239AM 243BK A DECAY 1966AH02,1991RY01 14NDS 201411 239AM H TYP=FUL$AUT=E. BROWNE, J. K. TULI$CIT=NDS 122, 293 (2014)$ 239AM2 H CUT=30-Jun-2013$ 239AM D Recalculated HF.Remove comment on favored alpha (E.Browne,March 2002). 239AM D New HF's differ about 20% from old values. Don't know why!(E. Browne). 239AM C AG: 1956CH77, 1966AH02 239AM C XK: RI=8 3 239AM C 2013NI13: calculated branching ratios to three rotational bands. 239AM2C OTHERS: 2011ZH36, 2010NI02 239AM CA E From 1966AH02 (semi) recalibrated by 1991RY01 239AM CA IA From 1966AH02. Intensity per 100 ALPHA decays 239AM CA HF Using R0(239AM)=1.496, average of R0(238PU)=1.5013 10, 239AM2CA R0(240PU)=1.4979 7, R0(238CM)=1.490 20, and R0(240CM)=1.495 12 239AM3CA (1998AK04). HF values are approximate because of the imprecise value 239AM4CA of AP 0.15% for the alpha-particle branching. 239AM DG CC$ FROM BrIcc v2.2 (31-Mar-2008) 2008KiAA, "Frozen Orbitals" appr. 239AM CG E From 1966AH02 (AG-semi), 1956CH77 (AG-scin) 239AM CG RI Photon intensity per 100 ALPHA decays (1966AH02,1956CH77) 239AM CG M(A) Multipolarity is E1 or E2 from relative photon and XK 239AM2CG intensities. However, the ratio of reduced transition probabilities 239AM3CG suggests E1 multipolarity. 239AM CL J From adopted levels 239AM CL BAND(A)$GS ROTATIONAL BAND. CALCULATED |a BRANCHING=29.8% (2013NI13) 239AM CL BAND(B)$ROTATIONAL BAND BUILT ON 187 LEVEL. 239AM2CL CALCULATED |a BRANCHING=52.8% (2013NI13) 239AM CL BAND(C)$FAVORED ROTATIONAL BAND BUILT ON 557 LEVEL 239AM2CL CALCULATED |a BRANCHING=17.5% (2013NI13) 243BK P 0.0 (3/2-) 4.5 H 2 6874 4 239AM N 1.0 AP 0.0015 AP 239AM PN 239AM L 0.0 (5/2)- 11.9 H 1 A 239AM A 6761 4 15.4 10 1190 AP 239AM L 40.7 7 (7/2-) A 239AM A 6721 4 12.5 9 982 AP 239AM G 42 3 4 [M1] 79 20 ? 239AMS G LC=59 15$MC=15 4$NC+=5.2 13 239AMS G NC=4.0 10$OC=1.00 25$PC=0.19 5$QC=0.012 3 239AM CG RI is inconsistent with decay scheme; RI LE 0.3 from transition 239AM2CG intensity balance. 239AM L 94 6 (9/2-) A 239AM A 6669 4 1.2 AP 6060 AP 239AM L 156 7 (11/2-) A 239AM A 6608 5 0.7 AP 5560 AP 239AM L 187.1 5 (5/2+) B 239AM A 6577 4 25.6 16 111 AP 239AM G 146.4 5 8 3 (E1) 0.215 4 A 239AMS G KC=0.164 3$LC=0.0384 7$MC=0.00943 16$NC+=0.00329 6 239AMS G NC=0.00255 5$OC=0.000622 11$PC=0.0001077 18$QC=4.53E-6 8 239AM G 187.1 5 40 10(E1) 0.1220 19 A 239AMS G KC=0.0943 15$LC=0.0208 4$MC=0.00509 8$NC+=0.00178 3 239AMS G NC=0.001380 22$OC=0.000338 6$PC=5.96E-5 10$QC=2.68E-6 4 239AM L 220 6 (7/2+) B 239AM A 6545 4 19.4 13 104 AP 239AM L 260 6 (9/2+) B 239AM A 6505 4 6.9 7 195 AP 239AM L 317 7 (11/2+) B 239AM A 6449 5 0.7 2 1060 AP 239AM L 370 AP(13/2+) B 239AM A 6397 AP 0.2 AP 2120 AP 239AM L 557 6 (3/2-) C 239AM A 6213 4 13.6 9 4.1 AP 239AM G 536 10 10 LT[E2] 0.0473 22 & ? 239AM3 G FL=40.7 239AMS G KC=0.0283 11$LC=0.0139 9$MC=0.00369 24$NC+=0.00131 9 239AMS G NC=0.00101 7$OC=0.000248 16$PC=4.4E-5 3$QC=1.30E-6 6 239AM CG E probable unresolved doublet to GS and 40.7 levels. RI has not 239AM2CG been divided. 239AM G 536 10 10 LT[M1,E2] 0.16 11 & ? 239AM3 G FL=0.0 239AMS G KC=0.12 10$LC=0.028 15$MC=0.007 4$NC+=0.0025 12 239AMS G NC=0.0019 9$OC=0.00048 23$PC=9.E-5 5$QC=5.E-6 4 239AM CG E probable unresolved doublet to GS and 40.7 levels. RI has not 239AM2CG been divided. 239AM L 586 6 (5/2-) C 239AM A 6185 4 3.9 5 10 AP