65CU    65NI B- DECAY (2.5175 H)      1987JU05,1990LO03,1973RA1025NDS    202505
 65CU  H TYP=FUL$AUT=Jun Chen$CIT=NDS 202, 59 (2025)$CUT=25-Feb-2025$
 65CU DB EAV,LOGFT$FROM BetaShape v2.4 (Jun-2024) 2023MO21.
 65CU DG CC$FROM BrIcc v2.3e (17-Jun-2020) 2008Ki07, "Frozen Orbitals" appr.
 65CU dL E$Least-squares fitting is done by GLSC (version 28-Aug-2024)
 65CU c  1987Ju05: {+65}Ni source was produced from irradiation of enriched
 65CU2c  {+64}Ni metal with thermal neutrons at Technabsexport, USSR. |b
 65CU3c  particles were detected with a gas-flow proportional counter; |g rays
 65CU4c  were detected with two co-axial Ge detectors. Measured E|g, I|g, I|b,
 65CU5c  |b(t), 4|p|b|g-coin. Deduced parent T{-1/2}, relative |g-ray emission
 65CU6c  probabilities and absolute emission probabilites for 1482|g.
 65CU c  1973Ra10: {+65}Ni source was from {+64}Ni(n,|g). Measured E|g, I|g with
 65CU2c  a Ge(Li) detector. Deduced levels, |b-decay branching ratios,
 65CU3c  log {Ift}.
 65CU c  1990Lo03: {+65}Ni source was produced by {+65}Ni(n,|g) with thermal
 65CU2c  neutrons from the CONSORT II reactor on an enriched {+64}Ni target.
 65CU3c  |b particles were detected with a beta detector and |g rays were
 65CU4c  detected with Ge(Li) detectors. Measured E|g, I|g, I|b, 4|p|b|g-coin.
 65CU5c  Deduced relative and absolute |g-ray emission probabilies. Comparisons
 65CU6c  with available data.
 65CU c  1971Me14,1980RuZY: {+65}Ni source was from {+64}Ni(n,|g) at the NRU
 65CU2c  rabbit facility, Canada. Measured E|g, I|g, I|b{+-}, |b(t),
 65CU3c  4|p|b|g-coin. Deduced parent T{-1/2}, absolute emission probability of
 65CU4c  1482|g.
 65CU d  1980RuZY: T{-1/2} and |g emission probabilities for 33 radio-nuclides
 65CU2d  are discussed along with an assessment of data uncertainties
 65CU c  1972Pa30: {+65}Ni source was from {+64}Ni(n,|g) with neutrons from the
 65CU2c  the 5 MV reactor of DEMOCRITOS NRC. |g rays were detected with a Ge(Li)
 65CU3c  and a NaI(Tl) detector. Measured E|g, I|g, |g|g-coin. Deduced levels,
 65CU4c  |b-decay branching ratios, absolute |g-ray emission probabilies based
 65CU5c  an known value of %I|b(g.s.)=58
 65CU c  1972Co31: {+65}Ni source was from {+64}Ni(n,|g) with thermal neutrons
 65CU2c  from the Brookhaven High Flux Beam Reactor (HFBR). |g rays were
 65CU3c  detected with Ge(Li) detectors. Measured E|g, I|g, |g|g-coin. Deduced
 65CU4c  relative and absolute |g-ray emission probabilies, with the latter
 65CU5c  deduced by the authors based on an assumption of a combined yield of
 65CU6c  45.5% for 366|g, 1116|g and 1482|g
 65CU c  1963Cl06: {+65}Ni source was from {+64}Ni(n,|g) with thermal neutrons
 65CU2c  from the Materials Testing Reactor of National Reactor Testing Station
 65CU3c  in Idaho. |g rays were detected with NaI(Tl) detectors; |b particles
 65CU4c  were detected with a 4|p |b-flow proportional counter. Measured E|g,
 65CU5c  I|g, |g|g-coin, |g|g(|q), 4|p|b|g-coin, |b(t). Deduced parent T{-1/2},
 65CU6c  relative and absolute |g-ray emission probabilies, with the latter
 65CU7c  determined by comparions of relative |g-ray intensities with absolute
 65CU8c  disintegration from 4|b|g-coin measurements.
 65CU c  1976Kr09: {+65}Ni source was from {+64}Ni(n,|g) with thermal neutrons
 65CU2c  from the Los Alamos Omega West Reactor. |g rays were detected with a
 65CU3c  Ge(Li) detector. Measured E|g, I|g, |g(|q). Deduced |g-ray
 65CU4c  multipolarties and mixing ratios.
 65CU c  1968Re04: measured {+65}Ni T{-1/2} at ORNL
 65CU c  1968At03,1969Be28: measured |b-|g circular polarization correlations
 65CU2c  for 1116|g at the Lawrence Radiation Laboratory, Livermore.
 65CU c  1977Ba64: {+65}Ni T{-1/2} at JAERI.
 65CU c  1965Sp07: {+65}Ni source was from irradiation of 99.98% purified
 65CU2c  metallic Ni with neutrons from the FiR-1 reactor at Otaniemi, Finland.
 65CU3c  |g rays were detected with NaI(Tl) and Ge(Li) detectors. Measured E|g,
 65CU4c  I|g, |g|g-coin, |g|g(|q). Deduced levels, J, |p, |g-ray
 65CU5c  multipolarities, mixing ratios, and absolute emission probabilies
 65CU6c  by assuming %I|b(g.s.)=57 taken from 1949Si21
 65CU c  1964Fr04: measured E|g, I|g, E|b{+-}, I|b{+-} with a magnetic
 65CU2c  spectrometer for |b particles and a NaI for |g rays at the Nuclear
 65CU3c  Research Institute, Czechosl. Acad. Sci., Rez. Deduced absolute
 65CU4c  |g-ray emission probabilies by comparion of |g-ray intensities with
 65CU5c  measured total number of decays
 65CU c  1960Ja16: measured E|g, I|g, |g|g(|q) using NaI(Tl) detectors at the
 65CU2c  Atomic Energy Establishment, India. Deduced levels, J, |p, |g-ray
 65CU3c  multipolarities, and absolute |g-ray emission probabilities based on
 65CU4c  %I|b(g.s.)=57 taken from 1949Si21
 65CU c  1960Ri06: measured E|g, I|g, |g(t) with a NaI(Tl) detector at the
 65CU2c  Instituut voor Kernphysisch Onderzoek in Amsterdam. Deduced parent
 65CU3c  T{-1/2}, relative |g-ray emission probabilities
 65CU c  Others: 1949Si21, 1958Ha11, 1962Ba27, 1964Ma05, 1972RaZN
 65CU c  The decay scheme is considered fairly complete by the evaluator.
 65CU cB IB$From |g+ce intensity imbalance at each level for excited levels
 65CU cG E$From 1973Ra10, except as noted.
 65CU cG RI$Relative intensity from 1987Ju05, unless otherwise noted. For
 65CU2cG values from 1972Co31, no uncertainty is given by the authors and
 65CU3cG the quoted uncertainties are estimated by the evaluator based on those
 65CU4cG for absolute intensities as listed in Table I of 1972Co31
 65CU cG M,MR$From Adopted Gammas. Supporting arguments and values from this
 65CU2cG data are given under comments where available
 65CU dG MR$note that the following |d values from the previous evaluation
 65CU2dG (2010Br10) as quoted from analysis of |g|g(|q) data of 1965Sp07,
 65CU3dG can be traced back to 1986Wa02 update of A=65 and are likely deduced
 65CU4dG by the evaluator of 1986Wa02 from A{-2} and A{-4} in 1965Sp07 using
 65CU5dG the DELTA code for calculating mixing ratio from measured A{-2} and
 65CU6dG A{-4} of |g|g(|q):
 65CU7dG |d=-0.031 {I5} or +9.4 {I5} for 366|g; |d=-2.8 {I3} or +0.20 {I4} for
 65CU8dG 508|g; |d=-0.08 {I5} or +4.8 {I+26-13} for 610|g
 65CU cL E$From a least-squares fit to |g-ray energies
 65CU cL J,T$From Adopted Levels. Supporting arguments for J|p from this dataset
 65CU2cL are given under comments where available
 65NI  P 0           5/2-              2.5175 H  5               2137.9   7
 65NI cP J,T$From Adopted Levels.
 65NI cP QP$From 2021Wa16
 65CU  N 0.2359    14          1.0       1.0
 65CU cN NR$From absolute %I|g(1482)=23.59 {I14}, determined using 4|p|b|g-coin
 65CU2cN (1987Ju05). Other: 21.95 {I28} (1990Lo03), 23.5 {I8} (1971Me14), 25.0
 65CU3cN {I20} (1963Cl06), 24 (1964Fr04). Note that the value in 1990Lo03
 65CU4cN is lower than values from other studies. 1990Lo03 mention this
 65CU5cN discrepancy but state that it cannot be resolved in their work. The
 65CU6cN evaluator has adopted the value from 1987Ju05 which agrees with most
 65CU7cN of other studies.
 65CU PN                                                                     4
 65CU  L 0           3/2-
 65CU  B             59.19   19          6.595   2
 65CUS B EAV=874.03 33
 65CU cB E$measured value: 2140 {I10} from 1964Fr04 with %I|b=58 {I5}
 65CU cB IB$from 100-|S%I(|b to excited level). Other: 58 {I5} from measured
 65CU2cB |b intensity compared to the measured total number of decays (1964Fr04)
 65CU  L 770.63    13 1/2-             101 FS    6
 65CU  G 770.6     2 0.395   16 M1+E2    0.099   6
 65CU2 G %IG=0.093 4
 65CUS G  CC=0.000384 5$KC=0.000345 5$LC=3.41E-5 5$MC=4.80E-6 7
 65CUS G  NC=1.470E-7 21
 65CU cG E$others: 770.7 {I3} (1972Pa30), 771.0 {I10} (1972Co31), 770 {I10}
 65CU2cG (1963Cl06)
 65CU cG RI$weighted average of 0.439 {I30} (1987Ju05), 0.44 {I4} (1990Lo03),
 65CU2cG 0.380 {I16} (1973Ra10), 0.3 {I1} (1963Cl06), 0.3 {I1} (1972Co31).
 65CU3cG Others: 0.28 {I3} (1972Pa30) (outlier), |?0.3 (1960Ja16), <0.13
 65CU4cG (1964Fr04)
 65CU  L 1115.55   3  5/2-             0.285 PS  11
 65CU cL J$5/2- from |b|g(CP) in 1969Be28; spin=5/2 from |g|g(|q) in 1960Ja16,
 65CU2cL 1963Cl06, 1965Sp07
 65CU  B             10.32   9           6.072   5
 65CUS B EAV=371.26 30
 65CU cB E$measured value: 1020 {I25} from 1964Fr04 with %I|b=11 {I3}
 65CU  G 344.9       0.0040  4                                                 ?
 65CU2 G %IG=9.4E-4 10
 65CU cG E,RI$tentatively placed in 1973Ra10 only
 65CU  G 1115.53   4 65.8    2 M1+E2     -0.34   5                           C
 65CU2 G %IG=15.52 11
 65CUS G  CC=0.0001833 27$KC=0.0001639 24$LC=1.615E-5 24$MC=2.271E-6 33
 65CUS G  NC=6.97E-8 10$IPC=9.61E-7 18
 65CU cG E$others: 1115.5 {I1} (1972Pa30), 1115.4 {I3} (1972Co31), 1114 {I3}
 65CU2cG (1963Cl06), 1117 {I2} (1965Sp07), 1115 {I5} (1964Fr04)
 65CU cG RI$weighted average of 65.4 {I4} (1987Ju05), 66.0 {I2} (1990Lo03),
 65CU2cG 64.4 {I16} (1973Ra10), 60.0 {I25} (1972Pa30), 63 {I3} (1963Cl06), 63
 65CU3cG {I5} with Ge(Li) and 58 {I5} with NaI(Tl) (1965Sp07), 63 {I7}
 65CU4cG (1972Co31). Others: 64 (1960Ri06), 48 (1960Ja16), 71 (1964Fr04)
 65CU cG MR$value from this dataset: -0.4 {I+2-1} from measured |g(|q)
 65CU2cG anisotropy from oriented nuclei (1976Kr09)
 65CU cG $|b|g(CP) data, asymmetry A=0.23 {I4} (1968At03) and A=0.292
 65CU2cG {I37} (1969Be28) consistent with a 5/2-(|b{+-})5/2-(|g)3/2- cascade.
 65CU  L 1481.83   4  7/2-             0.45 PS   +11-9
 65CU cL J$spin=7/2 from |g|g(|q) in 1960Ja16, 1965Sp07
 65CU  B             28.36   17          4.919   5
 65CUS B EAV=220.22 28
 65CU cB E$measured value: 650 {I30} from 1964Fr04 with %I|b=30 {I5}
 65CU  G 366.27    3 20.15   15 M1+E2    -0.03   1     2.02E-3 3             C
 65CU2 G %IG=4.75 5
 65CUS G  KC=0.001810 25$LC=0.0001812 25$MC=2.55E-5 4
 65CUS G  NC=7.74E-7 11
 65CU cG E$others: 366.3 {I1} (1972Pa30), 366.4 {I3} (1972Co31), 365 {I5}
 65CU2cG (1963Cl06), 366 {I1} (1965Sp07), 370 {I5} (1964Fr04)
 65CU cG RI$weighted average of 20.37 {I22} (1987Ju05), 20.15 {I14} (1990Lo03),
 65CU2cG 20.2 {I6} (1973Ra10), 18.6 {I8} (1972Pa30), 18 {I1} (1963Cl06), 21
 65CU3cG {I2} (1960Ri06), 12 {I5} with Ge(Li) and 17 {I5} with NaI(Tl)
 65CU4cG (1965Sp07), 19 {I3} (1972Co31). Others: 19 (1960Ja16), 19 (1964Fr04)
 65CU cG MR$value from this dataset: -0.033 {I30} from measured |g(|q)
 65CU2cG anisotropy from oriented nuclei (1976Kr09)
 65CU dG MR$note that the previous evaluation quote |d=-0.031 {I5} or +9.4 {I5}
 65CU2dG from analysis of |g|g(|q) data of 1965Sp07, but it is unclear where
 65CU3dG and how those values are obtained since they are not reported in
 65CU4dG 1965Sp07
 65CU cG $366|g-1116|g(|q): A{-2}=+0.189 {I5}, A{-4}=+0.013 {I8} (1963Cl06);
 65CU2cG A{-2}=+0.172 {I6}, A{-4}=+0.013 {I10} (1965Sp07)
 65CU  G 710       10 0.024  LT                                                ?
 65CU2 G %IG LT 0.0057
 65CU cG E,RI$from 1963Cl06 only
 65CU  G 1481.84   5 100       E2
 65CU2 G %IG=24
 65CUS G  CC=0.0001922 27$KC=0.0001008 14$LC=9.92E-6 14$MC=1.395E-6 20
 65CUS G  NC=4.27E-8 6$IPC=8.00E-5 11
 65CU cG E$others: 1481.9 {I1} (1972Pa30), 1481.7 {I3} (1972Co31), 1480 {I5}
 65CU2cG (1963Cl06), 1483 {I3} (1965Sp07), 1480 {I5} (1964Fr04)
 65CU  L 1623.44   5 5/2-              0.86 PS   +31-20
 65CU cL J$spin=3/2,5/2 from |g|g(|q) in 1965Sp07
 65CU  B             0.854   10          6.06    1
 65CUS B EAV=165.51 26
 65CU  G 507.9     1 1.216   10 M1+E2    +0.20   3                           C
 65CU2 G %IG=0.2869 29
 65CUS G  CC=0.000980 17$KC=0.000880 15$LC=8.76E-5 15$MC=1.232E-5 21
 65CUS G  NC=3.75E-7 6
 65CU cG E$from 1972Pa30. Others: 507.8 {I2} (1973Ra10), 507.8 {I6} (1972Co31),
 65CU2cG 509 {I7} (1963Cl06), 508 {I10} (1965Sp07), 510 {I5} (1964Fr04).
 65CU cG RI$weighted average of 1.240 {I19} (1987Ju05), 1.21 {I1} (1990Lo03),
 65CU2cG 1.28 {I8} (1973Ra10), 1.15 {I5} (1972Pa30), 1.5 {I2} (1963Cl06), 1.9
 65CU3cG {I5} with NaI(Tl) (1965Sp07), 1.1 {I3} (1972Co31). Others: 0.5
 65CU4cG (1960Ja16), 1.5 (1964Fr04)
 65CU cG $507|g-1116|g(|q): A{-2}=-0.200 {I35}, A{-4}=-0.013 {I57} (1965Sp07).
 65CU cG MR$-2.8 {I2} or +0.20 {I3} reported in 1976Kr09, from re-analysis of
 65CU2cG |g|g(|q) data of 1965Sp07. |g(|q) anisotropy from 1976Kr09 favors
 65CU3cG +0.20 {I3}, which is adopted in Adopted Gammas
 65CU  G 852.7     2 0.331   20
 65CU2 G %IG=0.078 5
 65CU cG E$others: 852.7 {I3} (1972Pa30), 852.8 {I10} (1972Co31), 855 {I10}
 65CU2cG (1963Cl06), 855 {I10} (1965Sp07)
 65CU cG RI$weighted average of 0.41 {I5} (1987Ju05), 0.40 {I5} (1990Lo03),
 65CU2cG 0.340 {I16} (1973Ra10), 0.26 {I3} (1972Pa30), 0.3 {I1} (1963Cl06),
 65CU3cG 1.0 {I5} with NaI(Tl) (1965Sp07), 0.2 {I1} (1972Co31). Others: |?0.2
 65CU4cG (1960Ja16), <0.13 (1964Fr04)
 65CU  G 1623.42   6 2.07    3  M1+E2    -0.75   +30-45
 65CU2 G %IG=0.488 8
 65CUS G  CC=0.000208 9$KC=8.07E-5 16$LC=7.92E-6 16$MC=1.114E-6 23
 65CUS G  NC=3.43E-8 7$IPC=0.000118 7
 65CU cG E$others: 1623.5 {I2} (1972Pa30), 1622.6 {I5} (1972Co31), 1625 {I10}
 65CU2cG (1963Cl06), 1625 {I3} (1965Sp07), 1620 {I10} (1964Fr04)
 65CU cG RI$weighted average of 2.11 {I6} (1987Ju05), 2.06 {I2} (1990Lo03),
 65CU2cG 2.08 {I8} (1973Ra10), 1.88 {I12} (1972Pa30), 2.8 {I4} (1963Cl06), 2.4
 65CU3cG {I2} (1960Ri06), 1.5 {I5} with Ge(Li) and 4 {I1} with NaI(Tl)
 65CU4cG (1965Sp07), 2.1 {I5} (1972Co31). Others: 3.4 (1960Ja16), 2.1 (1964Fr04)
 65CU cG M,MR$D+Q and |d from measured |g(|q) anisotropy from oriented nuclei
 65CU2cG (1976Kr09). The same value is adopted in Adopted Gammas
 65CU  L 1724.98   5  3/2-             77 FS     +17-13
 65CU cL J$spin=5/2 from |g|g(|q) in 1965Sp07 is inconsistent
 65CU  B             0.546   8           5.93    1
 65CUS B EAV=128.06 25
 65CU  G 609.5     1 0.674   21 [M1+E2]  0.5     LT                          C
 65CU2 G %IG=0.159 5
 65CUS G  CC=0.00067 4$KC=0.000602 33$LC=5.98E-5 34$MC=8.4E-6 5
 65CUS G  NC=2.56E-7 14
 65CU cG E$1972Pa30. Others: 609.3 {I2} (1973Ra10), 609.8 {I5} (1972Co31), 611
 65CU2cG {I7} (1963Cl06), 608 {I10} (1965Sp07), 610 {I5} (1964Fr04).
 65CU cG RI$weighted average of 0.655 {I17} (1987Ju05), 0.73 {I2} (1990Lo03),
 65CU2cG 0.624 {I36} (1973Ra10), 0.57 {I5} (1972Pa30), 1.0 {I2} (1963Cl06), 0.6
 65CU3cG {I3} with NaI(Tl) (1965Sp07), 0.6 {I2} (1972Co31). Others: 0.2
 65CU4cG (1960Ja16), 0.9 (1964Fr04)
 65CU cG $610|g-1116|g(|q): A{-2}=0.209 {I69}, A{-4}=-0.160 {I111} (1965Sp07).
 65CU dG MR$note that the previous evaluation quote |d=-0.08 {I5} or +4.9
 65CU2dG {+26-13} from analysis of |g|g(|q) data of 1965Sp07, but it is unclear
 65CU3dG where and how those values are obtained since they are not reported in
 65CU4dG 1965Sp07.
 65CU  G 954.5     3 0.015   LT
 65CU2 G %IG LT 0.0035
 65CU cG E$others: 954.5 (1990Lo03), 960 (1963Cl06), 950 (1960Ja16)
 65CU cG RI$others: 0.040 {I4} (1973Ra10), <0.024 (1963Cl06), |?0.1 (1960Ja16)
 65CU  G 1724.92   6 1.63    1 M1+E2     0.32    5
 65CU2 G %IG=0.3845 33
 65CUS G  CC=0.0002269 34$KC=7.092E-5 99$LC=6.96E-6 10$MC=9.79E-7 14
 65CUS G  NC=3.01E-8 4$IPC=0.0001480 23
 65CU cG M,MR$D+Q and |d=-0.15 {I+31-35} or <-4.6 or >+2.3 from measured |g(|q)
 65CU2cG anisotropy from oriented nuclei (1976Kr09). Adopted in Adopted Gammas
 65CU cG E$others: 1725.0 {I2} (1972Pa30), 1725.2 {I5} (1972Co31), 1724 {I10}
 65CU2cG (1963Cl06), 1725 {I3} (1965Sp07), 1720 {I10} (1964Fr04)
 65CU cG RI$weighted average of 1.69 {I5} (1987Ju05), 1.62 {I1} (1990Lo03), 1.68
 65CU2cG {I8} (1973Ra10), 1.61 {I10} (1972Pa30), 1.8 {I2} (1963Cl06), 2.2 {I2}
 65CU3cG (1960Ri06), 1.4 {I5} with Ge(Li) and 2.5 {I5} with NaI(Tl) (1965Sp07),
 65CU4cG 1.7 {I5} (1972Co31). Others: 2.1 (1960Ja16), 1.9 (1964Fr04)