ENTRY G0060 20210526 G047G006000000001 SUBENT G0060001 20210526 G047G006000100001 BIB 9 40 G006000100002 TITLE Dipole strength distribution in 206Pb for the G006000100003 evaluation of the neutron capture cross section of G006000100004 205Pb G006000100005 AUTHOR (T.Shizuma, N.Iwamoto, A.Makinaga, R.Massarczyk, G006000100006 R.Schwengner, R.Beyer, D.Bemmerer, M.Dietz, G006000100007 A.Junghans, T.Koegler, F.Ludwig, S.Reinicke, S.Schulz,G006000100008 S.Urlass, A.Wagner) G006000100009 INSTITUTE (2JPNIRS,2JPNJAE,2JPNHOK,1USALAS,2GERZFK) G006000100010 (2JPNJPN) JEIN Institute for Fundamental Science, KyotoG006000100011 REFERENCE (J,PR/C,98,064317,2018) G006000100012 FACILITY (LINAC,2GERZFK) ELBE G006000100013 INC-SOURCE (BRST) Ee=10.5 MeV (470 uA in average, micropulse G006000100014 repetition rate of 13 MHz) on Nb foil (5 um thick). G006000100015 The bremsstrahlung was collimated by an Al collimator G006000100016 with a length of 2.6 m and an opening angle of 5 mrad.G006000100017 Low-energy part of the bremsstrahlung spectrum was G006000100018 reduced by Al absorber (10 cm thick) behind the Nb G006000100019 radiator. G006000100020 SAMPLE (82-PB-206,ENR=0.993) G006000100021 3940 mg enriched 206Pb disk (20 mm diam., tilted by G006000100022 45 deg). G006000100023 (5-B-11,ENR=0.995) G006000100024 400 mg enriched 11B disk (20 mm in diam.) for flux G006000100025 determination G006000100026 DETECTOR (HPGE) Four HPGe detectors with relative efficiencies G006000100027 of 100% and 60%. G006000100028 Two HPGe detectors at 90 deg relative to the photon G006000100029 beam direction and at distance of 28 cm from the G006000100030 target. G006000100031 Two HPGe detectors at 127 deg relative to the photon G006000100032 beam direction and at distance of 32 cm from the G006000100033 target. G006000100034 Absorbers (8 mm Pb+3 mm Cu at 90 deg, 3 mm Pb+3 mm Cu G006000100035 at 127 deg) were placed in front of HPGe detectors G006000100036 to reduce the count rate due to low-energy photons. G006000100037 (BGO) All HPGe detectors were surrounded by BGO G006000100038 scintillation detectors. G006000100039 HISTORY (20181229C) On G006000100040 (20190110R) On. Data received from T.Shizuma G006000100041 (20210526A) On. Major revision in 003. G006000100042 ENDBIB 40 0 G006000100043 NOCOMMON 0 0 G006000100044 ENDSUBENT 43 0 G006000199999 SUBENT G0060002 20190108 G043G0060 2 1 BIB 4 24 G0060 2 2 REACTION 1(82-PB-206(G,0),,EN) G0060 2 3 Measured at 127 deg G0060 2 4 2((82-PB-206(G,EL)82-PB-206,,DA,,RES)// G0060 2 5 (82-PB-206(G,EL)82-PB-206,,DA,,RES)) G0060 2 6 90 deg/127 deg intensity ratio G0060 2 7 3(82-PB-206(G,0),,J) G0060 2 8 4((82-PB-206(G,EL),,WID,,SQ)/(82-PB-206(G,SCT),,WID)) G0060 2 9 5((82-PB-206(G,EL),,WID)/(82-PB-206(G,SCT),,WID)) G0060 2 10 Elastic scattering branching ratio G0060 2 11 FLAG (1.) Transition into the ground state coincides with a G0060 2 12 possible branch of the state at 5580 keV. G0060 2 13 (2.) Possible branch to the first 2+ state coincides G0060 2 14 with the transition at 4778 keV. G0060 2 15 (3.) Transition into the ground state coincides with a G0060 2 16 possible branch of the state at 7881 keV. G0060 2 17 (4.) Possible branch to the first 2+ state coincides G0060 2 18 with the transition at 7078 keV. G0060 2 19 ERR-ANALYS1(DATA-ERR) Peak fitting error G0060 2 20 2(DATA-ERR) No information on source of uncertainty G0060 2 21 4(DATA-ERR) Statistical and systematic uncertainties G0060 2 22 (associated with strength normalization, photon flux, G0060 2 23 and efficiency) G0060 2 24 5(DATA-ERR) No information on source of uncertainty G0060 2 25 STATUS (TABLE) Table I of Phys.Rev.C98(2018)064317 G0060 2 26 ENDBIB 24 0 G0060 2 27 COMMON 2 3 G0060 2 28 ANG-NM 2ANG-DN 2 G0060 2 29 ADEG ADEG G0060 2 30 90. 127. G0060 2 31 ENDCOMMON 3 0 G0060 2 32 DATA 10 88 G0060 2 33 DATA 1DATA-ERR 1DATA 2DATA-ERR 2DATA 3DATA 4G0060 2 34 DATA-ERR 4DATA 5DATA-ERR 5FLAG G0060 2 35 KEV KEV NO-DIM NO-DIM NO-DIM EV G0060 2 36 EV NO-DIM NO-DIM NO-DIM G0060 2 37 3742.7 0.2 0.35 0.14 1. 0.13 G0060 2 38 0.02 1.0 G0060 2 39 4115.2 0.1 2.09 0.20 2. 0.21 G0060 2 40 0.02 1.0 G0060 2 41 4146.1 0.7 1.3 0.3 1. 0.05 G0060 2 42 0.02 1.0 G0060 2 43 4328.0 0.1 0.66 0.11 1. 0.33 G0060 2 44 0.03 1.0 G0060 2 45 4603.8 0.1 0.63 0.15 1. 0.30 G0060 2 46 0.03 1.0 G0060 2 47 4690.7 0.2 0.8 0.3 1. 0.13 G0060 2 48 0.02 1.0 G0060 2 49 4778.2 0.5 0.83 0.11 1. 0.48 G0060 2 50 0.12 0.85 0.06 1. G0060 2 51 4805.2 0.3 0.8 0.4 1. 0.06 G0060 2 52 0.01 1.0 G0060 2 53 4932.6 0.3 3.0 0.9 2. 0.07 G0060 2 54 0.01 1.0 G0060 2 55 4971.1 0.1 0.93 0.15 1. 0.71 G0060 2 56 0.05 1.0 G0060 2 57 5037.8 0.1 0.79 0.07 1. 2.33 G0060 2 58 0.16 0.92 0.05 G0060 2 59 5127.6 0.2 0.86 0.19 1. 0.23 G0060 2 60 0.03 1.0 G0060 2 61 5377.2 0.3 0.92 0.21 1. 0.23 G0060 2 62 0.05 1.0 G0060 2 63 5459.0 0.5 0.61 0.23 1. 0.14 G0060 2 64 0.03 0.48 0.10 G0060 2 65 5470.2 0.1 0.82 0.12 1. 0.49 G0060 2 66 0.04 1.0 G0060 2 67 5524.5 0.2 0.88 0.11 1. 0.56 G0060 2 68 0.06 1.0 G0060 2 69 5579.9 0.1 0.87 0.09 1. 1.23 G0060 2 70 0.09 1.0 2. G0060 2 71 5615.2 0.1 0.81 0.07 1. 1.77 G0060 2 72 0.12 0.91 0.05 G0060 2 73 5692.9 0.1 0.81 0.11 1. 0.88 G0060 2 74 0.07 1.0 G0060 2 75 5721.7 0.6 0.71 0.24 1. 0.19 G0060 2 76 0.05 0.57 0.08 G0060 2 77 5732.0 0.1 0.70 0.07 1. 0.99 G0060 2 78 0.12 1.0 G0060 2 79 5761.3 0.1 0.73 0.12 1. 0.72 G0060 2 80 0.06 1.0 G0060 2 81 5799.3 0.1 0.86 0.09 1. 2.16 G0060 2 82 0.16 1.0 G0060 2 83 5818.3 0.3 0.84 0.24 1. 0.18 G0060 2 84 0.04 1.0 G0060 2 85 5845.8 0.1 0.89 0.10 1. 0.99 G0060 2 86 0.08 1.0 G0060 2 87 5857.0 0.1 0.85 0.08 1. 1.79 G0060 2 88 0.13 1.0 G0060 2 89 5902.4 0.1 0.77 0.06 1. 2.88 G0060 2 90 0.20 1.0 G0060 2 91 5951.4 0.6 0.54 0.24 1. 0.13 G0060 2 92 0.05 1.0 G0060 2 93 5959.4 0.6 1.06 0.11 1. 0.53 G0060 2 94 0.14 1.0 G0060 2 95 5999.4 0.6 1.00 0.16 1. 0.18 G0060 2 96 0.04 1.0 G0060 2 97 6019.7 0.2 1.07 0.14 1. 0.73 G0060 2 98 0.06 1.0 G0060 2 99 6100.3 0.6 1.33 0.16 1. 0.24 G0060 2 100 0.05 1.0 G0060 2 101 6149.1 0.5 0.7 0.3 1. 0.16 G0060 2 102 0.04 1.0 G0060 2 103 6185.8 0.6 2.1 0.5 2. 0.16 G0060 2 104 0.02 1.0 G0060 2 105 6200.0 0.8 1.1 0.4 1. 0.20 G0060 2 106 0.05 1.0 G0060 2 107 6409.1 0.2 0.86 0.11 1. 0.96 G0060 2 108 0.09 1.0 G0060 2 109 6419.8 0.2 0.89 0.13 1. 0.82 G0060 2 110 0.07 1.0 G0060 2 111 6432.5 0.3 0.98 0.18 1. 0.58 G0060 2 112 0.06 1.0 G0060 2 113 6442.6 0.5 0.79 0.22 1. 0.38 G0060 2 114 0.05 1.0 G0060 2 115 6458.8 0.6 0.55 0.14 1. 0.36 G0060 2 116 0.08 1.0 G0060 2 117 6467.8 0.2 0.84 0.12 1. 0.76 G0060 2 118 0.09 0.83 0.05 G0060 2 119 6508.6 0.1 0.87 0.11 1. 1.79 G0060 2 120 0.14 1.0 G0060 2 121 6531.3 0.2 0.91 0.16 1. 0.34 G0060 2 122 0.05 1.0 G0060 2 123 6691.9 0.3 1.15 0.25 1. 0.37 G0060 2 124 0.05 1.0 G0060 2 125 6723.5 0.1 0.78 0.07 1. 3.12 G0060 2 126 0.22 0.86 0.05 G0060 2 127 6819.7 0.1 0.75 0.06 1. 3.88 G0060 2 128 0.27 1.0 G0060 2 129 6933.8 0.1 0.73 0.09 1. 1.65 G0060 2 130 0.13 1.0 G0060 2 131 7061.5 0.1 0.76 0.10 1. 3.14 G0060 2 132 0.27 1.0 G0060 2 133 7077.6 0.2 0.63 0.11 1. 1.83 G0060 2 134 0.19 0.74 0.06 3. G0060 2 135 7128.2 0.2 0.89 0.15 1. 1.20 G0060 2 136 0.12 1.0 G0060 2 137 7158.5 0.5 0.88 0.20 1. 0.79 G0060 2 138 0.11 1.0 G0060 2 139 7181.1 0.4 0.72 0.14 1. 0.85 G0060 2 140 0.10 1.0 G0060 2 141 7199.8 0.3 0.67 0.10 1. 1.61 G0060 2 142 0.15 1.0 G0060 2 143 7238.7 0.6 0.71 0.22 1. 0.57 G0060 2 144 0.10 1.0 G0060 2 145 7258.6 0.4 0.85 0.17 1. 0.90 G0060 2 146 0.11 1.0 G0060 2 147 7302.6 0.3 0.79 0.12 1. 1.90 G0060 2 148 0.18 1.0 G0060 2 149 7312.6 0.3 0.76 0.12 1. 1.89 G0060 2 150 0.18 1.0 G0060 2 151 7338.2 0.7 0.9 0.4 1. 1.06 G0060 2 152 0.42 1.0 G0060 2 153 7362.9 0.3 0.62 0.18 1. 0.52 G0060 2 154 0.09 1.0 G0060 2 155 7387.5 0.2 0.97 0.16 1. 0.87 G0060 2 156 0.09 1.0 G0060 2 157 7404.5 0.3 0.92 0.17 1. 0.61 G0060 2 158 0.07 1.0 G0060 2 159 7414.1 0.3 0.83 0.14 1. 0.79 G0060 2 160 0.08 1.0 G0060 2 161 7424.1 0.2 1.07 0.13 1. 1.32 G0060 2 162 0.12 1.0 G0060 2 163 7464.8 0.5 0.8 0.5 1. 2.19 G0060 2 164 0.53 1.0 G0060 2 165 7486.1 0.2 0.93 0.12 1. 1.91 G0060 2 166 0.17 1.0 G0060 2 167 7493.5 0.3 0.79 0.13 1. 1.19 G0060 2 168 0.12 1.0 G0060 2 169 7505.9 0.1 0.68 0.09 1. 2.00 G0060 2 170 0.16 0.66 0.04 G0060 2 171 7542.9 0.1 0.86 0.08 1. 3.28 G0060 2 172 0.24 1.0 G0060 2 173 7556.4 0.4 0.79 0.25 1. 0.48 G0060 2 174 0.07 1.0 G0060 2 175 7571.4 0.3 0.91 0.14 1. 0.65 G0060 2 176 0.09 1.0 G0060 2 177 7597.3 1.4 0.91 0.21 1. 0.27 G0060 2 178 0.08 1.0 G0060 2 179 7627.6 0.5 0.88 0.13 1. 0.53 G0060 2 180 0.13 1.0 G0060 2 181 7645.9 0.3 0.66 0.18 1. 0.31 G0060 2 182 0.07 1.0 G0060 2 183 7669.7 0.3 0.7 0.3 1. 0.50 G0060 2 184 0.09 1.0 G0060 2 185 7715.5 0.4 0.68 0.19 1. 1.10 G0060 2 186 0.16 1.0 G0060 2 187 7781.1 0.3 0.61 0.12 1. 0.68 G0060 2 188 0.12 1.0 G0060 2 189 7798.4 0.7 0.59 0.12 1. 0.58 G0060 2 190 0.13 1.0 G0060 2 191 7815.4 0.3 0.79 0.09 1. 1.60 G0060 2 192 0.20 0.87 0.05 G0060 2 193 7845.5 0.3 0.84 0.28 1. 1.83 G0060 2 194 0.22 0.71 0.07 G0060 2 195 7881.1 0.3 0.87 0.10 1. 1.46 G0060 2 196 0.13 1.0 4. G0060 2 197 7891.2 0.2 0.76 0.08 1. 1.95 G0060 2 198 0.16 0.55 0.04 G0060 2 199 7904.3 0.2 0.74 0.08 1. 2.47 G0060 2 200 0.20 0.70 0.04 G0060 2 201 7930.3 0.7 1.0 0.3 1. 0.43 G0060 2 202 0.11 1.0 G0060 2 203 7944.7 0.4 0.89 0.17 1. 0.75 G0060 2 204 0.12 1.0 G0060 2 205 8001.6 0.3 0.74 0.10 1. 2.64 G0060 2 206 0.30 1.0 G0060 2 207 8046.5 0.4 0.87 0.08 1. 0.79 G0060 2 208 0.17 1.0 G0060 2 209 8079.8 0.7 0.88 0.11 1. 0.41 G0060 2 210 0.09 1.0 G0060 2 211 8118.5 0.4 0.82 0.10 1. 0.37 G0060 2 212 0.08 1.0 G0060 2 213 ENDDATA 180 0 G0060 2 214 ENDSUBENT 213 0 G0060 299999 SUBENT G0060003 20210526 G047G006000300001 BIB 6 12 G006000300002 REACTION (82-PB-206(G,SCT)82-PB-206,,SIG) G006000300003 ANALYSIS Absorption (scattering) cross section was derived by G006000300004 dividing the (g,g0) elastic scattering cross section G006000300005 by the ground state transition branching ratio. G006000300006 CORRECTION Selection of ground state transitions and estimation G006000300007 of ground state transition branching ratios were done G006000300008 by simulating gamma-ray cascades by the Monte Carlo G006000300009 code DICEBOX with the level schemes obtained by the G006000300010 code gammaDEX. G006000300011 ERR-ANALYS (DATA-ERR) No information on the source of uncertainty G006000300012 STATUS (TABLE) Plotted in Fig.6 of Phys.Rev.C98(2018)064317 G006000300013 HISTORY (20210526A) On. REACTION(SF1,SF4): 32-GE-74->82-PB-206 G006000300014 ENDBIB 12 0 G006000300015 NOCOMMON 0 0 G006000300016 DATA 3 35 G006000300017 EN DATA DATA-ERR G006000300018 MEV MB MB G006000300019 4.6 10. 9. G006000300020 4.7 14. 8. G006000300021 4.8 9. 7. G006000300022 4.9 9. 7. G006000300023 5.0 40. 13. G006000300024 5.1 25. 8. G006000300025 5.2 25. 7. G006000300026 5.3 29. 7. G006000300027 5.4 26. 5. G006000300028 5.5 30. 6. G006000300029 5.6 32. 6. G006000300030 5.7 26. 3. G006000300031 5.8 22.3 1.7 G006000300032 5.9 26.7 2.3 G006000300033 6.0 16.3 1.3 G006000300034 6.1 16.8 1.2 G006000300035 6.2 23.1 1.9 G006000300036 6.3 24.8 2.1 G006000300037 6.4 28.1 2.8 G006000300038 6.5 39. 3. G006000300039 6.6 39. 3. G006000300040 6.7 38. 4. G006000300041 6.8 50. 4. G006000300042 6.9 47. 4. G006000300043 7.0 53. 4. G006000300044 7.1 59. 4. G006000300045 7.2 59. 4. G006000300046 7.3 58. 6. G006000300047 7.4 54. 5. G006000300048 7.5 69. 5. G006000300049 7.6 49. 5. G006000300050 7.7 50. 4. G006000300051 7.8 54. 5. G006000300052 7.9 51. 5. G006000300053 8.0 41. 5. G006000300054 ENDDATA 37 0 G006000300055 ENDSUBENT 54 0 G006000399999 ENDENTRY 3 0 G006099999999