2 shell of 15 cm thickness and 10 cm 2281300200011 inner radius. Resolution is 7% at 2.5 MeV gamma 2281300200012 energy, peak efficiency 90 % at 1 MeV 2281300200013 SAMPLE (48-CD-110,ENR=0.9551) .Cadmium metallic pellets 2281300200014 without canning,diameter 14.8 mm, thickness 2281300200015 1.7 mm(7.7312E-3 atoms/barn), weight 2.4978 gram. 2281300200016 Cd-110 content is 95.51%, Cd-111 content is 1.59%, 2281300200017 Cd-112 content is 13.26%, Cd-113 content is 0.50%, 2281300200018 Cd-114 content is 0.91%, Cd-116 content is 0.14%. 2281300200019 STATUS (TABLE) Data from table 5 of PR/C,66,(2),025801 2281300200020 ERR-ANALYS (ERR-T) Total error includes ERR-S, ERR-SYS 2281300200021 (ERR-SYS) Total systematic error includes ERR-1 - ERR-72281300200022 (ERR-1) Error due to flight path uncertainty 2281300200023 (ERR-2) Error due to neutron flux normalization 2281300200024 (ERR-3) Error due to sample mass and elemental 2281300200025 impurities 2281300200026 (ERR-4) Error due to isotopic composition 2281300200027 (ERR-5) Error due to isotopic correction 2281300200028 (ERR-6) Error due to multiple scattering and self- 2281300200029 shielding in sample 2281300200030 (ERR-7) Error due to undetected events 2281300200031 HISTORY (20121231U) SD: ERR-ANALYS and SAMPLE update. 2281300200032 ENDBIB 30 0 2281300200033 COMMON 8 6 2281300200034 ERR-SYS ERR-1 ERR-2 ERR-3 ERR-4 ERR-5 2281300200035 ERR-6 ERR-7 2281300200036 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT 2281300200037 PER-CENT PER-CENT 2281300200038 0.7 0.1 0.2 0.1 0.2 0.22281300200039 0.5 0.4 2281300200040 ENDCOMMON 6 0 2281300200041 DATA 5 18 2281300200042 EN-MIN EN-MAX DATA ERR-S ERR-T 2281300200043 KEV KEV NO-DIM PER-CENT PER-CENT 2281300200044 3. 5. 0.3536 3.7 3.8 2281300200045 5. 7.5 0.3137 2.2 2.3 2281300200046 7.5 10. 0.4530 1.6 1.7 2281300200047 10. 12.5 0.3975 1.3 1.5 2281300200048 12.5 15. 0.5014 1.1 1.3 2281300200049 15. 20. 0.5203 0.7 1.0 2281300200050 20. 25. 0.4910 0.6 0.9 2281300200051 25. 30. 0.4360 0.5 0.8 2281300200052 30. 40. 0.4285 0.4 0.8 2281300200053 40. 50. 0.4098 0.4 0.8 2281300200054 50. 60. 0.4131 0.4 0.8 2281300200055 60. 80. 0.3857 0.4 0.8 2281300200056 80. 100. 0.3757 0.4 0.8 2281300200057 100. 120. 0.3629 0.4 0.9 2281300200058 120. 150. 0.3559 0.6 0.9 2281300200059 150. 175. 0.3599 0.7 1.0 2281300200060 175. 200. 0.3535 0.7 1.0 2281300200061 200. 225. 0.3656 1.0 1.2 2281300200062 ENDDATA 20 0 2281300200063 ENDSUBENT 62 0 2281300299999 SUBENT 22813003 20121231 22342281300300001 BIB 8 31 2281300300002 REACTION ((48-CD-111(N,G)48-CD-112,,SIG,,AV)/ 2281300300003 (79-AU-197(N,G)79-AU-198,,SIG,,AV)) Averaged over 2281300300004 energy interval given in data section 2281300300005 MONITOR .Absolute measurement 2281300300006 METHOD (TOF) Flight path is 78.8 cm, time resolution 1.2 ns/m 2281300300007 (GSPEC) 2281300300008 DETECTOR (SCIN,D4PI) Karlsruhe 4pi-Ba-F2 detector consisting of 2281300300009 42 hexagonal and pentagonal crystals forming 2281300300010 a spherical Ba-F2 shell of 15 cm thickness and 10 cm 2281300300011 inner radius. Resolution is 7% at 2.5 MeV gamma 2281300300012 energy, peak efficiency 90% at 1 MeV 2281300300013 SAMPLE (48-CD-111,ENR=0.9592) .Cadmium metallic pellets 2281300300014 without canning,diameter 15.0 mm, thickness 2281300300015 1.5 mm (6.4349E-3 atoms/barn), weight 2.0971 gram. 2281300300016 Cd-110 content is 0.34%, Cd-111 content is 95.92%, 2281300300017 Cd-112 content is 2.16%, Cd-113 content is 0.49%, 2281300300018 Cd-114 content is 0.96% Cd-116 content is 0.13%. 2281300300019 STATUS (TABLE) Data from Table V of PR/C,66,(2),025801 2281300300020 ERR-ANALYS (ERR-T) Total error includes ERR-S, ERR-SYS 2281300300021 (ERR-SYS) Total systematic error includes ERR-1 - ERR-82281300300022 (ERR-1) Error due to flight path uncertainty 2281300300023 (ERR-2) Error due to neutron flux normalization 2281300300024 (ERR-3) Error due to sample mass and elemental 2281300300025 impurities 2281300300026 (ERR-4) Error due to isotopic composition 2281300300027 (ERR-5) Error due to isotopic correction 2281300300028 (ERR-6) Error due to multiple scattering and self- 2281300300029 shielding in sample 2281300300030 (ERR-7) Error due to undetected events 2281300300031 (ERR-8) Error due to background from scattered neutrons2281300300032 HISTORY (20121231U) SD: ERR-ANALYS and SAMPLE update. 2281300300033 ENDBIB 31 0 2281300300034 COMMON 9 6 2281300300035 ERR-SYS ERR-1 ERR-2 ERR-3 ERR-4 ERR-5 2281300300036 ERR-6 ERR-7 ERR-8 2281300300037 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT 2281300300038 PER-CENT PER-CENT PER-CENT 2281300300039 1.6 0.1 0.2 0.1 0.2 0.22281300300040 0.4 1.1 1.0 2281300300041 ENDCOMMON 6 0 2281300300042 DATA 5 18 2281300300043 EN-MIN EN-MAX DATA ERR-S ERR-T 2281300300044 KEV KEV NO-DIM PER-CENT PER-CENT 2281300300045 3. 5. 0.7008 3.1 3.5 2281300300046 5. 7.5 0.8381 1.7 2.3 2281300300047 7.5 10. 0.9999 1.5 2.2 2281300300048 10. 12.5 1.0794 1.1 1.9 2281300300049 12.5 15. 1.2277 1.0 1.9 2281300300050 15. 20. 1.3221 0.6 1.7 2281300300051 20. 25. 1.5162 0.5 1.7 2281300300052 25. 30. 1.5000 0.4 1.6 2281300300053 30. 40. 1.5156 0.3 1.6 2281300300054 40. 50. 1.4807 0.3 1.6 2281300300055 50. 60. 1.4874 0.3 1.6 2281300300056 60. 80. 1.4230 0.3 1.6 2281300300057 80. 100. 1.4164 0.3 1.6 2281300300058 100. 120. 1.3484 0.3 1.6 2281300300059 120. 150. 1.2793 0.5 1.7 2281300300060 150. 175. 1.2210 0.6 1.7 2281300300061 175. 200. 1.1904 0.6 1.7 2281300300062 200. 225. 1.2071 0.8 1.8 2281300300063 ENDDATA 20 0 2281300300064 ENDSUBENT 63 0 2281300399999 SUBENT 22813004 20121231 22342281300400001 BIB 8 31 2281300400002 REACTION ((48-CD-112(N,G)48-CD-113,,SIG,,AV)/ 2281300400003 (79-AU-197(N,G)79-AU-198,,SIG,,AV)) Averaged over 2281300400004 energy interval given in data section 2281300400005 MONITOR .Absolute measurement 2281300400006 METHOD (TOF) Flight path is 78.8 cm, time resolution 1.2 ns/m 2281300400007 (GSPEC) 2281300400008 DETECTOR (SCIN,D4PI) Karlsruhe 4pi-Ba-F2 detector consisting of 2281300400009 42 hexagonal and pentagonal crystals forming 2281300400010 a spherical Ba-F2 shell of 15 cm thickness and 10 cm 2281300400011 inner radius. Resolution is 7% at 2.5 MeV gamma 2281300400012 energy, peak efficiency 90 % at 1 MeV 2281300400013 SAMPLE (48-CD-112,ENR=0.9792) .Cadmium metallic pellets 2281300400014 without canning,diameter 14.8 mm, thickness 2281300400015 1.7 mm (7.5389E-3 atoms/barn), weight 2.4913 gram. 2281300400016 Cd-110 content is 0.09%, Cd-111 content is 0.21%, 2281300400017 Cd-112 content is 97.92%, Cd-113 content is 0.91%, 2281300400018 Cd-114 content is 0.78% Cd-116 content is 0.09%. 2281300400019 STATUS (TABLE) Data from table V of PR/C,66,(2),025801 2281300400020 ERR-ANALYS (ERR-T) Total error includes ERR-S, ERR-SYS 2281300400021 (ERR-SYS) Total systematic error includes ERR-1 - ERR-72281300400022 (ERR-1) Error due to flight path uncertainty 2281300400023 (ERR-2) Error due to neutron flux normalization 2281300400024 (ERR-3) Error due to sample mass and elemental 2281300400025 impurities 2281300400026 (ERR-4) Error due to isotopic composition 2281300400027 (ERR-5) Error due to isotopic correction 2281300400028 (ERR-6) Error due to multiple scattering and self- 2281300400029 shielding in sample 2281300400030 (ERR-7) Error due to undetected events 2281300400031 (ERR-8) Error due to background from scattered neutrons2281300400032 HISTORY (20121231U) SD: ERR-ANALYS and SAMPLE update. 2281300400033 ENDBIB 31 0 2281300400034 COMMON 8 6 2281300400035 ERR-SYS ERR-1 ERR-2 ERR-3 ERR-4 ERR-5 2281300400036 ERR-6 ERR-7 2281300400037 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT 2281300400038 PER-CENT PER-CENT 2281300400039 0.8 0.1 0.2 0.1 0.2 0.22281300400040 0.6 0.4 2281300400041 ENDCOMMON 6 0 2281300400042 DATA 5 18 2281300400043 EN-MIN EN-MAX DATA ERR-S ERR-T 2281300400044 KEV KEV NO-DIM PER-CENT PER-CENT 2281300400045 3. 5. 0.2920 3.7 3.8 2281300400046 5. 7.5 0.2885 2.1 2.2 2281300400047 7.5 10. 0.3484 1.7 1.9 2281300400048 10. 12.5 0.3635 1.3 1.5 2281300400049 12.5 15. 0.4529 1.1 1.4 2281300400050 15. 20. 0.3435 0.7 1.1 2281300400051 20. 25. 0.3981 0.6 1.0 2281300400052 25. 30. 0.3248 0.6 1.0 2281300400053 30. 40. 0.3248 0.4 0.9 2281300400054 40. 50. 0.3190 0.5 0.9 2281300400055 50. 60. 0.3230 0.4 0.9 2281300400056 60. 80. 0.3149 0.4 0.9 2281300400057 80. 100. 0.3132 0.4 0.9 2281300400058 100. 120. 0.2958 0.4 0.9 2281300400059 120. 150. 0.2924 0.7 1.1 2281300400060 150. 175. 0.3025 0.7 1.1 2281300400061 175. 200. 0.3119 0.8 1.1 2281300400062 200. 225. 0.3112 1.0 1.1 2281300400063 ENDDATA 20 0 2281300400064 ENDSUBENT 63 0 2281300499999 SUBENT 22813005 20121231 22342281300500001 BIB 8 31 2281300500002 REACTION ((48-CD-113(N,G)48-CD-114,,SIG,,AV)/ 2281300500003 (79-AU-197(N,G)79-AU-198,,SIG,,AV)) Averaged over 2281300500004 energy interval given in data section 2281300500005 MONITOR .Absolute measurement 2281300500006 METHOD (TOF) Flight path is 78.8 cm, time resolution 1.2ns/m 2281300500007 (GSPEC) 2281300500008 DETECTOR (SCIN,D4PI) Karlsruhe 4pi-Ba-F2 detector consisting of 2281300500009 42 hexagonal and pentagonal crystals forming 2281300500010 a spherical Ba-F2 shell of 15 cm thickness and 10 cm 2281300500011 inner radius. Resolution is 7% at 2.5 MeV gamma 2281300500012 energy, peak efficiency 90 % at 1 MeV 2281300500013 SAMPLE (48-CD-113,ENR=0.9533) .Cadmium metallic pellets 2281300500014 without canning,diameter 14.8 mm, thickness 2281300500015 0.7 mm (2.9615E-3 atoms/barn), weight 0.9820 gram. 2281300500016 Cd-110 content is 0.12%, Cd-111 content is 0.18%, 2281300500017 Cd-112 content is 1.71%, Cd-113 content is 95.33%, 2281300500018 Cd-114 content is 2.45% Cd-116 content is 0.21%. 2281300500019 STATUS (TABLE) Data from table V of PR/C,66,(2),025801 2281300500020 ERR-ANALYS (ERR-T) Total error includes ERR-S, ERR-SYS 2281300500021 (ERR-SYS) Total systematic error includes ERR-1 - ERR-82281300500022 (ERR-1) Error due to flight path uncertainty 2281300500023 (ERR-2) Error due to neutron flux normalization 2281300500024 (ERR-3) Error due to sample mass and elemental 2281300500025 impurities 2281300500026 (ERR-4) Error due to isotopic composition 2281300500027 (ERR-5) Error due to isotopic correction 2281300500028 (ERR-6) Error due to multiple scattering and self- 2281300500029 shielding in sample 2281300500030 (ERR-7) Error due to undetected events 2281300500031 (ERR-8) Error due to background from scattered neutrons2281300500032 HISTORY (20121231A) SD: ERR-ANALYS and SAMPLE update. 2281300500033 ENDBIB 31 0 2281300500034 COMMON 9 6 2281300500035 ERR-SYS ERR-1 ERR-2 ERR-3 ERR-4 ERR-5 2281300500036 ERR-6 ERR-7 ERR-8 2281300500037 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT 2281300500038 PER-CENT PER-CENT PER-CENT 2281300500039 1.6 0.1 0.2 0.1 0.2 0.22281300500040 0.4 1.1 1.0 2281300500041 ENDCOMMON 6 0 2281300500042 DATA 5 18 2281300500043 EN-MIN EN-MAX DATA ERR-S ERR-T 2281300500044 KEV KEV NO-DIM PER-CENT PER-CENT 2281300500045 3. 5. 0.5949 5.5 5.7 2281300500046 5. 7.5 0.8279 2.4 2.9 2281300500047 7.5 10. 1.0227 1.9 2.5 2281300500048 10. 12.5 1.0107 1.4 2.1 2281300500049 12.5 15. 1.0964 1.2 1.0 2281300500050 15. 20. 1.2889 0.7 1.7 2281300500051 20. 25. 1.3724 0.6 1.7 2281300500052 25. 30. 1.3310 0.5 1.7 2281300500053 30. 40. 1.2761 0.4 1.6 2281300500054 40. 50. 1.3144 0.4 1.6 2281300500055 50. 60. 1.2572 0.4 1.6 2281300500056 60. 80. 1.2093 0.3 1.6 2281300500057 80. 100. 1.1882 0.3 1.6 2281300500058 100. 120. 1.1473 0.4 1.6 2281300500059 120. 150. 1.0911 0.6 1.7 2281300500060 150. 175. 1.0527 0.6 1.7 2281300500061 175. 200. 1.0298 0.7 1.7 2281300500062 200. 225. 1.0241 1.0 1.9 2281300500063 ENDDATA 20 0 2281300500064 ENDSUBENT 63 0 2281300599999 SUBENT 22813006 20121231 22342281300600001 BIB 8 30 2281300600002 REACTION ((48-CD-114(N,G)48-CD-115,,SIG,,AV)/ 2281300600003 (79-AU-197(N,G)79-AU-198,,SIG,,AV)) Averaged over 2281300600004 energy interval given in data section 2281300600005 MONITOR .Absolute measurement 2281300600006 METHOD (TOF) Flight path is 78.8 cm, time resolution 1.2ns/m 2281300600007 (GSPEC) 2281300600008 DETECTOR (SCIN,D4PI) Karlsruhe 4pi-Ba-F2 detector consisting of 2281300600009 42 hexagonal and pentagonal crystals forming 2281300600010 a spherical Ba-F2 shell of 15 cm thickness and 10 cm 2281300600011 inner radius. Resolution is 7% at 2.5 MeV gamma 2281300600012 energy, peak efficiency 90 % at 1 MeV 2281300600013 SAMPLE (48-CD-114,ENR=0.9907) .Cadmium metallic pellets 2281300600014 without canning,diameter 14.8 mm, thickness 2281300600015 2.7 mm (11.941e-3 atoms/barn), weight 3.9942 gram. 2281300600016 Cd-110 content is 0.07%, Cd-111 content is 0.09%, 2281300600017 Cd-112 content is 0.28%, Cd-113 content is 0.26%, 2281300600018 Cd-114 content is 99.07% Cd-116 content is 0.23%. 2281300600019 STATUS (TABLE) Data from table V of PR/C,66,(2),025801 2281300600020 ERR-ANALYS (ERR-T) Total error includes ERR-S, ERR-SYS 2281300600021 (ERR-SYS) Total systematic error includes ERR-1 - ERR-72281300600022 (ERR-1) Error due to flight path uncertainty 2281300600023 (ERR-2) Error due to neutron flux normalization 2281300600024 (ERR-3) Error due to sample mass and elemental 2281300600025 impurities 2281300600026 (ERR-4) Error due to isotopic composition 2281300600027 (ERR-5) Error due to isotopic correction 2281300600028 (ERR-6) Error due to multiple scattering and self- 2281300600029 shielding in sample 2281300600030 (ERR-7) Error due to undetected events 2281300600031 HISTORY (20121231U) SD: ERR-ANALYS and SAMPLE update. 2281300600032 ENDBIB 30 0 2281300600033 COMMON 8 6 2281300600034 ERR-SYS ERR-1 ERR-2 ERR-3 ERR-4 ERR-5 2281300600035 ERR-6 ERR-7 2281300600036 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT 2281300600037 PER-CENT PER-CENT 2281300600038 0.9 0.1 0.2 0.1 0.2 0.22281300600039 0.7 0.4 2281300600040 ENDCOMMON 6 0 2281300600041 DATA 5 18 2281300600042 EN-MIN EN-MAX DATA ERR-S ERR-T 2281300600043 KEV KEV NO-DIM PER-CENT PER-CENT 2281300600044 3. 5. 0.1542 5.6 5.7 2281300600045 5. 7.5 0.2165 2.4 2.6 2281300600046 7.5 10. 0.2524 1.9 2.1 2281300600047 10. 12.5 0.2516 1.4 1.7 2281300600048 12.5 15. 0.2544 1.3 1.6 2281300600049 15. 20. 0.2410 0.8 1.2 2281300600050 20. 25. 0.2577 0.7 1.1 2281300600051 25. 30. 0.2399 0.6 1.1 2281300600052 30. 40. 0.2389 0.5 1.0 2281300600053 40. 50. 0.2239 0.5 1.0 2281300600054 50. 60. 0.2056 0.5 1.0 2281300600055 60. 80. 0.2151 0.4 1.0 2281300600056 80. 100. 0.2104 0.5 1.0 2281300600057 100. 120. 0.2151 0.5 1.0 2281300600058 120. 150. 0.2142 0.7 1.1 2281300600059 150. 175. 0.2170 0.8 1.2 2281300600060 175. 200. 0.2129 0.8 1.2 2281300600061 200. 225. 0.2228 1.1 1.4 2281300600062 ENDDATA 20 0 2281300600063 ENDSUBENT 62 0 2281300699999 SUBENT 22813007 20121231 22342281300700001 BIB 8 30 2281300700002 REACTION ((48-CD-116(N,G)48-CD-117,,SIG,,AV)/ 2281300700003 (79-AU-197(N,G)79-AU-198,,SIG,,AV)) Averaged over 2281300700004 energy interval given in data section 2281300700005 MONITOR .Absolute measurement 2281300700006 METHOD (TOF) Flight path is 78.8 cm, time resolution 1.2ns/m 2281300700007 (GSPEC) 2281300700008 DETECTOR (SCIN,D4PI) Karlsruhe 4pi-Ba-F2 detector consisting of 2281300700009 42 hexagonal and pentagonal crystals forming 2281300700010 a spherical Ba-F2 shell of 15 cm thickness and 10 cm 2281300700011 inner radius. Resolution is 7% at 2.5 MeV gamma 2281300700012 energy, peak efficiency 90 % at 1 MeV 2281300700013 SAMPLE (48-CD-116,ENR=0.9240) .Cadmium metallic pellets 2281300700014 without canning,diameter 14.8 mm, thickness 2281300700015 2.7 mm (11.941e-3 atoms/barn), weight 3.9942 gram. 2281300700016 Cd-110 content is 0.57%, Cd-111 content is 0.60%, 2281300700017 Cd-112 content is 1.72%, Cd-113 content is 1.10%, 2281300700018 Cd-114 content is 3.61% Cd-116 content is 92.40%. 2281300700019 STATUS (TABLE) Data from table V of PR/C,66,(2),025801 2281300700020 ERR-ANALYS (ERR-T) Total error includes ERR-S, ERR-SYS 2281300700021 (ERR-SYS) Total systematic error includes ERR-1 - ERR-72281300700022 (ERR-1) Error due to flight path uncertainty 2281300700023 (ERR-2) Error due to neutron flux normalization 2281300700024 (ERR-3) Error due to sample mass and elemental 2281300700025 impurities 2281300700026 (ERR-4) Error due to isotopic composition 2281300700027 (ERR-5) Error due to isotopic correction 2281300700028 (ERR-6) Error due to multiple scattering and self- 2281300700029 shielding in sample 2281300700030 (ERR-7) Error due to undetected events 2281300700031 HISTORY (20121231U) SD: ERR-ANALYS and SAMPLE update. 2281300700032 ENDBIB 30 0 2281300700033 COMMON 8 6 2281300700034 ERR-SYS ERR-1 ERR-2 ERR-3 ERR-4 ERR-5 2281300700035 ERR-6 ERR-7 2281300700036 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT 2281300700037 PER-CENT PER-CENT 2281300700038 1.1 0.1 0.2 0.1 0.2 0.22281300700039 0.9 0.4 2281300700040 ENDCOMMON 6 0 2281300700041 DATA 5 18 2281300700042 EN-MIN EN-MAX DATA ERR-S ERR-T 2281300700043 KEV KEV NO-DIM PER-CENT PER-CENT 2281300700044 3. 5. 0.1103 8.3 8.4 2281300700045 5. 7.5 0.0973 5.2 5.3 2281300700046 7.5 10. 0.1292 3.5 3.7 2281300700047 10. 12.5 0.1361 2.4 2.6 2281300700048 12.5 15. 0.1374 1.1 2.4 2281300700049 15. 20. 0.1620 1.2 1.6 2281300700050 20. 25. 0.1510 1.1 1.6 2281300700051 25. 30. 0.1443 0.9 1.4 2281300700052 30. 40. 0.1285 0.7 1.1 2281300700053 40. 50. 0.1282 0.8 1.1 2281300700054 50. 60. 0.1306 0.7 1.1 2281300700055 60. 80. 0.1226 0.7 1.1 2281300700056 80. 100. 0.1317 0.7 1.1 2281300700057 100. 120. 0.1228 0.7 1.1 2281300700058 120. 150. 0.1286 1.1 1.6 2281300700059 150. 175. 0.1315 1.1 1.6 2281300700060 175. 200. 0.1361 1.2 1.6 2281300700061 200. 225. 0.1398 1.4 1.8 2281300700062 ENDDATA 20 0 2281300700063 ENDSUBENT 62 0 2281300799999 SUBENT 22813008 20121231 22342281300800001 BIB 6 18 2281300800002 REACTION (48-CD-110(N,G)48-CD-111,,SIG,,AV) Averaged over 2281300800003 energy interval given in data section 2281300800004 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 2281300800005 MONIT-REF (22099002,W.Ratynski+,J,PR/C,37,595,1988) 2281300800006 (,R.L.Macklin,W,MACKLIN,1982) 2281300800007 The experimental ratios were converted into absolute 2281300800008 cross sections by means of the gold cross section of 2281300800009 Macklin (priv.comm.), after normalization by a factor 2281300800010 of 0.989 to the absolute value of Ratynski et. al. 2281300800011 STATUS (TABLE) Data from table VI of PR/C,66,(2),025801 2281300800012 (DEP,22813002) 2281300800013 ERR-ANALYS (DATA-ERR) Total uncertainty from ratio. 2281300800014 Uncertainties of cross-sections can be calculated from 2281300800015 the uncertainty of the cross-section ratio by adding 2281300800016 quadratically uncertainty of the gold standard 2281300800017 (MONIT-ERR) uncertainty of the gold standard 2281300800018 HISTORY (20121219A) SD: MONIT-ERR, COMMON were added. 2281300800019 MONIT-REF, ERR-ANALYS update. 2281300800020 ENDBIB 18 0 2281300800021 COMMON 1 3 2281300800022 MONIT-ERR 2281300800023 PER-CENT 2281300800024 1.5 2281300800025 ENDCOMMON 3 0 2281300800026 DATA 5 18 2281300800027 EN-MIN EN-MAX DATA DATA-ERR MONIT 2281300800028 KEV KEV MB PER-CENT MB 2281300800029 3. 5. 801.5 3.8 2266.7 2281300800030 5. 7.5 541.7 2.3 1726.7 2281300800031 7.5 10. 550.7 1.7 1215.7 2281300800032 10. 12.5 424.0 1.5 1066.7 2281300800033 12.5 15. 440.2 1.3 878.0 2281300800034 15. 20. 384.4 1.0 738.8 2281300800035 20. 25. 294.6 0.9 600.0 2281300800036 25. 30. 248.9 0.8 570.8 2281300800037 30. 40. 214.4 0.8 500.4 2281300800038 40. 50. 177.6 0.8 433.3 2281300800039 50. 60. 161.0 0.8 389.6 2281300800040 60. 80. 134.8 0.8 349.4 2281300800041 80. 100. 112.1 0.8 298.3 2281300800042 100. 120. 105.3 0.9 290.1 2281300800043 120. 150. 97.6 0.9 274.1 2281300800044 150. 175. 94.9 1.0 263.7 2281300800045 175. 200. 89.3 1.0 252.6 2281300800046 200. 225. 90.9 1.2 248.5 2281300800047 ENDDATA 20 0 2281300800048 ENDSUBENT 47 0 2281300899999 SUBENT 22813009 20121231 22342281300900001 BIB 6 18 2281300900002 REACTION (48-CD-111(N,G)48-CD-112,,SIG,,AV) Averaged over 2281300900003 energy interval given in data section 2281300900004 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 2281300900005 MONIT-REF (22099002,W.Ratynski+,J,PR/C,37,595,1988) 2281300900006 (,R.L.Macklin,W,MACKLIN,1982) 2281300900007 The experimental ratios were converted into absolute 2281300900008 cross sections by means of the gold cross section of 2281300900009 Macklin (priv.comm.), after normalization by a factor 2281300900010 of 0.989 to the absolute value of Ratynski et. al. 2281300900011 STATUS (TABLE) Data from table VI of PR/C,66,(2),025801 2281300900012 (DEP,22813003) 2281300900013 ERR-ANALYS (DATA-ERR) Total uncertainty from ratio. 2281300900014 Uncertainties of cross-sections can be calculated from 2281300900015 the uncertainty of the cross-section ratio by adding 2281300900016 quadratically uncertainty of the gold standard 2281300900017 (MONIT-ERR) uncertainty of the gold standard 2281300900018 HISTORY (20121219A) SD: MONIT-ERR, COMMON were added. 2281300900019 MONIT-REF, ERR-ANALYS update. 2281300900020 ENDBIB 18 0 2281300900021 COMMON 1 3 2281300900022 MONIT-ERR 2281300900023 PER-CENT 2281300900024 1.5 2281300900025 ENDCOMMON 3 0 2281300900026 DATA 5 18 2281300900027 EN-MIN EN-MAX DATA DATA-ERR MONIT 2281300900028 KEV KEV MB PER-CENT MB 2281300900029 3. 5. 1589. 3.5 2266.7 2281300900030 5. 7.5 1447. 2.3 1726.7 2281300900031 7.5 10. 1216. 2.2 1215.7 2281300900032 10. 12.5 1151. 1.9 1066.7 2281300900033 12.5 15. 1078. 1.9 878. 2281300900034 15. 20. 976.8 1.7 738.8 2281300900035 20. 25. 909.8 1.7 600. 2281300900036 25. 30. 856.2 1.6 570.8 2281300900037 30. 40. 757.4 1.6 500.4 2281300900038 40. 50. 641.6 1.6 433.3 2281300900039 50. 60. 579.6 1.6 389.6 2281300900040 60. 80. 497.1 1.6 349.4 2281300900041 80. 100. 422.5 1.6 298.3 2281300900042 100. 120. 391.2 1.6 290.1 2281300900043 120. 150. 350.7 1.7 274.1 2281300900044 150. 175. 321.9 1.7 263.7 2281300900045 175. 200. 300.7 1.7 252.6 2281300900046 200. 225. 299.9 1.8 248.5 2281300900047 ENDDATA 20 0 2281300900048 ENDSUBENT 47 0 2281300999999 SUBENT 22813010 20121231 22342281301000001 BIB 6 18 2281301000002 REACTION (48-CD-112(N,G)48-CD-113,,SIG,,AV) Averaged over 2281301000003 energy interval given in data section 2281301000004 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 2281301000005 MONIT-REF (22099002,W.Ratynski+,J,PR/C,37,595,1988) 2281301000006 (,R.L.Macklin,W,MACKLIN,1982) 2281301000007 The experimental ratios were converted into absolute 2281301000008 cross sections by means of the gold cross section of 2281301000009 Macklin (priv.comm.), after normalization by a factor 2281301000010 of 0.989 to the absolute value of Ratynski et. al. 2281301000011 STATUS (TABLE) Data from table VI of PR/C,66,(2),025801 2281301000012 (DEP,22813004) 2281301000013 ERR-ANALYS (DATA-ERR) Total uncertainty from ratio. 2281301000014 Uncertainties of cross-sections can be calculated from 2281301000015 the uncertainty of the cross-section ratio by adding 2281301000016 quadratically uncertainty of the gold standard 2281301000017 (MONIT-ERR) uncertainty of the gold standard 2281301000018 HISTORY (20121219A) SD: MONIT-ERR, COMMON were added. 2281301000019 MONIT-REF, ERR-ANALYS update. 2281301000020 ENDBIB 18 0 2281301000021 COMMON 1 3 2281301000022 MONIT-ERR 2281301000023 PER-CENT 2281301000024 1.5 2281301000025 ENDCOMMON 3 0 2281301000026 DATA 5 18 2281301000027 EN-MIN EN-MAX DATA DATA-ERR MONIT 2281301000028 KEV KEV MB PER-CENT MB 2281301000029 3. 5. 662.0 3.7 2266.7 2281301000030 5. 7.5 498.2 2.2 1726.7 2281301000031 7.5 10. 423.6 1.6 1215.7 2281301000032 10. 12.5 387.8 1.3 1066.7 2281301000033 12.5 15. 397.6 1.1 878. 2281301000034 15. 20. 253.8 0.7 738.8 2281301000035 20. 25. 238.9 0.6 600. 2281301000036 25. 30. 185.4 0.5 570.8 2281301000037 30. 40. 162.5 0.4 500.4 2281301000038 40. 50. 138.2 0.4 433.3 2281301000039 50. 60. 125.9 0.4 389.6 2281301000040 60. 80. 110.0 0.4 349.4 2281301000041 80. 100. 93.4 0.4 298.3 2281301000042 100. 120. 85.8 0.4 290.1 2281301000043 120. 150. 80.2 0.6 274.1 2281301000044 150. 175. 79.7 0.7 263.7 2281301000045 175. 200. 78.8 0.7 252.6 2281301000046 200. 225. 77.3 1.0 248.5 2281301000047 ENDDATA 20 0 2281301000048 ENDSUBENT 47 0 2281301099999 SUBENT 22813011 20121231 22342281301100001 BIB 6 18 2281301100002 REACTION (48-CD-113(N,G)48-CD-114,,SIG,,AV) Averaged over 2281301100003 energy interval given in data section 2281301100004 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 2281301100005 MONIT-REF (22099002,W.Ratynski+,J,PR/C,37,595,1988) 2281301100006 (,R.L.Macklin,W,MACKLIN,1982) 2281301100007 The experimental ratios were converted into absolute 2281301100008 cross sections by means of the gold cross section of 2281301100009 Macklin (priv.comm.), after normalization by a factor 2281301100010 of 0.989 to the absolute value of Ratynski et. al. 2281301100011 STATUS (TABLE) Data from table VI of PR/C,66,(2),025801 2281301100012 (DEP,22813005) 2281301100013 ERR-ANALYS (DATA-ERR) Total uncertainty from ratio. 2281301100014 Uncertainties of cross-sections can be calculated from 2281301100015 the uncertainty of the cross-section ratio by adding 2281301100016 quadratically uncertainty of the gold standard 2281301100017 (MONIT-ERR) uncertainty of the gold standard 2281301100018 HISTORY (20121219A) SD: MONIT-ERR, COMMON were added. 2281301100019 MONIT-REF, ERR-ANALYS update. 2281301100020 ENDBIB 18 0 2281301100021 COMMON 1 3 2281301100022 MONIT-ERR 2281301100023 PER-CENT 2281301100024 1.5 2281301100025 ENDCOMMON 3 0 2281301100026 DATA 5 18 2281301100027 EN-MIN EN-MAX DATA DATA-ERR MONIT 2281301100028 KEV KEV MB PER-CENT MB 2281301100029 3. 5. 1348. 3.1 2266.7 2281301100030 5. 7.5 1430. 1.7 1726.7 2281301100031 7.5 10. 1243. 1.5 1215.7 2281301100032 10. 12.5 1078. 1.1 1066.7 2281301100033 12.5 15. 962.7 1.0 878. 2281301100034 15. 20. 952.2 0.6 738.8 2281301100035 20. 25. 823.5 0.5 600. 2281301100036 25. 30. 759.8 0.4 570.8 2281301100037 30. 40. 638.5 0.3 500.4 2281301100038 40. 50. 569.6 0.3 433.3 2281301100039 50. 60. 489.9 0.3 389.6 2281301100040 60. 80. 422.5 0.3 349.4 2281301100041 80. 100. 354.5 0.3 298.3 2281301100042 100. 120. 332.9 0.3 290.1 2281301100043 120. 150. 299.1 0.5 274.1 2281301100044 150. 175. 277.5 0.6 263.7 2281301100045 175. 200. 260.1 0.6 252.6 2281301100046 200. 225. 254.5 0.8 248.5 2281301100047 ENDDATA 20 0 2281301100048 ENDSUBENT 47 0 2281301199999 SUBENT 22813012 20121231 22342281301200001 BIB 6 18 2281301200002 REACTION (48-CD-114(N,G)48-CD-115,,SIG,,AV) Averaged over 2281301200003 energy interval given in data section 2281301200004 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 2281301200005 MONIT-REF (22099002,W.Ratynski+,J,PR/C,37,595,1988) 2281301200006 (,R.L.Macklin,W,MACKLIN,1982) 2281301200007 The experimental ratios were converted into absolute 2281301200008 cross sections by means of the gold cross section of 2281301200009 Macklin (priv.comm.), after normalization by a factor 2281301200010 of 0.989 to the absolute value of Ratynski et. al. 2281301200011 STATUS (TABLE) Data from table VI of PR/C,66,(2),025801 2281301200012 (DEP,22813006) 2281301200013 ERR-ANALYS (DATA-ERR) Total uncertainty from ratio. 2281301200014 Uncertainties of cross-sections can be calculated from 2281301200015 the uncertainty of the cross-section ratio by adding 2281301200016 quadratically uncertainty of the gold standard 2281301200017 (MONIT-ERR) uncertainty of the gold standard 2281301200018 HISTORY (20121219A) SD: MONIT-ERR, COMMON were added. 2281301200019 MONIT-REF, ERR-ANALYS update. 2281301200020 ENDBIB 18 0 2281301200021 COMMON 1 3 2281301200022 MONIT-ERR 2281301200023 PER-CENT 2281301200024 1.5 2281301200025 ENDCOMMON 3 0 2281301200026 DATA 5 18 2281301200027 EN-MIN EN-MAX DATA DATA-ERR MONIT 2281301200028 KEV KEV MB PER-CENT MB 2281301200029 3. 5. 349.5 5.6 2266.7 2281301200030 5. 7.5 373.8 2.4 1726.7 2281301200031 7.5 10. 306.8 1.9 1215.7 2281301200032 10. 12.5 268.4 1.4 1066.7 2281301200033 12.5 15. 223.3 1.3 878. 2281301200034 15. 20. 177.4 0.8 738.8 2281301200035 20. 25. 154.7 0.7 600. 2281301200036 25. 30. 137.0 0.6 570.8 2281301200037 30. 40. 119.6 0.5 500.4 2281301200038 40. 50. 97.0 0.5 433.3 2281301200039 50. 60. 80.1 0.5 389.6 2281301200040 60. 80. 75.2 0.4 349.4 2281301200041 80. 100. 62.8 0.5 298.3 2281301200042 100. 120. 62.4 0.5 290.1 2281301200043 120. 150. 58.7 0.7 274.1 2281301200044 150. 175. 57.2 0.8 263.7 2281301200045 175. 200. 53.8 0.8 252.6 2281301200046 200. 225. 55.4 1.1 248.5 2281301200047 ENDDATA 20 0 2281301200048 ENDSUBENT 47 0 2281301299999 SUBENT 22813013 20121231 22342281301300001 BIB 6 18 2281301300002 REACTION (48-CD-116(N,G)48-CD-117,,SIG,,AV) Averaged over 2281301300003 energy interval given in data section 2281301300004 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 2281301300005 MONIT-REF (22099002,W.Ratynski+,J,PR/C,37,595,1988) 2281301300006 (,R.L.Macklin,W,MACKLIN,1982) 2281301300007 The experimental ratios were converted into absolute 2281301300008 cross sections by means of the gold cross section of 2281301300009 Macklin (priv.comm.), after normalization by a factor 2281301300010 of 0.989 to the absolute value of Ratynski et. al. 2281301300011 STATUS (TABLE) Data from table VI of PR/C,66,(2),025801 2281301300012 (DEP,22813007) 2281301300013 ERR-ANALYS (DATA-ERR) Total uncertainty from ratio. 2281301300014 Uncertainties of cross-sections can be calculated from 2281301300015 the uncertainty of the cross-section ratio by adding 2281301300016 quadratically uncertainty of the gold standard 2281301300017 (MONIT-ERR) uncertainty of the gold standard 2281301300018 HISTORY (20121219A) SD: MONIT-ERR, COMMON were added. 2281301300019 MONIT-REF, ERR-ANALYS update. 2281301300020 ENDBIB 18 0 2281301300021 COMMON 1 3 2281301300022 MONIT-ERR 2281301300023 PER-CENT 2281301300024 1.5 2281301300025 ENDCOMMON 3 0 2281301300026 DATA 5 18 2281301300027 EN-MIN EN-MAX DATA DATA-ERR MONIT 2281301300028 KEV KEV MB PER-CENT MB 2281301300029 3. 5. 250.0 8.3 2266.7 2281301300030 5. 7.5 165.1 5.2 1726.7 2281301300031 7.5 10. 157.1 3.5 1215.7 2281301300032 10. 12.5 145.2 2.4 1066.7 2281301300033 12.5 15. 120.7 1.1 878. 2281301300034 15. 20. 119.7 1.2 738.8 2281301300035 20. 25. 90.6 1.1 600. 2281301300036 25. 30. 82.3 0.9 570.8 2281301300037 30. 40. 64.3 0.7 500.4 2281301300038 40. 50. 55.5 0.8 433.3 2281301300039 50. 60. 50.9 0.7 389.6 2281301300040 60. 80. 42.8 0.7 349.4 2281301300041 80. 100. 39.3 0.7 298.3 2281301300042 100. 120. 35.6 0.7 290.1 2281301300043 120. 150. 35.3 1.1 274.1 2281301300044 150. 175. 34.7 1.1 263.7 2281301300045 175. 200. 34.4 1.2 252.6 2281301300046 200. 225. 34.7 1.4 248.5 2281301300047 ENDDATA 20 0 2281301300048 ENDSUBENT 47 0 2281301399999 SUBENT 22813014 20121231 22342281301400001 BIB 8 40 2281301400002 REACTION (48-CD-110(N,G)48-CD-111,,SIG,,MXW,DERIV) 2281301400003 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 2281301400004 ANALYSIS .Maxwellian-averaged cross-sections were calculated 2281301400005 for energy interval 0-700 keV by dividing it into 2281301400006 three parts according cross-section's sources. 2281301400007 The contribution I-1 was determined by normalizing the 2281301400008 cross sections of Kopecky (see REL-REF) to the present 2281301400009 data in the interval between 3 to 15 keV. 2281301400010 The dominant part I-2 between 3 and 225 keV is provided2281301400011 by the present experiment. These data were obtained by 2281301400012 sufficient resolution in neutron energy to exclude 2281301400013 systematic uncertainties that may result in calculation2281301400014 of the Maxwellian average if the energy grid is too 2281301400015 coarse. 2281301400016 At typical s-process temperatures the energy interval 2281301400017 from 225 to 700 keV contributes very little to the 2281301400018 Maxwellian average. For this part, the data of 2281301400019 Kopecky (see REL-REF) were normalized to the present 2281301400020 results between 50 and 225 keV. 2281301400021 REL-REF (R,,J.Kopecky+,R,INDC(NDS)-362,1997) - data for I-1 and2281301400022 I-3 intervals were taken from this ref. and normalized 2281301400023 to present experiment 2281301400024 MISC-COL (MISC1) I-1 2281301400025 (MISC2) I-2 2281301400026 (MISC3) I-3 2281301400027 STATUS (TABLE) Data from Table VIII of PR/C,66,(2),025801 2281301400028 and Tbl.21 of FZKA-6619 2281301400029 (DEP,22813002) 2281301400030 (DEP,22813008) 2281301400031 ERR-ANALYS (ERR-T) Total error 2281301400032 (ERR-S) Statistical uncertainty 2281301400033 (ERR-SYS) total systematic error of Maxwell. averaging 2281301400034 Systematic uncertainties are correspond to the 2281301400035 uncertainties of the cross section ratios. 2281301400036 The 1.5% uncertainty of the gold standard is not 2281301400037 included here, since it cancels out in most 2281301400038 applications of relevance for nuclear astrophysics 2281301400039 HISTORY (20121231A) SD: EN-MEAN -> KT and data were corrected; 2281301400040 MISC col. was deleted; MISC1, MISC2, MISC3 were added.2281301400041 BIB update. SF9=DERIV was added to REACTION code. 2281301400042 ENDBIB 40 0 2281301400043 NOCOMMON 0 0 2281301400044 DATA 11 14 2281301400045 KT DATA ERR-S ERR-SYS ERR-T MISC1 2281301400046 MISC1-ERR MISC2 MISC2-ERR MISC3 MISC3-ERR 2281301400047 KEV MB MB MB MB MB 2281301400048 MB MB MB MB MB 2281301400049 8. 512.9 4.7 3.6 5.9 60.62281301400050 3.0 452.3 3.6 0.0 2281301400051 10. 455.5 3.4 3.2 4.7 40.42281301400052 2.0 415.1 2.7 0.0 2281301400053 15. 361.1 1.9 2.5 3.1 18.92281301400054 0.9 342.2 1.7 0.0 2281301400055 20. 303.4 1.3 2.1 2.5 10.92281301400056 0.5 292.5 1.2 0.0 2281301400057 25. 264.4 1.1 1.9 2.2 7.12281301400058 0.4 257.2 1.0 0.1 2281301400059 30. 236.5 0.9 1.7 1.9 5.02281301400060 0.3 231.0 0.8 0.5 2281301400061 40. 199.1 0.6 1.4 1.5 2.82281301400062 0.1 194.0 0.6 2.3 0.1 2281301400063 50. 175.6 0.5 1.2 1.3 1.82281301400064 0.1 168.9 0.5 5.9 0.2 2281301400065 52. 172.0 0.5 1.2 1.3 1.72281301400066 0.1 163.5 0.5 6.8 0.2 2281301400067 60. 159.7 0.5 1.1 1.2 1.32281301400068 0.1 147.6 0.4 10.8 0.3 2281301400069 70. 148.3 0.7 1.0 1.2 0.92281301400070 0.0 131.0 0.4 16.4 0.6 2281301400071 80. 139.7 0.9 1.0 1.3 0.72281301400072 0.0 116.9 0.4 22.1 0.8 2281301400073 90. 133.2 1.1 0.9 1.4 0.62281301400074 0.0 104.9 0.3 27.7 1.1 2281301400075 100. 127.8 1.3 0.9 1.6 0.52281301400076 0.0 94.5 0.3 32.8 1.3 2281301400077 ENDDATA 32 0 2281301400078 ENDSUBENT 77 0 2281301499999 SUBENT 22813015 20121231 22342281301500001 BIB 8 40 2281301500002 REACTION (48-CD-111(N,G)48-CD-112,,SIG,,MXW,DERIV) 2281301500003 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 2281301500004 ANALYSIS .Maxwellian-averaged cross-sections were calculated 2281301500005 for energy interval 0-700 keV by dividing it into 2281301500006 three parts according cross-section's sources. 2281301500007 The contribution I-1 was determined by normalizing the 2281301500008 cross sections of Kopecky (see REL-REF) to the present 2281301500009 data in the interval between 3 to 15 keV. 2281301500010 The dominant part I-2 between 3 and 225 keV is provided2281301500011 by the present experiment. These data were obtained by 2281301500012 sufficient resolution in neutron energy to exclude 2281301500013 systematic uncertainties that may result in calculation2281301500014 of the Maxwellian average if the energy grid is too 2281301500015 coarse. 2281301500016 At typical s-process temperatures the energy interval 2281301500017 from 225 to 700 keV contributes very little to the 2281301500018 Maxwellian average. For this part, the data of 2281301500019 Kopecky (see REL-REF) were normalized to the present 2281301500020 results between 50 and 225 keV. 2281301500021 REL-REF (R,,J.Kopecky+,R,INDC(NDS)-362,1997) - data for I-1 and2281301500022 I-3 intervals were taken from this ref. and normalized 2281301500023 to present experiment 2281301500024 MISC-COL (MISC1) I-1 2281301500025 (MISC2) I-2 2281301500026 (MISC3) I-3 2281301500027 STATUS (TABLE) Data from Table VIII of PR/C,66,(2),025801 2281301500028 and Tbl.21 of FZKA-6619 2281301500029 (DEP,22813003) 2281301500030 (DEP,22813009) 2281301500031 ERR-ANALYS (ERR-T) Total error 2281301500032 (ERR-S) Statistical uncertainty 2281301500033 (ERR-SYS) total systematic error of Maxwell. averaging 2281301500034 Systematic uncertainties are correspond to the 2281301500035 uncertainties of the cross section ratios. 2281301500036 The 1.5% uncertainty of the gold standard is not 2281301500037 included here, since it cancels out in most 2281301500038 applications of relevance for nuclear astrophysics 2281301500039 HISTORY (20121231A) SD: EN-MEAN -> KT and data were corrected; 2281301500040 MISC col. was deleted; MISC1, MISC2, MISC3 were added.2281301500041 BIB update. SF9=DERIV was added to REACTION code. 2281301500042 ENDBIB 40 0 2281301500043 NOCOMMON 0 0 2281301500044 DATA 11 14 2281301500045 KT DATA ERR-S ERR-SYS ERR-T MISC1 2281301500046 MISC1-ERR MISC2 MISC2-ERR MISC3 MISC3-ERR 2281301500047 KEV MB MB MB MB MB 2281301500048 MB MB MB MB MB 2281301500049 8. 1335. 11. 21. 24. 173.22281301500050 8.7 1162. 6.7 0.0 2281301500051 10. 1222. 7.9 20. 22. 115.62281301500052 5.8 1106. 5.3 0.0 2281301500053 15. 1034. 4.4 17. 18. 54.32281301500054 2.7 979.6 3.5 0.0 2281301500055 20. 911. 3.1 15. 15. 31.42281301500056 1.6 880.0 2.6 0.0 2281301500057 25. 823. 2.4 13. 13. 20.52281301500058 1.0 801.8 2.2 0.4 2281301500059 30. 754. 2.0 12. 12. 14.42281301500060 0.7 738.7 1.9 1.3 2281301500061 40. 656. 1.6 10. 10. 8.22281301500062 0.4 640.8 1.5 6.5 0.2 2281301500063 50. 586. 1.4 9.4 10. 5.32281301500064 0.3 564.9 1.3 15.8 0.4 2281301500065 52. 574. 1.4 9.2 9.3 4.92281301500066 0.2 551.4 1.3 18.1 0.5 2281301500067 60. 533. 1.5 8.5 9. 3.72281301500068 0.2 501.9 1.2 27.8 0.8 2281301500069 70. 491. 1.7 7.9 8.1 2.12281301500070 0.1 448.1 1.1 40.5 1.3 2281301500071 80. 456. 2.0 7.3 8. 2.12281301500072 0.1 401.6 1.0 52.6 1.7 2281301500073 90. 426. 2.4 6.8 7.2 1.72281301500074 0.1 361.3 0.9 63.4 2.2 2281301500075 100. 400. 2.7 6.4 7. 1.32281301500076 0.1 326.2 0.8 72.7 2.6 2281301500077 ENDDATA 32 0 2281301500078 ENDSUBENT 77 0 2281301599999 SUBENT 22813016 20121231 22342281301600001 BIB 8 40 2281301600002 REACTION (48-CD-112(N,G)48-CD-113,,SIG,,MXW,DERIV) 2281301600003 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 2281301600004 ANALYSIS .Maxwellian-averaged cross-sections were calculated 2281301600005 for energy interval 0-700 keV by dividing it into 2281301600006 three parts according cross-section's sources. 2281301600007 The contribution I-1 was determined by normalizing the 2281301600008 cross sections of Kopecky (see REL-REF) to the present 2281301600009 data in the interval between 3 to 15 keV. 2281301600010 The dominant part I-2 between 3 and 225 keV is provided2281301600011 by the present experiment. These data were obtained by 2281301600012 sufficient resolution in neutron energy to exclude 2281301600013 systematic uncertainties that may result in calculation2281301600014 of the Maxwellian average if the energy grid is too 2281301600015 coarse. 2281301600016 At typical s-process temperatures the energy interval 2281301600017 from 225 to 700 keV contributes very little to the 2281301600018 Maxwellian average. For this part, the data of 2281301600019 Kopecky (see REL-REF) were normalized to the present 2281301600020 results between 50 and 225 keV. 2281301600021 REL-REF (R,,J.Kopecky+,R,INDC(NDS)-362,1997) - data for I-1 and2281301600022 I-3 intervals were taken from this ref. and normalized 2281301600023 to present experiment 2281301600024 MISC-COL (MISC1) I-1 2281301600025 (MISC2) I-2 2281301600026 (MISC3) I-3 2281301600027 STATUS (TABLE) Data from Table VIII of PR/C,66,(2),025801 2281301600028 and Tbl.21 of FZKA-6619 2281301600029 (DEP,22813004) 2281301600030 (DEP,22813010) 2281301600031 ERR-ANALYS (ERR-T) Total error 2281301600032 (ERR-S) Statistical uncertainty 2281301600033 (ERR-SYS) total systematic error of Maxwell. averaging 2281301600034 Systematic uncertainties are correspond to the 2281301600035 uncertainties of the cross section ratios. 2281301600036 The 1.5% uncertainty of the gold standard is not 2281301600037 included here, since it cancels out in most 2281301600038 applications of relevance for nuclear astrophysics 2281301600039 HISTORY (20121231A) SD: EN-MEAN -> KT and data were corrected; 2281301600040 MISC col. was deleted; MISC1, MISC2, MISC3 were added.2281301600041 BIB update. SF9=DERIV was added to REACTION code. 2281301600042 ENDBIB 40 0 2281301600043 NOCOMMON 0 0 2281301600044 DATA 11 14 2281301600045 KT DATA ERR-S ERR-SYS ERR-T MISC1 2281301600046 MISC1-ERR MISC2 MISC2-ERR MISC3 MISC3-ERR 2281301600047 KEV MB MB MB MB MB 2281301600048 MB MB MB MB MB 2281301600049 8. 419.5 3.9 3.4 5.2 49.8 2281301600050 2.5 369.7 3.0 0.0 2281301600051 10. 369.0 2.9 3.0 4.2 33.32281301600052 1.7 335.7 2.3 0.0 2281301600053 15. 288.4 1.6 2.3 2.8 15.72281301600054 0.8 272.7 1.4 0.0 2281301600055 20. 241.0 1.1 1.9 2.2 9.12281301600056 0.5 231.9 1.0 0.0 2281301600057 25. 209.8 0.9 1.7 1.9 5.92281301600058 0.3 203.8 0.8 0.1 2281301600059 30. 187.9 0.7 1.5 1.7 4.22281301600060 0.2 183.3 0.7 0.4 2281301600061 40. 159.1 0.5 1.3 1.4 2.42281301600062 0.1 154.7 0.5 2.0 0.1 2281301600063 50. 141.2 0.4 1.1 1.2 1.52281301600064 0.1 134.6 0.4 5.1 0.1 2281301600065 52. 138.5 0.5 1.1 1.2 1.42281301600066 0.1 131.2 0.4 5.9 0.2 2281301600067 60. 129.4 0.5 1.0 1.1 1.12281301600068 0.1 118.9 0.4 9.4 0.3 2281301600069 70. 120.9 0.6 1.1 1.2 0.82281301600070 0.0 105.9 0.3 14.2 0.2 2281301600071 80. 114.7 0.8 0.9 1.2 0.62281301600072 0.0 94.9 0.3 19.2 0.7 2281301600073 90. 109.7 0.9 0.9 1.3 0.52281301600074 0.0 85.3 0.3 23.9 0.9 2281301600075 100. 105.8 1.1 0.8 1.4 0.42281301600076 0.0 77.1 0.3 28.3 1.1 2281301600077 ENDDATA 32 0 2281301600078 ENDSUBENT 77 0 2281301699999 SUBENT 22813017 20121231 22342281301700001 BIB 8 40 2281301700002 REACTION (48-CD-113(N,G)48-CD-114,,SIG,,MXW,DERIV) 2281301700003 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 2281301700004 ANALYSIS .Maxwellian-averaged cross-sections were calculated 2281301700005 for energy interval 0-700 keV by dividing it into 2281301700006 three parts according cross-section's sources. 2281301700007 The contribution I-1 was determined by normalizing the 2281301700008 cross sections of Kopecky (see REL-REF) to the present 2281301700009 data in the interval between 3 to 15 keV. 2281301700010 The dominant part I-2 between 3 and 225 keV is provided2281301700011 by the present experiment. These data were obtained by 2281301700012 sufficient resolution in neutron energy to exclude 2281301700013 systematic uncertainties that may result in calculation2281301700014 of the Maxwellian average if the energy grid is too 2281301700015 coarse. 2281301700016 At typical s-process temperatures the energy interval 2281301700017 from 225 to 700 keV contributes very little to the 2281301700018 Maxwellian average. For this part, the data of 2281301700019 Kopecky (see REL-REF) were normalized to the present 2281301700020 results between 50 and 225 keV. 2281301700021 REL-REF (R,,J.Kopecky+,R,INDC(NDS)-362,1997) - data for I-1 and2281301700022 I-3 intervals were taken from this ref. and normalized 2281301700023 to present experiment 2281301700024 MISC-COL (MISC1) I-1 2281301700025 (MISC2) I-2 2281301700026 (MISC3) I-3 2281301700027 STATUS (TABLE) Data from Table VIII of PR/C,66,(2),025801 2281301700028 and Tbl.21 of FZKA-6619 2281301700029 (DEP,22813005) 2281301700030 (DEP,22813011) 2281301700031 ERR-ANALYS (ERR-T) Total error 2281301700032 (ERR-S) Statistical uncertainty 2281301700033 (ERR-SYS) total systematic error of Maxwell. averaging 2281301700034 Systematic uncertainties are correspond to the 2281301700035 uncertainties of the cross section ratios. 2281301700036 The 1.5% uncertainty of the gold standard is not 2281301700037 included here, since it cancels out in most 2281301700038 applications of relevance for nuclear astrophysics 2281301700039 HISTORY (20121231A) SD: EN-MEAN -> KT and data were corrected; 2281301700040 MISC col. was deleted; MISC1, MISC2, MISC3 were added.2281301700041 BIB update.SF9=DERIV was added to REACTION code. 2281301700042 ENDBIB 40 0 2281301700043 NOCOMMON 0 0 2281301700044 DATA 11 14 2281301700045 KT DATA ERR-S ERR-SYS ERR-T MISC1 2281301700046 MISC1-ERR MISC2 MISC2-ERR MISC3 MISC3-ERR 2281301700047 KEV MB MB MB MB MB 2281301700048 MB MB MB MB MB 2281301700049 8. 1236. 12. 20. 23. 149.02281301700050 7.5 1087. 9.0 0.0 2281301700051 10. 1127. 8.5 18. 20. 99.52281301700052 5.0 1027. 6.9 0.0 2281301700053 15. 940. 4.8 15. 16. 46.92281301700054 2.3 893.5 4.2 0.0 2281301700055 20. 819. 3.3 13. 13. 27.22281301700056 1.4 792.1 3.0 0.0 2281301700057 25. 733. 2.6 12. 12. 17.72281301700058 0.9 714.6 2.4 0.3 2281301700059 30. 667. 2.1 11. 11. 12.42281301700060 0.6 653.6 2.0 1.3 2281301700061 40. 575. 1.6 9.2 9.3 7.12281301700062 0.4 561.6 1.5 6.5 0.2 2281301700063 50. 513. 1.4 8.2 8.3 4.62281301700064 0.2 492.1 1.3 16.5 0.5 2281301700065 52. 503. 1.4 8.1 8.2 4.22281301700066 0.2 480.0 1.3 19.0 0.6 2281301700067 60. 469. 1.4 7.5 8. 3.22281301700068 0.2 435.6 1.1 30.0 0.9 2281301700069 70. 436. 1.8 7.0 7.2 2.42281301700070 0.1 388.0 1.0 45.2 1.5 2281301700071 80. 409. 2.3 6.6 7.0 1.82281301700072 0.1 347.2 0.9 60.4 2.1 2281301700073 90. 388. 2.9 6.2 7. 1.42281301700074 0.1 311.9 0.8 74.9 2.8 2281301700075 100. 371. 3.6 5.9 7. 1.22281301700076 0.1 281.3 0.8 88.0 3.5 2281301700077 ENDDATA 32 0 2281301700078 ENDSUBENT 77 0 2281301799999 SUBENT 22813018 20121231 22342281301800001 BIB 8 40 2281301800002 REACTION (48-CD-114(N,G)48-CD-115,,SIG,,MXW,DERIV) 2281301800003 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 2281301800004 ANALYSIS .Maxwellian-averaged cross-sections were calculated 2281301800005 for energy interval 0-700 keV by dividing it into 2281301800006 three parts according cross-section's sources. 2281301800007 The contribution I-1 was determined by normalizing the 2281301800008 cross sections of Kopecky (see REL-REF) to the present 2281301800009 data in the interval between 3 to 15 keV. 2281301800010 The dominant part I-2 between 3 and 225 keV is provided2281301800011 by the present experiment. These data were obtained by 2281301800012 sufficient resolution in neutron energy to exclude 2281301800013 systematic uncertainties that may result in calculation2281301800014 of the Maxwellian average if the energy grid is too 2281301800015 coarse. 2281301800016 At typical s-process temperatures the energy interval 2281301800017 from 225 to 700 keV contributes very little to the 2281301800018 Maxwellian average. For this part, the data of 2281301800019 Kopecky (see REL-REF) were normalized to the present 2281301800020 results between 50 and 225 keV. 2281301800021 REL-REF (R,,J.Kopecky+,R,INDC(NDS)-362,1997) - data for I-1 and2281301800022 I-3 intervals were taken from this ref. and normalized 2281301800023 to present experiment 2281301800024 MISC-COL (MISC1) I-1 2281301800025 (MISC2) I-2 2281301800026 (MISC3) I-3 2281301800027 STATUS (TABLE) Data from Table VIII of PR/C,66,(2),025801 2281301800028 and Tbl.21 of FZKA-6619 2281301800029 (DEP,22813006) 2281301800030 (DEP,22813012) 2281301800031 ERR-ANALYS (ERR-T) Total error 2281301800032 (ERR-S) Statistical uncertainty 2281301800033 (ERR-SYS) total systematic error of Maxwell. averaging 2281301800034 Systematic uncertainties are correspond to the 2281301800035 uncertainties of the cross section ratios. 2281301800036 The 1.5% uncertainty of the gold standard is not 2281301800037 included here, since it cancels out in most 2281301800038 applications of relevance for nuclear astrophysics 2281301800039 HISTORY (20121231A) SD: EN-MEAN -> KT and data were corrected; 2281301800040 MISC col. was deleted; MISC1, MISC2, MISC3 were added.2281301800041 BIB update. SF9=DERIV was added to REACTION code. 2281301800042 ENDBIB 40 0 2281301800043 NOCOMMON 0 0 2281301800044 DATA 11 14 2281301800045 KT DATA ERR-S ERR-SYS ERR-T MISC1 2281301800046 MISC1-ERR MISC2 MISC2-ERR MISC3 MISC3-ERR 2281301800047 KEV MB MB MB MB MB 2281301800048 MB MB MB MB MB 2281301800049 8. 285.8 3.1 2.6 4.0 39.32281301800050 2.0 246.5 2.4 0.0 2281301800051 10. 251.5 2.2 2.3 3.2 26.22281301800052 1.3 255.3 1.8 0.0 2281301800053 15. 197.1 1.3 1.8 2.2 12.32281301800054 0.6 184.8 1.1 0.0 2281301800055 20. 165.1 0.9 1.5 1.7 7.12281301800056 0.4 158.0 0.8 0.0 2281301800057 25. 144.0 0.6 1.3 1.4 4.62281301800058 0.2 139.3 0.6 0.1 2281301800059 30. 129.2 0.5 1.2 1.3 3.22281301800060 0.2 125.7 0.5 0.3 2281301800061 40. 109.9 0.4 1.0 1.1 1.92281301800062 0.1 106.6 0.4 1.4 2281301800063 50. 97.9 0.4 0.9 1.0 1.22281301800064 0.1 93.1 0.4 3.6 0.1 2281301800065 52. 96.0 0.3 0.9 0.9 1.12281301800066 0.1 90.8 0.3 4.1 0.1 2281301800067 60. 89.8 0.4 0.8 0.9 0.82281301800068 0.0 82.5 0.3 6.5 0.2 2281301800069 70. 84.1 0.4 0.8 0.9 0.62281301800070 0.0 73.6 0.3 9.9 0.3 2281301800071 80. 79.9 0.6 0.7 0.9 0.52281301800072 0.0 66.0 0.3 13.4 0.5 2281301800073 90. 76.6 0.6 0.7 0.9 0.42281301800074 0.0 59.5 0.2 16.7 0.6 2281301800075 100. 73.8 0.8 0.7 1.1 0.32281301800076 0.0 53.8 0.2 19.7 0.8 2281301800077 ENDDATA 32 0 2281301800078 ENDSUBENT 77 0 2281301899999 SUBENT 22813019 20121231 22342281301900001 BIB 8 40 2281301900002 REACTION (48-CD-116(N,G)48-CD-117,,SIG,,MXW,DERIV) 2281301900003 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 2281301900004 ANALYSIS .Maxwellian-averaged cross-sections were calculated 2281301900005 for energy interval 0-700 keV by dividing it into 2281301900006 three parts according cross-section's sources. 2281301900007 The contribution I-1 was determined by normalizing the 2281301900008 cross sections of Kopecky (see REL-REF) to the present 2281301900009 data in the interval between 3 to 15 keV. 2281301900010 The dominant part I-2 between 3 and 225 keV is provided2281301900011 by the present experiment. These data were obtained by 2281301900012 sufficient resolution in neutron energy to exclude 2281301900013 systematic uncertainties that may result in calculation2281301900014 of the Maxwellian average if the energy grid is too 2281301900015 coarse. 2281301900016 At typical s-process temperatures the energy interval 2281301900017 from 225 to 700 keV contributes very little to the 2281301900018 Maxwellian average. For this part, the data of 2281301900019 Kopecky (see REL-REF) were normalized to the present 2281301900020 results between 50 and 225 keV. 2281301900021 REL-REF (R,,J.Kopecky+,R,INDC(NDS)-362,1997) - data for I-1 and2281301900022 I-3 intervals were taken from this ref. and normalized 2281301900023 to present experiment 2281301900024 MISC-COL (MISC1) I-1 2281301900025 (MISC2) I-2 2281301900026 (MISC3) I-3 2281301900027 STATUS (TABLE) Data from Table VIII of PR/C,66,(2),025801 2281301900028 and Tbl.21 of FZKA-6619 2281301900029 (DEP,22813007) 2281301900030 (DEP,22813013) 2281301900031 ERR-ANALYS (ERR-T) Total error 2281301900032 (ERR-S) Statistical uncertainty 2281301900033 (ERR-SYS) total systematic error of Maxwell. averaging 2281301900034 Systematic uncertainties are correspond to the 2281301900035 uncertainties of the cross section ratios. 2281301900036 The 1.5% uncertainty of the gold standard is not 2281301900037 included here, since it cancels out in most 2281301900038 applications of relevance for nuclear astrophysics 2281301900039 HISTORY (20121231A) SD: EN-MEAN -> KT and data were corrected; 2281301900040 MISC col. was deleted; MISC1, MISC2, MISC3 were added.2281301900041 BIB update. SF9=DERIV was added to REACTION code. 2281301900042 ENDBIB 40 0 2281301900043 NOCOMMON 0 0 2281301900044 DATA 11 14 2281301900045 KT DATA ERR-S ERR-SYS ERR-T MISC1 2281301900046 MISC1-ERR MISC2 MISC2-ERR MISC3 MISC3-ERR 2281301900047 KEV MB MB MB MB MB 2281301900048 MB MB MB MB MB 2281301900049 8. 159.0 2.6 2.7 3.1 20.22281301900050 1.0 138.8 2.4 0.0 2281301900051 10. 141.1 1.9 1.6 2.5 13.52281301900052 0.7 127.6 1.8 0.0 2281301900053 15. 112.1 1.1 1.2 1.6 6.42281301900054 0.3 105.7 1.1 0.0 2281301900055 20. 94.6 0.8 1.0 1.3 3.72281301900056 0.2 90.9 0.8 0.0 2281301900057 25. 82.9 0.6 0.9 1.1 2.42281301900058 0.1 80.5 0.6 0.0 2281301900059 30. 74.8 0.5 0.8 0.9 1.72281301900060 0.1 72.9 0.5 0.2 2281301900061 40. 64.1 0.4 0.7 0.8 1.02281301900062 0.1 62.2 0.4 0.9 2281301900063 50. 57.7 0.3 0.6 0.7 0.62281301900064 0.0 54.7 0.3 2.4 0.1 2281301900065 52. 56.7 0.3 0.6 0.7 0.62281301900066 0.0 53.4 0.3 2.7 0.1 2281301900067 60. 53.4 0.3 0.6 0.7 0.42281301900068 0.0 48.7 0.3 4.3 0.1 2281301900069 70. 50.4 0.4 0.6 0.7 0.32281301900070 0.0 43.6 0.3 6.5 0.2 2281301900071 80. 48.2 0.4 0.5 0.7 0.22281301900072 0.0 39.2 0.2 8.8 0.3 2281301900073 90. 46.5 0.4 0.5 0.6 0.22281301900074 0.0 35.4 0.2 10.9 0.4 2281301900075 100. 45.2 0.5 0.5 0.7 0.22281301900076 0.0 32.1 0.2 12.9 0.5 2281301900077 ENDDATA 32 0 2281301900078 ENDSUBENT 77 0 2281301999999 SUBENT 22813020 20121231 22342281302000001 BIB 7 17 2281302000002 REACTION (48-CD-110(N,TOT),,SIG,,AV) Averaged over energy 2281302000003 interval given in data section 2281302000004 DETECTOR (GLASD) Li-6 glass detector 2281302000005 METHOD (TOF) Flight base is 260 cm 2281302000006 SAMPLE (48-CD-110,ENR=0.9551) .Cadmium metallic pellets 2281302000007 without canning,diameter 14.8 mm, thickness 2281302000008 1.7 mm(7.7312E-3 atoms/barn), weight 2.4978 gram. 2281302000009 Cd-110 content is 95.51%, 2281302000010 Cd-111 content is 1.59%, Cd-112 content is 13.26%, 2281302000011 Cd-113 content is 0.50%, Cd-114 content is 0.91% 2281302000012 Cd-116 content is 0.14%. 2281302000013 ERR-ANALYS (DATA-ERR) The quoted uncertainties were obtained 2281302000014 under the assumption that they are inversely 2281302000015 proportional to the fraction of neutrons interacting 2281302000016 in the sample, A=1-T, where T is the transmission. 2281302000017 STATUS (TABLE) Data from table III of PR/C,66,(2),025801 2281302000018 HISTORY (20121231U) SD: ERR-ANALYS update. 2281302000019 ENDBIB 17 0 2281302000020 COMMON 1 3 2281302000021 DATA-ERR 2281302000022 PER-CENT 2281302000023 4.1 2281302000024 ENDCOMMON 3 0 2281302000025 DATA 3 9 2281302000026 EN-MIN EN-MAX DATA 2281302000027 KEV KEV B 2281302000028 10. 15. 6.0 2281302000029 15. 20. 7.8 2281302000030 20. 30. 7.1 2281302000031 30. 40. 6.8 2281302000032 40. 60. 7.2 2281302000033 60. 80. 7.6 2281302000034 80. 100. 7.8 2281302000035 100. 150. 7.2 2281302000036 150. 200. 7.6 2281302000037 ENDDATA 11 0 2281302000038 ENDSUBENT 37 0 2281302099999 SUBENT 22813021 20121231 22342281302100001 BIB 7 16 2281302100002 REACTION (48-CD-111(N,TOT),,SIG,,AV) Averaged over energy 2281302100003 interval given in data section 2281302100004 METHOD (TOF) Flight base is 260 cm 2281302100005 DETECTOR (GLASD) Li-6 glass detector 2281302100006 SAMPLE (48-CD-111,ENR=0.9592) .Cadmium metallic pellets 2281302100007 without canning,diameter 15.0 mm, thickness 2281302100008 1.5 mm (6.4349E-3 atoms/barn), weight 2.0971 gram. 2281302100009 Cd-110 content is 0.34%, Cd-111 content is 95.92%, 2281302100010 Cd-112 content is 2.16%, Cd-113 content is 0.49%, 2281302100011 Cd-114 content is 0.96% Cd-116 content is 0.13%. 2281302100012 ERR-ANALYS (DATA-ERR) The quoted uncertainties were obtained 2281302100013 under the assumption that they are inversely 2281302100014 proportional to the fraction of neutrons interacting 2281302100015 in the sample, A=1-T, where T is the transmission. 2281302100016 STATUS (TABLE) Data from table III of PR/C,66,(2),025801 2281302100017 HISTORY (20121231U) SD: ERR-ANALYS update. 2281302100018 ENDBIB 16 0 2281302100019 COMMON 1 3 2281302100020 DATA-ERR 2281302100021 PER-CENT 2281302100022 4.7 2281302100023 ENDCOMMON 3 0 2281302100024 DATA 3 9 2281302100025 EN-MIN EN-MAX DATA 2281302100026 KEV KEV B 2281302100027 10. 15. 7.4 2281302100028 15. 20. 7.4 2281302100029 20. 30. 6.8 2281302100030 30. 40. 7.3 2281302100031 40. 60. 7.3 2281302100032 60. 80. 7.3 2281302100033 80. 100. 7.3 2281302100034 100. 150. 7.8 2281302100035 150. 200. 7.6 2281302100036 ENDDATA 11 0 2281302100037 ENDSUBENT 36 0 2281302199999 SUBENT 22813022 20121231 22342281302200001 BIB 7 16 2281302200002 REACTION (48-CD-112(N,TOT),,SIG,,AV) Averaged over energy 2281302200003 interval given in data section 2281302200004 DETECTOR (GLASD) Li-6 glass detector 2281302200005 METHOD (TOF) Flight base is 260 cm 2281302200006 SAMPLE (48-CD-112,ENR=0.9792) .Cadmium metallic pellets 2281302200007 without canning,diameter 14.8 mm, thickness 2281302200008 1.7 mm (7.5389E-3 atoms/barn), weight 2.4913 gram. 2281302200009 Cd-110 content is 0.09%, Cd-111 content is 0.21%, 2281302200010 Cd-112 content is 97.92%, Cd-113 content is 0.91%, 2281302200011 Cd-114 content is 0.78% Cd-116 content is 0.09%. 2281302200012 ERR-ANALYS (DATA-ERR) The quoted uncertainties were obtained 2281302200013 under the assumption that they are inversely 2281302200014 proportional to the fraction of neutrons interacting 2281302200015 in the sample, A=1-T, where T is the transmission. 2281302200016 STATUS (TABLE) Data from table III of PR/C,66,(2),025801 2281302200017 HISTORY (20121231U) SD: ERR-ANALYS update. 2281302200018 ENDBIB 16 0 2281302200019 COMMON 1 3 2281302200020 DATA-ERR 2281302200021 PER-CENT 2281302200022 4.5 2281302200023 ENDCOMMON 3 0 2281302200024 DATA 3 9 2281302200025 EN-MIN EN-MAX DATA 2281302200026 KEV KEV B 2281302200027 10. 15. 6.5 2281302200028 15. 20. 6.9 2281302200029 20. 30. 6.8 2281302200030 30. 40. 6.5 2281302200031 40. 60. 6.8 2281302200032 60. 80. 7.2 2281302200033 80. 100. 7.2 2281302200034 100. 150. 7.4 2281302200035 150. 200. 7.5 2281302200036 ENDDATA 11 0 2281302200037 ENDSUBENT 36 0 2281302299999 SUBENT 22813023 20121231 22342281302300001 BIB 7 16 2281302300002 REACTION (48-CD-113(N,TOT),,SIG,,AV) Averaged over energy 2281302300003 interval given in data section 2281302300004 METHOD (TOF) Flight base is 260 cm 2281302300005 DETECTOR (GLASD) Li-6 glass detector 2281302300006 SAMPLE (48-CD-113,ENR=0.9533) .Cadmium metallic pellets 2281302300007 without canning,diameter 14.8 mm, thickness 2281302300008 0.7 mm (2.9615E-3 atoms/barn), weight 0.9820 gram. 2281302300009 Cd-110 content is 0.12%, Cd-111 content is 0.18%, 2281302300010 Cd-112 content is 1.71%, Cd-113 content is 95.33%, 2281302300011 Cd-114 content is 2.45% Cd-116 content is 0.21%. 2281302300012 ERR-ANALYS (DATA-ERR) The quoted uncertainties were obtained 2281302300013 under the assumption that they are inversely 2281302300014 proportional to the fraction of neutrons interacting 2281302300015 in the sample, A=1-T, where T is the transmission. 2281302300016 STATUS (TABLE) Data from table III of PR/C,66,(2),025801 2281302300017 HISTORY (20121231U) SD: ERR-ANALYS update. 2281302300018 ENDBIB 16 0 2281302300019 COMMON 1 3 2281302300020 DATA-ERR 2281302300021 PER-CENT 2281302300022 9.3 2281302300023 ENDCOMMON 3 0 2281302300024 DATA 3 9 2281302300025 EN-MIN EN-MAX DATA 2281302300026 KEV KEV B 2281302300027 10. 15. 8. 2281302300028 15. 20. 9.6 2281302300029 20. 30. 8.5 2281302300030 30. 40. 8.7 2281302300031 40. 60. 8.9 2281302300032 60. 80. 9.1 2281302300033 80. 100. 8.0 2281302300034 100. 150. 8.6 2281302300035 150. 200. 7.9 2281302300036 ENDDATA 11 0 2281302300037 ENDSUBENT 36 0 2281302399999 SUBENT 22813024 20121231 22342281302400001 BIB 7 16 2281302400002 REACTION (48-CD-114(N,TOT),,SIG,,AV) Averaged over energy 2281302400003 interval given in data section 2281302400004 DETECTOR (GLASD) Li-6 glass detector 2281302400005 METHOD (TOF) Flight base is 260 cm 2281302400006 SAMPLE (48-CD-114,ENR=0.9907) .Cadmium metallic pellets 2281302400007 without canning,diameter 14.8 mm, thickness 2281302400008 2.7 mm (11.941E-3 atoms/barn), weight 3.9942 gram. 2281302400009 Cd-110 content is 0.07%, Cd-111 content is 0.09%, 2281302400010 Cd-112 content is 0.28%, Cd-113 content is 0.26%, 2281302400011 Cd-114 content is 99.07% Cd-116 content is 0.23%. 2281302400012 ERR-ANALYS (DATA-ERR) The quoted uncertainties were obtained 2281302400013 under the assumption that they are inversely 2281302400014 proportional to the fraction of neutrons interacting 2281302400015 in the sample, A=1-T, where T is the transmission. 2281302400016 STATUS (TABLE) Data from table III of PR/C,66,(2),025801 2281302400017 HISTORY (20121231U) SD: ERR-ANALYS update. 2281302400018 ENDBIB 16 0 2281302400019 COMMON 1 3 2281302400020 DATA-ERR 2281302400021 PER-CENT 2281302400022 2.9 2281302400023 ENDCOMMON 3 0 2281302400024 DATA 3 9 2281302400025 EN-MIN EN-MAX DATA 2281302400026 KEV KEV B 2281302400027 10. 15. 6.3 2281302400028 15. 20. 7.1 2281302400029 20. 30. 6.6 2281302400030 30. 40. 7.2 2281302400031 40. 60. 7.2 2281302400032 60. 80. 7.5 2281302400033 80. 100. 7.2 2281302400034 100. 150. 7.5 2281302400035 150. 200. 7.4 2281302400036 ENDDATA 11 0 2281302400037 ENDSUBENT 36 0 2281302499999 SUBENT 22813025 20121231 22342281302500001 BIB 7 16 2281302500002 REACTION (48-CD-116(N,TOT),,SIG,,AV) Averaged over energy 2281302500003 interval given in data section 2281302500004 METHOD (TOF) Flight base is 260 cm 2281302500005 DETECTOR (GLASD) Li-6 glass detector 2281302500006 SAMPLE (48-CD-116,ENR=0.9240) .Cadmium metallic pellets 2281302500007 without canning,diameter 14.8 mm, thickness 2281302500008 2.7 mm (11.941E-3 atoms/barn), weight 3.9942 gram. 2281302500009 Cd-110 content is 0.57%, Cd-111 content is 0.60%, 2281302500010 Cd-112 content is 1.72%, Cd-113 content is 1.10%, 2281302500011 Cd-114 content is 3.61% Cd-116 content is 92.40%. 2281302500012 ERR-ANALYS (DATA-ERR) The quoted uncertainties were obtained 2281302500013 under the assumption that they are inversely 2281302500014 proportional to the fraction of neutrons interacting 2281302500015 in the sample, A=1-T, where T is the transmission. 2281302500016 STATUS (TABLE) Data from table III of PR/C,66,(2),025801 2281302500017 HISTORY (20121231U) SD: ERR-ANALYS update. 2281302500018 ENDBIB 16 0 2281302500019 COMMON 1 3 2281302500020 DATA-ERR 2281302500021 PER-CENT 2281302500022 2.1 2281302500023 ENDCOMMON 3 0 2281302500024 DATA 3 9 2281302500025 EN-MIN EN-MAX DATA 2281302500026 KEV KEV B 2281302500027 10. 15. 4.8 2281302500028 15. 20. 6.2 2281302500029 20. 30. 6.1 2281302500030 30. 40. 5.6 2281302500031 40. 60. 6.7 2281302500032 60. 80. 6.6 2281302500033 80. 100. 7.1 2281302500034 100. 150. 7.2 2281302500035 150. 200. 7.1 2281302500036 ENDDATA 11 0 2281302500037 ENDSUBENT 36 0 2281302599999 SUBENT 22813026 20121231 22342281302600001 BIB 6 10 2281302600002 REACTION (6-C-12(N,TOT),,SIG,,AV) Averaged over energy 2281302600003 interval given in data section 2281302600004 METHOD (TOF) Flight base is 260 cm 2281302600005 DETECTOR (GLASD) Li-6 glass detector 2281302600006 ERR-ANALYS (DATA-ERR) The quoted uncertainties were obtained 2281302600007 under the assumption that they are inversely 2281302600008 proportional to the fraction of neutrons interacting 2281302600009 in the sample, A=1-T, where T is the transmission. 2281302600010 STATUS (TABLE) Data from table III of PR/C,66,(2),025801 2281302600011 HISTORY (20121231U) SD: ERR-ANALYS update. 2281302600012 ENDBIB 10 0 2281302600013 COMMON 1 3 2281302600014 DATA-ERR 2281302600015 PER-CENT 2281302600016 2. 2281302600017 ENDCOMMON 3 0 2281302600018 DATA 3 9 2281302600019 EN-MIN EN-MAX DATA 2281302600020 KEV KEV B 2281302600021 10. 15. 4.47 2281302600022 15. 20. 4.98 2281302600023 20. 30. 4.78 2281302600024 30. 40. 4.74 2281302600025 40. 60. 4.75 2281302600026 60. 80. 4.68 2281302600027 80. 100. 4.58 2281302600028 100. 150. 4.40 2281302600029 150. 200. 4.15 2281302600030 ENDDATA 11 0 2281302600031 ENDSUBENT 30 0 2281302699999 SUBENT 22813027 20121231 22342281302700001 BIB 6 10 2281302700002 REACTION (79-AU-197(N,TOT),,SIG,,AV) Averaged over energy 2281302700003 interval given in data section 2281302700004 METHOD (TOF) Flight base is 260 cm 2281302700005 DETECTOR (GLASD) Li-6 glass detector 2281302700006 ERR-ANALYS (DATA-ERR) The quoted uncertainties were obtained 2281302700007 under the assumption that they are inversely 2281302700008 proportional to the fraction of neutrons interacting 2281302700009 in the sample, A=1-T, where T is the transmission. 2281302700010 STATUS (TABLE) Data from table III of PR/C,66,(2),025801 2281302700011 HISTORY (20121231U) SD: ERR-ANALYS update. 2281302700012 ENDBIB 10 0 2281302700013 COMMON 1 3 2281302700014 DATA-ERR 2281302700015 PER-CENT 2281302700016 8. 2281302700017 ENDCOMMON 3 0 2281302700018 DATA 3 9 2281302700019 EN-MIN EN-MAX DATA 2281302700020 KEV KEV B 2281302700021 10. 15. 12.9 2281302700022 15. 20. 15.4 2281302700023 20. 30. 13.6 2281302700024 30. 40. 12.5 2281302700025 40. 60. 11.6 2281302700026 60. 80. 11.3 2281302700027 80. 100. 10.6 2281302700028 100. 150. 10.5 2281302700029 150. 200. 9.8 2281302700030 ENDDATA 11 0 2281302700031 ENDSUBENT 30 0 2281302799999 ENDENTRY 27 0 2281399999999