62ZN 62GA EC DECAY (116.123 MS) 2020MA59,2008FI07,2008BE2125NDS 202507
62ZN H TYP=FUL$AUT=Balraj Singh, Huang Xiaolong, and Wang Xianghan$
62ZN2 H CIT=NDS 204, 1 (2025)$CUT=30-Jun-2023$
62ZN c 2020Ma59: {+62}Ga produced in the ZrC(p,X),E(p)=479 MeV at the ISAC
62ZN2c facility at TRIUMF. Detected |b{++} particles
62ZN3c with SCEPTAR array of 20 plastic scintillators. Measured E|g, I|g,
62ZN4c |b|g-, |g|g- and |b|g|g-coin, |g|g(|q) using GRIFFIN array of 16 HPGe
62ZN5c clover detectors, each Compton-suppressed by 20-element BGO detectors,
62ZN6c and SCEPTAR array of plastic scintillators for |b particles. Deduced
62ZN7c precise |b{++}+|e branch to the g.s. of {+62}Zn. Deduced
62ZN8c isospin-symmetry breaking in superallowed Fermi |b decay from
62ZN9c 0+ to 0+ state. Deduced isospin-mixing correction |d{-C1}=0.110% {I9}
62ZN2c in {+62}Ga superallowed decay to the excited 0+ states in {+62}Zn, as
62ZN3c compared to evaluated |d{-C1}=0.275% {I55} in 2015Ha07
62ZN c 2008Fi07: {+62}Ga produced in the Zr(p,X) reaction using 500 MeV
62ZN2c protons produced at the ISAC facility at TRIUMF. Detected |b{++}
62ZN3c particles with SCEPTAR array of 20 plastic scintillators. Measured E|g,
62ZN4c I|g, |g|g, |b|g coin using 8|p array of 20 HPGe detectors with
62ZN5c Compton-suppression and SCEPTAR array of plastic scintillators for |b
62ZN6c particles. Deduced precise and accurate |b{++}+|e branch to
62ZN7c g.s. of {+62}Zn and associated log {Ift} value relevant to
62ZN8c superallowed |b decay from 0+ to 0+ state and breaking of isospin
62ZN9c symmetry.
62ZN c 2008Be21, 2005Ca06: {+62}Ga was produced in bombardment of {+64}Zn
62ZN2c target by 48 MeV protons at IGISOL facility in Jyvaskyla. Fusion
62ZN3c evaporation residues were thermalized in helium gas and singly-charged
62ZN4c ions were mass analyzed. JYFLTRAP facility was used to separate {+62}Ga
62ZN5c from other isobaric activities. Penning-trap separated {+62}Ga was
62ZN6c used for measurement of E|g and I|g. Different measurement cycles were
62ZN7c used on the mass-separated source in another setup. Detection
62ZN8c system consisted of three HPGe clover detectors (for |g rays), and 4|p
62ZN9c cylindrical plastic scintillators for |b particles. Measured E|g, I|g,
62ZNAc |g|g and |b|g coin. Half-life measurement in 2005Ca06
62ZN c 2008Gr03: E=500 MeV protons produced at TRIUMF cyclotron. {+62}Ga beam
62ZN2c produced using TRILIS. Measured |b particles using 4|p gas counter
62ZN3c and 20 plastic scintillators. Detected |g rays with 8|p |g-ray
62ZN4c spectrometer. Measured precise half-life of {+62}Ga decay
62ZN c 2006Hy02 (also 2005Hy04): {+62}Ga was produced in spallation reaction
62ZN2c by 500 MeV protons on a ZrC target. Mass-separated 30-keV {+62}Ga beam
62ZN3c was obtained using a laser ion source at TRIUMF-ISAC facility and
62ZN4c implanted in a Mylar tape for |g and |b counting.
62ZN5c Measured E|g, I|g, |g|g, |b, |b|g coin using 8|p array
62ZN6c of 20 Compton-suppressed HPGe detectors for |g rays and an array of 20
62ZN7c plastic scintillators for |b rays. Half-life measurement is reported
62ZN8c by 2005Hy04. Same group as 2008Fi07 and 2008Gr03
62ZN c 2004Bl03: {+62}Ga from {+28}Si({+40}Ca,np|a) at GSI; measured
62ZN2c half-life, |b|g coin
62ZN c 2003Hy02: {+62}Ga from {+1}H({+64}Zn,3n) at 42 MeV/nucleon; measured
62ZN2c E|g, I|g, half-life, branching ratios at the Texas A&M University K500
62ZN3c Superconducting Cyclotron.
62ZN c 2002Lo13 (also 2002Bl17): {+62}Ga from fragmentation of {+78}Kr beam,
62ZN2c GANIL facility, measured half-life
62ZN c 1993Wi18, 1993Wi03: {+58}Ni({+84}Kr,X) E=75 MeV/nucleon. Measured
62ZNxc half-life using A1200 radioactive-beam facility at the NSCL-MSU.
62ZN c 1979Da04: from {+58}Ni({+6}Li,2n), E=25 MeV, |DE-E telescopes (plastic
62ZN2c or semiconductors), T{-1/2}, Q(|e) at Argonne FN tandem accelerator.
62ZN c 1978Al23: from {+58}Ni({+6}Li,2n), E=25 MeV, plastic scintillator,
62ZNxc half-life at Brookhaven National Laboratory.
62ZN c 1978Ch11 (also 1973ChYF): from {+64}Zn(p,3n), E=44 MeV, plastic
62ZN2c scintillator, Ge(Li), half-life, Q(|b{++}) at the synchrocyclotron of
62ZN3c the Institute for Nuclear Study, University of Tokyo.
62ZN c 1976BaXP: from Zn(p,3n), E=44 MeV, half-life at McGill University
62ZN2c cyclotron facility
62ZN c 1976JaZP: from {+46}Ti({+19}F,3n) and {+50}Cr({+16}O,p3n), plastic
62ZN2c scintillator, half-life at Chalk-River tandem accelerator.
62ZN c 1973ChYF: from {+64}Zn(p,3n), E=32-52 MeV, plastic scintillator, Ge(Li)
62ZN2c at the synchrocyclotron of the Institute for Nuclear Study, University
62ZN3c of Tokyo.
62ZN c 2008Fi07, 2008Gr03, 2006Hy02 (also 2005Hy04) are from the same group
62ZN c 2008Be21, 2005Ca06, 2004Bl03, 2002Lo13 (also 2002Bl17) share some of
62ZN2c the same authors, but some of the studies are at different facilities
62ZN c Review of superallowed (0+ to 0+) |b decays: 2010To12, 2009Er02,
62ZN2c 2009Ha12, 2008To03, 2005Ha27, 2002Ha27; also 2006Ha12, 2005Ha15,
62ZN3c 2005Ha65 conference papers.
62ZN d Theory: 2011Sa08 (log |{Ift} values)
62ZN d 2008FiZX superseded by 2008Fi07
62ZN d 2008GrZO superseded by 2008Gr03
62ZN d 2006HyZZ superseded by 2006Hy02
62ZN d 2000DoZX, 2000DoZZ, 2001DoZZ, 2003BlZZ, 2004CaZX superseded by
62ZN2d 2004Bl03 and 2005Ca06
62ZN c References and notes on half-life measurement of {+62}Ga decay:
62ZN c 2008Gr03: {+62}Ga beam from TRIUMF ISAC using resonant ionization
62ZN2c laser ion source and mass separation, positron detection using 4|p
62ZN3c continuous flow gas proportional counter. Yields and activities
62ZN4c of {+62}Cu, {+62m}Co, {+62g}Co, {+62}Mn and {+62}Fe contaminants were
62ZN5c estimated from |b|g coin. data. Systematic and statistical
62ZN6c uncertainties described in detail.
62ZN c 2005Ca06: {+62}Ga beam from IGISOL at Jyvaskyla. Positron detection
62ZN2c using 4|p cylindrical plastic scintillator. Presence of {+62}Cu
62ZN3c activity was considered as a constant background. Systematic and
62ZN4c statistical uncertainties described in detail.
62ZN c 2004Bl03: {+62}Ga beam from {+28}Si({+40}Ca,|apn) at 4.84 MeV/nucleon
62ZN2c at GSI facility. Mass-analyzed beam and positron detection using 4|p
62ZN3c gas detector and |g by HPGe detector. {+62}Cu and {+62}Zn impurities
62ZN4c were taken into account. Systematic and statistical uncertainties
62ZN5c described in detail.
62ZN c 2003Hy02: {+62}Ga beam from {+1}H({+64}Zn,3n) at 42 MeV/nucleon
62ZN2c at Texas A&M facility. Mass-analyzed beam was 80-94% pure {+62}Ga.
62ZN3c Positron detection using 4|p gas proportional chamber. {+58}Cu and
62ZN4c {+54}Co impurities quantified. The |g spectrum was measured
62ZN5c by HPGe detector. Maximum likelihood method. Uncertainty analysis not
62ZN6c discussed fully.
62ZN c 2002Lo13 (also 2002Bl17): {+62}Ga from fragmentation of {+78}Kr beam,
62ZN2c GANIL facility, decay curve of |b{++} particles correlated with
62ZN3c implants shown; no discussion of uncertainties
62ZN c Total decay energy of 9181.2 keV {I7} deduced (by RADLIST code) from
62ZN2c proposed decay scheme is in agreement with the expected value of
62ZN3c 9181.1 keV {I4}, indicating that decay scheme is complete
62ZN cE TI$From |g+ce intensity balance at each level.
62ZN cG E$From 2020Ma59.
62ZN cG RI$From 2020Ma59. Intensities are per 100 decays of {+62}Ga. Note that
62ZN2cG 2020Ma59 listed intensities per 10{+6} decays of {+62}Ga.
62ZN cG E(x)$According to caption for level-scheme Fig. 6 in 2020Ma59, |g rays
62ZN2cG with intensities consistent with zero within 1.5|s are shown
62ZN3cG as tentative
62ZN cG M$From the Adopted Levels, Gammas dataset.
62ZN cL E$From least-squares fit to E|g data, with the
62ZN2cL inclusion of tentatively placed transitions. Normalized |h{+2}=2.4
62ZN3cL is somewhat larger than critical |h{+2} of 1.6, as the 3425.3|g from
62ZN4cL 3424.1 level is poorly fitted. Values in Table I of 2020Ma59 are
62ZN5cL listed under comments, when different.
62ZN cL J$From the Adopted Levels. Assignments given by 2020Ma59, based on
62ZN2cL previous assignment and from their |g|g(|q) data are listed in
62ZN3cL comments, if different from those in the Adopted Levels. Other
62ZN4cL exceptions are noted.
62ZN cL T$from the Adopted Levels
62ZN cL E(A),J(A)$From (p,t) study by 2013Le25. This level is not included
62ZN2cL in the Adopted Levels, as there is no direct evidence of its population
62ZN3cL in {+62}Ga |e decay from |g-ray observation
62GA P 0.0 0+ 116.123 MS25 9181.1 4
62GA cP T$From {+62}Ga Adopted Levels. 2020Ma59 take value of 116.121 ms {I21}
62GA2cP from 2008Gr03, where weighted average of their measurement and several
62GA3cP previous values was taken, and which was also adopted in the 2012
62GA4cP ENSDF evaluation. The revised value here includes newer measurement
62GA5cP by 2013Da16.
62GA cP QP$From 2021Wa16. 2020Ma59 quote 9181.4 {I1} from mass
62GA2cP measurement by 2006Er03
62ZN N 1.0 1.0 1.0
62ZN cN NR$Absolute |g-ray intensities are measured by 2020Ma59
62ZN PN 4
62ZN L 0.0 0+ 9.197 H 20
62ZN E 99.7200 21 0.1377 21 3.4983014 99.8577 29
62ZN2 E TI=99.8577 +23-29
62ZNS E EAV=3838.23 20$CK=0.001220 34$CL=1.357E-4 38$CM+=2.42E-5 6
62ZN cE TI$99.8577 {I+23-29} (2020Ma59), obtained by subtracting the sum of
62ZN2cE the observed g.s. feeding |g-ray intensity and the unobserved |g-ray
62ZN3cE feeding to g.s. from 100. Others: 99.858 {I8} (2008Fi07, from
62ZN4cE 100-|b feeding to excited states deduced from measured values and
62ZN5cE missing intensity estimated from shell model calculations);
62ZN6cE 99.893 {I24} (2008Be21, from measured I|g(to g.s.)=0.086 {I9}, and
62ZN7cE theoretically predicted unobserved I|g(to g.s.)=0.025 {I7} from higher
62ZN8cE 1+,0+ states); 99.861 {I11} (2006Hy02, previous value from
62ZN9cE the same group as 2008Fi07), 99.8 {I1} (2005Ca06), 99.85 {I+5-15}
62ZNAcE (2003Hy02), 99.88 {I3} (2002Bl17); 99.862 {I11} (2020Ha30 evaluation).
62ZNBcE Superallowed 0+ to 0+ |b transition. Using the averaged half-life,
62ZNCcE 2008Fi07 deduced {Ift}=3074.3 {I11} or log| {Ift}=3.4877 {I2}.
62ZNDcE 2020Ha30 evaluation gives T{-1/2}=116.121 ms {I40}, and
62ZNEcE {Ift}=3074.1 {I15} or log| {Ift}=3.4877 {I2}
62ZN cE E$9171 {I26} (1979Da04, from measured |b{++} endpoint)
62ZN L 953.84 6 2+ 2.93 PS 21
62ZN E 0.0018 LT 7.3E-6 LT 10.1 GT 0.0018 LT ?
62ZNS E EAV=3363.10 19$CK=0.00359 10$CL=4.00E-4 11$CM+=7.14E-5 19
62ZN G 953.7 1 0.0839 14 E2
62ZN cG $Other E|g=953.9 {I2} (2008Fi07), 953.7 {I2} (2006Hy02)
62ZN cG RI$others: 0.0850 {I19} (2008Fi07), 0.086 {I9} (2008Be21), 0.0809 {I33}
62ZN2cG (2006Hy02), 0.11 {I4} (2005Ca06), 0.120 {I21} (2003Hy02), 0.12 {I3}
62ZN3cG (2002Bl17), 0.106 {I17} (2000DoZX)
62ZN L 1804.62 6 2+ 2.63 PS 42
62ZN E 0.0005 LT 3.0E-6 LT 10.3 GT 0.0005 LT ?
62ZNS E EAV=2953.98 19$CK=0.00524 15$CL=5.84E-4 16$CM+=1.043E-4 27
62ZN G 850.7 1 0.0088 3 M1+E2 -5.1 +29-34
62ZN cG $Others: E|g=850.9 {I2}, I|g=0.0100 {I7} (2008Fi07);
62ZN2cG E|g=850.8 {I2}, I|g=0.0090 {I14} (2006Hy02); I|g=0.021 {I8} (2008Be21)
62ZN cG MR$from (851|g)(954|g)(|q) (2020Ma59), in exact agreement with |d value
62ZN2cG from 1981Wa09 in {+58}Ni({+6}Li,np|g) reaction.
62ZN G 1804.6 1 0.0075 3 E2
62ZN cG $Others: E|g=1805.0 {I4}, I|g=0.0070 {I6} (2008Fi07); E|g=1804.2 {I3},
62ZN2cG I|g=0.0081 {I14} (2006Hy02)
62ZN L 2342.35 8 0+
62ZN cL E$2342.1 {I1} (2020Ma59)
62ZN cL J$from (1388|g)(954|g)(|q) in 2020Ma59. J|p=2+, as proposed in 2013Le25
62ZN2cL from L(p,t)=2, and also in 2019Le11 is
62ZN3cL excluded with 99.9% confidence in the present |g|g(|q) data. Note that
62ZN4cL firm 0+ was assigned for this level in {+62}Zn Adopted Levels in the
62ZN5cL ENSDF database of 2012, based on |g|g(|q) data in {+61}Ni({+3}He,2n|g);
62ZN6cL (2010Al28); L({+6}Li,d)=0 in 1977Fu03 and L(p,t)=0 in 1974Hi05
62ZN E 0.0097 7 0.35E-4 3 6.822 31 0.0097 7
62ZNS E EAV=2696.91 20$CK=0.00322 9$CL=3.58E-4 10$CM+=6.39E-5 17
62ZN G 1388.4 1 0.0188 4
62ZN cG $Others: E|g=1388.5 {I3}, I|g=0.0191 {I8} (2008Fi07); E|g=1388.1 {I2},
62ZN2cG I|g=0.0176 {I20} (2006Hy02); I|g=0.023 {I11} (2008Be21)
62ZN L 2803.24 10 2+ 0.167 PS LT
62ZN cL E$2803.2 {I1} (2020Ma59). A 2802.0 {I12} |g with I|g=0.0006 {I4}
62ZN2cL from 2008Fi07 from this level was not confirmed by 2020Ma59
62ZN E 0.0013 5 1.3E-5 5 9.39 17 0.0013 5
62ZNS E EAV=2476.02 20$CK=0.00882 25$CL=9.85E-4 27$CM+=1.757E-4 46
62ZN G 1849.4 1 0.0070 2 (M1(+E2))
62ZN cG $Others: E|g=1849.6 {I4}, I|g=0.0072 {I6} (2008Fi07); E|g=1850.1 {I3},
62ZN2cG I|g=0.0081 {I14} (2006Hy02); I|g=0.020 {I9} (2008Be21)
62ZN L 2884.2 4 2+ 0.153 PS LT
62ZN cL E$2885.1 {I5} (2020Ma59)
62ZN E 0.003 LT 3E-5 LT 9.0 GT 0.003 LT ?
62ZNS E EAV=2437.40 29$CK=0.00924 26$CL=0.001032 29$CM+=1.842E-4 48
62ZN G 1931.3 5 0.00065 16 (M1(+E2))
62ZN L 2961.53 10 (1+)
62ZN cL E$2961.4 {I5} (2020Ma59)
62ZN E 0.0014 4 7.1E-6 21 7.44 12 0.0014 4
62ZNS E EAV=2397.20 20$CK=0.00446 12$CL=4.96E-4 14$CM+=8.85E-5 23
62ZN G 619.1 1 0.00108 14
62ZN G 1156.8 2 0.0017 2
62ZN G 2962.3 8 0.00051 16
62ZN L 3046.38 11 0+
62ZN cL E$3046.3 {I1} (2020Ma59)
62ZN cL J$(2093|g)(954|g)(|q) in 2020Ma59 consistent with 0+, but also allows
62ZN2cL J=1,2,3,4. 2020Ma59 assign definite 0+, combining their |g|g(|q) data
62ZN3cL and L(p,t)=0 in 2013Le25
62ZN E 0.0045 2 2.39E-5 13 6.897 19 0.0045 2
62ZNS E EAV=2356.21 20$CK=0.00467 13$CL=5.20E-4 15$CM+=9.30E-5 24
62ZN G 2092.5 1 0.0046 2
62ZN cG $Other: E|g=2089.0 {I8}, I|g=0.0012 {I5} (2008Fi07, tentative |g)
62ZN L 3148.01 21 (0+,1-,2+)
62ZN cL E$3147.0 {I5} (2020Ma59)
62ZN cL J$(2+) in 2020Ma59
62ZN E 0.00021 LT 1.2E-6 LT 10.0 GT 0.00021 LT ?
62ZNS E EAV=2311.72 21$CK=0.00495 14$CL=5.52E-4 15$CM+=9.85E-5 26
62ZN G 2193.2 8 0.00022 9
62ZN L 3180.89 8 1(+)
62ZN cL E$3180.9 {I3} (2020Ma59)
62ZN cL J$(2227|g)(954|g)(|q) (2020Ma59) allows J=1,2,3,4; |g to 0+ and
62ZN2cL probable |b feeding by Gamow-Teller transition from 0+ parent does not
62ZN3cL permit J=2,3,4. Compiler's note: 1- is not completely excluded by
62ZN4cL log| {Ift} value
62ZN E 0.0337 8 1.93E-4 7 5.966 10 0.0339 8
62ZNS E EAV=2291.29 20$CK=0.00505 14$CL=5.62E-4 16$CM+=1.004E-4 26
62ZN G 295.5 14 0.0004136 ?
62ZN G 838.7 4 0.0007 3
62ZN G 1376.2 3 0.00080 19
62ZN G 2227.0 1 0.0282 6 (M1(+E2)) -0.01 8
62ZN cG $Others: E|g=2227.2 {I4}, I|g=0.0262 {I11} (2008Fi07); E|g=2227.1 {I3},
62ZN2cG I|g=0.0279 {I24} (2006Hy02); I|g=0.024 {I10} (2008Be21)
62ZN cG MR$from |g|g(|q) for J=1 for 3181 level
62ZN G 3180.8 1 0.00374 17
62ZN cG $Others: E|g=3181.3 {I6}, I|g=0.0042 {I5} (2008Fi07); E|g=3180.9 {I5},
62ZN2cG I|g=0.0023 {I8} (2006Hy02)
62ZN L 3340.5 3 (0+,1,2-)
62ZN cL E$3339.8 {I5} (2020Ma59)
62ZN cL J$(1+) in 2020Ma59
62ZN E 4.0E-4 19 2.5E-6 12 7.83 21 4.0E-4 19
62ZNS E EAV=2214.34 24$CK=0.00555 16$CL=6.18E-4 17$CM+=1.103E-4 29
62ZN G 2386.0 5 0.00064 15
62ZN L 3374.21 10 1-
62ZN cL E$3374.2 {I7} (2020Ma59)
62ZN cL J$(1) in 2020Ma59
62ZN E 0.00606 303.91E-5 22 6.632 21 0.0061 3
62ZNS E EAV=2198.10 20$CK=0.00566 16$CL=6.31E-4 18$CM+=1.126E-4 29
62ZN G 1031.4 2 0.00050 9
62ZN cG $Other: E|g=1032.0 {I5}, I|g=0.0006 {I5} (2008Fi07)
62ZN G 1569.7 1 0.0037 2
62ZN cG $Other: E|g=1569.8 {I4}, I|g=0.0030 {I5} (2008Fi07)
62ZN G 3374.1 2 0.00215 15
62ZN cG $Other: E|g=3373.5 {I8}, I|g=0.0018 {I4} (2008Fi07)
62ZN L 3424.13 11 (1+)
62ZN cL E$3424.6 {I7} (2020Ma59)
62ZN E 0.0064 6 4.3E-5 4 6.59 4 0.0064 6
62ZNS E EAV=2174.05 20$CK=0.00584 16$CL=6.50E-4 18$CM+=1.161E-4 30
62ZN G 1619.3 1 0.0040 2
62ZN G 2471.4 5 0.0012 5
62ZN G 3425.3 3 0.0012 2
62ZNF G FL=0.0
62ZN cG E$poor fit, level-energy difference gives E|g=3424.0 {I1}
62ZN L 3561.0 5 (0+,1,2-)
62ZN cL E$3560.9 {I5} (2020Ma59)
62ZN cL J$(1+) in 2020Ma59
62ZN E 3.9E-4 14 2.8E-6 11 7.75 16 3.9E-4 14
62ZNS E EAV=2108.18 29$CK=0.00636 18$CL=7.08E-4 20$CM+=1.264E-4 33
62ZN G 2607.1 5 0.00039 14
62ZN L 3690.6 9 (0+,1,2-)
62ZN cL E$3690.4 {I9} (2020Ma59)
62ZN cL J$(1+) in 2020Ma59
62ZN E 3.0E-4 10 2.4E-6 8 7.80 14 3.0E-4 10
62ZNS E EAV=2045.88 48$CK=0.00691 20$CL=7.70E-4 22$CM+=1.374E-4 36
62ZN G 2736.7 9 0.00030 10
62ZN L 3862 2 0+ A ?
62ZN E 2.2E-4 LE 1.9E-6 LE 7.9 GE 2.2E-4 LE ?
62ZNS E EAV=1963.6 10$CK=0.00774 22$CL=8.62E-4 25$CM+=1.540E-4 42
62ZN L 3936 6 0+ A ?
62ZN E 1.3E-4 LE 1.2E-6 LE 8.1 GE 1.3E-4 LE ?
62ZNS E EAV=1928.1 29$CK=0.00814 26$CL=9.07E-4 29$CM+=1.619E-4 48
62ZN L 4021.79 9 (1+)
62ZN cL E$4021.7 {I5} (2020Ma59)
62ZN E 0.0203 8 2.01E-4 10 5.817 17 0.0205 8
62ZNS E EAV=1886.99 20$CK=0.00864 24$CL=9.63E-4 27$CM+=1.719E-4 45
62ZN G 1218.5 6 0.0013 3
62ZN G 1680.4 4 0.0008 2
62ZN cG $Other: E|g=1679.3 {I6}, I|g=0.0008 {I5} (2008Fi07)
62ZN G 3067.8 2 0.00153 13
62ZN cG $Others: E|g=3068.1 {I8}, I|g=0.0016 {I4} (2008Fi07); E|g=3068.2 {I6},
62ZN2cG I|g=0.0014 {I7} (2006Hy02)
62ZN G 4021.6 1 0.0169 6
62ZN cG $Others: E|g=4021.7 {I8}, I|g=0.0149 {I10} (2008Fi07); E|g=4021.2 {I5},
62ZN2cG I|g=0.0160 {I21} (2006Hy02)
62ZN L 4322.6 4 (1+)
62ZN cL E$4322.4 {I9} (2020Ma59)
62ZN E 0.0016 3 1.9E-5 4 6.78 8 0.0016 3
62ZNS E EAV=1743.14 29$CK=0.01077 30$CL=0.001200 34$CM+=2.14E-4 6
62ZN G 1982.1 9 0.00008 5 x ?
62ZN G 2518.0 6 0.00097 14
62ZN G 3368.1 5 0.0005 2
62ZN L 4447.85 6 (1+)
62ZN cL E$4447.9 {I4} (2020Ma59)
62ZN E 0.0273 9 3.71E-4 16 5.473 14 0.0277 9
62ZNS E EAV=1683.39 19$CK=0.01186 33$CL=0.001322 37$CM+=2.36E-4 6
62ZN G 1107.4 6 0.00009 4
62ZN G 1644.6 2 0.0016 2
62ZN cG $Others: E|g=1644.7 {I5}, I|g=0.0021 {I5} (2008Fi07); E|g=1645.1 {I6},
62ZN2cG I|g=0.0026 {I11} (2006Hy02)
62ZN G 2105.4 1 0.0043 2
62ZN cG $Others: E|g=2105.9 {I4}, I|g=0.0061 {I6} (2008Fi07); E|g=2105.4 {I4},
62ZN2cG I|g=0.0069 {I14} (2006Hy02)
62ZN G 2643.2 1 0.00364 16
62ZN cG $Others: E|g=2643.9 {I6}, I|g=0.0026 {I5} (2008Fi07); E|g=2643.3 {I3},
62ZN2cG I|g=0.0031 {I10} (2006Hy02)
62ZN G 3493.9 1 0.0064 2
62ZN cG $Others: E|g=3493.9 {I7}, I|g=0.0058 {I6} (2008Fi07); E|g=3494.0 {I5},
62ZN2cG I|g=0.0052 {I13} (2006Hy02)
62ZN G 4447.7 1 0.0117 8
62ZN cG $Others: E|g=4447.8 {I9}, I|g=0.0109 {I8} (2008Fi07); E|g=4448.3 {I7},
62ZN2cG I|g=0.0104 {I18} (2006Hy02)
62ZN L 4531.6 5 (0+,1,2-)
62ZN cL E$4531.5 {I5} (2020Ma59)
62ZN cL J$(1+) in 2020Ma59
62ZN E 3.1E-4 12 4.5E-6 18 7.38 17 3.1E-4 12
62ZNS E EAV=1643.49 29$CK=0.01268 35$CL=0.001413 40$CM+=2.53E-4 7
62ZN G 3577.6 5 0.00031 12
62ZN L 4552 9 0+ A ?
62ZN E 2.4E-4 LE 3.6E-6 LE 7.5 GE 2.4E-4 LE ?
62ZNS E EAV=1633.7 43$CK=0.01289 45$CL=0.00144 5$CM+=2.57E-4 8
62ZN L 4894.35 9 (1+)
62ZN cL E$4894.4 {I5} (2020Ma59)
62ZN E 0.0093 9 1.85E-4 19 5.688 41 0.0095 9
62ZNS E EAV=1471.19 19$CK=0.01724 48$CL=0.00192 5$CM+=3.43E-4 9
62ZN G 1932.4 2 0.0019 2
62ZN G 2091.5 4 0.0007 2
62ZN cG $Others: E|g=2092.5 {I4}, I|g=0.0047 {I6} (2008Fi07); E|g=2091.4 {I5},
62ZN2cG I|g=0.0038 {I10} (2006Hy02)
62ZN G 3089.6 6 0.00013 9 x ?
62ZN cG $Other: E|g=3089.0 {I10}, I|g=0.0009 {I4} (2008Fi07)
62ZN G 3940.5 4 0.00032 14
62ZN G 4894.2 1 0.0064 8
62ZN cG $Others: E|g=4894.4 {I10}, I|g=0.0042 {I5} (2008Fi07);
62ZN2cG E|g=4894.9 {I19}, I|g=0.0063 {I16} (2006Hy02)
62ZN L 5210.91 8 (1+)
62ZN cL E$5210.8 {I4} (2020Ma59)
62ZN E 0.0134 11 3.6E-4 3 5.329 35 0.0138 11
62ZNS E EAV=1321.63 19$CK=0.0232 6$CL=0.00259 7$CM+=4.62E-4 12
62ZN G 1836.9 4 0.00024 10
62ZN G 2062.8 2 0.00016 12 x ?
62ZN G 2164.4 5 0.00011 6 x ?
62ZN G 2407.8 3 0.00117 15
62ZN cG $Other: E|g=2408.3 {I7}, I|g=0.0013 {I4} (2008Fi07)
62ZN G 2870.5 5 0.00111 4
62ZN cG E,RI$from e-mail reply of Dec 29, 2020 from A.D. Maclean, first author
62ZN2cG of 2020Ma59.
62ZNF G FL=2342.35
62ZN cG $Others: E|g=2869.8 {I7}, I|g=0.0017 {I4} (2008Fi07); E|g=2870.1 {I9},
62ZN2cG I|g=0.0026 {I13} (2006Hy02)
62ZN G 3405.8 5 0.00080 13
62ZN cG E$note that energy of this |g ray listed as 2870 is erroneous in
62ZN2cG level-scheme Fig. 6 of 2020Ma59
62ZN G 4256.9 1 0.0040 2
62ZN cG $Others: E|g=4256.6 {I9}, I|g=0.0029 {I4} (2008Fi07); E|g=4257.0 {I9},
62ZN2cG I|g=0.0030 {I12} (2006Hy02)
62ZN G 5210.6 1 0.0062 10
62ZN cG $Others: E|g=5211.5 {I11}, I|g=0.0051 {I6} (2008Fi07);
62ZN2cG E|g=5211.0 {I10}, I|g=0.0047 {I15} (2006Hy02)
62ZN L 5394.0 4 (1+)
62ZN cL E$5394.3 {I10} (2020Ma59)
62ZN E 0.00107 19 3.5E-5 6 6.30 8 0.0011 2
62ZNS E EAV=1235.52 28$CK=0.0280 8$CL=0.00312 9$CM+=5.57E-4 14
62ZN G 2589.9 7 0.00008 4
62ZN G 3051.6 7 0.00025 9 x
62ZN G 3589.6 4 0.0008 2
62ZN L 5507.73 23 (1+)
62ZN cL E$5508.0 {I11} (2020Ma59)
62ZN E 0.00174 29 6.5E-5 11 6.01 7 0.0018 3
62ZNS E EAV=1182.19 22$CK=0.0316 9$CL=0.00352 10$CM+=6.29E-4 16
62ZN G 2166.7 4 0.00015 10 ?
62ZN G 2624.2 4 0.00029 11
62ZN G 2704.4 3 0.00086 14
62ZN G 3164.1 7 0.00017 8
62ZN G 5508.0 7 0.00037 13
62ZN L 5583.8 4 (1+) ?
62ZN cL E$5583.8 {I4} (2020Ma59).
62ZN E 1.25E-4 48 0.5E-5 2 7.10 17 1.3E-4 5 ?
62ZNS E EAV=1146.60 28$CK=0.0344 9$CL=0.00383 11$CM+=6.84E-4 18
62ZN G 5583.5 4 0.00013 5 x ?
62ZN L 5919.8 4 (1+)
62ZN cL E$5919.6 {I6} (2020Ma59)
62ZN E 0.0015 5 0.9E-4 3 5.75 14 0.0016 5
62ZNS E EAV=990.17 28$CK=0.0514 14$CL=0.00574 15$CM+=0.001025 26
62ZN G 3577.7 6 0.00011 7 x ?
62ZN G 5919.2 5 0.0015 5
62ZN cG $Other: E|g=5920.5 {I17}, I|g=0.0008 {I4} (2008Fi07, tentative |g)