163ER 163TM EC DECAY (1.810 H) 1982VY07 10NDS 201005
163ER H TYP=FUL$AUT=C. W. REICH, BALRAJ SINGH$CIT=NDS 111, 1211 (2010)$
163ER2 H CUT=12-Apr-2010$
163ER D DATA SET UPDATED (OCTOBER, 2008) BY CW REICH TO INCLUDE CC VALUES
163ER2D FROM BRICC, SOME MODIFIED COMMENTS AND DIFFERENT NOTATION FOR THE
163ER3D GAMMA VIBRATION.
163ER c 1982Vy07 (also 1982Vy08): measured K| x ray, |g, ce, |b{++} (spect),
163ER2c ce|g. Chem, mass separation. Level scheme given by 1982Vy08
163ER c 1980Ab18 (also 1980Ab22): measured |g, ce. Chem. 47 |g rays
163ER2c measured up to 400 keV
163ER c 1976Ab09: measured |g, ce
163ER d 1982Vy08 (and 1982Vy07), 1980Ab18 (and 1980Ab22), and 1976Ab09 all
163ER2d share some common authors.
163ER c Others:
163ER c |g: 1963Gr14, 1967Gn01, 1975Gr44
163ER c ce: 1962Ha24, 1963Gr14, 1967Gn01, 1987BaZB, 1991GaZZ
163ER c ce|g(t): 1974An04
163ER c (x ray)|g(t)): 1969Ve05
163ER c E|e,I|e: 1960Bo29, 1964Gr37, 1982By03
163ER c T{-1/2} of {+163}Tm g.s.: 1961Bj02, 1963Ra15, 1963Gr14, 1969Ve05.
163ER2c Others: 1959Ha09, 1960Bo29, 1960Bu27
163ER c The decay scheme is from 1982Vy07 and 1982Vy08, superseding the level
163ER2c schemes of 1980Ab18, 1976Ab09, 1967Gn01 and 1963Gr14
163ER cE $I|g(|g{+|+})=4.7 {I6} relative to I|g(104|g)=100 (1982Vy07) compared
163ER2cE to 6.2 {I5} (5.4 {I3} excluding I|e's with upper limits and I|e(to
163ER3cE 91.6)) from the decay scheme.
163ER cE $I|g(104|g)/I|g(K| x ray)=0.135 {I3} (1982Vy07), compared to 0.208 {I6}
163ER2cE from the decay scheme, is indicative of a substantive |e feeding which
163ER3cE has not been placed. The measured I|b{++}=0.047 {I6} to levels above
163ER4cE 720 compared to 0.00074 {I5} also suggests that the |e feeding to
163ER5cE levels between 735 and 1060 has been underestimated. The
163ER5cE total-absorption |g spectroscopy measurements (NaI,Si(Li)) of 1982By03
163ER6cE also show a higher population of levels than observed in the present
163ERxcE decay scheme.
163ER cE $Intensity balance gives apparent |e feedings (none
163ER2cE expected from |DJ and |D|p) to the following levels, resulting in
163ER3cE anomalously low log| {Ift} values. Such feedings have been omitted from
163ER4cE the level scheme given here:
163ER5cE 91.5,7/2+ level (%|e=0.7 {I2}); 120.3,9/2+ level (%|e=0.14 {I6});
163ER6cE 190.0,9/2- level (%|e=0.11 {I4}); 664.78,5/2+ (%|e=0.24 {I6}). This
163ER7cE discrepancy is due either to misplaced |g rays or to missing |g rays,
163ER8cE or both.
163ER dE $I(|e+|b{++}) from decay scheme, except as noted.
163ER2dE Uncertainties include estimate of those caused by uncertain or
163ER3dE multiply-placed gammas.
163ER dE $I|b{++}(to g.s. and 69 level): upper limit estimated by the
163ER2dE evaluators from Fermi-Kurie analysis of 1982Vy07 and |b{++}/ce ratios.
163ER dE $I|e,I(|e+|b{++})(to g.s. and 69 level): from estimated
163ER2dE upper limit on I|b{++} and theoretical |e/|b{++} ratios.
163ER dE $I(|e+|b{++})(to 69 level)=1.1 {I9} from decay scheme.
163ER dE $I(|e+|b{++})(to 92 level)=0.9 {I3} inconsistent with
163ER2dE I(|e+|b{++})|<7.1|*10{+-6} from log| {Ift}|>12.8 expected for
163ER3dE 1/2+|)7/2+ transition.
163ER dE $I|b{++}(to 104 and 346 levels): relative intensities
163ER2dE obtained by 1982Vy07 from Fermi-Kurie analysis and normalized to
163ER3dE I|b{++}=0.41 {I3} from ce(K)(104.3|g)/|b{++}=98.9 {I35} and
163ER4dE I|b{++}=0.332 {I24} from |b{++}/ce(K)(655.8|g+666.1|g)=13.0 {I6}.
163ER5dE Renormalized by the evaluators from I|g normalization=0.188 {I9} to
163ER6dE 0.186 {I5}.
163ER dE $I|e,I(|e+|b{++})(to 104 and 346 levels): from I|b{++} and
163ER2dE theoretical |e/|b{++}.
163ER dE $I(|e+|b{++})(to 104 level): 2.2 {I15} from decay scheme.
163ER dE $I(|e+|b{++})(to 346 level): 5.5 {I5} from decay scheme.
163ER dE $I|b{++}(to levels between 541 and 735):
163ER2dE I|b(Emax=884)=0.136 {I7} compared to |SI|b(to|>540 and
163ER3dE |<735)=0.0122 {I5} from decay scheme.
163ER dE $I|e(to 684 and 780 levels) from decay scheme. Uncertainties
163ER2dE include estimate of those caused by uncertain or multiply-placed
163ER3dE gammas.
163ER dE $I|b{++}(to 735 and 856 levels): I|b(Emax=671)=0.032 {I4}
163ER2dE compared to |SI|b(to 735 and 856)=0.0069 {I8} from decay scheme.
163ER dE $I|b{++}(to levels |>963): I|b(Emax=453)=0.0146 {I13}
163ER2dE compared to |SI|b(to|>963)=0.0005 {I2} from decay scheme.
163ER cE TI,IE(E) From decay scheme, except as noted. Uncertainties include
163ER2cE estimate of those caused by uncertain or multiply-placed |g rays
163ER cE IB(A)$Relative intensities obtained by 1982Vy07 from Fermi-Kurie
163ER2cE analysis and normalized to I|b=0.41 {I3} from
163ER3cE ce(K)(104.3|g)/|b{++}=98.9 {I35} and I|b=0.332 {I24} from
163ER4cE |b{++}/ce(K)(655.8|g+666.1|g)=13.0 {I6}. Renormalized by the evaluators
163ERxcE from I|g normalization=0.188 {I9} to 0.186 {I5}.
163ER cE IE(A),TI(A)$From I|b{++} and theoretical |e/|b{++}
163ER cE IB(B)$Upper limit estimated (evaluators) from Fermi-Kurie analysis
163ER2cE of 1982Vy07 and theoretical |e/|b{++} ratios
163ER cE IE(B),TI(B)$From estimated upper limit on I|b{++} and theoretical
163ER2cE |e/|b{++} ratios
163ER cG $|a(K)exp: from 1982Vy07, except
163ER2cG as noted. |a(K)exp's available from 1976Ab09 and from 1980Ab18
163ER3cG (for E|g<400) are in general agreement with those from 1982Vy07.
163ER4cG Relative I|g's and Ice(K)'s normalized to |a(K)(104|g; M1)=0.218 by
163ER5cG 1982Vy07, 1980Ab18, and 1976Ab09
163ER cG $Subshell ratios are from 1980Ab18 or 1976Ab09
163ER cG $ce|g-coincidences from 1982Vy07 and |g|g-coincidences are from
163ER2cG 1976Ab09
163ER cG TI$Absolute intensities obtained by 1982Vy07 from Ice's and
163ER2cG theoretical |a's, except as noted. Renormalized by the evaluators from
163ER3cG I|g normalization=0.188 {I9} to 0.186 {I5}.
163ER cG E,RI$From 1982Vy07, unless otherwise stated. Least-squares analysis of
163ER2cG |g rays suggests that the uncertainties quoted by 1982Vy07 are
163ER3cG too low to be realistic. These should at least be doubled.
163ER cG M$From |a(K)exp's and subshell ratios given in comments.
163ER2cG 1982Vy07 appear to give only the dominant component when there is only
163ER3cG |a(K)exp. |d's added in these cases by the evaluators
163ER cG MR$From subshell ratios when available, otherwise from |a(K)exp
163ER cG E(H),RI(H)$|g from 1980Ab18 only. It is considered as uncertain
163ER2cG (evaluators) due to lack of confirmation by 1982Vy07.
163ER3cG Intensity is renormalized to 100 for 104|g
163ER cG E(G)$Tentative placement (evaluators) based on approximate (within
163ER2cG <1 keV) level-energy difference
163ER cG TI(Y)$Deduced (evaluators) from renormalized ce's of 1980Ab18 and |a's
163ER cG E(Z)$Poor fit, deviates by more than 2 |s's in the least-squares
163ER2cG analysis. It is possible that some of the |g rays in this
163ER3cG category are misplaced
163ER cG M(C)$E1,E2 from |a(K)exp. Multipolarity further restricted by
163ER2cG adopted |DJ|p
163ER cG M(B)$Large value of |a(K)exp suggests possibility of some E0 admixture
163ER tG $ ------------------------------------------------------------------
163ER tG $ The following unplaced |g rays reported by 1976Ab09 only
163ER2tG have been omitted, since these are not confirmed by 1982Vy07 or
163ER3tG 1980Ab18. (I|g renormalized by evaluators to I|g(104|g)=100 from
163ER+tG I|g=1940 {I37})
163ER2tG E|g I|g Mult. |a(K)exp E|g I|g Mul
163ER+tG t. |a(K)exp
163ER3tG ---------- ------- ------- ------- -------- -------- -------
163ER+tG -------
163ER4tG 63.67 {I5} 0.53 {I8} (E1) |? 0.7 755.4 {I3} 1.2 1
163ER+tG E2,(M1) 0.007
163ER5tG 96.35 {I10} 0.21 {I7} E1 <0.3 872.5 {I5} 0.3 1
163ER6tG 97.41 {I7} 0.55 {I9} (M1) |? 4 906.9 {I2}
163ER+tG 1.4 2 E2
163ER+tG 0.003
163ER7tG 98.29 {I7} 0.47 {I9} E1 0.14 936.4 {I4}
163ER+tG 0.5 1 E2
163ER+tG 0.003
163ER8tG 111.10 {I15} 0.07 {I4} M1 957.3 {I8}
163ER+tG 0.10 {I5}
163ER9tG 118.65 {I5} 0.61 {I10} E1 0.1 1011.3 {I6}
163ER+tG 0.4 1 E1,E2
163ER+tG <0.003
163ERAtG 147.7 {I2} 0.08 {I3} (M1) 1.0 1014.8 {I6}
163ER+tG 0.4 1 E2,(M1)
163ER+tG |?0.003
163ERBtG 152.7 {I1} 0.38 {I7} E1 |? 0.06 1018.8 {I6}
163ER+tG 0.4 1
163ERCtG 153.37 {I10} 0.49 {I8} E2 0.33 1022.5 {I7}
163ER+tG 0.3 1 M1,E2
163ER+tG 0.004
163ERXtG 287.6 {I4} 0.2 (I1} 1039.2 {I6}
163ER+tG 0.5 1 E2
163ER+tG 0.002
163EREtG 289.8 {I3} 0.35 {I18} 1108.0 {I7}
163ER+tG 0.22 {I10} (E2)
163ER+tG |?0.002
163ERFtG 697.0 {I6} 0.6 {I2} 1113.0 {I7}
163ER+tG 0.5 2
163ERGtG 727.3 {I3} 0.4 {I2} 1212.4 {I6}
163ER+tG 0.4 2 E2,(M1)
163ER+tG 0.002
163ERHtG 732.0 {I4} 0.4 {I2} M1 0.013 1302.9 {I5}
163ER+tG 1.1 21 E1,(E2)
163ER+tG <0.001
163ERItG 742.5 {I5} 0.3 {I1} E2,(M1) |? 0.007 1889.5 {I4}
163ER+tG 0.15 {I5}
163ERJtG 747.0 {I5} 0.3 {I1} M1 |? 0.014 2038.5 {I6}
163ER+tG 0.03 {I1}
163ERKtG --------------------------------------------------------------------
163ER cL $Bands: band structure suggested by 1976Ab09 and 1970Hj02
163ER2cL extended and confirmed by 1982Vy08.
163ER cL $Fragmentation of three-quasiparticle states: |?75% of the
163ER2cL decay of {+163}Tm goes to levels above 1 MeV. Of the 19 levels, seven
163ER3cL have J|p=3/2+ and for most of the others the large |e feedings make
163ER4cL J>3/2 very unlikely. This observed high density of 3/2+ levels may be
163ER5cL related to the fact that the three-quasiparticle states are highly
163ER6cL fragmented due to the interaction of the quasiparticle and collective
163ER7cL degrees of freedom. Note, however, that theory predicts this
163ER8cL fragmentation to be in the 2- to 3-MeV range.
163ER cL E$From least-squares fit to E|g's by assuming double the uncertainties
163ER2cL quoted by 1982Vy07. Least-squares analysis with the uncertainties
163ER3cL given by 1982Vy07 resulted in a poor fit with about 60 |g rays
163ER4cL out of a total of 225 |g rays deviating in energy by more
163ER5cL than 2 |s's. Doubling each uncertainty
163ER6cL improved the fit in that only 19 |g rays deviated by more
163ER7cL 2 |s's. All the discrepant cases are noted under comments. This
163ER8cL suggests that the uncertainties quoted by 1982Vy07 are underestimated.
163ER9cL The level energies are further rounded-off to nearest 0.01 keV
163ERAcL in view of poor fit to E|g's
163ER cL J$From adopted levels. Assignments proposed by 1982Vy08 based
163ER2cL on multipolarities and band structure are consistent
163ER CL BAND(A)$ |n5/2[523] band.
163ER CL BAND(B)$ |n5/2[642] band.
163ER2cL This is probably the dominant configuration, but this band most likely
163ER3cL also contains sizeable components of other orbitals originating from
163ER4cL the i{-13/2} spherical-shell-model state that are introduced by the
163ER5cL expected strong Coriolis coupling among these orbitals.
163ER CL BAND(D)$ |n3/2[521] band.
163ER CL BAND(E)$ |n1/2[521] band
163ER CL BAND(F)$ |n3/2[402] band (?).
163ER CL BAND(H)$ |n1/2[400] band.
163ER CL BAND(Z)$ |n3/2[651] band.
163ER CL BAND(Y)$ K-2 |g vibration built on the |n5/2[523] g.s.
163ER2cL The small value of the decoupling parameter excludes other
163ER3cL interpretations for this K=1/2 band. This band may have
163ER4cL some admixture of |n1/2[510]
163TM P 0 1/2+ 1.810 H 5 2439 3
163TM cP J,T$From the {+163}Tm adopted levels.
163TM cP QP$From 2009AuZZ, 2003Au03
163TM cP $Configuration=|p1/2[411]
163ER N 0.186 5 1. 1.0 1.
163ER cN NR from |SI|g(1+|a)(to g.s.)=98.2 {I18} (I(|e+|b{++})|<3.6
163ER2cN from log| {If{+1u}t}|>8.5 for first-forbidden unique transition).
163ER3cN Other: 0.188 {I9} from I|g(104|g)/I|g(K| x ray)=0.135 {I3} (1982Vy07);
163ER4cN 0.187 {I5} from |SI|g(1+|a)(to g.s.)=99.2 {I8} from estimated
163ERxcN I|b{++}(to g.s.)|<0.04.
163ER PN 3
163ER G 491.64 5 0.43 3 M1+E2 1.2 3 0.025 3
163ERS G KC=0.0207 25$LC=0.00344 25$MC=0.00077 6$NC+=0.000205 15
163ERS G NC=0.000179 13$OC=2.51E-5 20$PC=1.21E-6 16
163ER cG $|a(K)exp=0.021 {I2}
163ER G 493.83 4 0.74 4 M1+E2 1.7 3 0.0219 16
163ERS G KC=0.0178 14$LC=0.00314 15$MC=0.00071 3$NC+=0.000188 9
163ERS G NC=0.000164 8$OC=2.27E-5 12$PC=1.03E-6 9
163ER cG $|a(K)exp=0.0180 {I14}
163ER G 540.98 12 0.23 5 M1 0.0285
163ERS G KC=0.0241 4$LC=0.00347 5$MC=0.000767 11$NC+=0.000206 3
163ERS G NC=0.000179 3$OC=2.60E-5 4$PC=1.453E-6 21
163ER cG $|a(K)exp=0.037 {I12}
163ER G 563.80 5 0.69 16M1(+E2) 0.99 LE 0.022 4
163ERS G KC=0.019 3$LC=0.0028 4$MC=0.00062 7$NC+=0.000167 19
163ERS G NC=0.000145 17$OC=2.1E-5 3$PC=1.12E-6 19
163ER cG $|a(K)exp=0.022 {I6}
163ER G 756.17 7 1.17 9 M1 0.01227
163ERS G KC=0.01037 15$LC=0.001479 21$MC=0.000326 5$NC+=8.78E-5 13
163ERS G NC=7.61E-5 11$OC=1.105E-5 16$PC=6.22E-7 9
163ER cG $|a(K)exp=0.0121 {I12}
163ER G 779.93 5 3.54 13 M1 0.01136
163ERS G KC=0.00961 14$LC=0.001368 20$MC=0.000302 5$NC+=8.12E-5 12
163ERS G NC=7.04E-5 10$OC=1.022E-5 15$PC=5.76E-7 8
163ER cG $|a(K)exp=0.0116 {I7}
163ER cG $780|g+782|g in coin with ce(K)(69|g), ce(K)(80|g), and ce|g(104|g)
163ER G 781.88 9 2.03 9 E1,E2
163ER cG $|a(K)exp=0.0029 {I7}
163ERS G KC=0.0033 14
163ER G 785.72 14 0.46 6 E2(+M1) 2.2 GE 0.0061 5
163ERS G KC=0.0050 5$LC=0.00081 6$MC=0.000181 11$NC+=4.8E-5 3
163ERS G NC=4.2E-5 3$OC=5.9E-6 4$PC=2.9E-7 3
163ER cG $|a(K)exp=0.0045 {I10}
163ER G 846.57 12 0.83 12 E2 0.00477
163ERS G KC=0.00396 6$LC=0.000633 9$MC=0.0001416 20$NC+=3.77E-5 6
163ERS G NC=3.28E-5 5$OC=4.62E-6 7$PC=2.25E-7 4
163ER cG $|a(K)exp=0.0030 {I5}
163ER G 852.9 3 0.29 8
163ER G 892.8 2 0.65 13
163ER G 923.1 3 0.45 12E2(+M1) 1.6 GE 0.0045 5
163ERS G KC=0.0037 5$LC=0.00057 6$MC=0.000127 12$NC+=3.4E-5 4
163ERS G NC=2.9E-5 3$OC=4.2E-6 5$PC=2.2E-7 3
163ER cG $|a(K)exp=0.0032 {I10}
163ER G 1147.36 15 0.39 10
163ER G 1218.89 19 0.47 7
163ER G 1240.27 12 0.74 5 E2 0.00219
163ERS G KC=0.00184 3$LC=0.000269 4$MC=5.95E-5 9$NC+=2.58E-5 4
163ERS G NC=1.384E-5 20$OC=1.98E-6 3$PC=1.047E-7 15$IPC=9.90E-6 14
163ER cG $|a(K)exp=0.00174 {I26}
163ER G 1303.80 12 1.06 7
163ER G 1531.90 13 0.39 5 M1,E2 0.0019 4
163ERS G KC=0.0016 4$LC=0.00022 5$MC=4.8E-5 10$NC+=0.000105 12
163ERS G NC=1.12E-5 23$OC=1.6E-6 4$PC=9.1E-8 21$IPC=9.2E-5 9
163ER cG $|a(K)exp=0.0016 {I4}
163ER G 1626.58 16 0.26 5
163ER G 1654.47 8 0.58 7 E2(+M1) 1 GT 0.0015416
163ERS G KC=0.00119 13$LC=0.000167 18$MC=3.7E-5 4$NC+=0.000146 9
163ERS G NC=8.6E-6 9$OC=1.24E-6 14$PC=6.9E-8 9$IPC=0.000136 8
163ER cG $|a(K)exp=0.00113 {I19}
163ER G 1673.48 12 0.61 5 E1(+M2) 0.25 LT 0.0009810
163ERS G KC=0.00056 9$LC=7.6E-5 13$MC=1.7E-5 3$NC+=0.000322 8
163ERS G NC=3.9E-6 7$OC=5.6E-7 10$PC=3.2E-8 6$IPC=0.000317 9
163ER cG $|a(K)exp=0.00055 {I10}
163ER G 1729.7 3 0.18 4
163ER G 1790.12 5 0.83 7
163ER G 1793.38 7 1.01 3
163ER G 1835.69 20 0.125 19
163ER G 1879.6 2 0.146 18
163ER G 1913.88 14 0.090 14
163ER L 0.0 5/2- A
163ER E 0.04 LE 1.64 LE 8.8 GE 1.68 LEB1U?
163ERS E EAV=656.2 13 $CK=0.8064 $CL=0.1307 $CM+=0.03914
163ER L 69.23 1 5/2+ 8.3 NS 5 B
163ER cL E$from E|g. Level held fixed in least-squares analysis
163ER cL T$weighted average of 8.8 ns {I5} (1969Ve05,|g|g(t)) and 7.7 ns {I6}
163ERxcL (1974An04,|gce(t))
163ER E 0.04 LE 0.52 LE 7.9 GE 0.56 LEB ?
163ERS E EAV=613.4 14 $CK=0.7728 $CL=0.1201 $CM+=0.03573
163ER cE TI$0.7 {I6} from intensity balance
163ER G 69.229 3 62.4 14E1 0.853 C
163ERS G KC=0.699 10$LC=0.1202 17$MC=0.0267 4$NC+=0.00689 10
163ERS G NC=0.00607 9$OC=0.000791 11$PC=3.00E-5 5
163ER cG $|a(L1):|a(L2):|a(L3)=0.0701:0.0228:0.0286
163ER cG $L1:L2:L3=100:31.0 {I6}:38.5 {I8} (1987BaZB)
163ER cG M,MR$from adopted gammas. |d<0.05 from L-subshell ratios
163ER L 83.96 1 7/2- 0.92 NS 8 A
163ER cL T$ce|g(t) (1974An04)
163ER G 14.72 2 E1 11.13 1.2 3 Y ?
163ERS G L/T=0.713 7$M/T=0.165 3$N+/T=0.0394 8
163ERS G N/T=0.0357 7$O/T=0.00360 7$P/T=7.75E-5 15
163ER cG $|a(M1):|a(M2):|a(M3)=0.46:0.44:0.72
163ER cG E$|g from 1980Ab18 only. Placement is doubtful due to
163ER2cG intensity balance problems (evaluators)
163ER cG $M1:M2:M3=5 {I2}:5 {I2}:6 {I2}
163ER G 83.968 4 4.03 9 M1+E2 1.61 9 5.47 C
163ERS G KC=2.22 7$LC=2.49 8$MC=0.603 18$NC+=0.153 5
163ERS G NC=0.137 4$OC=0.0162 5$PC=0.000116 5
163ER cG $|a(L1):|a(L2):|a(L3)=0.20 {I6}:1.33 {I21}:1.35 {I22}
163ER cG $|a(K)exp=2.47 {I9}. |a(L3)exp=0.82 {I16} (1991GaZZ)
163ER cG $L1:L2:L3=100:435 {I38}:435 {I38} (1987BaZB)
163ER L 91.55 1 7/2+ B
163ER G 22.358 10 M1+E2 0.19 2 130 202.80 10
163ERS G L/T=0.77 8$M/T=0.18 4$N+/T=0.046 10
163ERS G N/T=0.041 9$O/T=0.0050 11$P/T=8.9E-5 14
163ER cG $|a(L1):|a(L2):|a(L3)=26 {I5}:34 {I7}:42 {I9}
163ER cG $L1:L2:L3=60 {I6}:78 {I8}:94 {I9}
163ER G 91.550 8 1.26 7 E1 0.411
163ERS G KC=0.340 5$LC=0.0552 8$MC=0.01223 18$NC+=0.00318 5
163ERS G NC=0.00279 4$OC=0.000371 6$PC=1.515E-5 22
163ER cG $|a(K)exp=0.33 {I8}
163ER L 104.32 1 3/2- 0.52 NS 5 D
163ER cL T$ce|g(t) (1974An04)
163ER dL $1970BaYN, 1972Af03, 1976AlZW and 1994MoZY probably refer to
163ER2dL the same measurement as in 1974An04
163ER E 2267 22 0.058 11 0.83 16 7.7 1 0.89 17A
163ERS E EAV=597.9 14 $CK=0.7774 $CL=0.1209 $CM+=0.03596
163ER cE TI$2.0 {I20} from intensity balance
163ER G 20.34 2 E2 4.33E3 0.241 21H ?
163ERS G N/T=0.0414 9$O/T=0.00473 10$P/T=1.78E-6 4
163ER cG $L2/L3=0.58 {I10}
163ERF G FLAG=Y
163ER G 35.05 3 E1 1.027 0.23 5 H ?
163ERS G L/T=0.396 4$M/T=0.0887 13$N+/T=0.0223 4
163ERS G N/T=0.0198 4$O/T=0.00239 4$P/T=7.29E-5 12
163ERS G L1C=0.342
163ER cG $|a(L1)exp=0.33 {I7} (1980Ab18)
163ERF G FLAG=Y
163ER G 104.320 3 100.0 19M1(+E2) 0.05 LT 2.52 C
163ERS G KC=2.11 3$LC=0.318 5$MC=0.0706 11$NC+=0.0190 3
163ERS G NC=0.01646 24$OC=0.00238 4$PC=0.0001303 19
163ER cG $|a(L1):|a(L2):|a(L3)=0.294:0.028:0.006
163ER cG MR$other: 0.11 {I6} from L1/L2=8.8 {I11} (1987BaZB)
163ER cG $K:L1:L2:L3=4263 {I400}:575 {I60}:43 {I5}:8.2 {I10}
163ER L 120.35 2 9/2+ B
163ER G 28.835 12 M1+E2 0.090 11 23.6 160.24 5
163ERS G L/T=0.75 4$M/T=0.169 15$N+/T=0.045 4
163ERS G N/T=0.039 4$O/T=0.0053 5$P/T=0.000227 15
163ER cG $|a(L1):|a(L2):|a(L3)=12.63 {I2}:3.3 {I6}:2.8 {I7}
163ER cG $L1:L2:L3=18 {I2}:6.0 {I6}:2.0 {I3}
163ER L 164.42 1 5/2- D
163ER E 0.027 12 1.8 8 8.6 2 1.8 8 1U
163ERS E EAV=585.3 13 $CK=0.8127 $CL=0.1326 $CM+=0.03974
163ER G 60.105 3 7.76 14M1+E2 0.222 8 12.77 19
163ERS G KC=9.87 14$LC=2.25 6$MC=0.514 14$NC+=0.135 4
163ERS G NC=0.119 3$OC=0.0159 4$PC=0.000621 9
163ER cG $|a(L1):|a(L2):|a(L3)=1.40:0.476 {I24}:0.41 {I3}
163ER cG $L1:L2:L3=100:34.5 {I12}:28.6 {I17} (1987BaZB)
163ER G 72.875 8 0.79 3 E1(+M2) 0.08 LT 1.0 3
163ERS G KC=0.81 20$LC=0.17 7$MC=0.039 16$NC+=0.010 5
163ERS G NC=0.009 4$OC=0.0012 6$PC=5.0E-5 24
163ER cG $|a(K)exp=0.78 {I14} (1980Ab18)
163ER G 80.460 7 2.80 8 M1+E2 0.048 10 5.32 C
163ERS G KC=4.45 7$LC=0.680 11$MC=0.1510 23$NC+=0.0405 6
163ERS G NC=0.0352 6$OC=0.00507 8$PC=0.000276 4
163ER cG $|a(L1):|a(L2):|a(L3)=0.623:0.060:0.013
163ER cG $|a(K)exp=4.8 {I2}
163ER cG $K:L1:L2:L3=251 {I30}:34 {I4}:3.4 {I4}:0.70 {I7}
163ER G 164.419 8 4.86 17M1+E2 0.135 21 0.690 C
163ERS G KC=0.577 9$LC=0.0880 13$MC=0.0196 3$NC+=0.00525 8
163ERS G NC=0.00456 7$OC=0.000656 10$PC=3.54E-5 6
163ER cG $|a(L1):|a(L2)=0.080:0.008
163ER cG $|a(K)exp=0.59 {I3}; K:L1:L2=56 {I8}:7.6 {I8}:0.8 {I1}
163ER L 190.01 8 9/2- A
163ER G 106.05 4 0.17 5 M1 2.40
163ERS G KC=2.02 3$LC=0.302 5$MC=0.0671 10$NC+=0.0180 3
163ERS G NC=0.01564 22$OC=0.00226 4$PC=0.0001244 18
163ER cG M$from adopted gammas
163ER cG $|a(K)exp=4.4 {I14}.
163ER dG $Probable typographical error in 1980Ab18 on Ice(K), which is 10% of
163ER2dG Ice(K) of 1982Vy07, which gives |a(K)exp={ 0.47 {I21}}
163ER L 249.53 1 7/2- D
163ER G 85.118 4 2.08 6 M1+E2 0.19 2 4.56 C
163ERS G KC=3.71 6$LC=0.656 21$MC=0.148 5$NC+=0.0393 13
163ERS G NC=0.0343 12$OC=0.00479 13$PC=0.000229 4
163ER cG $|a(L1):|a(L2):|a(L3)=0.518 {I4}:0.090 {I15}:0.053 {I16}
163ER cG $|a(K)exp=3.7 {I3}
163ER cG $K:L1:L2:L3=135 {I15}:21 {I2}:3.7 {I4}:2.3 {I3}
163ER G 129.21 3 0.48 8 E1 0.1646
163ERS G KC=0.1375 20$LC=0.0212 3$MC=0.00470 7$NC+=0.001231 18
163ERS G NC=0.001078 16$OC=0.0001464 21$PC=6.43E-6 9
163ER cG $|a(K)exp|?0.1 (1976Ab09)
163ER G 145.213 11 0.67 3 E2 0.755 C
163ERS G KC=0.406 6$LC=0.268 4$MC=0.0645 9$NC+=0.01641 23
163ERS G NC=0.01463 21$OC=0.001758 25$PC=1.774E-5 25
163ER cG $|a(L1):|a(L2):|a(L3)=0.041:0.12:0.11
163ER cG $|a(K)exp=0.50 {I6}
163ER cG $K:L1:L2:L3=5.2 {I8}:0.50 {I5}:1.7 {I2}:1.5 {I2}
163ER G 165.60 6 0.38 8 M1+E2 0.26 4 0.667 11
163ERS G KC=0.553 10$LC=0.0893 18$MC=0.0200 5$NC+=0.00534 11
163ERS G NC=0.00464 10$OC=0.000660 12$PC=3.37E-5 7
163ER cG $|a(L1):|a(L2):|a(L3)=0.076 {I1}:0.010 {I1}:0.0044 {I11}
163ER cG $|a(K)exp=0.58 {I17}. K:L1:L2:L3=4.2 {I9}:0.56 {I12}:0.08 {I2}:0.04
163ERxcG {I1}
163ER G 249.498 6 0.47 3 M1+E2 0.53 7 0.198 6
163ER3 G FL=0.0
163ERS G KC=0.163 5$LC=0.0275 4$MC=0.00619 10$NC+=0.001648 24
163ERS G NC=0.001437 21$OC=0.000202 3$PC=9.7E-6 4
163ER cG $|a(L1):|a(L2)=0.022:0.0038 {I5}
163ER cG $|a(K)exp=0.092 {I21}.
163ER2cG K:L1:L2=1.6 {I3}:0.22 {I3}:0.040 {I3}. ce(L2) derived from a complex
163ERxcG line
163ER L 345.62 1 1/2- E
163ER E 2091 2 0.19 2 5.3 5 6.80 4 5.5 5 A
163ERS E EAV=491.5 14 $CK=0.8030 $CL=0.1255 $CM+=0.03736
163ER cE TI 5.5 {I5} from decay scheme
163ER G 241.305 5 58.4 15M1 0.240 C
163ERS G KC=0.202 3$LC=0.0299 5$MC=0.00662 10$NC+=0.001779 25
163ERS G NC=0.001543 22$OC=0.000223 4$PC=1.237E-5 18
163ER cG $|a(L1):|a(L2)=0.0280:0.0022
163ER cG $K:L1:L2=200:30:3. |a(K)exp=0.188 {I7} for 239.6|g+241.3|g
163ER G 345.608 9 5.89 13E2 0.0453
163ERS G KC=0.0342 5$LC=0.00862 12$MC=0.00200 3$NC+=0.000521 8
163ERS G NC=0.000459 7$OC=5.99E-5 9$PC=1.80E-6 3
163ERS G L1C=0.0041$
163ER cG $|a(K)exp=0.036 {I3}, K/L1(from complex lines)=6.1 {I4}
163ER L 404.00 1 3/2- E
163ER E 0.054 9 1.8 3 7.23 7 1.9 3
163ERS E EAV=465.9 14 $CK=0.8077 $CL=0.1264 $CM+=0.03764
163ER G 58.35 2 M1+E2 0.73 17 18 8 0.25 4
163ER cG $Placement from 1976Ab09
163ER cG CC$near threshold for |a(K). |a(K) estimated as 8 {I8} (evaluators)
163ER cG $L1:L2:L3=1.5 {I5}:6.0 {I6}:3.0 {I3}. ce(L1) from complex line
163ERS G K/T=0.4 4$L/T=0.40 19$M/T=0.09 5$N+/T=0.026 13
163ER cG $|a(L1):|a(L2):|a(L3)=1.1 {I2}:3.1 {I9}:3.4 {I10}
163ER G 239.585 5 23.7 9 M1+E2 0.21 3 0.241 C
163ERS G KC=0.201 4$LC=0.0306 5$MC=0.00680 10$NC+=0.00182 3
163ERS G NC=0.001584 23$OC=0.000228 4$PC=1.228E-5 20
163ER cG $|a(L1):|a(L2):|a(L3)=0.0278 {I2}:0.00275 {I14}:0.00071 {I11}
163ER cG $|a(K)exp=0.188 {I7} for 239.6|g+241.3|g
163ER cG $K:L1:L2:L3=98 {I10}:13.2 {I15}:1.30 {I15}:0.33 {I4}
163ER G 299.667 8 24.5 5 M1+E2 0.21 6 0.1310 25 C
163ERS G KC=0.1099 23$LC=0.01645 24$MC=0.00365 6$NC+=0.000980 14
163ERS G NC=0.000851 13$OC=0.0001227 19$PC=6.69E-6 15
163ER cG $|a(L1):|a(L2):|a(L3)=0.015:0.0014 {I1}:0.00031 {I6}
163ER cG $|a(K)exp=0.110 {I4} for 297.9|g+299.7|g
163ER cG MR$from K:L1:L2:L3=58 {I6}:8.0 {I8}:0.70 {I7}:0.16 {I4}, assuming
163ER2cG insignificant contribution from 297.9|g (E1)
163ER G 320.057 18 1.66 7 E2 0.0568 C
163ERS G KC=0.0422 6$LC=0.01131 16$MC=0.00264 4$NC+=0.000684 10
163ERS G NC=0.000604 9$OC=7.82E-5 11$PC=2.20E-6 3
163ER cG $|a(L1):|a(L2)=0.0050:0.0039
163ER cG $|a(K)exp=0.042 {I6} (1980Ab18). K:L1:L2=1.5 {I2}:0.20 {I5}:0.15
163ERxcG {I5}
163ER G 403.989 10 5.66 14E2 0.0291 C
163ERS G KC=0.0225 4$LC=0.00508 8$MC=0.001172 17$NC+=0.000306 5
163ERS G NC=0.000270 4$OC=3.57E-5 5$PC=1.217E-6 17
163ER cG $|a(L1):|a(L2):|a(L3)=0.0027:0.0015:0.0009
163ER cG $|a(K)exp=0.0266 {I15}; K:L1:L2:L3=44:8:4:2
163ER L 439.54 1 5/2- E
163ER E 0.0056 9 0.98 15 8.65 7 0.99 15 1U
163ERS E EAV=466.3 13 $CK=0.8185 $CL=0.1353 $CM+=0.04064
163ER G 35.56 3 M1+E2 0.090 11 11.5 6 0.10 2
163ERS G L/T=0.716 23$M/T=0.162 10$N+/T=0.043 3
163ERS G N/T=0.0374 25$O/T=0.0052 4$P/T=0.000239 12
163ER cG $Placement from 1976Ab09
163ER cG $L1/L2=5.0 {I10}
163ER G 93.88 3 0.12 [E2] 3.74 H ?
163ERS G KC=1.240 18$LC=1.91 3$MC=0.466 7$NC+=0.1178 17
163ERS G NC=0.1054 15$OC=0.01234 18$PC=5.18E-5 8
163ER cG $|a(K)exp=0.9 (1976Ab09)
163ER G 190.006 6 7.68 16M1+E2 0.18 3 0.458 C
163ERS G KC=0.383 6$LC=0.0587 9$MC=0.01307 20$NC+=0.00350 6
163ERS G NC=0.00304 5$OC=0.000437 7$PC=2.34E-5 4
163ER cG $|a(L1):|a(L2):|a(L3)=0.053:0.0055 {I4}:0.0014 {I3}
163ER cG $|a(K)exp=0.393 {I15}. K:L1:L2:L3=58 {I6}:7.9 {I10}:0.8
163ERxcG {I1}:<0.3
163ER G 275.125 8 14.4 4 M1+E2 0.31 7 0.161 4 C
163ERS G KC=0.135 4$LC=0.0208 3$MC=0.00462 7$NC+=0.001238 18
163ERS G NC=0.001075 15$OC=0.0001542 23$PC=8.18E-6 24
163ER cG $|a(L1):|a(L2):|a(L3)=0.019:0.0018 {I1}:0.00045 {I9}
163ER cG $|a(K)exp=0.124 {I5}. K:L1:L2:L3=43 {I5}:5.8 {I6}:0.50 {I4}:0.20
163ERxcG {I2}
163ER G 335.219 12 3.18 8 M1+E2 0.66 14 0.084 5 C
163ERS G KC=0.069 5$LC=0.0114 3$MC=0.00256 6$NC+=0.000683 17
163ERS G NC=0.000595 14$OC=8.4E-5 3$PC=4.1E-6 3
163ER cG $|a(L1):|a(L2)=0.0094 {I5}:0.00159 {I17}
163ER cG $|a(K)exp=0.085 {I4}
163ER cG $K:L1:L2=4.9 {I6}:0.65 {I7}:0.11 {I2}
163ER G 355.624 13 2.57 7 M1 0.0848 C
163ERS G KC=0.0714 10$LC=0.01044 15$MC=0.00231 4$NC+=0.000621 9
163ERS G NC=0.000539 8$OC=7.81E-5 11$PC=4.35E-6 6
163ERS G L1C=0.0098$
163ER cG $|a(K)exp=0.082 {I4}. K/L1=7.1 {I22}
163ER G 439.575 17 1.99 17M1 0.0487
163ERS G KC=0.0410 6$LC=0.00596 9$MC=0.001318 19$NC+=0.000354 5
163ERS G NC=0.000307 5$OC=4.46E-5 7$PC=2.49E-6 4
163ER cG $|a(K)exp=0.04 (1976Ab09)
163ER L 462.48 2 3/2+ F
163ER E 0.045 3 1.91 12 7.19 3 1.96 12
163ERS E EAV=440.2 14 $CK=0.8119 $CL=0.1272 $CM+=0.03789
163ER G 297.87 3 2.57 9 (E1) 0.0189 ZC
163ER cG $Level-energy difference=298.07
163ERF G FL=164.42
163ERS G KC=0.01592 23$LC=0.00230 4$MC=0.000507 7$NC+=0.0001344 19
163ERS G NC=0.0001172 17$OC=1.646E-5 23$PC=8.22E-7 12
163ER cG $|a(K)exp=0.110 {I4} for 297.9|g+299.7|g
163ER G 358.174 10 3.92 9 E1 0.01204 C
163ERS G KC=0.01018 15$LC=0.001454 21$MC=0.000320 5$NC+=8.51E-5 12
163ERS G NC=7.41E-5 11$OC=1.047E-5 15$PC=5.34E-7 8
163ERS G L1C=0.00121$
163ER cG $|a(K)exp=0.0100 {I11}. K/L1=6.9 {I19}
163ER G 371.07 9 0.24 3 (E2) 0.0369
163ERS G KC=0.0282 4$LC=0.00675 10$MC=0.001563 22$NC+=0.000408 6
163ERS G NC=0.000359 5$OC=4.72E-5 7$PC=1.506E-6 22
163ER cG $|a(K)exp=0.023 {I4}
163ER G 393.261 11 7.37 15M1+E2 0.44 7 0.0596 17 C
163ERS G KC=0.0499 16$LC=0.00760 16$MC=0.00169 4$NC+=0.000453 9
163ERS G NC=0.000393 8$OC=5.64E-5 13$PC=3.00E-6 10
163ER cG $|a(L1):|a(L2)=0.0068:0.00074 {I5}
163ER cG $|a(K)exp=0.050 {I2}. K:L1:L2=8.0 {I15}:1.0 {I1}:0.10 {I1}
163ER L 526.33 4 5/2+ F
163ER G 361.97 4 0.42 4 E1 0.01174
163ERS G KC=0.00993 14$LC=0.001417 20$MC=0.000312 5$NC+=8.30E-5 12
163ERS G NC=7.23E-5 11$OC=1.021E-5 15$PC=5.21E-7 8
163ER cG $|a(K)exp=0.006 {I2}
163ER G 421.92 3 0.90 6 (E1) 0.00820 CC
163ERS G KC=0.00694 10$LC=0.000981 14$MC=0.000216 3$NC+=5.75E-5 8
163ERS G NC=5.01E-5 7$OC=7.10E-6 10$PC=3.68E-7 6
163ER cG $|a(K)exp=0.018 {I2}
163ER G 434.72 3 2.82 9 M1+E2 0.58 19 0.043 4 C
163ERS G KC=0.036 3$LC=0.0056 3$MC=0.00125 6$NC+=0.000334 16
163ERS G NC=0.000290 14$OC=4.15E-5 22$PC=2.17E-6 19
163ER cG $|a(K)exp=0.037 {I3}. L1/L2=3
163ER L 531.07 3 3/2+
163ER E 0.011 1 0.63 4 7.64 3 0.64 4
163ERS E EAV=410.1 14 $CK=0.8160 $CL=0.1281 $CM+=0.03816
163ER G 461.845 12 3.34 14M1+E2 0.90 16 0.0327 22 C
163ERS G KC=0.0271 20$LC=0.00438 19$MC=0.00098 4$NC+=0.000261 11
163ERS G NC=0.000227 10$OC=3.21E-5 16$PC=1.60E-6 13
163ER cG $|a(K)exp=0.0276 {I18}
163ER L 540.56 3 1/2+ H
163ER E 1906 3 0.062 3 3.54 17 6.89 2 3.60 17
163ERS E EAV=405.9 14 $CK=0.8165 $CL=0.1282 $CM+=0.03820
163ER cE IB I|b(Emax=884)=0.136 {I7} compared to |SI|b(to |>540 and
163ER2cE |<735)=0.0122 {I5} from decay scheme.
163ER G 78.041 24 0.42 6 M1(+E2) 0.6 LT 6.1 3
163ERS G KC=4.5 5$LC=1.2 5$MC=0.29 13$NC+=0.08 4
163ERS G NC=0.07 3$OC=0.009 4$PC=0.00027 3
163ER cG $|a(K)exp=5.0 {I9}
163ER G 436.24 6 0.85 5
163ER G 471.330 17 21.8 5 E2 0.0192 C
163ERS G KC=0.01516 22$LC=0.00311 5$MC=0.000713 10$NC+=0.000187 3
163ERS G NC=0.0001642 23$OC=2.21E-5 3$PC=8.34E-7 12
163ER cG $|a(L1):|a(L2):|a(L3)=0.0019:0.008:0.00044
163ER cG $|a(K)exp=0.0130 {I6}. K:L1:L2:L3=98:15:5:2.4
163ER L 574.08 3 3/2+
163ER E 0.012 1 0.78 8 7.53 5 0.79 8
163ERS E EAV=391.2 14 $CK=0.8182 $CL=0.1286 $CM+=0.03832
163ER G 324.49 15 0.28 3 C
163ER cG M$|a(K)exp=0.100 {I19} (1980Ab18) gives M1(+E2) with |d|<0.55, but
163ER2cG |DJ|p requires M2. No ce data available from 1982Vy07
163ER cG $|a(K)exp=0.100 {I19} (1980Ab18)
163ER G 409.77 5 0.82 6 C
163ER G 469.65 4 2.39 10E1 0.00642 C
163ERS G KC=0.00545 8$LC=0.000765 11$MC=0.0001683 24$NC+=4.48E-5 7
163ERS G NC=3.90E-5 6$OC=5.55E-6 8$PC=2.90E-7 4
163ER cG $|a(K)exp=0.008 (1976Ab09)
163ER G 504.878 14 6.3 3 M1+E2 0.8 5 0.027 6 C
163ERS G KC=0.023 5$LC=0.0035 5$MC=0.00078 11$NC+=0.00021 3
163ERS G NC=0.00018 3$OC=2.6E-5 4$PC=1.3E-6 4
163ER cG $|a(K)exp=0.023 {I2}
163ER L 619.36 2 3/2+ Z
163ER cL $1976Ab09 assigned the 619 level as a member of the 1/2[400] band.
163ER E 0.031 2 2.54 10 6.99 2 2.57 10
163ERS E EAV=371.3 14 $CK=0.8202 $CL=0.1291 $CM+=0.03847
163ER G 78.93 2 (M1,E2) 6.5 9 0.014 7 H ?
163ERF G FLAG=Y
163ER3 G FL=540.56
163ERS G K/T=0.43 15$L/T=0.34 20$M/T=0.08 6$N+/T=0.021 15
163ERS G N/T=0.018 14$O/T=0.0022 15$P/T=2.5E-5 15
163ER cG $K/L1|?7.3 {I20}. ce(L1) from complex line
163ER dG $KC GE 1.76 LE 4.83; |a(L1)|>0.167|<0.660
163ER G 454.954 17 1.71 6 C
163ER cG $|a(K)exp=0.02 (1976Ab09) gives M1,E2 but |DJ|p requires E1
163ER G 515.012 16 4.50 22E1+M2 0.186 18 0.0084 7 C
163ERS G KC=0.0071 6$LC=0.00107 9$MC=0.000237 20$NC+=6.4E-5 6
163ERS G NC=5.5E-5 5$OC=7.9E-6 7$PC=4.2E-7 4
163ER cG $|a(K)exp=0.0071 {I5}
163ER G 528.18 14 0.82 11(E2) 0.01430
163ERS G KC=0.01145 16$LC=0.00221 4$MC=0.000503 7$NC+=0.0001326 19
163ERS G NC=0.0001162 17$OC=1.580E-5 23$PC=6.37E-7 9
163ER cG M$|a(K)exp=0.030 {I5} gives M1(+E2), |d<0.3 but |DJ|p requires E2
163ER G 550.154 16 8.26 21M1(+E2) 0.27 LE 0.0268 7 C
163ERS G KC=0.0226 6$LC=0.00328 7$MC=0.000724 14$NC+=0.000195 4
163ERS G NC=0.000169 4$OC=2.45E-5 5$PC=1.36E-6 4
163ER cG $|a(K)exp=0.0240 {I13}
163ER G 619.44 10 0.35 5 E1+M2 0.17 8 0.0051 17
163ERS G KC=0.0043 14$LC=0.00062 23$MC=0.00014 6$NC+=3.7E-5 14
163ERS G NC=3.2E-5 13$OC=4.6E-6 18$PC=2.5E-7 10
163ER cG $|a(K)exp=0.0043 {I9}
163ER L 664.86 3 5/2+ Z
163ER E 0.0024 6 0.24 6 8.0 1 0.24 6 ?
163ER cE $Transition is suspect since log| {Ift} is too low
163ER2cE for a 1/2+ to 5/2+ transition
163ERS E EAV=351.4 14 $CK=0.8220 $CL=0.1295 $CM+=0.03862
163ER G 225.4 3 0.18 7 E1(+M2) 0.23 LT 0.07 4 H ?
163ERF G FLAG=G
163ERS G KC=0.06 3$LC=0.010 6$MC=0.0024 14$NC+=0.0006 4
163ERS G NC=0.0006 4$OC=8.E-5 5$PC=3.9E-6 23
163ER cG $|a(K)exp=0.06 {I3}
163ER G 415.15 6 0.47 4 E1 0.00851 C
163ERS G KC=0.00721 10$LC=0.001020 15$MC=0.000224 4$NC+=5.98E-5 9
163ERS G NC=5.20E-5 8$OC=7.38E-6 11$PC=3.82E-7 6
163ER cG $|a(K)exp=0.0064 {I13}
163ER G 500.51 2 0.76 12
163ER cG E$uncertainty from table in 1982Vy08. 1982Vy07 quote 0.12
163ER cG M$|a(K)exp=0.021 {I4} gives |d(E2/M1)=1.1 {I+8-4} but |DJ|p requires
163ERxcG E1
163ER G 560.51 5 0.66 16E1+M2 0.27 10 0.009 4 C
163ERS G KC=0.008 4$LC=0.0012 6$MC=0.00027 13$NC+=7.E-5 4
163ERS G NC=6.E-5 3$OC=9.E-6 4$PC=4.8E-7 22
163ER cG $|a(K)exp=0.0080 {I26}
163ER G 573.23 4 1.51 6 M1(+E2) 0.61 LE 0.0229 18 C
163ERS G KC=0.0192 16$LC=0.00282 18$MC=0.00062 4$NC+=0.000168 11
163ERS G NC=0.000146 9$OC=2.10E-5 14$PC=1.15E-6 10
163ER cG $|a(K)exp=0.021 {I3}
163ER G 595.35 5 1.28 9 E2 0.01064
163ER3 G FL=69.23
163ERS G KC=0.00862 12$LC=0.001571 22$MC=0.000356 5$NC+=9.40E-5 14
163ERS G NC=8.22E-5 12$OC=1.129E-5 16$PC=4.83E-7 7
163ER cG $|a(K)exp=0.0075 {I5}
163ER L 683.75 2 (1/2)- Y
163ER E 0.0047 6 0.52 7 7.65 6 0.52 7 E
163ERS E EAV=343.1 14 $CK=0.8226 $CL=0.1297 $CM+=0.03867
163ER G 338.28 8 0.72 5 M1 0.0968
163ERS G KC=0.0815 12$LC=0.01194 17$MC=0.00264 4$NC+=0.000711 10
163ERS G NC=0.000616 9$OC=8.93E-5 13$PC=4.96E-6 7
163ER cG $|a(L1):|a(L2)=0.011:0.0008
163ER cG $|a(K)exp=0.059 {I9}. K:L1:L2=1.1 {I2}:0.15 {I3}:<0.05
163ER G 520.1 2 0.28 6 E2 0.01487
163ER3 G FL=164.42
163ERS G KC=0.01189 17$LC=0.00231 4$MC=0.000527 8$NC+=0.0001388 20
163ERS G NC=0.0001216 17$OC=1.652E-5 24$PC=6.60E-7 10
163ER cG M$|a(K)exp=0.012 {I4} gives |d(E2/M1)|>1.7. |DJ|p requires E2
163ER G 579.510 13 8.53 19M1(+E2) 0.51 LE 0.0226 14 C
163ER3 G FL=104.32
163ERS G KC=0.0191 12$LC=0.00278 14$MC=0.00062 3$NC+=0.000165 8
163ERS G NC=0.000143 7$OC=2.07E-5 11$PC=1.15E-6 8
163ER cG $|a(L1):|a(L2)=0.0028:0.00018
163ER cG $|a(K)exp=0.0195 {I12}; K:L1:L2=50:8:<2 (1976Ab09)
163ER G 683.87 3 2.66 17(E2) 0.00767
163ERS G KC=0.00628 9$LC=0.001081 16$MC=0.000243 4$NC+=6.45E-5 9
163ERS G NC=5.63E-5 8$OC=7.82E-6 11$PC=3.55E-7 5
163ER cG M$|a(K)exp=0.0082 {I7} gives |d(E2/M1)=1.7 {I+6-3} but |DJ|p requires
163ERxcG E2
163ER L 717.39 3 3/2- Y
163ER E 0.0107 6 1.41 7 7.20 2 1.42 7
163ERS E EAV=328.3 14 $CK=0.8237 $CL=0.1300 $CM+=0.03877
163ER G 552.948 23 3.69 13M1 0.0270 C
163ERS G KC=0.0228 4$LC=0.00328 5$MC=0.000725 11$NC+=0.000195 3
163ERS G NC=0.0001690 24$OC=2.45E-5 4$PC=1.374E-6 20
163ER cG $|a(K)exp=0.0272 {I17}, possible contamination from
163ER2cG ce(L)(504.9|g) (evaluators)
163ER G 613.054 18 3.60 9 M1+E2 0.39 16 0.0193 12 C
163ERS G KC=0.0163 10$LC=0.00238 12$MC=0.000526 24$NC+=0.000141 7
163ERS G NC=0.000123 6$OC=1.77E-5 9$PC=9.8E-7 7
163ER cG $|a(K)exp=0.0166 {I9}
163ER G 633.77 9 0.78 7 C
163ER3 G FL=83.96
163ER cG M$|a(K)exp=0.0203 {I24} gives M1 but |DJ|p requires E2
163ER G 717.42 3 0.92 8 M1+E2 1.5 4 0.0091 11
163ERS G KC=0.0075 9$LC=0.00118 11$MC=0.000263 24$NC+=7.0E-5 7
163ERS G NC=6.1E-5 6$OC=8.7E-6 9$PC=4.4E-7 6
163ER cG $|a(K)exp=0.0077 {I8}
163ER L 735.38 2 1/2+,3/2+
163ER E 1693 7 0.0064 6 0.92 9 7.37 5 0.93 9
163ERS E EAV=320.4 14 $CK=0.8242 $CL=0.1302 $CM+=0.03882
163ER cE IB I|b(Emax=671)=0.032 {I4} compared to |SI|b(to 735 and
163ER2cE 856)=0.0069 {I8} from decay scheme.
163ER G 161.31 3 0.86 6 [M1,E2] 0.63 11
163ERS G KC=0.46 16$LC=0.13 4$MC=0.031 11$NC+=0.0079 25
163ERS G NC=0.0070 23$OC=0.00090 22$PC=2.6E-5 13
163ER cG M$|a(K)exp=0.12 (1976Ab09) gives E1 but |DJ|p requires M1,E2.
163ER2cG 1980Ab18 note that the peak is complex
163ER G 331.355 19 1.25 4 E1 0.01452
163ERS G KC=0.01227 18$LC=0.001760 25$MC=0.000388 6$NC+=0.0001031 15
163ERS G NC=8.98E-5 13$OC=1.265E-5 18$PC=6.39E-7 9
163ER cG $|a(K)exp=0.033 {I3}
163ER G 389.59 3 1.65 11E1 0.00987 C
163ER3 G FL=345.62
163ERS G KC=0.00835 12$LC=0.001186 17$MC=0.000261 4$NC+=6.95E-5 10
163ERS G NC=6.05E-5 9$OC=8.57E-6 12$PC=4.40E-7 7
163ER cG $|a(K)exp=0.029 {I3}. Other: 0.0071 {I15} (1980Ab18)
163ER G 666.178 19 11.04 25(E2) 0.00815 C
163ERS G KC=0.00666 10$LC=0.001158 17$MC=0.000261 4$NC+=6.91E-5 10
163ERS G NC=6.04E-5 9$OC=8.37E-6 12$PC=3.76E-7 6
163ER cG $|a(K)exp=0.0074 {I4}
163ER L 779.63 4 5/2- Y
163ER E 0.14 8 9.2 3 0.14 8 E1U?
163ERS E CK=0.8189 $CL=0.1384 $CM+=0.04174
163ER G 529.75 7 1.78 19M1+E2 0.8 4 0.024 4
163ER3 G FL=249.53
163ERS G KC=0.020 4$LC=0.0031 4$MC=0.00069 8$NC+=0.000184 22
163ERS G NC=0.000160 19$OC=2.3E-5 3$PC=1.18E-6 23
163ER cG $|a(K)exp=0.020 {I3}
163ER G 615.18 3 1.78 12M1+E2 0.56 21 0.0180 15 C
163ERS G KC=0.0151 13$LC=0.00224 15$MC=0.00050 3$NC+=0.000133 9
163ERS G NC=0.000116 8$OC=1.67E-5 12$PC=9.0E-7 8
163ER cG $|a(K)exp=0.0154 {I13}
163ER G 675.20 11 0.91 8 M1+E2 0.8 4 0.0130 22
163ERS G KC=0.0109 19$LC=0.00164 22$MC=0.00036 5$NC+=9.7E-5 13
163ERS G NC=8.5E-5 11$OC=1.21E-5 17$PC=6.5E-7 12
163ER cG $|a(K)exp=0.0112 {I19}
163ER G 688.12 11 1.09 11(E1) 0.00283
163ERS G KC=0.00241 4$LC=0.000331 5$MC=7.27E-5 11$NC+=1.94E-5 3
163ERS G NC=1.687E-5 24$OC=2.42E-6 4$PC=1.307E-7 19
163ER cG $|a(K)exp=0.006 (1976Ab09)
163ER G 695.81 12 0.70 8 M1+E2 0.7 4 0.0126 19 C
163ERS G KC=0.0106 17$LC=0.00156 20$MC=0.00035 5$NC+=9.3E-5 12
163ERS G NC=8.1E-5 10$OC=1.16E-5 16$PC=6.3E-7 11
163ER cG $|a(K)exp=0.0107 {I18}
163ER G 710.81 11 0.51 5
163ER3 G FL=69.23
163ER L 856.22 4 (3/2)-
163ER E 0.18 4 8.0 1 0.18 4
163ERS E EAV=267.0 14 $ CK=0.8265 $CL=0.1311 $CM+=0.03913
163ER G 606.4 2 0.64 4 [E2] 0.01018
163ERS G KC=0.00826 12$LC=0.001493 21$MC=0.000338 5$NC+=8.93E-5 13
163ERS G NC=7.81E-5 11$OC=1.074E-5 15$PC=4.64E-7 7
163ER cG M$|a(K)exp=0.0285 {I24} gives M1 but |DJ|p requires E2
163ER G 691.736 22 3.23 12M1 0.01532 C
163ERS G KC=0.01295 19$LC=0.00185 3$MC=0.000409 6$NC+=0.0001099 16
163ERS G NC=9.53E-5 14$OC=1.384E-5 20$PC=7.78E-7 11
163ER cG $|a(K)exp=0.0137 {I8}
163ER G 752.04 5 2.01 9 M1 0.01244 BC
163ERS G KC=0.01052 15$LC=0.001499 21$MC=0.000331 5$NC+=8.90E-5 13
163ERS G NC=7.71E-5 11$OC=1.120E-5 16$PC=6.31E-7 9
163ER cG $|a(K)exp=0.0129 {I9}
163ER L 963.29 8 (3/2)+
163ER E 1475 9 0.37 15 7.6 2 0.37 15
163ERS E EAV=219.7 14 $CK=0.8274 $CL=0.1319 $CM+=0.03938
163ER cE IB I|b(Emax=453)=0.0146 {I13} compared to |SI|b(to
163ER2cE |>963)=0.0005 {I2} from decay scheme.
163ER G 798.74 9 0.92 5 C
163ER cG M$|a(K)exp=0.010 (1976Ab09) gives M1,E2 but |DJ|p requires E1
163ER G 858.72 6 1.92 13(E1) 0.00183 C
163ERS G KC=0.001555 22$LC=0.000211 3$MC=4.63E-5 7$NC+=1.240E-5 18
163ERS G NC=1.077E-5 15$OC=1.549E-6 22$PC=8.50E-8 12
163ER cG $|a(K)exp=0.0026 {I3}
163ER G 894.26 11 1.4 7 [M1,E2] 0.0062 20 @C
163ERS G KC=0.0052 17$LC=0.00076 21$MC=0.00017 5$NC+=4.5E-5 13
163ERS G NC=3.9E-5 11$OC=5.7E-6 16$PC=3.1E-7 11
163ER cG RI$I|g=2.10 {I10} divided (evaluators) using |a(K)exp and assumed
163ERxcG mults
163ER cG $|a(K)exp=0.0040 {I4}
163ER L 985.67 8 5/2-
163ER E 0.75 14 8.2 2 0.75 14E1U
163ERS E CK=0.8165 $CL=0.1407 $CM+=0.04257
163ER G 411.66 7 0.53 4
163ER cG M$|a(K)exp=0.04 (1976Ab09) suggests M1,E2 but |DJ|p requires E1
163ER G 640.4 2 0.40 6
163ER G 735.97 10 0.61 8 E2(+M1) 2.46 GE 0.0070 5 C
163ERS G KC=0.0058 5$LC=0.00094 5$MC=0.000211 11$NC+=5.6E-5 3
163ERS G NC=4.9E-5 3$OC=6.9E-6 4$PC=3.3E-7 3
163ER cG $|a(K)exp=0.0054 {I8}
163ER G 821.3 2 0.36 10
163ER G 881.4 3 0.25 6(M1) 0.00840
163ERS G KC=0.00711 10$LC=0.001008 15$MC=0.000222 4$NC+=5.98E-5 9
163ERS G NC=5.18E-5 8$OC=7.53E-6 11$PC=4.25E-7 6
163ER cG $|a(K)exp=0.014 {I4}
163ER G 894.26 11 0.7 7 [E1] 1.69E-3 @C
163ERS G KC=0.001439 21$LC=0.000195 3$MC=4.28E-5 6$NC+=1.145E-5 16
163ERS G NC=9.94E-6 14$OC=1.431E-6 20$PC=7.87E-8 11
163ER G 902.18 14 0.55 13M1+E2 0.9 7 0.0062 16
163ERS G KC=0.0053 14$LC=0.00077 17$MC=0.00017 4$NC+=4.6E-5 10
163ERS G NC=4.0E-5 9$OC=5.7E-6 13$PC=3.1E-7 9
163ER cG $|a(K)exp=0.0054 {I13}
163ER G 916.81 9 1.10 11E1 1.61E-3
163ER3 G FL=69.23
163ERS G KC=0.001373 20$LC=0.000186 3$MC=4.07E-5 6$NC+=1.091E-5 16
163ERS G NC=9.47E-6 14$OC=1.364E-6 20$PC=7.51E-8 11
163ER cG $|a(K)exp=0.00151 {I24}
163ER L 1059.75 4 3/2-
163ER E 0.79 5 7.25 3 E
163ERS E CK=0.8274 $CL=0.1325 $CM+=0.03960
163ER G 375.87 5 0.83 7 M1+E2 1.1 3 0.053 6
163ERS G KC=0.043 6$LC=0.0076 5$MC=0.00172 9$NC+=0.000456 24
163ERS G NC=0.000398 20$OC=5.5E-5 4$PC=2.5E-6 4
163ERS G L1C=0.00565$
163ER cG M$from |a(K)exp=0.043 {I4}. K/L1=7.3 {I17}
163ER G 655.760 20 4.25 10M1(+E2) 0.38 LE 0.0169 7 C
163ERS G KC=0.0143 6$LC=0.00206 7$MC=0.000456 14$NC+=0.000123 4
163ERS G NC=0.000106 4$OC=1.54E-5 5$PC=8.6E-7 4
163ER cG $|a(K)exp=0.0151 {I10}
163ER G 714.04 10 0.41 4 M1 0.01415 BC
163ERS G KC=0.01196 17$LC=0.001708 24$MC=0.000377 6$NC+=0.0001014 15
163ERS G NC=8.79E-5 13$OC=1.277E-5 18$PC=7.18E-7 10
163ER cG $|a(K)exp=0.020 {I2}
163ER G 975.19 4 2.00 10(E2) 0.00354 G ?
163ERF G FL=83.96
163ERS G KC=0.00296 5$LC=0.000455 7$MC=0.0001013 15$NC+=2.70E-5 4
163ERS G NC=2.35E-5 4$OC=3.33E-6 5$PC=1.683E-7 24
163ER cG $|a(K)exp=0.0038 {I3}
163ER cG $Level-energy difference=84.56
163ER G 991.0 4 0.31 9 (E1) 1.39E-3 C
163ERS G KC=0.001187 17$LC=0.0001601 23$MC=3.51E-5 5$NC+=9.39E-6 14
163ERS G NC=8.15E-6 12$OC=1.176E-6 17$PC=6.50E-8 10
163ER cG $|a(K)exp<0.003 (1976Ab09)
163ER L 1281.16 5 1/2+,3/2+
163ER E 0.62 5 7.20 4 E
163ERS E CK=0.8257 $CL=0.1341 $CM+=0.04016
163ER G 598.12 3 1.36 7 (E1) 0.00379 Z
163ERF G FL=683.75
163ERS G KC=0.00322 5$LC=0.000446 7$MC=9.80E-5 14$NC+=2.61E-5 4
163ERS G NC=2.27E-5 4$OC=3.25E-6 5$PC=1.738E-7 25
163ER cG $Level-energy difference=597.41
163ER cG $|a(K)exp|?0.003 (1976Ab09)
163ER G 1176.09 3 2.60 16E1 1.03E-3 ZC
163ERF G FL=104.32
163ERS G KC=0.000869 13$LC=0.0001164 17$MC=2.55E-5 4$NC+=2.10E-5 3
163ERS G NC=5.92E-6 9$OC=8.56E-7 12$PC=4.78E-8 7$IPC=1.414E-5 20
163ER cG $Level-energy difference=1176.83
163ER cG $|a(K)exp=0.00087 {I18}
163ER L 1369.46 3 3/2+
163ER E 7.84 26 6.02 2 E
163ERS E CK=0.8247 $CL=0.1349 $CM+=0.04044
163ER G 406.06 15 0.28 6 E2(+M1) 2.0 GE 0.032 4
163ERS G KC=0.025 3$LC=0.00523 25$MC=0.00120 5$NC+=0.000315 15
163ERS G NC=0.000276 12$OC=3.71E-5 21$PC=1.39E-6 19
163ER cG $|a(K)exp=0.022 {I6}
163ER G 589.13 11 0.37 6 Z
163ER cG $Level-energy difference=589.84
163ERF G FL=779.63
163ER G 749.6 3 0.32 9
163ER G 828.8 3 0.31 5 M1 0.00978
163ERS G KC=0.00827 12$LC=0.001175 17$MC=0.000259 4$NC+=6.97E-5 10
163ERS G NC=6.04E-5 9$OC=8.78E-6 13$PC=4.95E-7 7
163ER cG $|a(K)exp=0.0116 {I28}
163ER G 844.69 13 0.45 10 Z
163ER cG $Level-energy difference=843.15
163ERF G FL=526.33
163ER G 1205.019 24 13.1 3 E1 C
163ERS G KC=0.000832$
163ER cG $|a(K)exp=0.00083 {I5}
163ER G 1265.116 25 27.8 5 E1 C
163ERS G KC=0.000764$
163ER cG $|a(K)exp=0.00071 {I4}
163ER G 1300.41 6 2.78 17M1+E2 1.0 4 0.0027 3 C
163ERS G KC=0.0022 3$LC=0.00032 4$MC=7.0E-5 8$NC+=4.0E-5 3
163ERS G NC=1.62E-5 18$OC=2.3E-6 3$PC=1.30E-7 17$IPC=2.11E-5 10
163ER cG $|a(K)exp=0.00224 {I21}
163ER L 1514.61 3 3/2+
163ER E 2.72 12 6.35 2 E
163ERS E CK=0.8224 $CL=0.1366 $CM+=0.04104
163ER G 733.6 2 0.35 3 Z
163ER cG $Level-energy difference=734.98
163ERF G FL=779.63
163ER G 940.62 3 2.72 9 E2 0.00382 C
163ERS G KC=0.00318 5$LC=0.000494 7$MC=0.0001102 16$NC+=2.94E-5 5
163ERS G NC=2.56E-5 4$OC=3.62E-6 5$PC=1.81E-7 3
163ER cG $|a(K)exp=0.0026 {I2}
163ER G 1075.13 3 4.28 20E1 1.20E-3 C
163ERS G KC=0.001022 15$LC=0.0001373 20$MC=3.01E-5 5$NC+=8.06E-6 12
163ERS G NC=6.99E-6 10$OC=1.010E-6 15$PC=5.61E-8 8
163ER cG $|a(K)exp=0.00123 {I17}
163ER G 1168.97 5 2.3 3 E1 1.04E-3 C
163ERS G KC=0.000879 13$LC=0.0001177 17$MC=2.58E-5 4$NC+=1.90E-5 3
163ERS G NC=5.99E-6 9$OC=8.66E-7 13$PC=4.83E-8 7$IPC=1.208E-5 17
163ER cG $|a(K)exp=0.00088 {I14}
163ER G 1350.15 3 2.29 9 E1 8.94E-4 C
163ERS G KC=0.000682 10$LC=9.08E-5 13$MC=1.99E-5 3$NC+=0.0001011 15
163ERS G NC=4.62E-6 7$OC=6.69E-7 10$PC=3.75E-8 6$IPC=9.58E-5 14
163ER cG $|a(K)exp=0.00077 (1976Ab09)
163ER G 1410.19 3 2.47 9 E1 C
163ERS G KC=0.000633$
163ER cG $|a(K)exp=0.00070 {I9}
163ER G 1514.3 4 0.34 5
163ER L 1538.79 3 3/2+
163ER cL $Probable configuration=(|n5/2[523])~#(|p7/2[523])~#(|p1/2[411]), with
163ER2cL K|p=3/2+.
163ER E 16.9 6 5.53 2 E
163ERS E CK=0.8219 $CL=0.1369 $CM+=0.04115
163ER G 478.49 14 0.26 8
163ER3 G FL=1059.75
163ER G 575.1 3 0.25 7 [M1,E2] 0.018 7
163ERS G KC=0.015 6$LC=0.0023 7$MC=0.00052 14$NC+=0.00014 4
163ERS G NC=0.00012 4$OC=1.7E-5 5$PC=9.E-7 4
163ER G 759.41 9 1.25 7 C
163ER cG M$|a(K)exp=0.0060 {I7} gives M1,E2 but |DJ|p requires E1
163ER G 803.469 22 1.44 5 M1 0.01055 C
163ERS G KC=0.00893 13$LC=0.001270 18$MC=0.000280 4$NC+=7.53E-5 11
163ERS G NC=6.53E-5 10$OC=9.49E-6 14$PC=5.35E-7 8
163ER cG $|a(K)exp=0.0098 {I7}
163ER G 873.88 17 0.47 7 (E2) 0.00446 C
163ERS G KC=0.00370 6$LC=0.000587 9$MC=0.0001311 19$NC+=3.49E-5 5
163ERS G NC=3.04E-5 5$OC=4.29E-6 6$PC=2.11E-7 3
163ER cG $|a(K)exp=0.0028 {I12}
163ER G 997.67 19 0.47 9 M1+E2 1.3 9 0.0044 14
163ERS G KC=0.0037 12$LC=0.00055 16$MC=0.00012 4$NC+=3.2E-5 9
163ERS G NC=2.8E-5 8$OC=4.1E-6 12$PC=2.2E-7 8
163ER cG $|a(K)exp=0.0038 {I8}
163ER G 1099.38 3 2.82 17E1 1.15E-3 C
163ER3 G FL=439.54
163ERS G KC=0.000981 14$LC=0.0001318 19$MC=2.88E-5 4$NC+=7.73E-6 11
163ERS G NC=6.71E-6 10$OC=9.69E-7 14$PC=5.39E-8 8
163ER cG $|a(K)exp=0.00104 {I12}
163ER G 1135.28 9 1.81 17E1 1.09E-3 C
163ERF G FL=404.00
163ERS G KC=0.000926 13$LC=0.0001242 18$MC=2.72E-5 4$NC+=1.227E-5 18
163ERS G NC=6.32E-6 9$OC=9.13E-7 13$PC=5.09E-8 8$IPC=4.99E-6 8
163ER cG $|a(K)exp=0.0013 {I2}
163ER G 1192.34 19 0.86 8 (E1) 1.01E-3 C
163ER3 G FL=345.62
163ERS G KC=0.000848 12$LC=0.0001135 16$MC=2.48E-5 4$NC+=2.62E-5 4
163ERS G NC=5.78E-6 8$OC=8.35E-7 12$PC=4.66E-8 7$IPC=1.96E-5 3
163ER cG $|a(K)exp=0.0007 {I3}
163ER G 1374.34 3 23.0 6 E1 C
163ERS G KC=0.000661$
163ER cG $|a(K)exp=0.00066 {I4}
163ER G 1434.45 3 42.8 10E1 C
163ERS G KC=0.000614$
163ER cG $|a(K)exp=0.00062 {I4}
163ER G 1446.88 13 0.49 6
163ER G 1469.42 3 15.6 3 M1+E2 0.65 20 0.0022612 C
163ER3 G FL=69.23
163ERS G KC=0.00186 10$LC=0.000260 14$MC=5.7E-5 3$NC+=8.7E-5 3
163ERS G NC=1.33E-5 7$OC=1.94E-6 11$PC=1.09E-7 7$IPC=7.15E-5 20
163ER cG $|a(K)exp=0.00189 {I10}
163ER L 1569.80 2 3/2+
163ER E 9.7 3 5.74 2 E
163ERS E CK=0.8213 $CL=0.1374 $CM+=0.04132
163ER G 584.86 9 0.49 4 ZC
163ER cG $Level-energy difference=584.13
163ERF G FL=985.67
163ER G 790.12 6 1.65 11E1 0.00215 C
163ERS G KC=0.00183 3$LC=0.000249 4$MC=5.47E-5 8$NC+=1.464E-5 21
163ERS G NC=1.271E-5 18$OC=1.83E-6 3$PC=9.96E-8 14
163ER cG $|a(K)exp=0.0022 {I5}
163ER G 833.96 4 2.75 10M1+E2 1.2 3 0.0069 7 ZC
163ERF G FL=735.38
163ERS G KC=0.0057 6$LC=0.00086 8$MC=0.000191 16$NC+=5.1E-5 5
163ERS G NC=4.4E-5 4$OC=6.4E-6 6$PC=3.4E-7 4
163ER cG $Level-energy difference=834.42
163ER cG $|a(K)exp=0.0058 {I4}
163ER G 886.06 3 2.00 10E1 1.72E-3 C
163ERS G KC=0.001465 21$LC=0.000199 3$MC=4.35E-5 6$NC+=1.166E-5 17
163ERS G NC=1.012E-5 15$OC=1.457E-6 21$PC=8.01E-8 12
163ER cG $|a(K)exp=0.00183 {I21}
163ER G 905.6 2 1.16 18M1(+E2) 0.61 LE 0.0074 6
163ER3 G FL=664.86
163ERS G KC=0.0062 5$LC=0.00089 6$MC=0.000196 13$NC+=5.3E-5 4
163ERS G NC=4.6E-5 3$OC=6.6E-6 5$PC=3.7E-7 3
163ER cG $|a(K)exp=0.0075 {I16}
163ER G 950.85 7 1.03 7 M1+E2 0.9 3 0.0055 6
163ERF G FL=619.36
163ERS G KC=0.0047 6$LC=0.00068 7$MC=0.000150 15$NC+=4.0E-5 4
163ERS G NC=3.5E-5 4$OC=5.0E-6 5$PC=2.7E-7 4
163ER cG $|a(K)exp=0.0047 {I5}
163ER G 995.8 2 1.08 12M1(+E2) 0.43 LE 0.0060124
163ERS G KC=0.00509 21$LC=0.00072 3$MC=0.000159 6$NC+=4.27E-5 16
163ERS G NC=3.71E-5 14$OC=5.38E-6 21$PC=3.03E-7 13
163ER cG $|a(K)exp=0.0058 {I8}
163ER G 1029.18 6 0.81 10E2 0.00317
163ERS G KC=0.00265 4$LC=0.000403 6$MC=8.96E-5 13$NC+=2.39E-5 4
163ERS G NC=2.08E-5 3$OC=2.96E-6 5$PC=1.510E-7 22
163ER cG $|a(K)exp=0.0022 {I4}
163ER G 1042.66 9 0.74 12M1(+E2) 1.2 LE 0.0048 8 Z
163ERF G FL=526.33
163ERS G KC=0.0041 7$LC=0.00058 9$MC=0.000129 18$NC+=3.5E-5 5
163ERS G NC=3.0E-5 5$OC=4.4E-6 7$PC=2.4E-7 4
163ER cG $Level-energy difference=1043.46
163ER cG $|a(K)exp=0.0044 {I9}
163ER G 1130.224 23 12.3 4 E1 1.10E-3 C
163ERS G KC=0.000933 13$LC=0.0001252 18$MC=2.74E-5 4$NC+=1.162E-5 17
163ERS G NC=6.37E-6 9$OC=9.21E-7 13$PC=5.13E-8 8$IPC=4.28E-6 6
163ER cG $|a(K)exp=0.00096 {I6}
163ER G 1165.6 2 0.76 12 C
163ER G 1224.152 24 11.2 3 E1 C
163ERS G KC=0.000809$
163ER cG $|a(K)exp=0.00072 {I4}
163ER G 1405.36 3 4.11 14E1 C
163ERS G KC=0.000636$
163ER cG $|a(K)exp=0.00068 {I8}
163ER G 1465.73 3 10.3 3 E1 ZC
163ER cG $Level-energy difference=1465.47
163ERF G FL=104.32
163ERS G KC=0.000592$
163ER cG $|a(K)exp=0.00078 {I6}
163ER G 1500.61 4 2.00 12M1+E2 0.9 4 0.0020421 C
163ERS G KC=0.00166 18$LC=0.000234 24$MC=5.1E-5 6$NC+=9.5E-5 6
163ERS G NC=1.20E-5 12$OC=1.74E-6 18$PC=9.7E-8 11$IPC=8.1E-5 4
163ER cG $|a(K)exp=0.00169 {I15}
163ER G 1569.65 10 0.43 6
163ER L 1593.03 4 3/2+
163ER E 2.46 9 6.31 2 E
163ERS E CK=0.8208 $CL=0.1377 $CM+=0.04145
163ER G 813.32 10 0.81 13E1 0.00203
163ERS G KC=0.001727 25$LC=0.000235 4$MC=5.16E-5 8$NC+=1.381E-5 20
163ERS G NC=1.199E-5 17$OC=1.724E-6 25$PC=9.42E-8 14
163ER cG $|a(K)exp=0.0020 {I4}
163ER G 928.06 11 0.74 11M1(+E2) 1.0 LE 0.0065 9
163ERS G KC=0.0055 8$LC=0.00079 10$MC=0.000175 21$NC+=4.7E-5 6
163ERS G NC=4.1E-5 5$OC=5.9E-6 8$PC=3.3E-7 5
163ER cG $|a(K)exp=0.0058 {I10}
163ER G 1052.37 13 0.56 8 (M1) 0.00545 B
163ERS G KC=0.00462 7$LC=0.000651 10$MC=0.0001434 20$NC+=3.86E-5 6
163ERS G NC=3.34E-5 5$OC=4.86E-6 7$PC=2.75E-7 4
163ER cG $|a(K)exp=0.0149 {I22}
163ER G 1153.45 3 5.64 16E1 1.06E-3 C
163ERS G KC=0.000900 13$LC=0.0001206 17$MC=2.64E-5 4$NC+=1.534E-5 22
163ERS G NC=6.14E-6 9$OC=8.87E-7 13$PC=4.94E-8 7$IPC=8.27E-6 12
163ER cG $|a(K)exp=0.00077 {I5}
163ER G 1189.00 13 0.42 11(E1) 1.02E-3 @C
163ERS G KC=0.000852 12$LC=0.0001141 16$MC=2.50E-5 4$NC+=2.51E-5 4
163ERS G NC=5.81E-6 9$OC=8.40E-7 12$PC=4.68E-8 7$IPC=1.84E-5 3
163ER cG RI$total I|g=0.85 {I11}
163ER cG $1982Vy07 place this |g from the 1593 level only.
163ER2cG Least-squares analysis suggests double placement (evaluators).
163ER3cG Equal intensity assigned, arbitrarily, in each place
163ER cG $|a(K)exp=0.0013 {I5}
163ER G 1247.44 3 4.87 13E1 C
163ERS G KC=0.000783$
163ER cG $|a(K)exp=0.00066 {I5}
163ER G 1489.04 10 0.41 7
163ER G 1593.05 11 0.22 6
163ER L 1653.15 6 3/2+
163ER E 1.11 5 6.59 2 E
163ERS E CK=0.8194 $CL=0.1388 $CM+=0.04182
163ER G 796.2 2 0.35 6 ?
163ER3 G FL=856.22
163ER G 1033.95 11 0.70 12
163ER cG M$|a(K)exp=0.001 (1976Ab09) gives E1 but |DJ|p requires M1,E2
163ER G 1213.52 15 0.72 10 C
163ER G 1307.26 11 0.94 7
163ER cG M$|a(K)exp=0.002 (1976Ab09) gives M1,E2 but |DJ|p requires E1
163ER G 1561.60 5 1.11 7 E2 1.49E-3 C
163ERS G KC=0.001186 17$LC=0.0001679 24$MC=3.70E-5 6$NC+=0.0001031 15
163ERS G NC=8.61E-6 12$OC=1.241E-6 18$PC=6.76E-8 10$IPC=9.32E-5 13
163ER cG $|a(K)exp=0.00141 {I15}
163ER G 1583.95 4 2.13 7 M1 0.00218 C
163ERS G KC=0.001742 25$LC=0.000242 4$MC=5.33E-5 8$NC+=0.0001383 20
163ERS G NC=1.243E-5 18$OC=1.81E-6 3$PC=1.031E-7 15$IPC=0.0001240 18
163ER cG $|a(K)exp=0.00158 {I11}
163ER L 1722.39 5 3/2+
163ER E 2.86 11 6.09 2 E
163ERS E CK=0.8174 $CL=0.1402 $CM+=0.04234
163ER G 662.67 11 1.42 16 C
163ER G 987.74 10 1.32 11M1+E2 1.1 4 0.0048 7 Z
163ERF G FL=735.38
163ERS G KC=0.0040 6$LC=0.00059 7$MC=0.000130 16$NC+=3.5E-5 5
163ERS G NC=3.0E-5 4$OC=4.3E-6 6$PC=2.4E-7 4
163ER cG $Level-energy difference=987.01
163ER cG $|a(K)exp=0.0040 {I5}
163ER G 1005.01 9 1.03 15E1 1.36E-3
163ERS G KC=0.001156 17$LC=0.0001559 22$MC=3.41E-5 5$NC+=9.15E-6 13
163ERS G NC=7.94E-6 12$OC=1.145E-6 16$PC=6.34E-8 9
163ER cG $|a(K)exp=0.0013 {I3}
163ER G 1037.1 4 0.67 7
163ER3 G FL=683.75
163ER cG M$|a(K)exp=0.003 (1976Ab09) gives M1,E2 but |DJ|p requires E1
163ER G 1181.94 16 0.81 11(E2) 0.00240
163ERS G KC=0.00202 3$LC=0.000298 5$MC=6.60E-5 10$NC+=2.11E-5 3
163ERS G NC=1.534E-5 22$OC=2.19E-6 3$PC=1.149E-7 16$IPC=3.49E-6 5
163ER cG $|a(K)exp=0.0024 {I6}
163ER G 1318.34 3 8.27 17 (E1) CC
163ERS G KC=0.00071$
163ER cG $|a(K)exp=0.00118 {I8}
163ER G 1376.79 10 1.83 18 C
163ER G 1618.20 19 0.19 7
163ER G 1631.4 4 0.16 5
163ER L 1801.56 4 3/2+
163ER cL $Probable configuration=(|n5/2[523])~#(|p7/2[523])~#(|p1/2[411]), with
163ER2cL K|p=1/2+
163ER E 12.9 4 5.33 2 E
163ERS E CK=0.8146 $CL=0.1424 $CM+=0.04309
163ER G 433.2 3 0.48 10M1+E2 1.1 8 0.036 13
163ER3 G FL=1369.46
163ERS G KC=0.030 11$LC=0.0050 10$MC=0.00113 21$NC+=0.00030 6
163ERS G NC=0.00026 5$OC=3.7E-5 9$PC=1.7E-6 8
163ER cG $|a(K)exp=0.030 {I8}
163ER G 837.94 13 0.32 11(M1) 0.00951
163ERS G KC=0.00805 12$LC=0.001143 16$MC=0.000252 4$NC+=6.78E-5 10
163ERS G NC=5.88E-5 9$OC=8.54E-6 12$PC=4.82E-7 7
163ER cG $|a(K)exp=0.009 {I3}
163ER G 945.27 3 4.67 12E1 1.52E-3 C
163ERS G KC=0.001296 19$LC=0.0001752 25$MC=3.84E-5 6$NC+=1.028E-5 15
163ERS G NC=8.93E-6 13$OC=1.287E-6 18$PC=7.10E-8 10
163ER cG $|a(K)exp=0.00146 {I12}
163ER G 1066.49 8 1.06 9 M1+E2 1.0 4 0.0041 6
163ER3 G FL=735.38
163ERS G KC=0.0035 5$LC=0.00050 6$MC=0.000111 14$NC+=3.0E-5 4
163ERS G NC=2.6E-5 4$OC=3.7E-6 5$PC=2.0E-7 3
163ER cG $|a(K)exp=0.0035 {I4}
163ER G 1261.20 8 1.30 14(M1) 0.00354 BC
163ERS G KC=0.00299 5$LC=0.000418 6$MC=9.21E-5 13$NC+=4.03E-5 6
163ERS G NC=2.15E-5 3$OC=3.13E-6 5$PC=1.775E-7 25$IPC=1.548E-5 22
163ER cG $|a(K)exp=0.0049 {I6}
163ER G 1338.62 14 0.49 12
163ER G 1397.52 3 37.8 8 E1 C
163ERS G KC=0.000643$
163ER cG $|a(K)exp=0.00065 {I4}
163ER G 1455.94 3 19.5 6 E1 C
163ERS G KC=0.000599$
163ER cG $|a(K)exp=0.00057 {I4}
163ER G 1637.46 12 0.45 10 C
163ER G 1697.22 4 2.60 12E1 C
163ERS G KC=0.000463$
163ER cG $|a(K)exp=0.00050 {I7}
163ER G 1732.92 15 0.87 4 (M1) 0.00186
163ER3 G FL=69.23
163ERS G KC=0.001412 20$LC=0.000196 3$MC=4.31E-5 6$NC+=0.000209 3
163ERS G NC=1.004E-5 14$OC=1.463E-6 21$PC=8.34E-8 12$IPC=0.000197 3
163ER cG $|a(K)exp|?0.002 (1976Ab09)
163ER L 1826.49 3 3/2+
163ER E 5.33 17 5.68 2 E
163ERS E CK=0.8135 $CL=0.1431 $CM+=0.04337
163ER G 457.07 5 0.74 7 M1,E2 0.032 12
163ERS G KC=0.027 11$LC=0.0044 10$MC=0.00099 21$NC+=0.00026 6
163ERS G NC=0.00023 5$OC=3.2E-5 8$PC=1.6E-6 7
163ER cG $|a(K)exp=0.027 {I12}
163ER G 863.2 3 0.29 10M1,E2 0.0067 22
163ERS G KC=0.0056 19$LC=0.00083 23$MC=0.00018 5$NC+=4.9E-5 14
163ERS G NC=4.3E-5 12$OC=6.2E-6 18$PC=3.3E-7 12
163ER cG $|a(K)exp=0.0064 {I25}
163ER G 1046.9 2 0.69 8
163ER cG M$|a(K)exp=0.0024 {I5} gives E2 but |DJ|p requires E1
163ER G 1091.01 4 1.78 18M1+E2 1.0 4 0.0039 6 C
163ERS G KC=0.0033 5$LC=0.00047 6$MC=0.000105 13$NC+=2.8E-5 4
163ERS G NC=2.4E-5 3$OC=3.5E-6 5$PC=1.9E-7 3
163ER cG $|a(K)exp=0.0034 {I4}
163ER G 1142.51 5 4.33 15E1 1.08E-3 C
163ER3 G FL=683.75
163ERS G KC=0.000915 13$LC=0.0001227 18$MC=2.69E-5 4$NC+=1.335E-5 19
163ERS G NC=6.25E-6 9$OC=9.03E-7 13$PC=5.03E-8 7$IPC=6.15E-6 9
163ER cG $|a(K)exp=0.00072 {I7}
163ER G 1285.82 5 1.80 14M1+E2 0.7 4 0.0029 4 C
163ERS G KC=0.0025 3$LC=0.00035 4$MC=7.7E-5 9$NC+=4.0E-5 3
163ERS G NC=1.80E-5 19$OC=2.6E-6 3$PC=1.46E-7 18$IPC=1.89E-5 9
163ER cG $|a(K)exp=0.0025 {I3}
163ER G 1365.6 5 0.34 11M1 0.00295 B
163ER3 G FL=462.48
163ERS G KC=0.00247 4$LC=0.000345 5$MC=7.60E-5 11$NC+=6.03E-5 9
163ERS G NC=1.773E-5 25$OC=2.58E-6 4$PC=1.467E-7 21$IPC=3.98E-5 6
163ER cG $|a(K)exp=0.0032 {I14}
163ER G 1386.99 3 5.83 14E1 C
163ERS G KC=0.000651$
163ER cG $|a(K)exp=0.00063 {I5}
163ER G 1422.58 12 0.58 7
163ER cG $|a(K)exp=0.002 (1976Ab09)
163ER G 1480.94 3 3.33 22 E1 C
163ERS G KC=0.000582$
163ER cG $|a(K)exp=0.00046 {I14}
163ER G 1662.12 5 5.35 20E1 C
163ERS G KC=0.000480$
163ER cG $|a(K)exp=0.00063 {I4}
163ER G 1722.37 5 2.80 10E1 C
163ER3 G FL=104.32
163ERS G KC=0.000452$
163ER cG $|a(K)exp=0.00037 {I4}
163ER G 1741.75 9 0.45 3 ZC
163ER cG $Level-energy difference=1742.52
163ERF G FL=83.96
163ER cG $|a(K)exp=0.001 (1976Ab09) gives M1,E2 but |DJ|p requires M2
163ER G 1757.25 14 0.34 3
163ER L 1853.54 4 3/2+
163ER E 2.06 8 6.05 2 E
163ERS E CK=0.8122 $CL=0.1441 $CM+=0.04371
163ER G 484.03 4 1.41 14M1(+E2) 0.94 LE 0.033 5
163ERS G KC=0.028 5$LC=0.0042 5$MC=0.00094 9$NC+=0.000251 25
163ERS G NC=0.000218 21$OC=3.1E-5 4$PC=1.7E-6 3
163ER cG $|a(K)exp=0.028 {I4}
163ER G 1689.15 4 1.98 12 E1 C
163ERS G KC=0.000467$
163ER cG $|a(K)exp=0.00046 {I7}
163ER G 1749.22 4 5.53 19 E1 C
163ERS G KC=0.000441$
163ER cG $|a(K)exp=0.000361 {I23}
163ER G 1784.29 4 2.03 9 E2 1.28E-3 C
163ERS G KC=0.000927 13$LC=0.0001293 18$MC=2.84E-5 4$NC+=0.000192 3
163ERS G NC=6.62E-6 10$OC=9.56E-7 14$PC=5.28E-8 8$IPC=0.000184 3
163ER cG $|a(K)exp=0.00109 {I8}
163ER G 1853.33 12 0.15 3
163ER L 1872.79 6 (3/2)+
163ER E 2.48 14 5.93 3 E
163ERS E CK=0.8112 $CL=0.1448 $CM+=0.04397
163ER G 303.06 9 0.38 4 (E2) 0.0670
163ERS G KC=0.0491 7$LC=0.01377 20$MC=0.00322 5$NC+=0.000834 12
163ERS G NC=0.000737 11$OC=9.48E-5 14$PC=2.53E-6 4
163ER cG $|a(K)exp|?0.05 (1976Ab09)
163ER G 908.18 18 1.10 21E2(+M1) 2.0 GE 0.0045 4 Z
163ERF G FL=963.29
163ERS G KC=0.0037 4$LC=0.00058 4$MC=0.000128 9$NC+=3.42E-5 25
163ERS G NC=2.98E-5 21$OC=4.2E-6 4$PC=2.15E-7 21
163ER cG $Level-energy difference=909.50
163ER cG $|a(K)exp=0.0034 {I7}
163ER G 1137.10 10 2.01 11M1(+E2) 0.57 LE 0.0042825 C
163ERS G KC=0.00363 21$LC=0.00051 3$MC=0.000113 6$NC+=3.15E-5 17
163ERS G NC=2.63E-5 14$OC=3.82E-6 21$PC=2.15E-7 14$IPC=1.19E-6 4
163ER cG $|a(K)exp=0.0039 {I4}
163ER G 1189.00 13 0.42 11(E1) @C
163ERS G KC=0.000852$
163ER cG $|a(K)exp=0.0013 {I5}
163ER G 1332.13 7 0.70 12M1(+E2) 0.91 LE 0.0029 3
163ERS G KC=0.00239 24$LC=0.00034 3$MC=7.4E-5 7$NC+=4.9E-5 3
163ERS G NC=1.73E-5 16$OC=2.51E-6 24$PC=1.41E-7 15$IPC=2.93E-5 13
163ER cG $|a(K)exp=0.0028 {I6}
163ER G 1345.82 19 0.36 7 M1,E2
163ERS G KC=0.0021 5$
163ER cG $|a(K)exp=0.0040 {I20}
163ER G 1709.03 6 0.73 4 (E1) ZC
163ERF G FL=164.42
163ER cG $Level-energy difference=1708.36
163ERS G KC=0.000458$
163ER cG $|a(K)exp=0.00034 {I15}
163ER G 1767.65 10 0.99 5 ZC
163ERF G FL=104.32
163ER cG $Level-energy difference=1768.46
163ER G 1803.55 5 6.96 19E2 1.26E-3 C
163ERS G KC=0.000909 13$LC=0.0001266 18$MC=2.79E-5 4$NC+=0.000200 3
163ERS G NC=6.48E-6 9$OC=9.37E-7 14$PC=5.17E-8 8$IPC=0.000192 3
163ER cG $|a(K)exp=0.00096 {I6}
163ER L 1917.48 7 (3/2)+
163ER E 0.75 4 6.38 3 E
163ERS E CK=0.8086 $CL=0.1467 $CM+=0.04466 6
163ER G 380.57 17 0.19 4 (E2) 0.0344 Z
163ERF G FL=1538.79
163ERS G KC=0.0264 4$LC=0.00620 9$MC=0.001433 21$NC+=0.000374 6
163ERS G NC=0.000329 5$OC=4.34E-5 7$PC=1.413E-6 20
163ER cG $Level-energy difference=378.69
163ER cG $|a(K)exp=0.036 {I9}
163ER G 547.96 14 0.47 7 [M1,E2] 0.020 8
163ERS G KC=0.017 7$LC=0.0027 7$MC=0.00060 15$NC+=0.00016 4
163ERS G NC=0.00014 4$OC=2.0E-5 6$PC=1.0E-6 5
163ER G 1251.90 10 1.08 5 E2 0.00215 Z?
163ERF G FL=664.86
163ERS G KC=0.00180 3$LC=0.000264 4$MC=5.84E-5 9$NC+=2.71E-5 4
163ERS G NC=1.357E-5 19$OC=1.94E-6 3$PC=1.028E-7 15$IPC=1.149E-5 17
163ER cG $Level-energy difference=1252.62
163ER cG $|a(K)exp=0.0019 {I3}
163ER G 1753.45 8 0.79 7 C
163ER3 G FL=164.42
163ER G 1813.60 7 0.249 21 ZC
163ER cG $Level-energy difference=1813.15
163ERF G FL=104.32
163ER G 1825.23 7 1.05 4 E2 1.25E-3 Z
163ERF G FL=91.55
163ERS G KC=0.000889 13$LC=0.0001237 18$MC=2.72E-5 4$NC+=0.000209 3
163ERS G NC=6.33E-6 9$OC=9.15E-7 13$PC=5.06E-8 7$IPC=0.000202 3
163ER cG $Level-energy difference=1825.92
163ER cG $|a(K)exp=0.00103 {I10}
163ER G 1848.22 9 0.20 6 (M1) 1.69E-3
163ERS G KC=0.001216 17$LC=0.0001682 24$MC=3.70E-5 6$NC+=0.000270 4
163ERS G NC=8.63E-6 12$OC=1.257E-6 18$PC=7.17E-8 10$IPC=0.000260 4
163ER cG $|a(K)exp=0.0015 {I8}
163ER L 2040.68 8 3/2+
163ER E 0.85 5 6.06 3 E
163ERS E CK=0.7978 $CL=0.1547 3 $CM+=0.04751 10
163ER G 447.90 16 0.41 10[M1,E2] 0.034 13
163ERS G KC=0.028 11$LC=0.0047 11$MC=0.00105 21$NC+=0.00028 6
163ERS G NC=0.00024 5$OC=3.4E-5 9$PC=1.7E-6 8
163ER G 1323.64 18 0.49 12(E1) C
163ERS G KC=0.000706$
163ER cG $|a(K)exp<0.002 (1976Ab09)
163ER G 1577.66 15 0.28 3
163ER G 1876.23 6 1.20 11 E1 C
163ERS G KC=0.000393$
163ER cG $|a(K)exp=0.00041 {I8}
163ER G 1936.38 6 1.96 5 E1 C
163ERS G KC=0.000374$
163ER cG $|a(K)exp=0.00029 {I3}
163ER G 1971.2 2 0.050 13
163ER G 2040.76 16 0.174 26
163ER L 2052.50 6 3/2-
163ER E 1.15 7 5.90 3 E
163ERS E CK=0.7963 $CL=0.1558 3 $CM+=0.04790 11
163ER G 1273.17 14 0.97 18M1(+E2) 0.68 LE 0.0032423 C
163ERS G KC=0.00274 19$LC=0.000385 25$MC=8.5E-5 6$NC+=4.00E-5 20
163ERS G NC=1.98E-5 13$OC=2.87E-6 19$PC=1.62E-7 12$IPC=1.72E-5 6
163ER cG $|a(K)exp=0.0033 {I7}
163ER G 1525.97 4 4.04 20E1 C
163ERS G KC=0.000553
163ER cG $|a(K)exp=0.00054 {I9}
163ER G 1649.3 3 0.29 11 C
163ER G 1888.1 3 0.11 6
163ER G 1948.40 5 0.36 3 C
163ER3 G FL=104.32
163ER G 1983.24 8 0.35 3
163ER G 2052.8 2 0.086 8
163ER L 2122.21 11 1/2(-),3/2
163ER E 0.16 2 6.55 6 E
163ERS E CK=0.7849 $CL=0.1642 5 $CM+=0.05094 17
163ER G 400.74 17 0.35 6
163ER3 G FL=1722.39
163ER G 1158.0 2 0.29 16 G ?
163ER3 G FL=963.29
163ER cG M$|a(K)exp=0.0028 {I16} consistent with E2
163ER G 1957.57 7 0.29 4 C
163ER G 2017.96 9 0.249 16
163ER L 2243.21 19 3/2-
163ER E 0.15 2 6.06 6 E
163ERS E CK=0.7373 23 $CL=0.1991 17 $CM+=0.0637 7
163ER G 417.89 9 0.31 5 G ?
163ERF G FL=1826.49
163ER G 961.61 12 0.65 12E1 1.47E-3
163ERS G KC=0.001255 18$LC=0.0001696 24$MC=3.72E-5 6$NC+=9.95E-6 14
163ERS G NC=8.64E-6 12$OC=1.245E-6 18$PC=6.87E-8 10
163ER cG $|a(K)exp=0.0012 {I4}
163ER G 2079.0 4 0.077 10
163ER G 2159.98 16 0.083 12
163ER3 G FL=83.96
163ER L 2274.5 10 1/2(-),3/2
163ER E 0.008 4 7.1 2 E
163ERS E CK=0.707 4 $CL=0.221 3 $CM+=0.0718 11
163ER G 473.76 5 1.08 10 G ?
163ER cG M$|a(K)exp=0.025 {I5} gives M1+E2, |d=1.0 {I5}
163ER G 2274.5 5 0.042 18