66ZN 66GA EC DECAY 2004BEZR,2002BA38 10NDS 201004
66ZN H TYP=FUL$AUT=E. BROWNE, J. K. TULI$CIT=NDS 111, 1093 (2010)$
66ZN2 H CUT=3-Mar-2009$
66ZN D Modified by E. Browne (June 2, 2009). New BRICC, etc..
66ZN C 2004BeZR: Data evaluated by E. Browne for the Decay Data Evaluation
66ZN2C Project (^DDEP). A detailed description of the evaluation procedures
66ZN3C used is given in www.nucleide.org/DDEP_WG/^DDEPdata.htm.
66ZN C 2002Ba38: Reports a combination of G-ray intensity measurements from
66ZN2C two laboratories: The Lawrence Berkeley National Laboratory (USA), and
66ZN3C the Budapest Neutron Center (Hungary).
66ZN C Berkeley measurement: Activity produced by 66ZN(P,N), E=17.5 MeV
66ZN2C using a GT 99% pure natural zinc target. Detector: Hyper-pure Ge.
66ZN3C The relative detector efficiency was calibrated with sources of 56CO,
66ZN4C 152EU, 154EU, and 228TH. Absolute detector efficiency was determined
66ZN5C using sources of 60CO, 137CS, and a 13C(238PU) source, which provided
66ZN6C a 6129-keV G ray produced via the 13C(A,N)16O reaction.
66ZN C Budapest measurement: Activity produced by 66ZN(P,N), E=14.5 MeV,
66ZN2C using a target of 99.0 % 1 enriched 66ZN. Detector: hyper-pure Ge
66ZN3C with a Compton-suppression system. The detector efficiency was
66ZN4C calibrated with sources of 133BA and 152EU, as well as using capture
66ZN5C G rays from the 35CL(N,G) reaction.
66ZN C 2000Ra36: G-ray activity measured with a large hyper-pure
66ZN2C Compton-suppressed Ge detector. Its efficiency was calibrated using
66ZN3C the following sources: 22NA, 54MN, 57CO, 60CO, 88Y, 133BA, 137CS,
66ZN4C 152EU, 207BI, 241AM, 226RA, and 228TH. Also using capture G rays from
66ZN5C the 12C(N,G) and 14N(N,G) reactions.
66ZN C 1994En02: Activity produced by 63CU(A,N), E=18 MeV using a target
66ZN2C of high-purity natural copper. Detector: GELI with a
66ZN3C Compton-suppression shield. Detector efficiency was internally
66ZN4C calibrated with the strongest G rays from 66GA decay.
66ZN c 1960Sc06: E|g, I|g, |g|g coincidences, |g|g(|q), E|b+, I|b{++},
66ZN2c |b{++}|g coincidences, and internal conversion; magnetic spectrometer,
66ZN3c scintillators
66ZN c Others: 1953Ma01, 1966Ac02, 1966Co05, 1966Fr13, 1966Wi13, 1967Ca12,
66ZN2c 1967Va13, 1967Vr03, 1969St08, 1970Ph01, 1971Ca14, 1972GeZF, 1975Mc07,
66ZN3c and 1993Al15.
66ZN c 1963Ca03: |b{++} spectrum, analyzed shape of g.s. transition;
66ZN2c magnetic spectrometer, proportional counters, scintillators
66ZN c 1952Mu35: E|g, I|g, |g|g coincidences, E|b+, and I|b{++}; magnetic
66ZN2c spectrometer, lead radiator, scintillators
66ZN c 1950La55: E|g, I|g, E|b+, I|b{++}, |b{++}|g coincidences, and Auger
66ZN2c electrons; magnetic spectrometer, gas counters, uranium radiator
66ZN cE Analysis of the {+66}Ga |b{++} spectrum has established that
66ZN2cE the g.s. transition has a non-statistical shape (1963Ca03).
66ZN cE IB,IE From I(|e+|b{++}) and theoretical |e/|b{++} ratios, except
66ZN2cE for the g.s.
66ZN CG RI The relative intensities of the strongest G rays are values
66ZN2CG recommended in 2004BeZR and 2002Ba38. These are weighted averages of
66ZN3CG results from Berkeley, Budapest, and from those reported in 2000Ra36.
66ZN4CG The relative intensities of weaker G rays are weighted averages of
66ZN5CG values reported in 1970Ph01, 1971Ca14, and 1994En02.
66ZN6CG Relative G-ray intensities in 1970Ph01 have been corrected
66ZN7CG for a systematic inaccuracy in the detector efficiency calibration
66ZN8CG above 1050 keV. Correction factor
66ZN9CG f=1.116 - 0.155 EG (MeV) + 0.0397 EG (MeV) X EG (MeV) (2002Ba38).
66ZNACG Uncertainties in RI are statistical values given by authors.
66ZN CG MR(P) From GG(THETA) in 66GA EC decay (2002Ga20).
66ZN CG E(Q) From 2000He14. These values are based on a revised energy
66ZN2CG scale that uses the new adjusted fundamental constants and wave
66ZN3CG lengths deduced from an updated value of the lattice spacing of Si
66ZN4CG crystals [Cohen and Taylor 1987Co39]. Helmer and van der Leun
66ZN5CG (2000He14) fitted the adjusted G-ray energies of 66GA to a level
66ZN6CG scheme and deduced their recommended values from level-energy
66ZN7CG differences.
66ZN CG E G rays with precise energies are from 2000He14. Those with
66ZN2CG less precise energies are from 1993Al15 and 1994En02, but adjusted
66ZN3CG to those in 2000He14 using a least-squares procedure (2004BeZR).
66ZN4CG The difference between these two energy scales has been used
66ZN5CG as a systematic adjustment, and applied to the the energies
66ZN6CG given here. Thus, the uncertainties in the G-ray energies presented
66ZN7CG in this evaluation are just statistical, as reported by authors.
66ZN CL J,T$From Adopted Levels.
66GA P 0.0 0+ 9.49 H 3 5175 3
66ZN N 0.37 2 1.0 1.0
66ZN PN 4
66ZN CN NR The decay scheme normalization has been deduced as in
66ZN2CN 2004BeZR, based on the following results:
66ZN3CN ICE(1039G)/IB+(GS)= 2.08E-4 10 (1960Sc06).
66ZN4CN IB+(GS)/SUMOF IB+{-i}= 0.8697 (1960Sc06).
66ZN5CN ICE(1039G, E2)/RI(1039G)= 2.69E-4 4, and using theoretical
66ZN6CN conversion coefficients interpolated using the ^BRICC computer code.
66ZN7CN Therefore, RI(1039G)/SUMOF IB+{-i}= 2.08E-4 10 X 0.8697/2.69E-4 4
66ZN8CN =0.67 3. Also SUMOF IB+{-i}/SUMOF IE{-i}= 1.265 from decay scheme and
66ZN9CN theoretical values of IB+{-i}/IE{-i} for each level.
66ZNACN Using SUMOF IB+{-i} + SUMOF IE{-i}= 100% gives SUMOF IB+{-i}= 55.8% 24
66ZNBCN and RI(1069G)= 0.67 3 X 55.8% 24= 37% 2, thus NR=0.37 2.
66ZN G 171.9 2 0.028 1
66ZN G 3724.8 100.0065 10
66ZN G 3806.3 100.0066 11
66ZN G 3827.5 8 0.0190 22
66ZN L 0 0+ STABLE
66ZN E 5175 3 51 4 0.48 4 7.88 4 51 4
66ZN cE E from endpoint of |b{++} spectrum=4153 {I3} (1963Ca03)
66ZNS E EAV=1904.1 15 $CK=0.008365 18$CL=0.00092 $CM+=0.0001639 4
66ZN L 1039.2279 212+ 1.68 PS 3
66ZN G 1039.220 3 100.0 3 E2
66ZNF G FLAG=Q
66ZN cG |a(K)exp+|a(L)exp=2.7|*10{+-4} {I4} (1960Sc06)
66ZN cG M M1,E2 from ce data (1960Sc06)
66ZNS G CC=0.000269 4$KC=0.000241 4$LC=2.41E-5 4$MC=3.46E-6 5$NC+=1.384E-7 20
66ZNS G NC=1.384E-7 20
66ZN L 1872.7653 242+ 0.19 PS 7
66ZN G 833.5324 2115.93 6 M1+E2 -1.6 2
66ZNF G FLAG=PQ
66ZN cG |a(K)exp+|a(L)exp=4.3|*10{+-4} {I6} (1960Sc06)
66ZN cG M D+Q from |g|g(|q); M1,E2 from ce data (1960Sc06)
66ZNS G CC=0.000434 9$KC=0.000389 8$LC=3.91E-5 8$MC=5.60E-6 11$NC+=2.24E-7 5
66ZNS G NC=2.24E-7 5
66ZN CG MR Other value: -1.9 3 (1974Kr16)
66ZN G 1872.740 6 0.062 4 [E2]
66ZNS G CC=0.000328 5$KC=7.04E-5 10$LC=6.99E-6 10$MC=1.001E-6 14$NC+=0.000250 4
66ZNS G NC=4.05E-8 6$IPC=0.000250 4
66ZN L 2372.353 40+ 0.21 PS GT
66ZN E 2860 50 0.30 3 0.038 3 8.46 4 0.34 3
66ZNS E EAV=781.6 14 $CK=0.0977 5 $CL=0.01079 5 $CM+=0.001920 9
66ZN cE E from |b{++} endpoint energy of 1840 {I50} (1963Ca03)
66ZN G 499.590 6 0.013 3 E2
66ZNS G CC=0.00199 3$KC=0.001782 25$LC=0.000182 3$MC=2.61E-5 4
66ZNS G NC=1.013E-6 15
66ZN G 1333.112 5 3.175 13E2
66ZNF G FLAG=Q
66ZN cG |a(K)exp+|a(L)exp=1.1|*10{+-4} {I4} (1960Sc06)
66ZNS G CC=0.000190 3$KC=0.0001383 20$LC=1.379E-5 20$MC=1.98E-6 3$NC+=3.61E-5 5
66ZNS G NC=7.96E-8 12$IPC=3.61E-5 5
66ZN L 2780.157 72+ 0.26 PS 7
66ZN G 907.390 190.059 4 M1+E2 0.13 24
66ZNF G FLAG=P
66ZNS G CC=0.000306 9$KC=0.000275 8$LC=2.74E-5 8$MC=3.93E-6 11$NC+=1.59E-7 5
66ZNS G NC=1.59E-7 5
66ZN CG MR Other value: -3 +{I1}-{I9} (2002Ga20)
66ZN G 1740.904 160.0773 10M1+E2 0.33 28
66ZNF G FLAG=P
66ZNS G CC=0.000241 8$KC=7.74E-5 13$LC=7.67E-6 13$MC=1.100E-6 19$NC+=0.000155 7
66ZNS G NC=4.47E-8 8$IPC=0.000155 7
66ZN G 2780.095 160.334 8 E2
66ZNF G FLAG=Q
66ZNS G CC=0.000722 11$KC=3.51E-5 5$LC=3.47E-6 5$MC=4.98E-7 7$NC+=0.000683 10
66ZNS G NC=2.02E-8 3$IPC=0.000683 10
66ZN L 2826.69 5 3- 0.180 PS 7
66ZN E 0.0053 8 0.0017 3 9.66 7 0.0070 11
66ZNS E EAV=575.3 14 $CK=0.2112 12 $CL=0.02335 13 $CM+=0.004156 23
66ZN G 953.93 9 0.0027 3
66ZN G 1787.44 9 0.0240 20(E1)
66ZN cG |d(M2/E1)=-0.04 {I5} (1977Ne04).
66ZNS G CC=0.000526 8$KC=4.21E-5 6$LC=4.16E-6 6$MC=5.95E-7 9$NC+=0.000479 7
66ZNS G NC=2.41E-8 4$IPC=0.000479 7
66ZN L 2938.074 32+ 0.044 PS 16
66ZN G 1065.305 9 0.0063 12
66ZN G 1898.823 8 1.051 8 (M1+E2) 0.03 1
66ZNF G FLAG=Q
66ZNS G CC=0.000288 4$KC=6.58E-5 10$LC=6.52E-6 10$MC=9.35E-7 13$NC+=0.000215 3
66ZNS G NC=3.80E-8 6$IPC=0.000215 3
66ZN CG MR From G(THETA) in 66ZN(N,N'G) (1980KaZD).
66ZN2CG Other value: 0.00 6 (2002Ga20).
66ZN L 3105.040 40+
66ZN G 1232.264 8 1.35 5
66ZN G 2065.778 7 0.084 4
66ZNF G FLAG=Q
66ZN L 3212.582 82+ 0.083 PS +21-14
66ZN G 2173.319 150.228 12
66ZNF G FLAG=Q
66ZN G 3212.499 190.0050 10
66ZN L 3228.885 31+ 0.12 PS 3
66ZN E 1920 50 3.7 3 3.7 3 6.14 4 7.4 6
66ZNS E EAV=397.1 14 $CK=0.4458 24 $CL=0.0494 3 $CM+=0.00879 5
66ZN cE E from |b{++} endpoint energy=900 {I50} (1952Mu35) E|b+|?880
66ZN2cE (1950La55)
66ZN G 290.8105 110.133 4
66ZN G 448.73 2 0.290 10M1(+E2) -0.02 3
66ZNF G FLAG=P
66ZNS G CC=0.001419 20$KC=0.001272 18$LC=0.0001283 19$MC=1.84E-5 3$NC+=7.39E-7
66ZNS G NC=7.39E-7 11
66ZN G 856.527 100.301 17
66ZN G 1356.104 9 0.96 10
66ZN G 2189.616 6 14.42 6 M1+E2 0.12 2
66ZNF G FLAG=PQ
66ZNS G CC=0.000398 6$KC=5.12E-5 8$LC=5.07E-6 7$MC=7.26E-7 11$NC+=0.000341 5
66ZNS G NC=2.95E-8 5$IPC=0.000341 5
66ZN cG |a(K)exp+|a(L)exp=0.49|*10{+-4} {I8} (1960Sc06)
66ZN cG M M1+E2 from ce data (1969Sc06)
66ZN G 3228.800 6 4.082 22M1
66ZNF G FLAG=Q
66ZNS G CC=0.000812 12$KC=2.68E-4 6$LC=2.64E-6 4$MC=3.79E-7 6
66ZNS G NC=1.544E-8 22$IPC=0.000782 11
66ZN L 3331.441 62+ 0.083 PS +21-14
66ZN G 551.284 220.0189 16
66ZN G 1458.662 120.261 6 (M1+E2) -0.01 9
66ZNF G FLAG=PQ
66ZNS G CC=0.0001741 25$KC=0.0001070 15$LC=1.062E-5 15$MC=1.523E-6 22
66ZNS G NC=6.18E-8 9$IPC=5.49E-5 8
66ZN G 2292.171 130.046 3
66ZN G 3331.351 140.061 8
66ZN L 3380.944 41- 20 FS 5
66ZN E 0.70 6 1.31 11 6.53 4 2.01 17
66ZNS E EAV=331.1 13 $CK=0.575 3 $CL=0.0637 3 $CM+=0.01134 6
66ZN G 442.873 140.042 3
66ZN G 600.788 210.0365 23
66ZN G 1008.588 120.160 20
66ZN G 1508.158 7 1.497 7
66ZNF G FLAG=Q
66ZN G 2341.673 110.0086 17
66ZN G 3380.850 6 3.960 23
66ZNF G FLAG=Q
66ZN L 3427.406 181,2-
66ZN E 0.0020 5 0.0047 11 8.95 11 0.0067 16
66ZNS E EAV=311.1 13 $CK=0.616 3 $CL=0.0683 3 $CM+=0.01215 6
66ZN G 1554.62 3 0.050 3
66ZN L 3432.408 41- 30 FS +19-8
66ZN E 0.16 2 0.39 4 7.03 4 0.55 5
66ZNS E EAV=308.9 13 $CK=0.620 3 $CL=0.0688 3 $CM+=0.01224 6
66ZN G 494.336 130.0152 20
66ZN G 1060.051 110.042 3
66ZN G 1559.627 100.059 4
66ZN G 2393.129 7 0.635 20E1
66ZNF G FLAG=Q
66ZNS G CC=0.000924 13$KC=2.73E-5 4$LC=2.70E-6 4$MC=3.86E-7 6$NC+=0.000894 13
66ZNS G NC=1.569E-8 22$IPC=0.000894 13
66ZN CG MR=-0.04 5, GG(THETA) (2002Ga20).
66ZN G 3432.309 7 0.777 10
66ZNF G FLAG=Q
66ZN L 3507.249 232+
66ZN G 680.56 100.0040 11
66ZN G 1634.46 7 0.0095 15
66ZN G 2467.97 7 0.0228 19
66ZN L 3531.692 140+
66ZN G 2492.42 3 0.060 4
66ZN L 3576.370 224+
66ZN G 749.68 100.0037 11
66ZN G 796.21 5 0.0079 17
66ZN G 1703.59 5 0.015 5
66ZN G 2537.09 5 0.014 3
66ZN L 3670.72 5 2+
66ZN G 1797.94 9 0.0051 14
66ZN G 2631.44 9 0.008 3
66ZN L 3738.207 21 + 9.7 FS +30-18
66ZN E 0.000419 0.0068 15 8.62 10 0.0072 16
66ZNS E EAV=179.2 13 $CK=0.8342 13 $CL=0.09266 15 $CM+=0.01650 3
66ZN G 800.13 5 0.0027 14
66ZN G 2698.92 5 0.0100 17
66ZN G 3738.10 5 0.0374 20
66ZN L 3753.01 4 4+
66ZN G 2713.73 5 0.017 5
66ZN L 3791.123 31+
66ZN E 1420 50 0.94 8 26.0 21 5.00 4 26.9 22
66ZNS E EAV=157.0 13 $CK=0.8534 10 $CL=0.09483 11 $CM+=0.016887 19
66ZN cE E from |b{++} endpoint energy=400 {I50} (1952Mu35). E|b+|?400,
66ZN2cE no uncertainty given (1950La55).
66ZN G 283.87 3 0.0097 21
66ZN G 410.178 120.177 7
66ZN G 459.683 140.237 10
66ZN G 562.241 100.0179 17
66ZN G 578.540 190.159 20
66ZN G 686.080 6 0.681 20
66ZNF G FLAG=Q
66ZN G 853.038 8 0.205 5 M1+E2 0.37 18
66ZNF G FLAG=PQ
66ZNS G CC=0.000357 11$KC=0.000321 10$LC=3.20E-5 11$MC=4.59E-6 15$NC+=1.85E-7 6
66ZNS G NC=1.85E-7 6
66ZN G 1010.957 190.073 4
66ZN G 1418.754 5 1.657 8
66ZNF G FLAG=Q
66ZN G 1918.329 5 5.368 23M1+E2 -0.07 3
66ZNF G FLAG=PQ
66ZNS G CC=0.000295 5$KC=6.47E-5 9$LC=6.40E-6 9$MC=9.18E-7 13$NC+=0.000223 4
66ZNS G NC=3.73E-8 6$IPC=0.000223 4
66ZN cG |a(K)exp+|a(L)exp=1.1|*10{+-4} {I4} (1960Sc06)
66ZN G 2751.835 5 61.3 3 (M1+E2) -0.12 2
66ZNF G FLAG=PQ
66ZNS G CC=0.000626 9$KC=3.48E-5 5$LC=3.43E-6 5$MC=4.92E-7 7$NC+=0.000588 9
66ZNS G NC=2.00E-8 3$IPC=0.000588 9
66ZN cG |a(K)exp+|a(L)exp=0.38|*10{+-4} {I5} (1960Sc06)
66ZN cG M D+Q from |g|g(|q); M1+E2 from ce data (1960Sc06)
66ZN CG MR Other values: -0.09 3 or +3.5 4, GG(THETA) (1960Sc06).
66ZN G 3791.004 8 2.941 24 M1
66ZNS G CC=0.001017 16$KC=2.08E-5 3$LC=2.05E-6 3$MC=2.95E-7 5
66ZNS G NC=1.200E-8 17$IPC=0.000994 14
66ZN L 3825.0 3 0+
66ZN E 7.3E-5 15 0.0029 6 8.93 9 0.0030 6
66ZNS E EAV=142.9 13 $CK=0.8627 $CL=0.09589 $CM+=0.01708
66ZN G 2785.7 3 0.0080 14
66ZN L 3882.424 10(2)+
66ZN E 1.6E-5 11 0.0014 9 9.2 3 0.0014 9
66ZNS E EAV=118.9 13 $CK=0.8737 $CL=0.09718 $CM+=0.01731
66ZN G 2009.628 160.0083 17
66ZN G 2843.130 160.0045 9
66ZN L 4085.983 41+
66ZN E 1.67 14 5.99 4 1.67 14
66ZNS E CK=0.8839 $CL=0.09855 $CM+=0.01756
66ZN G 347.77 5 0.0048 15
66ZN G 554.28 3 0.0122 13
66ZN G 653.568 140.0036 12
66ZN G 658.57 3 0.0203 21
66ZN G 705.031 150.0102 11
66ZN G 857.093 9 0.040 12
66ZN G 873.392 210.046 3
66ZN G 980.934 130.131 5
66ZN G 1147.896 100.212 7 M1+E2 -0.18 5
66ZNF G FLAG=P
66ZNS G CC=0.000192 3$KC=0.0001708 25$LC=1.700E-5 25$MC=2.44E-6 4$NC+=2.28E-6 4
66ZNS G NC=9.87E-8 14$IPC=2.18E-6 4
66ZN G 1305.807 210.0107 12
66ZN G 1713.602 120.066 3
66ZN G 2213.181 9 0.354 12M1+E2 -0.23 5
66ZNF G FLAG=PQ
66ZNS G CC=0.000410 6$KC=5.03E-5 7$LC=4.98E-6 7$MC=7.14E-7 10$NC+=0.000354 6
66ZNS G NC=2.90E-8 4$IPC=0.000354 6
66ZN CG MR Other value: 4.9+{I16}-{I9} (2002Ga20).
66ZN G 3046.684 9 0.154 6 M1+E2 -0.8 2
66ZNF G FLAG=P
66ZNS G CC=0.000778 16$KC=2.97E-5 5$LC=2.94E-6 5$MC=4.21E-7 6$NC+=0.000745 16
66ZNS G NC=1.712E-8 25$IPC=0.000745 16
66ZN G 4085.853 9 3.445 20M1
66ZNF G FLAG=Q
66ZNS G CC=0.001117 16$KC=1.86E-5 3$LC=1.83E-6 3$MC=2.63E-7 4
66ZNS G NC=1.070E-8 15$IPC=0.001096 16
66ZN L 4295.339 41+ 4.2 FS +18-9
66ZN dL J from log| {Ift}=5.23 {I4} from 0+.
66ZN E 6.2 5 5.23 4 6.2 5
66ZNS E CK=0.8835 $CL=0.09888 $CM+=0.01762
66ZN G 412.916 160.0091 13
66ZN G 557.13 5 0.0166 17M1+E2
66ZNS G CC=0.0011 3$KC=0.00103 25$LC=0.00010 3$MC=1.5E-5 4$NC+=5.9E-7 14
66ZNS G NC=5.9E-7 14
66ZN G 718.97 5 0.0268 20
66ZN G 763.64 3 0.0240 20
66ZN G 862.926 130.0410 20
66ZN G 867.93 3 0.0117 14
66ZN G 914.388 140.073 4
66ZN G 963.892 150.039 3
66ZN G 1066.450 120.0064 12
66ZN G 1082.75 2 0.0358 20
66ZN G 1190.287 7 0.345 19
66ZN G 1357.250 120.44 13M1+E2 -0.18 5
66ZNF G FLAG=P
66ZNS G CC=0.0001689 24$KC=0.0001231 18$LC=1.223E-5 18$MC=1.753E-6 25
66ZNS G NC=7.11E-8 10$IPC=3.18E-5 5
66ZN CG MR Other value: 5+ {I2}-{I1} (2002Ga20).
66ZN G 1515.162 200.0167 15
66ZN G 2422.525 7 5.085 24M1(+E2) 0.01 3
66ZNF G FLAG=PQ
66ZNS G CC=0.000491 7$KC=4.30E-5 6$LC=4.25E-6 6$MC=6.10E-7 9$NC+=0.000443 7
66ZNS G NC=2.48E-8 4$IPC=0.000443 7
66ZN CG MR Other value: 2.2 2 (2002Ga20).
66ZN G 3256.021 9 0.254 10M1+E2 1.5 2
66ZNF G FLAG=P
66ZNS G CC=0.000889 14$KC=2.70E-5 4$LC=2.66E-6 4$MC=3.81E-7 6$NC+=0.000859 14
66ZNS G NC=1.552E-8 22$IPC=0.000859 14
66ZN G 4295.187 1010.30 8
66ZN cG |a(K)exp+|a(L)exp=0.18|*10{+-4} {I6} (1960Sc06)
66ZN L 4461.409 51+ 7.0 FS +12-3
66ZN dL J from log| {Ift}=5.54 {I4} from 0+
66ZN E 1.96 17 5.54 4 1.96 17
66ZNS E CK=0.8830 $CL=0.09927 $CM+=0.01770
66ZN G 375.398 170.0058 16
66ZN G 670.251 140.0110 18
66ZN G 708.36 5 0.0234 19
66ZN G 723.17 5 0.0093 13
66ZN G 885.00 5 0.0051 13
66ZN G 929.68 3 0.0123 15
66ZN G 954.12 7 0.0121 17
66ZN G 1129.923 180.0367 21
66ZN G 1232.480 150.15 5
66ZN G 1248.779 220.0027 9
66ZN G 1356.320 150.33 5
66ZN G 1523.279 150.0148 13
66ZN G 2088.985 130.031 7
66ZN G 2588.553 130.071 4 M1+E2 0.35 27
66ZNF G FLAG=P
66ZNS G CC=0.000568 16$KC=3.86E-5 6$LC=3.81E-6 6$MC=5.47E-7 9$NC+=0.000525 16
66ZNS G NC=2.22E-8 4$IPC=0.000525 16
66ZN G 3422.040 8 2.314 16M1+E2 -0.06 2
66ZN3 G FL=1039.2279
66ZNF G FLAG=PQ
66ZNS G CC=0.000885 13$KC=2.44E-5 4$LC=2.41E-6 4$MC=3.46E-7 5$NC+=0.000858 12
66ZNS G NC=1.408E-8 20$IPC=0.000858 12
66ZN G 4461.202 9 2.26 3
66ZN3 G FL=0
66ZNF G FLAG=Q
66ZN L 4638.24 141
66ZN E 0.0042 10 7.96 11 0.0042 10
66ZNS E CK=0.8822 $CL=0.09997 $CM+=0.01785
66ZN G 1106.53 240.0033 10
66ZN G 1409.35 240.0043 18
66ZN G 2265.84 240.0037 14
66ZN L 4675.6 5 1+
66ZN E 0.0015 5 8.35 15 0.0015 5
66ZNS E CK=0.8819 $CL=0.1002 $CM+=0.01789
66ZN G 2802.8 5 0.0040 11
66ZN L 4806.199 51+ 3.8 FS +13-8
66ZN dL J$from log| {Ift}=4.89 {I4} from 0+
66ZN E 2.30 19 4.89 4 2.30 19
66ZNS E CK=0.8806 $CL=0.1013 $CM+=0.01811
66ZN G 1015.081 180.033 8
66ZN G 1135.47 9 0.0128 13
66ZN G 1274.50 3 0.0189 15
66ZN G 1298.95 7 0.0103 12
66ZN G 1425.25 2 0.0163 13
66ZN G 1577.308 200.0108 16
66ZN G 1868.105 200.073 15
66ZN G 2026.016 250.0070 16
66ZN G 2433.807 180.0201 17
66ZN G 2933.358 9 0.576 8 M1+E2 1.6 2
66ZNF G FLAG=P
66ZNS G CC=0.000762 12$KC=3.19E-5 5$LC=3.15E-6 5$MC=4.52E-7 7$NC+=0.000727 12
66ZNS G NC=1.84E-8 3$IPC=0.000727 12
66ZN G 3766.850 9 0.403 15M1+E2 0.11 4
66ZNF G FLAG=PQ
66ZNS G CC=0.001009 15$KC=2.11E-5 3$LC=2.08E-6 3$MC=2.98E-7 5$NC+=0.000986 14
66ZNS G NC=1.212E-8 17$IPC=0.000986 14
66ZN G 4806.007 9 5.03 3
66ZNF G FLAG=Q
66ZN CG E$G-ray often used for the efficiency calibration of germanium
66ZN2CG detectors.
66ZN L 4849.93 3 1+
66ZN E 0.033 4 6.62 6 0.033 4
66ZNS E CK=0.8799 $CL=0.1018 $CM+=0.01823
66ZN G 1468.97 5 0.0037 10
66ZN G 2977.08 4 0.062 6
66ZN G 3810.59 5 0.0248 22
66ZN L 4866.056 161+
66ZN E 0.047 6 6.42 6 0.047 6
66ZNS E CK=0.8796 $CL=0.1021 $CM+=0.01828
66ZN G 1195.32 9 0.0025 9
66ZN G 1433.63 4 0.0050 10
66ZN G 1534.60 4 0.016 4
66ZN G 1927.96 4 0.0061 20
66ZN G 2085.86 4 0.006 4
66ZN G 2993.21 3 0.085 8
66ZN G 4865.87 4 0.0075 6
66ZN L 4958.2 4 1+
66ZN E 0.0020 5 7.48 11 0.0020 5
66ZNS E CK=0.8770 $CL=0.10429 11 $CM+=0.018726 22
66ZN G 3085.4 4 0.0053 13
66ZN L 5005.8 3 1+
66ZN E 0.0012218 7.47 7 0.00122 18
66ZNS E CK=0.8744 $CL=0.10644 18 $CM+=0.01916 4
66ZN G 5005.6 3 0.0033 4