216FR 220AC A DECAY 1997SH09 07NDS 200705
216FR H TYP=ERR$AUT=J. Tuli$DAT=15-Jul-2011$COM=corrected N record$
216FR H TYP=FUL$AUT=S. -C. WU$CIT=NDS 108, 1057 (2007)$CUT=1-Mar-2007$
216FR cA $All data are from 1997Sh09, unless otherwise noted
216FR cA HF r{-0}({+216}Fr)=1.556 {I6}, unweighted average of
216FR2cA r{-0}({+214}Rn)=1.563 {I4}, r{-0}({+216}Rn)=1.554 {I6},
216FR3cA r{-0}({+216}Ra)=1.566 {I9}, r{-0}({+218}Ra)=1.539 {I9}
216FR cG $All data are from 1997Sh09
216FR cG RI I|g per 1000 |a's
216FR cG M The method of |a measurements is not given
216FR cL $1997Sh09: measured: E|a, I|a, E|g, I|g, ce, |a|g, |a(ce), |g(ce).
216FR2cL Source: {+224}Pa + {+220}Ac in secular equilibrium produced by
216FRxcL {+209}Bi({+18}O,2n). Ge, Ge(Li), Si(Li) detectors.
216FR cL $1971EpZY: measured: |a, |a|g, |g|g, |a|g(t)
216FR cL $1970Bo13: measured: |a
216FR cL E From least squares fit to E|g
216FR cL J Assignments of J|p and configuration are those suggested
216FR2cL by 1997Sh09. The J|p assignments are based on |g multipolarities, on
216FR3cL HF in |a decay, and on proposed configuration assignments;
216FR4cL all levels have been assigned negative parity.
216FR CL BAND(A) CONF=((P,H9/2,+5,9/2-)(N,G9/2,+3,9/2+))
216FR CL BAND(B) CONF=((P,H9/2,+4,0)(P,F7/2,+1,7/2-)(N,G9/2,+3,9/2+))
216FR CL BAND(C) CONF=((P,H9/2,+5,9/2-)(N,G9/2,+2,0)(N,I11/2,+1,11/2+))
220AC P 0 26.4 MS 2 8348 4
216FR N 0.1 1.0
216FR PN 3
216FR G 112.7 3 5.7 20
216FR G 127.1 4 3 AP
216FR G 151.5 4 7.0 25
216FR G 169.2 3 4.3 11
216FR G 179.3 4 3.8 13
216FR G 197.3 5 3 AP
216FR G 214.8 3 5.1 16
216FR G 221.3 3 6.2 18
216FR G 238.8 3 10.5 28
216FR G 260.8 5 5.0 17
216FR G 263.6 4 6.2 20
216FR G 265.4 4 9 3
216FR L 0 1- A
216FR A 8194 4 3005
216FR cA E|a=8195 {I10}, I|a=3 {I1} (1970Bo13)
216FR L 133.3 1 3- 71 NS 5 AM
216FR2 L %A GT 50
216FR cL T from 1971EpZY
216FR cL %A From intensity balance at the 133.3-keV level (evaluator)
216FR A 8063 2 2507
216FR G 133.3 1 82 7 E2 2.65
216FRS G KC=0.314 5$LC=1.717 25$MC=0.464 7$NC+=0.1504 22
216FRS G NC=0.1218 18$OC=0.0253 4$PC=0.00329 5$QC=1.302E-5 19
216FR cG M K/L<0.2, L2/L3=2.0 {I5}
216FR L 141.6 2 (0)- A
216FR A 8055 4 1186
216FR cA E|a=8060 {I10}, I|a=6 {I1} (1970Bo13)
216FR G 141.6 2 13.2 30M1 5.32
216FRS G KC=4.29 7$LC=0.787 12$MC=0.188 3$NC+=0.0620 9
216FRS G NC=0.0492 8$OC=0.01099 16$PC=0.00176 3$QC=9.85E-5 15
216FR cG M K| x ray/g=4 {I1}
216FR L 191.2 2 (5)- A
216FR A 8006 3 1135
216FR cA E|a=8005 {I10}, I|a=5 {I3} (1970Bo13)
216FR G 57.9 1 6.6 20E2 118.3 20
216FRS G LC=87.2 15$MC=23.5 4$NC+=7.60 13
216FRS G NC=6.16 10$OC=1.274 21$PC=0.163 3$QC=0.000257 4
216FR cG M |a(L)exp=50 {I20}
216FR L 212.0 2 2,3 B
216FR G 78.6 2 5 2
216FR L 226.1 2 (4)- A
216FR A 7971 4 673
216FR cA E|a=7985 {I10}, I|a=4 {I2} (1970Bo13)
216FR G 34.9 3 2 AP(M1) 61.5 18
216FRS G LC=46.6 14$MC=11.1 4$NC+=3.68 11
216FRS G NC=2.92 9$OC=0.653 20$PC=0.105 3$QC=0.00587 18
216FR cG M from intensity balance E2 and higher multipolarities are
216FR2cG ruled out.
216FR G 92.8 1 37 5 M1 3.50
216FRS G LC=2.66 4$MC=0.634 9$NC+=0.210 3
216FRS G NC=0.1661 24$OC=0.0371 6$PC=0.00596 9$QC=0.000333 5
216FR cG M |a(L)exp=2.3 {I5}
216FR L 247.8 0,1,2 B ?
216FR G 247.8 4 4.7 14 ?
216FR cG E$transition assigned as deexciting the Ex=247.8 state
216FR2cG in the level scheme; not assigned in the gamma ray transitions table.
216FR L 249.4 2 3,4- B
216FR G 37.4 3 2 AP
216FR cG M from intensity balance |g is not E2
216FR cG M M1 gives I(|g+ce)|?106, E2 gives I(|g+ce)|?2000, E1 gives
216FRxcG I(|g+ce)|?3
216FR L 254.4 2 (2) A
216FR A 7944 2 AP 1110 AP
216FR G 42.5 2 3 AP
216FR G 121.0 2 8.0 14
216FR G 254.4 5 5.4 17
216FR L 290.4 2 3,4,5 B
216FR G 64.3 1 18 3
216FR cG M from intensity balance, not E2 (I(|g+ce)=1307); M1 gives
216FRxcG I(|g+ce)=212
216FR L 344.2 2 4,5- C
216FR A 7855 26 46
216FR cA E|a=7850 {I10}, I|a=24 {I2}
216FR G 53.6 2 3 AP
216FR G 94.8 1 25 4
216FR G 118.2 2 13.5 35(M1) 8.90
216FRS G KC=7.16 11$LC=1.321 20$MC=0.315 5$NC+=0.1042 16
216FRS G NC=0.0826 13$OC=0.0185 3$PC=0.00296 5$QC=0.0001654 25
216FR cG M |a(K)exp>3
216FR G 153.1 2 18.2 35
216FR L 349.3 3 2,3,4 C
216FR A 7850 5 231
216FR G 137.3 2 15 3
216FR L 409.3 2 2,3,4,5- C
216FR A 7792 10 76
216FR cA E|a=7790 {I10}, I|a=13 {I2} (1970Bo13)
216FR G 160.0 1 33 5 M1 3.76
216FRS G KC=3.03 5$LC=0.555 8$MC=0.1324 19$NC+=0.0438 7
216FRS G NC=0.0347 5$OC=0.00776 11$PC=0.001244 18$QC=6.95E-5 10
216FR cG M K/L=5 {I1}
216FR L 493.4 2 3,4,5- C
216FR A 7709 11 38
216FR G 149.0 3 9.5 28
216FR G 203.6 5 3 AP
216FR G 243.7 2 18 4 M1 1.156
216FRS G KC=0.932 14$LC=0.1696 24$MC=0.0404 6$NC+=0.01336 19
216FRS G NC=0.01059 15$OC=0.00237 4$PC=0.000380 6$QC=2.12E-5 3
216FR cG M |a(K)exp=1.1 {I5}
216FR G 267.8 3 18 4 M1 0.890
216FRS G KC=0.718 11$LC=0.1304 19$MC=0.0310 5$NC+=0.01027 15
216FRS G NC=0.00814 12$OC=0.00182 3$PC=0.000292 5$QC=1.629E-5 24
216FR cG M |a(K)exp=1.2 {I5}
216FR L 532.1 2 3,4,5 C
216FR A 7670 8 40
216FR cA E|a=7680 {I20}, I|a=21 {I5} (1970Bo13)
216FR G 123.3 3 5.5 14
216FR G 182.8 3 5.4 16
216FR G 187.8 2 14.4 30
216FR G 305.6 4 10 4
216FR L 539.4 4 3,4,5- C
216FR A 7664 4 75
216FR G 130.4 4 4 AP
216FR G 312.9 4 14 2 (M1) 0.580
216FRS G KC=0.468 7$LC=0.0848 13$MC=0.0202 3$NC+=0.00667 10
216FRS G NC=0.00529 8$OC=0.001182 17$PC=0.000190 3$QC=1.059E-5 16
216FR cG M |a(K)exp|?0.7
216FR L 550.9 2 (3)- C
216FR A 7652 9 31
216FR G 206.7 2 12 3
216FR G 296.4 3 20 5 M1 0.673
216FRS G KC=0.543 8$LC=0.0985 14$MC=0.0234 4$NC+=0.00775 11
216FRS G NC=0.00614 9$OC=0.001373 20$PC=0.000220 4$QC=1.229E-5 18
216FR cG M |a(K)exp=0.8 {I4}
216FR G 301.4 3 13 4
216FR L 568.8 4 4,5- C
216FR A 7635 4 61
216FR G 342.7 3 35 5 M1 0.452
216FRS G KC=0.365 6$LC=0.0660 10$MC=0.01570 23$NC+=0.00519 8
216FRS G NC=0.00412 6$OC=0.000920 13$PC=0.0001476 21$QC=8.24E-6 12
216FR cG M |a(K)exp=0.5 {I2}
216FR G 378.0 10 2 AP
216FR L 581.5 3 (3) C
216FR A 7622 4 55
216FR cA E|a=7610 {I20}, I|a=9 {I4} (1970Bo13)
216FR G 172.2 3 5.0 13
216FR G 327.0 6 4 AP
216FR G 390.2 5 6.6 25
216FR G 448.4 10 2 AP