59CO 59NI EC DECAY 1991JA02,2015PF02 18NDS 201808
59CO H TYP=FUL$AUT=M. Shamsuzzoha Basunia$CIT=NDS 151, 1 (2018)$
59CO2 H CUT=1-Apr-2018$
59CO C Others: 1951BR05, 1951WI14, 1956SA32, 1963SC06, 1974CH06, 1976BE02.
59CO C 1991Ja02: 59NI activity was prepared by neutron irradiation of 188 mg
59CO2C Ni metal enriched to 99.927% in 58NI for 167 days at a neutron flux of
59CO3C 1.3 |* 10{+14} cm{+-2} s{+-1}. After chemical separation from
59CO4C contaminant activities, 10 mm diameter pellets were prepared. ^K
59CO5C x-rays were measured with a Si(Li) detector. Also internal
59CO6C bremsstrahlung in coincidence with ^K x-ray was measured using Si(Li)
59CO7C detector and a proportional counter.
59CO C 2015Pf02: Re-analysis of |g spectrum coincident with cobalt K x-rays
59CO2c observed in the decay of {+59}Ni from 1991Ja02. The high energy side,
59CO3c E|g > 600 keV, cannot be reproduced with a radiative electron capture
59CO4c calculation. A considerably better description is obtained when
59CO5c a virtual |b- transition to the 1099 keV level is introduced.
59CO CE For studies of internal bremsstrahlung spectrum,
59CO2CE see 1956SA32, 1963SC06, 1976BE02, 1991JA02.
59CO CL J From Adopted Levels.
59CO N 1.0 1.0 1.0
59NI P 0.0 3/2- 7.6E+4 Y 5 1073.00 19
59CO L 0.0 7/2-
59CO E 3.7E-5 1299.99696 1 11.89 3 99.997 3
59COS E EAV=24.69 27$CK=0.8872$CL=0.09607$CM+=0.01672
59CO CE IB %IB+=3.7E-5 12 from I(B+)/I(ECK)=4.2E-7 13 (1991JA02),
59CO2CE assuming CK/EC=0.887. Other: I(B+)/I(EC)=1.5E-7 (1976BE02). Note that
59CO3CE allowed |b decay theory gives %IB+=0.00152 9, AP 2 orders of magnitude
59CO4CE larger than experiment.
59CO CE IE 99.997 - %IB+.
59CO CE ECL/ECK=0.121 2 (1974CH06).
59CO L 1099.256 3 3/2-
59CO cL E$The energy of this level exceeds the decay Q(|b{+-})value.
59CO2cL From re-analysis of |g spectrum coincident with cobalt K x-rays
59CO2cL observed in the decay of {+59}Ni in 1991Ja02, 2015Pf02 propose the
59CO3CL population through virtual or 'detour' transitions.
59CO E 3.41E-3 AP 0.00341 AP
59CO cE IE$The energy of this level exceeds the decay Q(|b{+-})value,
59CO2cE therefore it can be populated only through virtual or 'detour'
59CO3cE transitions. From the statement that the virtual and interference
59CO4cE of 2% and 2.3%, respectively, of
59CO5cE the integrated radiative electron capture gamma spectrum above
59CO6cE 195 keV, a branching ratio of 3.41|*10{+-3} per 100 decays
59CO7cE of {+59}Ni is deduced in 2015Pf02.