60MN 60MN IT DECAY:1.0 US 2009FO05 13NDS 201312
60MN H TYP=FUL$AUT=E. BROWNE, J. K. TULI$CIT=NDS 114, 1849 (2013)$
60MN2 H CUT=31-Dec-2012$
60MN c {+60}Mn produced through the {+9}Be({+238}U,X) reaction. {+238}U
60MN2c beam produced at E=8.00 MeV/nucleon by the K500 and K1200
60MN3c cyclotrons at the National Superconducting Laboratory at Michigan
60MN4c State University. Reaction products were separated using the A1900
60MN5c fragment separator and detected using two parallel plate avalanche
60MN6c counters, a Si |DE detector, four Si detectors, and a plastic
60MN7c scintillator. Measurements of the time-of-flight (tof), B|r and total
60MN8c kinetic energy were used to determine the atomic number, mass number
60MN9c and charge state of reaction products. The |g's were detected with one
60MNAc HPGe detector. Half-lives were measured using the time difference
60MNBc between implantation events and HPGe events, which was not suitable
60MNCc for measuring half-lives of less than 500 ns. Measured particle
60MNDc spectra, E|g, I|g, (particle)|g-coincidence and half-lives of
60MNEc isomeric states.
60MN c Isomer with half-life of 1.0 |ms {I+3-2} discovered but with an
60MN2c uncertain level scheme
60MN cG RI$ Photons per 100 fragments.
60MN P 114 1.0 US +3-2
60MN N 1 1 1
60MN dN NR$listed |g-ray intensity is per 100 fragments
60MN PN 3
60MN L 0 1+
60MN cL J$ from Adopted Levels, Gammas.
60MN L 114.0 7 (3+) 1.0 US +3-2 M ?
60MN cL E$ placement of 114|g and isomer energy are uncertain.
60MN2cL Level has not been included in Adopted Levels, Gammas.
60MN cL J$ from shell-model predictions
60MN cL T$ Measured in 2009Fo05 from time correlations between implanted
60MN2cL {+60}Mn nuclei and |g-ray events.
60MN G 114.0 7 100 ?