64ZN 64GA EC DECAY (2.627 M) 1975RA28,2007MI12,1967MA0421NDS 202112
64ZN H TYP=FUL$AUT=Balraj Singh and Jun Chen$CIT=NDS 178, 41 (2021).$
64ZN2 H CUT=12-Nov-2021$
64ZN c Decays mainly by |b{++} (only|?2% by |e)
64ZN c 1975Ra28: {+64}Ga produced in {+64}Zn(p,n),E(p)=10 MeV. Measured E|g,
64ZN2c I|g for 37 |g rays at the Oak Ridge Van de Graaff accelerator.
64ZN3c Discussed isospin-forbidden 0{++} |) 0{++} |b transitions.
64ZN c 2007Mi12: {+64}Ga produced in {+54}Fe({+12}C,pn),E({+12}C)=36 MeV
64ZN2c reaction. Measured E|g, I|g, |g|g-coin using three HPGe detectors at
64ZN5c the Bucharest FN Tandem accelerator facility.
64ZN6c Discussed staggering of |g vibrational band and E(5) critical point
64ZN7c symmetry.
64ZN c 1990SuZR: measured E|g, I|g, T{-1/2}, |b{++}+|e feeding to the
64ZN2c g.s. from the intensity of the annihilation radiation using
64ZN3c mass-separated sources produced in {+64}Zn(p,n),E(p)=16 MeV reaction
64ZN4c at the IGISOL facility of the cyclotron laboratory, Tohoku University.
64ZN c 1967Ma04: measured E|g, I|g, |g|g-coin for 25 |g rays, |b{++}|g
64ZN2c circular polarization at LBNL, Berkeley.
64ZN c 1967Ko02: measured E|g, I|g, |g|g- and |b|g-coin, T{-1/2}({+64}Ga)
64ZN2c at the Instituut voor Kernphysisch Onderzoek, Amsterdam.
64ZN c 1967Au04: measured E|g, I|g, Ge(Li) detector. Values of E|g and I|g,
64ZN2c without uncertainties, for 21 |g rays are listed in 1967Ve09 evaluation
64ZN c 1960Ja07: measured E|g, I|g, |g|g- and |b|g-coin, E|b, I|b, half-life
64ZN2c of {+64}Ga decay; 13 |g rays reported in this work, with intensities
64ZN3c for 11 of these.
64ZN c Other measurements:
64ZN c 1987Yo03: measured half-life of {+64}Ga decay
64ZN c 1985Pa07 (also 1983Pa05): conversion electron study for excited 0+
64ZN2c states.
64ZN c 1980Na15: measured half-life of {+64}Ga decay.
64ZN d 1980NaZS is superseded by 1980Na15
64ZN c 1976Mo12 (also 1977ReZK thesis): measured E(|b{++}), shape factors
64ZN c 1972Mo08: measured half-life of {+64}Ga decay.
64ZN c 1966De10: measured |b{++}|g circular polarization, establishing
64ZN2c spin of 0 for {+64}Ga parent.
64ZN c 1953Co14: identified {+64}Ga activity, and measured half-life and
64ZN2c E|g for three |g rays
64ZN c 1953Cr15: identified {+64}Ga activity, and measured its half-life
64ZN d Theoretical calculations of Fermi matrix elements:
64ZN2d 1981Ya01, 1972Ya05, 1970Ko41, 1968Kr10, 1966Va27
64ZN cE TI$From |g-transition intensity balance at each excited state.
64ZN2cE For g.s. feeding, measured value of 24.7% {I10} (1990SuZR).
64ZN3cE In-out intensity balances at levels, where no feedings are expected
64ZN4cE from |DJ|p values: 1.3% {I7} for 991.5 level, -0.8% {I7} for 1799.4
64ZN5cE level.
64ZN cG $Following unplaced |g rays reported only by 1967Ko02 with E|g and I|g
64ZN2cG are omitted as not confirmed in later studies: 427.1 {I5} (I|g=4 {I2})
64ZN3cG (I|g<0.017 in 1973Da01, <0.8 in 1967Ko02, most likely from {+64}Ge
64ZN4cG decay); 3869 {I2} (I|g=0.5 {I2}, <0.2 in 1967Ma04); 4215 {I3}
64ZN5cG (I|g=0.6 {I4}, <0.14 in 1967Ma04); 4749 {I5} (I|g=0.3 {I2}, <0.06 in
64ZN6cG 1967Ma04); 5190 {I30} (I|g=0.05 {I3}, <0.06 in 1967Ma04); 5310 {I30}
64ZN7cG (I|g=0.05 {I3}, <0.06 in 1967Ma04).
64ZN cG $Following unplaced |g rays reported only by 1967Ma04 with E|g and I|g
64ZN2cG are omitted as not confirmed in later studies: 1909.8 (I|g<1.2, <0.3 in
64ZN3cG 1975Ra28); 2240 (I|g=1.2, <0.4 in 1975Ra28); 2632 {I2} (I|g=0.8 {I6},
64ZN4cG <0.3 in 1975Ra28)
64ZN cG E$From weighted average of available values from 2007Mi12 and 1975Ra28,
64ZN2cG unless otherwise noted. Values from 1990SuZR are given without
64ZN3cG uncertainties, and seem systematically higher by 0.5 to 2 keV, as
64ZN4cG compared to those in 2007Mi12 and 1975Ra28. Values in 1967Ma04
64ZN5cG and 1967Ko02 are in general agreement, but less precise.
64ZN cG RI$From unweighted average of available values from 2007Mi12, 1975Ra28,
64ZN2cG and 1967Ma04, unless otherwise noted. Values from 1990SuZR are in
64ZN3cG general agreement with those from 2007Mi12 and 1975Ra28, but are given
64ZN4cG without uncertainties. Values in 1967Ko02 are not in good agreement,
64ZN5cG and are less precise.
64ZN cG M,MR$From the Adopted dataset for definite assignments or those in
64ZN2cG parentheses. Assignments in square brackets are assumed from |DJ|p
64ZN cG $Measured intensity of annihilation radiation=453 {I14}, relative
64ZN2cG to 100 for 991.6|g (1975Ra28)
64ZN cL E$From a least-squares fit to E|g data
64ZN cL J,T$From the Adopted Levels
64GA P 0.0 0+ 2.627 M 12 7171.2 15
64GA cP J,T$From {+64}Ga Adopted Levels. Spin=0 from |b|g circular
64GA2cP polarization measurements by 1966De10 and 1967Ma04
64GA cP QP$From 2021Wa16
64ZN N 0.483 7 1.0 1.0
64ZN cN NR$Deduced from I(|e+|b{++})(to g.s.)=24.7% {I10} (1990SuZR, from
64ZN2cN intensity of the annihilation radiation using a mass-separated {+64}Ga
64ZN3cN source), theoretical |e/|b{++} ratios, and transition intensity balance
64ZN4cN at each level. Other measured values of g.s. |b{++}+|e feeding:
64ZN5cN 33.8% {I11} (1975Ra28, from measured intensity of annihilation
64ZN6cN radiation, accounting for contribution from {+61}Cu and {+66}Ga
64ZN7cN decays); 21.4% {I11} (1967Ko02, probably from |b{++} spectrum);
64ZN8cN 25% (1960Ja07, |b{++} spectrum). Value from 1990SuZR is preferred by
64ZN9cN the evaluators as only in this work a mass separated source of {+64}Ga
64ZNAcN was used, with less or no contamination from other activities
64ZNBcN contributing to the intensity of the annihilation radiation. Other I|g
64ZNCcN normalization=0.48 (1990SuZR), 0.431 (1975Ra28), 0.486 (1967Ma04).
64ZN PN 3
64ZN L 0.0 0+
64ZN E 24.6 10 0.073 3 6.65 2 24.7 10
64ZNS E EAV=2875.75 74$CK=0.002627 2$CL=0.0002890 2$CM+=5.141E-5 4
64ZN cE IB$from 1990SuZR. Others: 33.8% {I11} (1975Ra28, from annihilation
64ZN2cE radiation); 21.4% {I11} (1967Ko02);
64ZN2cE 25% (1960Ja07, from measured I|b{++})
64ZN cE E$measured E|b=6050 {I30} (1960Ja07). Other: 1976Mo12 obtain E|b=5972
64ZN2cE {I13}, but point out that high energy effects in the detector will
64ZN3cE reduce the observed E|b+. In a later work the authors (1977ReZK)
64ZN4cE ascribe a discrepancy of |?100 keV in the Q(|b{+-}) value to a
64ZNxcE possible shape factor
64ZN cE LOGFT$this is the lowest log| {Ift} value of all the well-known
64ZN2cE 0+ to 0+ isospin-forbidden transitions
64ZN L 991.54 7 2+ 1.94 PS 5
64ZN G 991.56 10 100 E2
64ZN2 G %IG=48.3 7
64ZNS G CC=0.000300 4$KC=0.000269 4$LC=2.70E-5 4$MC=3.87E-6 5
64ZNS G NC=1.546E-7 22
64ZN cG $E|g=991.6 {I1}, I|g=100 (2007Mi12)
64ZN cG $E|g=992.03, I|g=100,, I|g(absolute)=48.0 (1990SuZR)
64ZN cG $E|g=991.51 {I10}, I|g=100 (1975Ra28)
64ZN cG $E|g=991.0 {I5} in text, I|g=100, I|g(absolute)=48.6 (1967Ma04)
64ZN cG $E|g=992.2 {I5}, I|g=100 {I3} (1967Ko02)
64ZN L 1799.45 8 2+ 2.0 PS 2
64ZN G 807.93 10 30.0 11E2+M1 -3.9 7
64ZN2 G %IG=14.5 6
64ZNS G CC=0.000494 8$KC=0.000442 7$LC=4.46E-5 7$MC=6.38E-6 10
64ZNS G NC=2.54E-7 4
64ZN cG $E|g=808.0 {I1}, I|g=30.7 {I18} (2007Mi12)
64ZN cG $E|g=808.40, I|g=31.9, I|g(absolute)=15.3 (1990SuZR)
64ZN cG $E|g=807.85 {I10}, I|g=31.6 {I5} (1975Ra28)
64ZN cG $E|g=807.8 {I5}, I|g=27.8 {I4}, I|g(absolute)=13.5 {I2} (1967Ma04)
64ZN cG $E|g=809.4 {I4}, I|g=32 {I2} (1967Ko02)
64ZN G 1799.53 15 8.5 3 E2
64ZN2 G %IG=4.11 15
64ZNS G CC=0.000300 4$KC=7.59E-5 11$LC=7.53E-6 11$MC=1.080E-6 15
64ZNS G NC=4.37E-8 6$IPC=0.0002158 30
64ZN cG $E|g=1799.7 {I2}, I|g=9.11 {I64} (2007Mi12)
64ZN cG $E|g=1800.29, I|g=8.3, I|g(absolute)=4.0 (1990SuZR)
64ZN cG $E|g=1799.43 {I15}, I|g=8.3 {I3} (1975Ra28)
64ZN cG $E|g=1799.2 {I5}, I|g=8.6 {I8}, I|g(absolute)=4.2 {I4} (1967Ma04)
64ZN cG $E|g=1798 {I4}, I|g=12 {I3} (1967Ko02)
64ZN L 1910.28 8 0+ 0.95 NS 5
64ZN E 0.3 LT 0.003 LT 7.8 GT 0.3 LT ?
64ZNS E EAV=1945.59 73$CK=0.007872 9$CL=0.0008669 9$CM+=0.00015419
64ZN cE TI$-0.1 {I4} from transition intensity balance
64ZN G 110.7 1 0.59 19[E2] 0.447 6
64ZN2 G %IG=0.28 9
64ZNS G NC=0.0002072 30
64ZNS G KC=0.394 6$LC=0.0465 7$MC=0.00657 10
64ZN cG E,RI$from 2007Mi12. Other: E|g=110.9 from ce data (1985Pa07,1983Pa05).
64ZN2cG I|g=0.50 {I5} from I|g(111|g)/I|g(919|g)=0.027
64ZN3cG {I3} in (p,p'|g) data (1985Pa07,1983Pa05)
64ZN G 918.84 10 17.6 6 E2
64ZN2 G %IG=8.50 32
64ZNS G CC=0.000361 5$KC=0.000324 5$LC=3.25E-5 5$MC=4.66E-6 7
64ZNS G NC=1.859E-7 26
64ZN cG $E|g=918.9 {I1}, I|g=17.4 {I11} (2007Mi12)
64ZN cG $E|g=919.40, I|g=17.7, I|g(absolute)=8.6 (1990SuZR)
64ZN cG $E|g=918.78 {I10}, I|g=18.7 {I4} (1975Ra28)
64ZN cG $E|g=918.5 {I5}, I|g=16.7 {I4}, I|g(absolute)=8.1 {I2} (1967Ma04)
64ZN cG $E|g=919.1 {I4}, I|g=17 {I2} (1967Ko02)
64ZN G 1910 E0 S
64ZN cG E$from ce data in (p,p'|g) (1985Pa07,1983Pa05)
64ZN L 2609.48 9 0+ 0.20 PS 8
64ZN cL $An 809-keV transition from this level to the 1799-keV level was
64ZN2cL not observed in |g|g-coin data of 2007Mi12. An upper limit of 0.5%
64ZN3cL for the intensity from branching ratio I|g(809)/[I|g(809)+I|g(1618|g)],
64ZN4cL was given by the authors.
64ZN E 0.21 LT 0.0032 LT 7.6 GT 0.21 LT ?
64ZNS E EAV=1609.16 72$CK=0.013391 17$CL=0.0014754 1$CM+=0.0002624 4
64ZN cE TI$0.07 {I14} from transition intensity balance
64ZN G 1617.77 23 3.74 19E2
64ZN2 G %IG=1.81 10
64ZNS G CC=0.0002385 33$KC=9.32E-5 13$LC=9.27E-6 13$MC=1.328E-6 19
64ZNS G NC=5.37E-8 8$IPC=0.0001347 19
64ZN cG $E|g=1618.0 {I2}, I|g=3.72 {I25} (2007Mi12)
64ZN cG $E|g=1618.47, I|g=3.75, I|g(absolute)=1.8 (1990SuZR)
64ZN cG $E|g=1617.54 {I20}, I|g=3.81 {I19} (1975Ra28)
64ZN cG $E|g=1617.2 {I8}, I|g=3.7 {I10}, I|g(absolute)=1.8 {I5} (1967Ma04)
64ZN G 2609 E0 S
64ZN cG E$from pair conversion data in (p,p'|g) (1985Pa07,1983Pa05)
64ZN L 3186.77 8 1+ 0.042 PS 10
64ZN E 29.8 7 0.781 19 5.11 1 30.6 7
64ZNS E EAV=1333.93 72$CK=0.02260 4$CL=0.002491 4$CM+=0.0004432 7
64ZN G 577.3 1 0.21 4 [M1]
64ZN2 G %IG=0.101 19
64ZNS G CC=0.000803 11$KC=0.000720 10$LC=7.23E-5 10$MC=1.037E-5 15
64ZNS G NC=4.18E-7 6
64ZN cG E,RI$|g from 2007Mi12 only
64ZN G 1276.38 10 13.1 3 (M1)
64ZN2 G %IG=6.33 17
64ZNS G CC=0.0001708 24$KC=0.0001382 19$LC=1.373E-5 19$MC=1.969E-6 28
64ZNS G NC=7.99E-8 11$IPC=1.682E-5 24
64ZN cG $E|g=1276.4 {I1}, I|g=13.5 {I10} (2007Mi12)
64ZN cG $E|g=1276.94, I|g=13.3, I|g(absolute)=6.4 (1990SuZR)
64ZN cG $E|g=1276.37 {I10}, I|g=12.9 {I3} (1975Ra28)
64ZN cG $E|g=1276.4 {I5}, I|g=13.0 {I6}, I|g(absolute)=6.3 {I3} (1967Ma04)
64ZN cG $E|g=1276.6 {I20}, I|g=13 {I3} (1967Ko02)
64ZN G 1387.34 10 27.5 7 [M1+E2]
64ZN2 G %IG=13.3 4
64ZNS G CC=0.000180 12$KC=0.000122 5$LC=1.22E-5 5$MC=1.75E-6 7
64ZNS G NC=7.06E-8 28$IPC=4.4E-5 6
64ZN cG $E|g=1387.4 {I1}, I|g=26.5 {I23} (2007Mi12)
64ZN cG $E|g=1387.83, I|g=26.7, I|g(absolute)=12.8 (1990SuZR)
64ZN cG $E|g=1387.27 {I10}, I|g=27.3 {I7} (1975Ra28)
64ZN cG $E|g=1386.8 {I5}, I|g=28.8 {I8}, I|g(absolute)=14.0 {I4} (1967Ma04)
64ZN cG $E|g=1387.8 {I14}, I|g=30 {I3} (1967Ko02)
64ZN G 2195.22 10 22.1 5 [M1+E2]
64ZN2 G %IG=10.68 29
64ZNS G CC=0.000433 33$KC=5.18E-5 11$LC=5.13E-6 11$MC=7.35E-7 16
64ZNS G NC=2.99E-8 6$IPC=0.000375 32
64ZN cG $E|g=2195.1 {I2}, I|g=21.9 {I21} (2007Mi12)
64ZN cG $E|g=2195.85, I|g=20.2, I|g(absolute)=9.7 (1990SuZR)
64ZN cG $E|g=2195.25 {I10}, I|g=21.4 {I5} (1975Ra28)
64ZN cG $E|g=2195.0 {I7}, I|g=23.0 {I10}, I|g(absolute)=11.2 {I5} (1967Ma04)
64ZN cG $E|g=2195.6 {I9}, I|g=26 {I4} (1967Ko02)
64ZN G 3186.8 2 0.41 8 [M1]
64ZN2 G %IG=0.20 4
64ZNS G CC=0.000796 11$KC=2.74E-5 4$LC=2.70E-6 4$MC=3.87E-7 5
64ZNS G NC=1.576E-8 22$IPC=0.000766 11
64ZN cG $E|g=3186.8{I2}, I|g=0.47 {I8} (2007Mi12)
64ZN cG $E|g=3188.9, I|g=0.27, I|g(absolute)=0.13 (1990SuZR)
64ZN cG $E|g=3187 {I2}, I|g=0.35 {I10} (1975Ra28)
64ZN cG $E|g=3189 {I2}, I|g|<0.9 (1967Ko02)
64ZN L 3261.93 11 1 0.4 PS +7-2
64ZN E 2.33 13 0.066 4 6.17 3 2.40 13
64ZNS E EAV=1298.30 72$CK=0.02437 4$CL=0.002687 5$CM+=0.0004780 8
64ZN G 1352 2 0.3 LT [D] ?
64ZN2 G %IG LT 0.145
64ZN cG $E|g=1352 {I2}, I|g<0.3 from |g|g-coin (1975Ra28)
64ZN G 1461.3 1 0.21 LT ?
64ZN2 G %IG LT 0.10
64ZNF G FL=1799.45
64ZN cG RI$from |g|g-coin data in 2007Mi12
64ZN cG $This |g fits poorly in the decay scheme, E|g not used in the
64ZN2cG least-squares fitting procedure. Level-energy difference=1462.5.
64ZN3cG In 1975Ra28 and 1990SuZR, it is possible that contribution from
64ZN4cG background line near this energy from {+40}K decay is not fully
64ZN5cG subtracted
64ZN cG $E|g=1461.3 {I1}, I|g<0.21 (2007Mi12)
64ZN cG $E|g=1461.56, I|g=0.81, I|g(absolute)=0.39 (1990SuZR)
64ZN cG $E|g=1462 {I2}, I|g=0.70 {I10} (1975Ra28)
64ZN G 2270.38 10 4.67 24
64ZN2 G %IG=2.26 12
64ZN cG $E|g=2270.2 {I2}, I|g=4.87 {I54} (2007Mi12)
64ZN cG $E|g=2271.08, I|g=4.58, I|g(absolute)=2.2 (1990SuZR)
64ZN cG $E|g=2270.42 {I10}, I|g=4.84 {I24} (1975Ra28)
64ZN cG $E|g=2270.4 {I9}, I|g=4.3 {I6}, I|g(absolute)=2.1 {I3} (1967Ma04)
64ZN cG $E|g=2272 {I2}, I|g=4 {I2} (1967Ko02)
64ZN G 3261.7 2 0.29 2 [D]
64ZN2 G %IG=0.140 10
64ZN cG $E|g=3261.7 {I2}, I|g=0.31 {I2} (2007Mi12)
64ZN cG $E|g=3262.97, I|g=0.31, I|g(absolute)=0.15 (1990SuZR)
64ZN cG $E|g=3261 {I2}, I|g=0.27 {I8} (1975Ra28)
64ZN cG $E|g=3264, I|g|<1 (1967Ko02)
64ZN L 3321.8 12 (1) ?
64ZN E 0.23 5 0.0070 15 7.1 1 0.24 5 ?
64ZNS E EAV=1269.96 91$CK=0.02591 6$CL=0.002857 6$CM+=0.0005083 1
64ZN G 1411.3 15 0.31 9
64ZN2 G %IG=0.15 4
64ZN cG $E|g=1411, I|g=0.10, I|g(absolute)=0.05 (1990SuZR)
64ZN cG $E|g=1411.3 {I15}, I|g=0.31 {I9} (1975Ra28)
64ZN G 3322 2 0.18 5
64ZN2 G %IG=0.087 24
64ZN cG $E|g=3324.68, I|g=0.33, I|g(absolute)=0.15 (1990SuZR)
64ZN cG $E|g=3322 {I2}, I|g=0.18 {I5} (1975Ra28)
64ZN L 3366.00 8 1+ 0.023 PS 8
64ZN E 28.2 7 0.892 23 5.01 1 29.1 7 C
64ZNS E EAV=1249.06 71$CK=0.02714 5$CL=0.002992 5$CM+=0.0005323 9
64ZN cE IB$75% (1960Ja07) for a |b{++} group at 2790 {I80} (most likely a
64ZN2cE composite of |b{++} groups to the 3187+3262+3366 levels)
64ZN cE $(|b{++})(3366|g+3425|g)(circ pol): asymmetry parameter
64ZN2cE =-1.00 {I5} (1967Ma04), -0.94 {I14} (1966De10) agrees with
64ZNxcE 0(|b{++})1(|g)0 sequence
64ZN G 756.58 10 2.86 15 [M1]
64ZN2 G %IG=1.38 8
64ZNS G CC=0.000446 6$KC=0.000400 6$LC=4.00E-5 6$MC=5.74E-6 8
64ZNS G NC=2.319E-7 32
64ZN cG $E|g=756.6 {I1}, I|g=2.77 {I19} (2007Mi12)
64ZN cG $E|g=757.07, I|g=2.92, I|g(absolute)=1.4 (1990SuZR)
64ZN cG $E|g=756.52 {I20}, I|g=2.90 {I15} (1975Ra28)
64ZN cG $E|g=756.7 {I7}, I|g=2.9 {I2}, I|g(absolute)=1.4 {I1} (1967Ma04)
64ZN G 1455.84 12 4.44 22 [M1]
64ZN2 G %IG=2.14 11
64ZNS G CC=0.0001737 24$KC=0.0001074 15$LC=1.066E-5 15$MC=1.528E-6 21
64ZNS G NC=6.20E-8 9$IPC=5.41E-5 8
64ZN cG $E|g=1455.9 {I1}, I|g=4.5 {I3} (2007Mi12)
64ZN cG $E|g=1454.95, I|g=4.38, I|g(absolute)=2.1 (1990SuZR)
64ZN cG $E|g=1455.59 {I20}, I|g=4.33 {I22} (1975Ra28)
64ZN cG $E|g=1455.2 {I7}, I|g=4.5 {I4}, I|g(absolute)=2.2 {I2} (1967Ma04)
64ZN G 1566.59 20 5.02 29 [M1+E2]
64ZN2 G %IG=2.42 14
64ZNS G CC=0.000208 16$KC=9.64E-5 32$LC=9.58E-6 33$MC=1.37E-6 5
64ZNS G NC=5.56E-8 17$IPC=0.000100 12
64ZN cG $E|g=1566.7 {I2}, I|g=4.65 {I36} (2007Mi12)
64ZN cG $E|g=1567.19, I|g=4.38, I|g(absolute)=2.21 (1990SuZR)
64ZN cG $E|g=1566.47 {I20}, I|g=4.82 {I23} (1975Ra28)
64ZN cG $E|g=1566.5 {I6}, I|g=5.6 {I6}, I|g(absolute)=2.7 {I3} (1967Ma04)
64ZN cG $E|g=1568 {I2}, I|g=11 {I4} (1967Ko02)
64ZN G 2374.30 10 16.1 4 [M1+E2]
64ZN2 G %IG=7.78 23
64ZNS G CC=0.00051 4$KC=4.52E-5 9$LC=4.47E-6 9$MC=6.41E-7 14
64ZNS G NC=2.61E-8 5$IPC=0.00046 4
64ZN cG $E|g=2374.2 {I2}, I|g=16.2 {I14} (2007Mi12)
64ZN cG $E|g=2375.27, I|g=15.8, I|g(absolute)=7.6 (1990SuZR)
64ZN cG $E|g=2374.32 {I10}, I|g=16.2 {I4} (1975Ra28)
64ZN cG $E|g=2374.8 {I7}, I|g=15.8 {I10}, I|g(absolute)=7.7 {I5} (1967Ma04)
64ZN cG $E|g=2374.7 {I14}, I|g=14 {I3} (1967Ko02)
64ZN G 3365.76 16 31.9 10 [M1]
64ZN2 G %IG=15.4 4
64ZNS G CC=0.000864 12$KC=2.508E-5 35$LC=2.475E-6 35$MC=3.55E-7 5
64ZNS G NC=1.445E-8 20$IPC=0.000836 12
64ZN cG E$weighted average of values from 2007Mi12, 1975Ra28 and 1967Ma04
64ZN cG $E|g=3365.3 {I2}, I|g=31.5 {I34} (2007Mi12)
64ZN cG $E|g=3367.52, I|g=32.3, I|g(absolute)=15.5 (1990SuZR)
64ZN cG $E|g=3365.87 {I10}, I|g=30.4 {I12} (1975Ra28)
64ZN cG $E|g=3365.8 {I9}, I|g=33.7 {I10}, I|g(absolute)=16.4 {I5} (1967Ma04)
64ZN cG $E|g=3366.9 {I16}, I|g=36 {I4} (1967Ko02)
64ZN L 3425.14 10 1+ 0.031 PS 7
64ZN E 6.6 3 0.22 1 5.60 2 6.8 3
64ZNS E EAV=1221.13 71$CK=0.02890 5$CL=0.003186 6$CM+=0.0005668 1
64ZN G 1514.7 2 0.47 8 [M1]
64ZN2 G %IG=0.23 4
64ZNS G CC=0.0001822 26$KC=9.97E-5 14$LC=9.89E-6 14$MC=1.418E-6 20
64ZNS G NC=5.76E-8 8$IPC=7.12E-5 10
64ZN cG $E|g=1514.7 {I2}, I|g=0.51 {I8} (2007Mi12)
64ZN cG $E|g=1515.2 {I10}, I|g=0.42 {I8} (1975Ra28)
64ZN G 1625.87 20 2.46 17[M1+E2]
64ZN2 G %IG=1.19 8
64ZNS G CC=0.000224 18$KC=8.98E-5 28$LC=8.92E-6 29$MC=1.28E-6 4
64ZNS G NC=5.18E-8 15$IPC=0.000123 15
64ZN cG RI$weighted average of values from 2007Mi12, 1975Ra28 and 1967Ma04
64ZN cG $E|g=1626.0 {I2}, I|g=2.49 {I17} (2007Mi12)
64ZN cG $E|g=1626.49, I|g=2.29, I|g(absolute)=1.1 (1990SuZR)
64ZN cG $E|g=1625.74 {I20}, I|g=2.42 {I17} (1975Ra28)
64ZN cG $E|g=1626.2 {I12}, I|g=2.7 {I6}, I|g(absolute)=1.3 {I3} (1967Ma04)
64ZN G 2433.6 2 1.31 12[M1+E2]
64ZN2 G %IG=0.63 6
64ZNS G CC=0.00053 4$KC=4.33E-5 9$LC=4.29E-6 9$MC=6.14E-7 13
64ZNS G NC=2.50E-8 5$IPC=0.00048 4
64ZN cG RI$weighted average of values from 2007Mi12, 1975Ra28 and 1967Ma04
64ZN cG $E|g=2433.6 {I2}, I|g=1.26 {I12} (2007Mi12)
64ZN cG $E|g=2434.4, I|g=1.29, I|g(absolute)=0.62 (1990SuZR)
64ZN cG $E|g=2433.7 {I3}, I|g=1.36 {I13} (1975Ra28)
64ZN cG $E|g=2433.5 {I15}, I|g=1.2 {I4}, I|g(absolute)=0.6 {I2} (1967Ma04)
64ZN G 3424.97 15 9.9 5 [M1]
64ZN2 G %IG=4.78 24
64ZNS G CC=0.000886 12$KC=2.440E-5 34$LC=2.408E-6 34$MC=3.45E-7 5
64ZNS G NC=1.406E-8 20$IPC=0.000859 12
64ZN cG $E|g=3424.8 {I2}, I|g=10.1 {I10} (2007Mi12)
64ZN cG $E|g=3426.55, I|g=10.0, I|g(absolute)=4.8 (1990SuZR)
64ZN cG $E|g=3425.06 {I15}, I|g=9.4 {I5} (1975Ra28)
64ZN cG $E|g=3424.8 {I9}, I|g=10.1 {I8}, I|g(absolute)=4.9 {I4} (1967Ma04)
64ZN cG $E|g=3426.2 {I18}, I|g=10 {I1} (1967Ko02)
64ZN L 3795.00 11 1+
64ZN E 3.83 16 0.201 9 5.56 2 4.03 17
64ZNS E EAV=1047.34 71$CK=0.04419 9$CL=0.004875 9$CM+=0.0008673 1
64ZN G 1185.4 1 0.17 9 [M1]
64ZN2 G %IG=0.08 4
64ZNS G CC=0.0001827 26$KC=0.0001596 22$LC=1.588E-5 22$MC=2.277E-6 32
64ZNS G NC=9.23E-8 13$IPC=4.81E-6 7
64ZN cG $E|g=1185.4 {I1}, I|g<0.16 (2007Mi12)
64ZN cG $E|g=1186, I|g=0.23, I|g(absolute)=0.11 (1990SuZR)
64ZN cG $E|g=1186.0 {I10}, I|g=0.26 {I6} (1975Ra28)
64ZN G 1995.9 2 3.84 22[M1+E2]
64ZN2 G %IG=1.85 11
64ZNS G CC=0.000351 28$KC=6.14E-5 14$LC=6.08E-6 15$MC=8.72E-7 21
64ZNS G NC=3.54E-8 8$IPC=0.000283 27
64ZN cG $E|g=1996.0 {I2}, I|g=3.93 {I34} (2007Mi12)
64ZN cG $E|g=1996.41, I|g=3.54, I|g(absolute)=1.7 (1990SuZR)
64ZN cG $E|g=1995.8 {I3}, I|g=3.69 {I22} (1975Ra28)
64ZN cG $E|g=1996.1 {I10}, I|g=3.9 {I6}, I|g(absolute)=1.9 {I3} (1967Ma04)
64ZN cG $E|g=1995.0 {I5}, I|g=12 {I4} (1967Ko02)
64ZN G 2803.3 3 1.50 14[M1+E2]
64ZN2 G %IG=0.72 7
64ZNS G CC=0.00069 4$KC=3.42E-5 7$LC=3.38E-6 7$MC=4.84E-7 10
64ZNS G NC=1.97E-8 4$IPC=0.00065 4
64ZN cG RI$unweighted average of values from 2007Mi12 and 1975Ra28
64ZN cG $E|g=2803.1 {I2}, I|g=1.51 {I19} (2007Mi12)
64ZN cG $E|g=2804.23, I|g=1.54, I|g(absolute)=0.74 (1990SuZR)
64ZN cG $E|g=2803.7 {I3}, I|g=1.49 {I14} (1975Ra28)
64ZN cG $E|g=2803.9 {I10}, I|g=2.5 {I6}, I|g(absolute)=1.2 {I3} (1967Ma04)
64ZN cG $E|g=2806 {I2}, I|g=1.5 {I9} (1967Ko02)
64ZN G 3795.1 3 2.83 17[M1] 1.02E-3 1
64ZN2 G %IG=1.37 8
64ZNS G KC=2.080E-5 29$LC=2.052E-6 29$MC=2.94E-7 4
64ZNS G NC=1.198E-8 17$IPC=0.000995 14
64ZN cG RI$from 1975Ra28
64ZN cG $E|g=3797.23, I|g=2.92, I|g(absolute)=1.4 (1990SuZR)
64ZN cG $E|g=3795.1 {I3}, I|g=2.83 {I17} (1975Ra28)
64ZN cG $E|g=3794.5 {I10}, I|g=2.1 {I4}, I|g(absolute)=1.0 {I2} (1967Ma04)
64ZN cG $E|g=3795 {I2}, I|g=1.4 {I4} (1967Ko02)
64ZN L 4454.70 16 1+ 3.2 FS 6
64ZN E 1.16 7 0.168 10 5.44 3 1.33 8
64ZNS E EAV=742.10 69$CK=0.1119 3$CL=0.01236 3$CM+=0.002199 6
64ZN G 2544.4 2 0.35 6 [M1]
64ZN2 G %IG=0.169 29
64ZNS G CC=0.000541 8$KC=3.96E-5 6$LC=3.91E-6 5$MC=5.61E-7 8
64ZNS G NC=2.282E-8 32$IPC=0.000497 7
64ZN cG $E|g=2544.4 {I2}, I|g=0.30 {I6} (2007Mi12)
64ZN cG $E|g=2545.02, I|g=0.44, I|g(absolute)=0.21 (1990SuZR)
64ZN cG $E|g=2544.2 {I10}, I|g=0.40 {I8} (1975Ra28)
64ZN cG $E|g=2550 {I2}, I|g=2 {I2} (1967Ko02)
64ZN G 2655.2 2 0.58 10[M1+E2]
64ZN2 G %IG=0.28 5
64ZNS G CC=0.00063 4$KC=3.74E-5 8$LC=3.70E-6 8$MC=5.30E-7 11
64ZNS G NC=2.15E-8 4$IPC=0.00059 4
64ZN cG $E|g=2655.2 {I2}, I|g=0.51 {I7} (2007Mi12)
64ZN cG $E|g=2655.96, I|g=0.71, I|g(absolute)=0.34 (1990SuZR)
64ZN cG $E|g=2654.4 {I10}, I|g=0.65 {I10} (1975Ra28)
64ZN cG $E|g=2654, I|g<0.6, I|g(absolute)<0.3 (1967Ma04)
64ZN G 3462.4 10 0.10 2 [M1+E2]
64ZN2 G %IG=0.048 10
64ZNS G CC=0.00095 5$KC=2.43E-5 5$LC=2.40E-6 5$MC=3.44E-7 7
64ZNS G NC=1.401E-8 27$IPC=0.00092 5
64ZN cG $E|g=3462.4 {I10}, I|g=0.10 {I2} (1975Ra28)
64ZN cG $E|g=3465, I|g|<2 (1967Ko02)
64ZN G 4454.3 10 1.72 10[M1] 1.24E-3 2
64ZN2 G %IG=0.83 5
64ZNS G KC=1.633E-5 23$LC=1.610E-6 23$MC=2.307E-7 32
64ZNS G NC=9.40E-9 13$IPC=0.001217 17
64ZN cG RI$from 1975Ra28
64ZN cG $E|g=4455.88, I|g=2.02 (1990SuZR), I|g(absolute)=0.97
64ZN cG $E|g=4454.3 {I10}, I|g=1.72 {I10} (1975Ra28)
64ZN cG $E|g=4453.5 {I12}, I|g=1.0 {I2}, I|g(absolute)=0.5 {I1} (1967Ma04)
64ZN cG $E|g=4456.8 {I16}, I|g=2.1 {I5} (1967Ko02)
64ZN L 4608.8 2 (1)
64ZN E 0.12 2 0.023 3 6.26 7 0.14 2
64ZNS E EAV=671.93 69$CK=0.1445 4$CL=0.01596 5$CM+=0.002841 8
64ZN G 3617.1 2 0.22 4
64ZN2 G %IG=0.106 19
64ZN cG $E|g=3617.1 {I2}, I|g=0.21 {I4} (2007Mi12)
64ZN cG $E|g=3616.5 {I10}, I|g=0.24 {I8} (1975Ra28)
64ZN G 4609 2 0.07 AP
64ZN2 G %IG AP 0.034
64ZN cG E,RI$from 1975Ra28
64ZN cG $E|g=4610.60, I|g=0.13, I|g(absolute)=0.06 (1990SuZR)
64ZN cG $E|g=4609 {I2}, I|g|?0.07 (1975Ra28)
64ZN L 4713.1 2 (1)
64ZN E 0.15 3 0.037 8 6.0 1 0.19 4
64ZNS E EAV=624.73 69$CK=0.1732 5$CL=0.01915 6$CM+=0.003407 10
64ZN G 2103.6 2 0.35 8
64ZN2 G %IG=0.17 4
64ZN cG $E|g=2103.6 {I2}, I|g=0.35 {I9} (2007Mi12)
64ZN cG $E|g=2103.1, I|g=0.40, I|g(absolute)=0.19 (1990SuZR)
64ZN cG $E|g=2103 {I2}, I|g=0.35 {I8} (1975Ra28)
64ZN G 2913 2 0.02 ?
64ZN2 G %IG=0.010
64ZN cG E$from 1975Ra28
64ZN cG RI$from 1990SuZR. Other: <0.4 (1975Ra28)
64ZN cG $E|g=2915.21, I|g=0.02, I|g(absolute)=0.01 (1990SuZR)
64ZN cG $E|g=2913 {I2}, I|g<0.4 (1975Ra28)
64ZN cG $E|g=2910, I|g=0.4 (1967Ma04)
64ZN G 4712 2 0.04 AP
64ZN2 G %IG AP 0.019
64ZN cG $E|g=4712 {I2}, I|g|?0.04 (1975Ra28)