ENTRY B0129 20011220 0000B012900000001 SUBENT B0129001 20011220 0000B012900100001 BIB 9 43 B012900100002 TITLE Mechanism of Formation and Decay of the Compound B012900100003 Nuclei Gd-150 Produced by Two Entrance Channels B012900100004 (O-16 + BA-134) And (AR-40 + PD-110). B012900100005 AUTHOR (S.DELLA NEGRA, H.GAUVIN, H.JUNGCLAS, Y.LE BEYEC, B012900100006 M.LEFORT) B012900100007 INSTITUTE (2FR PAR) B012900100008 REFERENCE (J,ZP/A,282,65,1977) B012900100009 (J,ZP/A,282,75,1977). Comparison with Theory, See B012900100010 Add-Results. B012900100011 METHOD (EXTB,STTA,EDEG,BCINT) B012900100012 5 to 7 Different Beam Energy Values were Obtained by B012900100013 Tuning the Avf Cyclotron. Intermediate Energies were B012900100014 Obtained by Thin Al-Degraders. Their Thicknesses, B012900100015 Carefully Measured by Weighing and Alpha-Absorption, B012900100016 Were Chosen As to Never Exceed an Energy Loss of More B012900100017 Than 10%. Northcliffe and Schilling Tables (NUCL.DATA B012900100018 TABLES A7,233(1970)) Were Used to Calculate the Energy B012900100019 Loss. The Beam Energy was Determined Very Precisely B012900100020 Using Different Methods. B012900100021 The Targets were Placed at the Bottom of a Faraday Cup.B012900100022 At the Back of the Targets Al-Collectors were Placed B012900100023 Thick Enough to Stop the Recoiling Nuclei. B012900100024 (ACTIV) Iradiation and Cooling Times are Unknown. B012900100025 DETECTOR (GELI).Resolution 2.9 KeV. B012900100026 ADD-RES (COMP) B012900100027 From the Summation of All Individual Cross Sections B012900100028 A Complete Fusion Cross Section is Calculated. B012900100029 Complete Fusion Thresholds are Compared with B012900100030 Calculated Fusion Barriers. In the Secondary B012900100031 Reference a Systematic Comparison Between B012900100032 Experimental Excitation Functions and Results of B012900100033 Evaporation Calculations are Given. B012900100034 ERR-ANALYS (DATA-ERR) No Information About the Cross Section B012900100035 Errors is Given. Errors Quoted in the Data Section areB012900100036 In Most Cases Greater Than 15%. The Significance of B012900100037 These Errors is Uncertain. The Heavy Ion Energy was B012900100038 Known to Within 2% For the Individual Targets. B012900100039 HISTORY (19800325C)Nekw B012900100040 (19940718A) Some Corrections have Been Included by B012900100041 CAJAD B012900100042 (19981103A). Some Corrections For 'Reaction'. ConvertedB012900100043 To Lower Case. B012900100044 (20011219U) Last checking has been done. B012900100045 ENDBIB 43 0 B012900100046 NOCOMMON 0 0 B012900100047 ENDSUBENT 46 0 B012900199999 SUBENT B0129002 20011220 0000B012900200001 BIB 5 12 B012900200002 REACTION (56-BA-134(8-O-16,3N)64-GD-147,,SIG,,,EXP) B012900200003 RAD-DET (64-GD-147,DG) B012900200004 DECAY-DATA (64-GD-147,38.HR,DG,229.,0.57, B012900200005 DG,370.,0.132, B012900200006 DG,396.,0.262, B012900200007 DG,765.,0.095, B012900200008 DG,928.,0.165) B012900200009 FACILITY (ISOCY,2FR PAR) Variable Energy Cyclotron in Orsay. B012900200010 SAMPLE Ba-134 on Aluminium Backing, from 80% Enriched Barium B012900200011 Nitrate, Thickness 0.3 Mg/Cm**2. The Amount of Ba-134 B012900200012 Deposit was Measured After the Experiment by Isotope B012900200013 Dilution by Mass Spectrometry B012900200014 ENDBIB 12 0 B012900200015 NOCOMMON 0 0 B012900200016 DATA 3 9 B012900200017 EN DATA DATA-ERR B012900200018 MEV MB MB B012900200019 62.5 0.2 0.2 B012900200020 69. 149. 22. B012900200021 74. 214. 26. B012900200022 76.5 201. 28. B012900200023 82. 155. 22. B012900200024 83. 138. 18. B012900200025 89. 89. 11. B012900200026 95. 49. 6. B012900200027 101.5 22. 4. B012900200028 ENDDATA 11 0 B012900200029 ENDSUBENT 28 0 B012900299999 SUBENT B0129003 20011220 0000B012900300001 BIB 5 10 B012900300002 REACTION (56-BA-134(8-O-16,4N)64-GD-146,,SIG,,,EXP) B012900300003 RAD-DET (64-GD-146,DG) B012900300004 DECAY-DATA (64-GD-146,50.D,DG,114.8,0.45, B012900300005 DG,115.6,0.45, B012900300006 DG,154.,0.388) B012900300007 FACILITY (ISOCY,2FR PAR) Variable Energy Cyclotron in Orsay. B012900300008 SAMPLE Ba-134 on Aluminium Backing, from 80% Enriched Barium B012900300009 Nitrate, Thickness 0.3 Mg/Cm**2. The Amount of Ba-134 B012900300010 Deposit was Measured After the Experiment by Isotope B012900300011 Dilution by Mass Spectrometry B012900300012 ENDBIB 10 0 B012900300013 NOCOMMON 0 0 B012900300014 DATA 3 11 B012900300015 EN DATA DATA-ERR B012900300016 MEV MB MB B012900300017 69. 55. 7. B012900300018 74. 187. 28. B012900300019 76.5 197. 30. B012900300020 82. 439. B012900300021 83. 311. B012900300022 89. 516. 64. B012900300023 95. 382. 48. B012900300024 101.5 246. 32. B012900300025 106.5 134. 20. B012900300026 115. 37.8 7.6 B012900300027 116. 44.3 6.8 B012900300028 ENDDATA 13 0 B012900300029 ENDSUBENT 28 0 B012900399999 SUBENT B0129004 20011220 0000B012900400001 BIB 6 19 B012900400002 REACTION M(56-BA-134(8-O-16,5N)64-GD-145-M,,SIG,,,EXP) B012900400003 S(56-BA-134(8-O-16,5N)64-GD-145-G,M+,SIG,,,EXP) B012900400004 G(56-BA-134(8-O-16,5N)64-GD-145-G,,SIG,,,EXP) B012900400005 The Given Cross Section is Deduced from the B012900400006 Cross Sections For the Isomeric State and the Cross B012900400007 Section For the Sum of Isomeric and Groundstate. B012900400008 RAD-DET M(64-GD-145-M,DG) B012900400009 S(64-GD-145-G,DG) B012900400010 DECAY-DATAM(64-GD-145-M,85.SEC,DG,721.,0.83) Isomer Transition. B012900400011 S(64-GD-145-G,21.8MIN,DG,808.,0.091, B012900400012 DG,1041.,0.102, B012900400013 DG,1757.,0.346, B012900400014 DG,1880.,0.331) B012900400015 FACILITY (ISOCY,2FR PAR) Variable Energy Cyclotron in Orsay. B012900400016 SAMPLE Ba-134 on Aluminium Backing, from 80% Enriched Barium B012900400017 Nitrate, Thickness 0.3 Mg/Cm**2. The Amount of Ba-134 B012900400018 Deposit was Measured After the Experiment by Isotope B012900400019 Dilution by Mass Spectrometry B012900400020 STATUS G(DEP,B0129004) B012900400021 ENDBIB 19 0 B012900400022 NOCOMMON 0 0 B012900400023 DATA 7 14 B012900400024 EN DATA MDATA-ERR MDATA SDATA-ERR SDATA GB012900400025 DATA-ERR G B012900400026 MEV MB MB MB MB MB B012900400027 MB B012900400028 79. 11.6 4. B012900400029 B012900400030 79. 10.8 4. B012900400031 B012900400032 80.5 9. 3.6 13. 4.8 4.B012900400033 B012900400034 82. 15.7 6. 18.9 6.4 3.2B012900400035 B012900400036 82.5 28.7 6. B012900400037 B012900400038 89. 113.5 19. 145. 30. 32.B012900400039 B012900400040 95. 258. 38. 354. 62. 96.B012900400041 B012900400042 101.5 382. 42. 518. 58. 136.B012900400043 100. B012900400044 103. 394. 48. 443. 60. 49.B012900400045 B012900400046 106.5 352. 42. 472. 62. 120.B012900400047 104. B012900400048 107.5 289. 38. 378. 60. 89.B012900400049 B012900400050 114. 269. 40. 319. 54. 50.B012900400051 B012900400052 116. 185. 32. 202. 40. 17.B012900400053 B012900400054 123. 151. 153. 2.B012900400055 B012900400056 ENDDATA 32 0 B012900400057 ENDSUBENT 56 0 B012900499999 SUBENT B0129005 20011220 0000B012900500001 BIB 5 12 B012900500002 REACTION (56-BA-134(8-O-16,X)63-EU-147,(CUM),SIG,,,EXP) B012900500003 It is Uncertain, to Which Amount the Precursor B012900500004 Contributes, Since this Depends on Unknown ExperimentalB012900500005 Conditions, Comment by the Compiler of Kachapag. B012900500006 RAD-DET (63-EU-147,DG) B012900500007 DECAY-DATA (63-EU-147,22.D,DG,121.,0.23, B012900500008 DG,197.,0.276) B012900500009 FACILITY (ISOCY,2FR PAR) Variable Energy Cyclotron in Orsay. B012900500010 SAMPLE Ba-134 on Aluminium Backing, from 80% Enriched Barium B012900500011 Nitrate, Thickness 0.3 Mg/Cm**2. The Amount of Ba-134 B012900500012 Deposit was Measured After the Experiment by Isotope B012900500013 Dilution by Mass Spectrometry B012900500014 ENDBIB 12 0 B012900500015 NOCOMMON 0 0 B012900500016 DATA 3 4 B012900500017 EN DATA DATA-ERR B012900500018 MEV MB MB B012900500019 69. 9.6 B012900500020 74. 6.9 B012900500021 76.5 7.2 B012900500022 82. 3. 3. B012900500023 ENDDATA 6 0 B012900500024 ENDSUBENT 23 0 B012900599999 SUBENT B0129006 20011220 0000B012900600001 BIB 5 10 B012900600002 REACTION (56-BA-134(8-O-16,X)63-EU-146,,SIG,,,EXP) B012900600003 RAD-DET (63-EU-146,DG) B012900600004 DECAY-DATA (63-EU-146,4.6D,DG,633.,0.438, B012900600005 DG,634.,0.380, B012900600006 DG,747.,0.986) B012900600007 FACILITY (ISOCY,2FR PAR) Variable Energy Cyclotron in Orsay. B012900600008 SAMPLE Ba-134 on Aluminium Backing, from 80% Enriched Barium B012900600009 Nitrate, Thickness 0.3 Mg/Cm**2. The Amount of Ba-134 B012900600010 Deposit was Measured After the Experiment by Isotope B012900600011 Dilution by Mass Spectrometry B012900600012 ENDBIB 10 0 B012900600013 NOCOMMON 0 0 B012900600014 DATA 3 10 B012900600015 EN DATA DATA-ERR B012900600016 MEV MB MB B012900600017 69. 8.4 B012900600018 74. 22.6 4.8 B012900600019 76.5 22.6 B012900600020 82. 57. B012900600021 83. 48. B012900600022 89. 84. 15. B012900600023 95. 87. 14. B012900600024 101.5 53. 8. B012900600025 106.5 28. B012900600026 115. 8.9 3. B012900600027 ENDDATA 12 0 B012900600028 ENDSUBENT 27 0 B012900699999 SUBENT B0129007 20011220 0000B012900700001 BIB 5 10 B012900700002 REACTION (56-BA-134(8-O-16,X)63-EU-145,,SIG,,,EXP) B012900700003 RAD-DET (63-EU-145,DG) B012900700004 DECAY-DATA (63-EU-145,5.93D,DG,653.,0.15, B012900700005 DG,894.,0.67, B012900700006 DG,1658.,0.14) B012900700007 FACILITY (ISOCY,2FR PAR) Variable Energy Cyclotron in Orsay. B012900700008 SAMPLE Ba-134 on Aluminium Backing, from 80% Enriched Barium B012900700009 Nitrate, Thickness 0.3 Mg/Cm**2. The Amount of Ba-134 B012900700010 Deposit was Measured After the Experiment by Isotope B012900700011 Dilution by Mass Spectrometry B012900700012 ENDBIB 10 0 B012900700013 NOCOMMON 0 0 B012900700014 DATA 3 10 B012900700015 EN DATA DATA-ERR B012900700016 MEV MB MB B012900700017 74. 4.3 2.2 B012900700018 76.5 7.4 2. B012900700019 82. 29.5 4. B012900700020 83. 31. B012900700021 89. 131. B012900700022 95. 311. 34. B012900700023 101.5 425. 44. B012900700024 106.5 462. 48. B012900700025 115. 356. B012900700026 116. 409. B012900700027 ENDDATA 12 0 B012900700028 ENDSUBENT 27 0 B012900799999 SUBENT B0129008 20011220 0000B012900800001 BIB 6 10 B012900800002 REACTION (56-BA-134(8-O-16,X)62-SM-143-M,,SIG,,,EXP) B012900800003 COMMENT - By Compiler of CAJAD - Isomer State of Sm-143 can notB012900800004 Be Produced Due to Radioactive Decay of Eu-143. B012900800005 RAD-DET (62-SM-143-M,DG) B012900800006 DECAY-DATA (62-SM-143-M,62.SEC,DG,754.,1.0) B012900800007 FACILITY (ISOCY,2FR PAR) Variable Energy Cyclotron in Orsay. B012900800008 SAMPLE Ba-134 on Aluminium Backing, from 80% Enriched Barium B012900800009 Nitrate, Thickness 0.3 Mg/Cm**2. The Amount of Ba-134 B012900800010 Deposit was Measured After the Experiment by Isotope B012900800011 Dilution by Mass Spectrometry B012900800012 ENDBIB 10 0 B012900800013 NOCOMMON 0 0 B012900800014 DATA 3 7 B012900800015 EN DATA DATA-ERR B012900800016 MEV MB MB B012900800017 79. 21. 5. B012900800018 79. 20.6 5. B012900800019 80.5 21.6 4.2 B012900800020 82. 30.5 9. B012900800021 82.5 81. B012900800022 89. 116. 18. B012900800023 107.5 49. 10. B012900800024 ENDDATA 9 0 B012900800025 ENDSUBENT 24 0 B012900899999 SUBENT B0129009 20011220 0000B012900900001 BIB 6 13 B012900900002 REACTION (56-BA-134(8-O-16,X)62-SM-141-M,CUM,SIG,,,EXP) B012900900003 COMMENT - By Compiler of CAJAD - Sm-141-M is Dauther of B012900900004 Short-Lived Eu-141-M (T1/2=2.7SEC). B012900900005 RAD-DET (62-SM-141-M,DG) B012900900006 DECAY-DATA (62-SM-141-M,22.1MIN,DG,196.,0.72, B012900900007 DG,431.,0.392, B012900900008 DG,777.,0.200, B012900900009 DG,1786.,0.106) B012900900010 FACILITY (ISOCY,2FR PAR) Variable Energy Cyclotron in Orsay. B012900900011 SAMPLE Ba-134 on Aluminium Backing, from 80% Enriched Barium B012900900012 Nitrate, Thickness 0.3 Mg/Cm**2. The Amount of Ba-134 B012900900013 Deposit was Measured After the Experiment by Isotope B012900900014 Dilution by Mass Spectrometry B012900900015 ENDBIB 13 0 B012900900016 NOCOMMON 0 0 B012900900017 DATA 3 5 B012900900018 EN DATA DATA-ERR B012900900019 MEV MB MB B012900900020 103. 8.6 4. B012900900021 107.5 16.7 6. B012900900022 114. 49. 10. B012900900023 116. 70. 14. B012900900024 123. 111. B012900900025 ENDDATA 7 0 B012900900026 ENDSUBENT 25 0 B012900999999 SUBENT B0129010 20011220 0000B012901000001 BIB 6 13 B012901000002 REACTION (56-BA-134(8-O-16,X)60-ND-139-M,,SIG,,,EXP) B012901000003 COMMENT - By Compiler of CAJAD - Nd-139-M Production Due to B012901000004 Radioactive Decay of Pm-139 is Negligible. B012901000005 RAD-DET (60-ND-139-M,DG) B012901000006 DECAY-DATA (60-ND-139-M,5.5HR,DG,113.8,0.28, B012901000007 DG,708.,0.24, B012901000008 DG,738.,0.31, B012901000009 DG,982.,0.27) B012901000010 FACILITY (ISOCY,2FR PAR) Variable Energy Cyclotron in Orsay. B012901000011 SAMPLE Ba-134 on Aluminium Backing, from 80% Enriched Barium B012901000012 Nitrate, Thickness 0.3 Mg/Cm**2. The Amount of Ba-134 B012901000013 Deposit was Measured After the Experiment by Isotope B012901000014 Dilution by Mass Spectrometry B012901000015 ENDBIB 13 0 B012901000016 NOCOMMON 0 0 B012901000017 DATA 3 7 B012901000018 EN DATA DATA-ERR B012901000019 MEV MB MB B012901000020 101.5 2.7 B012901000021 106.5 8.6 2.2 B012901000022 107.5 13.5 B012901000023 114. 26.6 9. B012901000024 115. 22.6 B012901000025 116. 23.6 5. B012901000026 123. 28.5 5. B012901000027 ENDDATA 9 0 B012901000028 ENDSUBENT 27 0 B012901099999 SUBENT B0129011 20011220 0000B012901100001 BIB 6 11 B012901100002 REACTION (46-PD-110(18-AR-40,3N)64-GD-147,,SIG,,,EXP) B012901100003 RAD-DET (64-GD-147,DG) B012901100004 DECAY-DATA (64-GD-147,38.HR,DG,229.,0.57,DG,370.,0.132, B012901100005 DG,396.,0.262,DG,765.,0.095,DG,928.,0.165) B012901100006 FACILITY (ISOCY,2FR PAR) Alice Accelerator System at the B012901100007 Variable Energy Cyclotron in Orsay. B012901100008 SAMPLE Pd-110 Target, Enrichment 88%, Thickness 1.2 Mg/Cm**2 B012901100009 For Self-Supporting Target and 0.15 Mg/Cm**2 For B012901100010 Evaporated on Al-Backing Target. B012901100011 ERR-ANALYS (EN-ERR) The Heavy Ion Energy was Known to Within 2% B012901100012 For the Individual Targets. B012901100013 ENDBIB 11 0 B012901100014 NOCOMMON 0 0 B012901100015 DATA 4 14 B012901100016 EN EN-ERR DATA DATA-ERR B012901100017 MEV MEV MB MB B012901100018 140. 1. 11. 0.7 B012901100019 143. 1. 30. 3.4 B012901100020 149. 5. 30. 9. B012901100021 149. 1. 48. B012901100022 154. 1. 59. 9. B012901100023 158. 1. 46. B012901100024 159. 5. 44.5 7.5 B012901100025 163. 5. 51. 9. B012901100026 163. 1. 58. 4. B012901100027 168. 5. 38. 6. B012901100028 168. 1. 43. 6. B012901100029 175. 5. 44. 7.5 B012901100030 178. 5. 11.3 2.5 B012901100031 186. 5. 9.7 2. B012901100032 ENDDATA 16 0 B012901100033 ENDSUBENT 32 0 B012901199999 SUBENT B0129012 20011220 0000B012901200001 BIB 6 12 B012901200002 REACTION (46-PD-110(18-AR-40,4N)64-GD-146,,SIG,,,EXP) B012901200003 RAD-DET (64-GD-146,DG) B012901200004 DECAY-DATA (64-GD-146,50.D,DG,114.8,0.45, B012901200005 DG,115.6,0.45, B012901200006 DG,154.,0.388) B012901200007 FACILITY (ISOCY,2FR PAR) Alice Accelerator System at the B012901200008 Variable Energy Cyclotron in Orsay. B012901200009 SAMPLE Pd-110 Target, Enrichment 88%, Thickness 1.2 Mg/Cm**2 B012901200010 For Self-Supporting Target and 0.15 Mg/Cm**2 For B012901200011 Evaporated on Al-Backing Target. B012901200012 ERR-ANALYS (EN-ERR) The Heavy Ion Energy was Known to Within 2% B012901200013 For the Individual Targets. B012901200014 ENDBIB 12 0 B012901200015 NOCOMMON 0 0 B012901200016 DATA 4 15 B012901200017 EN EN-ERR DATA DATA-ERR B012901200018 MEV MEV MB MB B012901200019 140. 1. 21. B012901200020 143. 1. 81.5 6. B012901200021 149. 5. 76. 20. B012901200022 149. 1. 129. B012901200023 159. 5. 153. 22. B012901200024 163. 5. 156. 23. B012901200025 163. 1. 200. 23. B012901200026 168. 5. 165. 30. B012901200027 168. 1. 190. 12. B012901200028 175. 5. 165. 21. B012901200029 178. 5. 137. 20. B012901200030 186. 5. 108. 20. B012901200031 191. 1. 45. 9. B012901200032 197. 5. 24.7 5. B012901200033 207. 4. 8.9 35. B012901200034 ENDDATA 17 0 B012901200035 ENDSUBENT 34 0 B012901299999 SUBENT B0129013 20011220 0000B012901300001 BIB 7 19 B012901300002 REACTION M(46-PD-110(18-AR-40,5N)64-GD-145-M,,SIG,,,EXP) B012901300003 S(46-PD-110(18-AR-40,5N)64-GD-145,,SIG,,,EXP) B012901300004 G(46-PD-110(18-AR-40,5N)64-GD-145-G,,SIG,,,EXP) B012901300005 The Given Cross Section is Deduced from the B012901300006 Cross Sections For the Isomeric State and the Cross B012901300007 Section For the Sum of Isomeric and Groundstate. B012901300008 RAD-DET M(64-GD-145-M,DG) B012901300009 S(64-GD-145-G,DG) B012901300010 DECAY-DATAM(64-GD-145-M,85.SEC,DG,721.,0.83) Isomer Transition. B012901300011 S(64-GD-145-G,21.8MIN,DG,808.,0.091,DG,1041.,0.102, B012901300012 DG,1757.,0.346,DG,1880.,0.331) B012901300013 FACILITY (ISOCY,2FR PAR) Alice Accelerator System at the B012901300014 Variable Energy Cyclotron in Orsay. B012901300015 SAMPLE Pd-110 Target, Enrichment 88%, Thickness 1.2 Mg/Cm**2 B012901300016 For Self-Supporting Target and 0.15 Mg/Cm**2 For B012901300017 Evaporated on Al-Backing Target. B012901300018 ERR-ANALYS (EN-ERR) The Heavy Ion Energy was Known to Within 2% B012901300019 For the Individual Targets. B012901300020 STATUS G(DEP,B0129013) B012901300021 ENDBIB 19 0 B012901300022 NOCOMMON 0 0 B012901300023 DATA 7 21 B012901300024 EN EN-ERR DATA MDATA-ERR MDATA SDATA-ERR SB012901300025 DATA G B012901300026 MEV MEV MB MB MB MB B012901300027 MB B012901300028 143. 1. B012901300029 3. B012901300030 148. 1. 35. 5.B012901300031 B012901300032 149. 5. 34.5 10.5 B012901300033 B012901300034 149. 1. 34. 34. 6.B012901300035 B012901300036 154. 1. 88. 10. 93. 9.B012901300037 5. B012901300038 158. 1. 123. 16. 124. 14.B012901300039 B012901300040 158. 1. 150. 15. B012901300041 B012901300042 163. 5. 180. 20. B012901300043 B012901300044 163. 1. 188. 197. 26.B012901300045 9. B012901300046 163. 1. 194. 25. B012901300047 3. B012901300048 168. 1. 179. 9. 209. 21.B012901300049 30. B012901300050 176. 1. 180. 20. 201. 20.B012901300051 19. B012901300052 176. 1. 201. 14. B012901300053 B012901300054 178. 5. 132. 137. B012901300055 5. B012901300056 183. 1. 179. 14.B012901300057 B012901300058 191. 1. 160. 186. 20.B012901300059 26. B012901300060 191. 1. 186. 18. B012901300061 B012901300062 197. 5. 124. 145. 30.B012901300063 21. B012901300064 201. 1. 91. 114. 21.B012901300065 21. B012901300066 201. 1. 104. 17. B012901300067 10. B012901300068 207. 4. 70. 13. 70. B012901300069 B012901300070 ENDDATA 46 0 B012901300071 ENDSUBENT 70 0 B012901399999 SUBENT B0129014 20011220 0000B012901400001 BIB 6 12 B012901400002 REACTION (46-PD-110(18-AR-40,X)63-EU-146,,SIG,,,EXP) B012901400003 RAD-DET (63-EU-146,DG) B012901400004 DECAY-DATA (63-EU-146,4.6D,DG,633.,0.438, B012901400005 DG,634.,0.380, B012901400006 DG,747.,0.986) B012901400007 FACILITY (ISOCY,2FR PAR) Alice Accelerator System at the B012901400008 Variable Energy Cyclotron in Orsay. B012901400009 SAMPLE Pd-110 Target, Enrichment 88%, Thickness 1.2 Mg/Cm**2 B012901400010 For Self-Supporting Target and 0.15 Mg/Cm**2 For B012901400011 Evaporated on Al-Backing Target. B012901400012 ERR-ANALYS (EN-ERR) The Heavy Ion Energy was Known to Within 2% B012901400013 For the Individual Targets. B012901400014 ENDBIB 12 0 B012901400015 NOCOMMON 0 0 B012901400016 DATA 4 10 B012901400017 EN EN-ERR DATA DATA-ERR B012901400018 MEV MEV MB MB B012901400019 149. 5. 9.4 B012901400020 149. 1. 18. 5. B012901400021 159. 5. 18.2 3.4 B012901400022 163. 5. 23.6 6.5 B012901400023 168. 5. 26.5 6.6 B012901400024 168. 1. 28. B012901400025 175. 5. 25.6 7. B012901400026 178. 5. 15.5 3.6 B012901400027 186. 5. 15.9 3.8 B012901400028 197. 5. 3.8 1.1 B012901400029 ENDDATA 12 0 B012901400030 ENDSUBENT 29 0 B012901499999 SUBENT B0129015 20011220 0000B012901500001 BIB 5 10 B012901500002 REACTION (46-PD-110(18-AR-40,X)63-EU-145,CUM,SIG,,,EXP) B012901500003 RAD-DET (63-EU-145,DG) B012901500004 DECAY-DATA (63-EU-145,5.93D,DG,653.,0.15, B012901500005 DG,894.,0.67, B012901500006 DG,1658.,0.14) B012901500007 SAMPLE Pd-110 Target, Enrichment 88%, Thickness 1.2 Mg/Cm**2 B012901500008 For Self-Supporting Target and 0.15 Mg/Cm**2 For B012901500009 Evaporated on Al-Backing Target. B012901500010 ERR-ANALYS (EN-ERR) The Heavy Ion Energy was Known to Within 2% B012901500011 For the Individual Targets. B012901500012 ENDBIB 10 0 B012901500013 NOCOMMON 0 0 B012901500014 DATA 4 13 B012901500015 EN EN-ERR DATA DATA-ERR B012901500016 MEV MEV MB MB B012901500017 149. 1. 47. 10. B012901500018 159. 5. 96. 15. B012901500019 163. 5. 154. 26. B012901500020 163. 1. 208. 30. B012901500021 168. 5. 178. 32. B012901500022 168. 1. 242. 28. B012901500023 175. 5. 201. 29. B012901500024 178. 5. 180. 27. B012901500025 186. 5. 202. 26. B012901500026 191. 1. 210. 11. B012901500027 197. 5. 149. 19. B012901500028 207. 4. 77. 11. B012901500029 209. 1. 51.8 B012901500030 ENDDATA 15 0 B012901500031 ENDSUBENT 30 0 B012901599999 SUBENT B0129016 20011220 0000B012901600001 BIB 7 12 B012901600002 REACTION (46-PD-110(18-AR-40,X)62-SM-143-M,IND,SIG,,,EXP) B012901600003 COMMENT - By Compiler of CAJAD - Sm-143-M can not be Produced B012901600004 Due to Radioactive Decay of Eu-143. B012901600005 RAD-DET (62-SM-143-M,DG) B012901600006 DECAY-DATA (62-SM-143-M,62.SEC,DG,754.,1.0) B012901600007 FACILITY (ISOCY,2FR PAR) Alice Accelerator System at the B012901600008 Variable Energy Cyclotron in Orsay. B012901600009 SAMPLE Pd-110 Target, Enrichment 88%, Thickness 1.2 Mg/Cm**2 B012901600010 For Self-Supporting Target and 0.15 Mg/Cm**2 For B012901600011 Evaporated on Al-Backing Target. B012901600012 ERR-ANALYS (EN-ERR) The Heavy Ion Energy was Known to Within 2% B012901600013 For the Individual Targets. B012901600014 ENDBIB 12 0 B012901600015 NOCOMMON 0 0 B012901600016 DATA 4 7 B012901600017 EN EN-ERR DATA DATA-ERR B012901600018 MEV MEV MB MB B012901600019 144. 1. 22. B012901600020 149. 5. 33. B012901600021 154. 1. 42. 9. B012901600022 163. 1. 58. 10. B012901600023 168. 1. 58. B012901600024 197. 5. 49.3 9.3 B012901600025 207. 4. 23.8 4.7 B012901600026 ENDDATA 9 0 B012901600027 ENDSUBENT 26 0 B012901699999 SUBENT B0129017 20011220 0000B012901700001 BIB 7 15 B012901700002 REACTION (46-PD-110(18-AR-40,X)62-SM-141-M,CUM,SIG,,,EXP) B012901700003 COMMENT - By Compiler of CAJAD - Sm-141-M is Dauther of B012901700004 Short-Lived Eu-141-M (T1/2=2.7SEC). B012901700005 RAD-DET (62-SM-141-M,DG) B012901700006 DECAY-DATA (62-SM-141-M,22.1MIN,DG,196.,0.72, B012901700007 DG,431.,0.392, B012901700008 DG,777.,0.200, B012901700009 DG,1786.,0.106) B012901700010 SAMPLE Pd-110 Target, Enrichment 88%, Thickness 1.2 Mg/Cm**2 B012901700011 For Self-Supporting Target and 0.15 Mg/Cm**2 For B012901700012 Evaporated on Al-Backing Target. B012901700013 ERR-ANALYS (EN-ERR) The Heavy Ion Energy was Known to Within 2% B012901700014 For the Individual Targets. B012901700015 FACILITY (ISOCY,2FR PAR) Alice Accelerator System at the B012901700016 Variable Energy Cyclotron in Orsay. B012901700017 ENDBIB 15 0 B012901700018 NOCOMMON 0 0 B012901700019 DATA 4 12 B012901700020 EN EN-ERR DATA DATA-ERR B012901700021 MEV MEV MB MB B012901700022 163. 1. 2. B012901700023 168. 1. 6.2 2.5 B012901700024 176. 1. 13.1 1.4 B012901700025 178. 5. 7.2 2.7 B012901700026 186. 5. 17.5 4.5 B012901700027 191. 1. 45.4 10. B012901700028 197. 5. 41. 8.7 B012901700029 201. 1. 75. 8. B012901700030 207. 4. 59. 10. B012901700031 209. 1. 74. 10. B012901700032 225. 1. 46. 2.5 B012901700033 235. 1. 45.5 4.6 B012901700034 ENDDATA 14 0 B012901700035 ENDSUBENT 34 0 B012901799999 SUBENT B0129018 20011220 0000B012901800001 BIB 7 14 B012901800002 REACTION (46-PD-110(18-AR-40,X)61-PM-140-M,IND,SIG,,,EXP) B012901800003 COMMENT - By Compiler of CAJAD - Pm-140-M Production Due to B012901800004 Radioactive Decay of Sm-140 is Very Small. B012901800005 RAD-DET (61-PM-140-M,DG) B012901800006 DECAY-DATA (61-PM-140-M,6.0MIN,DG,418.,1.0, B012901800007 DG,775.,1.0, B012901800008 DG,1027.,1.0) B012901800009 SAMPLE Pd-110 Target, Enrichment 88%, Thickness 1.2 Mg/Cm**2 B012901800010 For Self-Supporting Target and 0.15 Mg/Cm**2 For B012901800011 Evaporated on Al-Backing Target. B012901800012 ERR-ANALYS (EN-ERR) The Heavy Ion Energy was Known to Within 2% B012901800013 For the Individual Targets. B012901800014 FACILITY (ISOCY,2FR PAR) Alice Accelerator System at the B012901800015 Variable Energy Cyclotron in Orsay. B012901800016 ENDBIB 14 0 B012901800017 NOCOMMON 0 0 B012901800018 DATA 4 5 B012901800019 EN EN-ERR DATA DATA-ERR B012901800020 MEV MEV MB MB B012901800021 186. 5. 6.4 2. B012901800022 197. 5. 8.4 1. B012901800023 207. 4. 14. B012901800024 225. 1. 26.5 2. B012901800025 235. 1. 27.5 2.9 B012901800026 ENDDATA 7 0 B012901800027 ENDSUBENT 26 0 B012901899999 SUBENT B0129019 20011220 0000B012901900001 BIB 7 15 B012901900002 REACTION (46-PD-110(18-AR-40,X)60-ND-139-M,IND,SIG,,,EXP) B012901900003 COMMENT - By Compiler of CAJAD - Nd-139-M Production Due to B012901900004 Radioactive Decay of Pm-139 is Very Small. B012901900005 RAD-DET (60-ND-139-M,DG) B012901900006 DECAY-DATA (60-ND-139-M,5.5HR,DG,113.8,0.28, B012901900007 DG,708.,0.24, B012901900008 DG,738.,0.31, B012901900009 DG,982.,0.27) B012901900010 SAMPLE Pd-110 Target, Enrichment 88%, Thickness 1.2 Mg/Cm**2 B012901900011 For Self-Supporting Target and 0.15 Mg/Cm**2 For B012901900012 Evaporated on Al-Backing Target. B012901900013 ERR-ANALYS (EN-ERR) The Heavy Ion Energy was Known to Within 2% B012901900014 For the Individual Targets. B012901900015 FACILITY (ISOCY,2FR PAR) Alice Accelerator System at the B012901900016 Variable Energy Cyclotron in Orsay. B012901900017 ENDBIB 15 0 B012901900018 NOCOMMON 0 0 B012901900019 DATA 4 3 B012901900020 EN EN-ERR DATA DATA-ERR B012901900021 MEV MEV MB MB B012901900022 186. 5. 5.6 1. B012901900023 197. 5. 9.6 B012901900024 201. 1. 10.8 B012901900025 ENDDATA 5 0 B012901900026 ENDSUBENT 25 0 B012901999999 ENDENTRY 19 0 B012999999999