221TH 208PB(16O,3NG):XUNDL-1 2013TA12 201305 221TH c Compiled (unevaluated) data set from 2013Ta12: 221TH2c Phys Rev C 87, 034319 (2013) 221TH c Compiled by B. Singh (McMaster); May 13, 2013 221TH c E=86 MeV. Measured E|g, I|g, |g|g, |g|g(|q)(DCO) using 14UD BARC-TIFR 221TH2c Pelletron facility and INGA array of 19 Compton-suppressed Clover Ge 221TH3c detectors. Reflection asymmetric octupole structures were observed. 221TH4c Comparison with cranking model calculations including octupole 221TH5c deformation 221TH d Details of gamma-ray data were requested from the first author 221TH2d on March 31, 2013, but none received as of May 13, 2013 221TH cG $ DCO ratios obtained for 90|', 157|' geometry. With gates on 221TH2cG stretched quadrupole transitions, expected DCO values are 1.0 221TH3cG for stretched quadrupoles and 0.5 for stretched dipoles 221TH cL E$ From least-squares fit (by compiler) to E|g data, assuming 221TH2cL 1 keV uncertainty for each |g ray 221TH CL BAND(A)$ Band based on (7/2)+. 221TH2cL This band and the one based on (13/2)- form a parity-doublet 221TH3cL octupole structure 221TH CL BAND(B)$ Band based on (13/2)-. 221TH2cL This band and the one based on (7/2)+ form a parity-doublet 221TH3cL octupole structure 221TH CL BAND(C)$ Band based on (13/2+). 221TH2cL This band and the one based on (15/2-) form a parity-doublet 221TH3cL octupole structure 221TH CL BAND(D)$ Band based on (15/2-). 221TH2cL This band and the one based on (13/2+) form a parity-doublet 221TH3cL octupole structure 221TH L 0.0 (7/2)+ A 221TH L 251.0 10(11/2)+ A 221TH G 251 221TH L 488.1 13 (13/2)- B 221TH G 237.1 221TH L 573.0 13(15/2)+ A 221TH G 85 221TH G 322 221TH L 736.0 13(13/2+) C 221TH G 485 D 221TH2 G DCO=0.60 7 221TH L 747.1 13(17/2)- B 221TH G 174 D 221TH2 G DCO=0.56 2 221TH G 259 221TH L 946.9 14(19/2)+ A 221TH G 200 D 221TH2 G DCO=0.53 3 221TH G 374 221TH L 991.0 13(15/2-) D 221TH G 255 221TH G 503 221TH L 1079.2 14(21/2)- B 221TH G 132 221TH G 332 221TH L 1143.0 13(17/2+) C 221TH G 152 221TH G 407 221TH G 570 221TH L 1356.5 15(23/2)+ A 221TH G 277 221TH G 410 221TH L 1365.1 14(19/2-) D 221TH G 222 221TH G 374 ? 221TH G 618 221TH L 1472.3 16(25/2)- B 221TH G 116 221TH G 393 221TH L 1608.1 14(21/2+) C 221TH G 243 221TH G 465 221TH L 1776.6 16(27/2)+ A 221TH G 304 221TH G 420 221TH L 1792.1 15(23/2-) D 221TH G 184 221TH G 427 221TH G 713 221TH L 1935.9 17 (29/2)- B 221TH G 159 221TH G 464 221TH L 1954.1 16(25/2+) C 221TH G 162 221TH G 346 221TH L 2209.8 18 (31/2)+ A 221TH G 274 221TH G 433 221TH L 2444.8 18 (33/2)- B 221TH G 235 221TH G 509 221TH L 2683.8 19 (35/2)+ A 221TH G 239 221TH G 474 221TH L 3196.8 22 (39/2)+ A 221TH G 513 221TH 207PB(18O,4NG):XUNDL-2 2014RE12 201410 221TH c Compiled (unevaluated) dataset from 2014Re12: 221TH2c Phys Rev C 90, 044318 (2014) 221TH c Compiled by B. Singh (McMaster); Oct 21, 2014 221TH c E({+18}O)=96 MeV. Measured E|g, I|g, |g|g, (particle)|g-coin, |g(|q) 221TH2c using Gammasphere array comprising 98 HPGe detectors with BGO 221TH3c Compton-suppression shields, and HERCULES evaporation residue detector 221TH4c of 64 elements at ATLAS-ANL facility. Target=92.8% enriched 470 221TH5c |mg/cm{+2} thick foil with a 7 |mg/cm{+2} thick carbon layer facing the 221TH6c beam. Deduced high-spin levels, J, |p, bands, B(M1)/B(E2) and 221TH7c B(E1)/B(E2) ratios, octupole correlations from interconnected 221TH8c alternating parity levels, alignments, and parity splittings. 221TH c Three parity-doublet octupole bands are reported in this work 221TH cG RI$Values are relative to 75 for the 250.9-keV ground-state transition 221TH cL E$ From least-squares fit (by compiler) to E|g data 221TH cL J$From |g(|q) data in 2014Re12 and band structures, assuming all 221TH2cL transitions are stretched E1, M1 or E2. 221TH CL BAND(A)$ Band based on 7/2+. 221TH2cL This band and the one based on 13/2- form a parity-doublet 221TH3cL octupole structure 221TH CL BAND(B)$ Band based on 13/2-. 221TH2cL This band and the one based on 7/2+ form a parity-doublet 221TH3cL octupole structure 221TH CL BAND(C)$Sequence based on 15/2-. 221TH2cL This sequence and the one based on 13/2+ form a parity-doublet 221TH3cL octupole structure 221TH CL BAND(D)$Sequence based on 13/2+. 221TH2cL This sequence and the one based on 15/2- form a parity-doublet 221TH3cL octupole structure 221TH CL BAND(E)$Sequence based on 21/2-. 221TH2cL This sequence of two levels and the one based on 23/2+ possibly form a 221TH3cL parity-doublet octupole structure 221TH CL BAND(F)$Sequence based on 23/2+. 221TH2cL This sequence of two levels and the one based on 21/2- possibly form a 221TH3cL parity-doublet octupole structure 221TH PN 5 221TH G 141.9 2 1.1 2 221TH L 0.0 7/2+ A 221TH L 250.90 10 11/2+ A 221TH G 250.9 1 75.0 30 221TH2 G A2=+0.152 29 $ A4=-0.035 34 221TH L 487.86 17 13/2- B 221TH G 237.1 2 35.9 19 221TH2 G A2=-0.183 14 $ A4=+0.014 17 221TH L 572.83 14 15/2+ A 221TH G 84.9 2 11.9 9 221TH2 G A2=-0.159 18 $ A4=+0.029 21 221TH G 321.9 1 34.9 12 221TH2 G A2=+0.201 20 $ A4=-0.007 26 221TH L 736.83 20 13/2+ D 221TH G 485.9 2 6.4 5 M1+E2 +0.10 +4-6 221TH2 G A2=-0.145 41 $ A4=+0.085 50 221TH L 746.78 16 17/2- B 221TH G 173.9 1 37.0 14 221TH2 G A2=-0.201 19 $ A4=+0.016 23 221TH G 259.1 2 2.6 2 221TH L 946.41 19 19/2+ A 221TH G 199.8 2 24.6 10 221TH2 G A2=-0.174 20 $ A4=+0.020 26 221TH G 373.6 2 8.3 3 221TH2 G A2=+0.149 41 $ A4=-0.067 54 221TH L 991.13 22 15/2- C 221TH G 254.4 3 2.4 3 221TH2 G A2=-0.186 30 $ A4=+0.030 39 221TH G 503.3 3 1.4 2 221TH2 G A2=-0.102 15 221TH L 1078.47 20 21/2- B 221TH G 132.1 2 17.3 9 221TH2 G A2=-0.190 23 $ A4=+0.028 30 221TH G 331.5 2 12.4 5 221TH2 G A2=+0.207 27 $ A4=-0.030 32 221TH L 1096.9 11 ? 221TH G 609 1 0.8 3 ? 221TH L 1143.48 21 17/2+ D 221TH G 152.3 2 1.6 2 221TH2 G A2=-0.188 27 $ A4=+0.023 37 221TH G 406.5 3 1.4 2 221TH2 G A2=+0.123 30 $ A4=-0.035 40 221TH G 570.7 3 1.5 3 221TH2 G A2=-0.29 20 221TH L 1355.81 24 23/2+ A 221TH G 277.4 2 15.1 6 221TH2 G A2=-0.178 16 $ A4=+0.022 23 221TH G 409.5 3 1.8 2 221TH2 G A2=+0.237 21 $ A4=-0.041 30 221TH L 1365.09 23 19/2- C 221TH G 221.5 2 3.6 3 221TH2 G A2=-0.178 31 $ A4=+0.043 58 221TH G 374.2 3 1.3 3 221TH2 G A2=+0.226 35 221TH G 618.3 4 3.3 4 M1+E2 +0.10 +4-8 221TH2 G A2=-0.103 20 $ A4=+0.076 26 221TH L 1442.1 3 21/2- E 221TH G 695.3 3 1.9 2 221TH2 G A2=+0.394 83 $ A4=-0.11 10 221TH L 1471.83 25 25/2- B 221TH G 116.0 2 5.7 4 221TH2 G A2=-0.202 26 $ A4=+0.036 37 221TH G 393.3 2 13.7 6 221TH2 G A2=+0.266 29 $ A4=-0.028 37 221TH L 1541.8 4 (21/2) 221TH G 595.4 3 0.7 2 221TH L 1607.84 25 21/2+ D 221TH G 242.6 2 3.2 3 221TH2 G A2=-0.207 28 $ A4=+0.032 37 221TH G 464.4 3 1.4 3 221TH L 1625.8 11 19/2 221TH G 879 1 0.9 2 221TH2 G A2=-0.28 11 221TH L 1688.5 3 23/2+ F 221TH G 246.4 3 1.2 2 221TH2 G A2=-0.294 88 $ A4=-0.03 11 221TH G 742.6 5 1.0 3 221TH2 G A2=+0.368 79 $ A4=-0.064 93 221TH L 1776.2 3 27/2+ A 221TH G 304.4 2 11.4 5 221TH2 G A2=-0.251 32 $ A4=+0.033 38 221TH G 420.6 3 1.3 2 221TH2 G A2=+0.284 43 221TH L 1792.2 3 23/2- C 221TH G 184.3 2 3.2 3 221TH2 G A2=-0.214 34 $ A4=+0.023 44 221TH G 427.4 3 2.3 4 221TH G 713.5 4 2.4 3 M1+E2 +0.10 +3-6 221TH2 G A2=-0.142 36 $ A4=+0.088 47 221TH L 1813.6 3 25/2- E 221TH G 125.3 2 1.0 2 221TH2 G A2=-0.277 55 $ A4=+0.041 88 221TH G 371.4 4 0.9 2 221TH G 735.0 3 2.7 3 221TH2 G A2=+0.315 34 $ A4=-0.089 47 221TH L 1845.4 11 21/2 221TH G 899 1 0.8 2 221TH2 G A2=-0.34 11 221TH L 1919.5 11 (23/2) 221TH G 841 1 0.8 2 221TH L 1935.2 3 29/2- B 221TH G 159.2 2 5.0 3 221TH2 G A2=+0.200 31 $ A4=+0.023 39 221TH cG $Positive A{-2} is inconsistent with |DJ=1, E1 for 159.2|g; sign 221TH2cG of A{-2} is possibly a misprint in table I of 2014Re12. 221TH2cG (Compiler's comment) 221TH G 463.3 2 9.6 5 221TH2 G A2=+0.290 11 $ A4=-0.041 13 221TH L 1953.9 4 25/2+ D 221TH G 161.9 3 3.4 4 221TH2 G A2=-0.235 31 $ A4=+0.039 39 221TH G 345.6 4 0.8 1 221TH G 599 1 0.7 2 ? 221TH L 1984.0 4 25/2(+) 221TH G 191.8 3 1.4 2 221TH2 G A2=-0.219 32 $ A4=-0.005 43 221TH L 2064.6 11 27/2(+) F 221TH G 251 1 1.5 GE 221TH cG RI$lower limit due to the presence of an unresolved doublet 221TH2 G A2=-0.30 10 $ A4=+0.10 11 221TH cG $A{-2} and A{-4} values obtained from gate on 250.9|g are approximate 221TH L 2163.3 5 27/2(-) C 221TH G 209.4 3 1.3 2 221TH2 G A2=-0.55 30 221TH L 2204.8 11 (25/2) 221TH G 849 1 0.7 2 221TH L 2210.0 4 31/2+ A 221TH G 274.8 2 9.3 4 221TH2 G A2=-0.200 46 $ A4=-0.025 60 221TH G 433.7 3 1.3 1 221TH2 G A2=+0.36 13 221TH L 2390.8 11 (27/2) ? 221TH G 919 1 0.5 2 ? 221TH L 2444.5 4 33/2- B 221TH G 234.5 3 6.5 4 221TH2 G A2=-0.195 26 $ A4=-0.003 36 221TH G 509.3 4 4.3 3 221TH2 G A2=+0.295 26 $ A4=-0.043 32 221TH L 2683.4 4 35/2+ A 221TH G 238.9 3 6.3 3 221TH2 G A2=-0.192 44 $ A4=+0.012 56 221TH G 473.4 4 2.9 2 221TH2 G A2=+0.268 40 $ A4=-0.033 49 221TH L 2970.9 5 37/2- B 221TH G 287.3 4 2.7 3 221TH2 G A2=-0.230 37 $ A4=+0.037 49 221TH G 526.5 4 1.4 2 221TH2 G A2=+0.34 10 221TH L 3196.4 5 39/2+ A 221TH G 225.4 4 1.7 3 221TH2 G A2=-0.218 52 $ A4=+0.052 69 221TH G 513.1 4 2.1 3 221TH2 G A2=+0.292 38 $ A4=-0.062 64 221TH L 3727.4 12 (43/2+) 221TH G 531 1 0.8 2 221TH 206PB(22NE,A3N):T1/2:XUNDL-3 2014LO10 201412 221TH c Compiled (unevaluated) dataset from 2014Lo10: 221TH c Eur Phys J A 50, 132 (2014) 221TH c Compiled by J.C. Batchelder (ORNL/ORAU), November 25, 2014 221TH c {+221}Th produced using the fusion evaporation reaction 221TH2c {+206}Pb({+22}Ne,|a3n), with 119 MeV {+22}Ne beam produced at FLNR 221TH3c facility (Dubna). Evaporation residue (Er) was separated using SHELS 221TH4c separator and then passed through a tof system and implanted into a 221TH5c DSSD in front of a HPGe. Position and time-correlated |a decays were 221TH6c used to identify Er. 221TH7c Measured E|a, I|a, E|g, |a|g-coin, and T{-1/2} of {+221}Th g.s. 221TH L 0.0 (7/2+) 1.78 MS 3 221TH cL J$from Adopted Levels of {+221}Th in ENSDF database 221TH cL T$obtained from a new alpha transition from {+221}Th decay 221TH2cL E|a=8243 keV. It is possible that this |a peak is the same as 221TH3cL the weak 8265 keV {I10} alpha group reported in 1990An10: 221TH4cL Zeit. Phys. A 337, 229 221TH 225U A DECAY:T:XUNDL-4 2019MI08 201909 221TH c Compiled (unevaluated) dataset from 2019Mi08: 221TH2c Nucl Phys A 987, 337 (2019) 221TH c Compiled by J. Chen (NSCL, MSU), May 28, 2019 221TH c 2019Mi08: {+225}U ions were produced by the fusion-evaporation 221TH2c reactions of E=212, 217, and 226 MeV (mid-target) {+48}Ca beams from 221TH3c the UNILAC accelerator at GSI on a |?530 |mg/cm{+2} {+181}Ta target 221TH4c sandwiched between carbon layers of 50 |mg/cm{+2} upstream and 10 221TH5c |mg/cm{+2} downstream. Evaporation residues (ERs) were separated by the 221TH6c SHIP velocity filter and implanted into the COMPAct Spectroscopy Set-up 221TH7c (COMPASS), consisting of a Double sided Silicon Strip Detector (DSSD), 221TH8c surrounded by 4 Single sided Silicon Strip Detectors (SSSDs). Measured 221TH9c energy and time spectra of correlations between Er and |a particles 221THAc from subsequent decays. Deduced halflife. 225U P 0.0 63 MS 7 8015 7 225U cP T$From time correlations between Er and subsequent |a decays 225U cP QP$From 2017Wa10 221TH N 1.0 221TH L 0 1.0 MS 2 221TH cL T$from time correlations between {+225}U |a decays and {+221}Th |a 221TH2cL decays 221TH A 7850 10 221TH 186W(40AR,2P3N):T:XUNDL-5 2021Hu19 202108 221TH c Compiled (unevaluated) dataset from 2021Hu19: Chin. Phys. C 45, 221TH2c 044003 (2021). 221TH c Compiled by S. Zhu, NNDC-BNL, July 14, 2021 221TH c 2021Hu19: {+221}Th was produced in {+186}W({+40}Ar,2p3n) with a beam 221TH2c at 198.7 MeV bombarding a {+186}W target with a thickness of 200 221TH3c |mg/cm{+2}; evaporation residues (Er) were separated in-flight by the 221TH4c gas-filled recoil separator SHANS and implanted in three 16-strip 221TH5c position-sensitive silicon detectors (PSSDs) mounted side-by-side at 221TH6c the focal plane. {+222}Pa was identified by Er-|a-|a-|a time and 221TH7c position correlations. Decay |g rays measured by two HPGe and one 221TH8c Clover HPGe detectors surrounding the focal plane. Measured E|a, I|a, 221TH9c T{-1/2} and E|g. 221TH L 0 (7/2+) 1.95 MS +38-27 221TH cL J$from Adopted levels of {+221}Th (2007Ja05). 221TH cL T$from 2021Hu19. 221TH 186W(40CA,X):T,EA:XUNDL-6 2019YA04 202205 221TH c Compiled (unevaluated) dataset from 2019Ya04: 221TH2c Eur. Phy. J A 55, 8 (2019) 221TH c Compiled by E.A. McCutchan (NNDC,BNL) April 28, 2022 221TH c E({+40}Ca)=206 MeV from the Sector-Focusing Cyclotron (SFC) 221TH2c of the Heavy Ion Research Facility in Lanzhou (HIRFL). 221TH3c Evaporation residues were identified 221TH4c and separated using SHANS separator and implanted into three 300-|mm 221TH5c double-sided silicon strip detectors. Measured E|a, I|a, 221TH6c (evaporation residue)|a correlations. Deduced T{-1/2} using digital 221TH7c pulse fitting method. 221TH L 0 2.28 US +70-43 221TH cL T$from 8152|a(t) (2019Ya04) 221TH cL $Measured E|a=8152 keV {I17} and E|a=8461 keV {I19} (2019Ya04) 221TH2cL extracted from pile-up traces. 221TH 208PB(18O,5N):XUNDL-7 2020PA44 202509 221TH c Compiled (unevaluated) dataset from 2020Pa44: Phys. Rev. C 102, 221TH2c 054335 (2020). 221TH c Compiled by G. G~urdal, April 17, 2024 221TH c {+221}Th was populated by the {+208}Pb({+18}O,5n) reaction at the 221TH2c Accelerator Laboratory of the University of Jyvaskyla in Finland. 95 221TH3c MeV {+18}O beam was incident upon a self-supporting 0.45 mg/cm{+2} 221TH4c thick {+208}Pb target. The target was located at the center of the 221TH5c SAGE spectrometer which was used to detect prompt |g rays and 221TH6c internal conversion electrons. Downstream of the target, recoiling 221TH7c evaporation residues were separated from fission fragments and 221TH8c unreacted beam ions using RITU gas-filled separator and were 221TH9c transported to its focal plane where the reaction products and their 221THac subsequent decays were studied using DSSDs, PIN-diode detectors and 221THbc Clover HPGe detectors, which are part of the GREAT spectrometer. The 221THcc reaction products were implanted into the DSSDs and the charged 221THdc particles emitted by the implanted nuclei were detected using 221THec PIN-diode detectors. X-rays and |g-rays emitted from implanted nuclei 221THfc were detected using 3 Clover HPGe detectors. Measured: Energy 221THgc deposited at DSSD, particle identification, E{-|a}, I{-|a}, 221THhc E{-|a+ce}, I{-|a+ce}, |Dt between implantation and |a-decay, E{-|g}, 221THic X-rays, I|g, |a|g coin., |g|g coin. Deduced: T{-1/2}. 221TH L 0 (7/2+) 1.73 MS 2 221TH cL $J{+|p} from the Adopted Levels of {+221}Th in ENSDF database. 221TH2cL T{-1/2} from 2020Pa44.