ADOPTED LEVELS for 124Ru
Author: Balraj Singh | Citation: ENSDF | Cutoff date: 20-JUL-2015
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=10750 keV SY | S(n)= 5130 keV SY | S(p)= 19140 keV CA | Q(α)= -13040 keV CA | ||
Reference: 2012WA38,1997MO25 |
E(level) (keV) | Jπ(level) | T1/2(level) |
0 | 0+ | 15 ms 3 % β- = 100 % β-n = ? % β-2n = ? |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0 | 0+ | 15 ms 3 % β- = 100 % β-n = ? % β-2n = ? | Measured σ=0.6 pb (2010Oh02), systematic uncertainty≈40%. Probability of misidentification of 124Ru isotope<0.001% (2010Oh02). |
2010Oh02: 124Ru nuclide identified in Be(238U,F) and Pb(238U,F) reactions with a 238U86+ beam energy of 345 MeV/nucleon produced by the cascade operation of the RBIF accelerator complex of the linear accelerator RILAC and four cyclotrons RRC, fRC, IRC and SRC. Identification of 124Ru nuclei was made on the basis of magnetic rigidity, time-of-flight and energy loss of the fragments using BigRIPS fragment separator. Experiments performed at RIKEN facility. Based on α/Q spectrum and Z versus α/Q plot, one count was assigned to 124Ru isotope. (Q=charge state)
2015Lo04: 124Ru nuclide produced at RIBF-RIKEN facility in 9Be(238U,F) reaction at E=345 MeV/nucleon with an average intensity of 6×1010 ions/s. Identification of 124Ru was made by determining atomic Z and mass-to-charge ratio α/Q, where Q=charge state of the ions. The selectivity of ions was based on magnetic rigidity, time-of-flight and energy loss. The separated nuclei were implanted at a rate of 50 ions/s in a stack of eight double-sided silicon-strip detector (WAS3ABi), surrounded by EURICA array of 84 HPGe detectors. Correlations were recorded between the implanted ions and β rays. The half-life of 124Ru isotope was measured from the correlated ion-β decay curves and maximum likelihood analysis technique as described in 2014Xu07. Comparison of measured half-lives with FRDM+QRPA, KTUY+GT2 and DF3+CQRPA theoretical calculations
2013Fa08: theoretical calculations of T1/2 and %β-n
2010No01: calculated potential energy surface, levels, S(2n), B(E2)
Q-value: Estimated uncertainties (2012Wa38): 720 for Q(β-), 780 for S(n)
Q-value: Q(β-) and S(n) from 2012Wa38; S(p) and Q(α) from theory (1997Mo25)
Q-value: S(2n)=8150 780, Q(β-n)=7020 720. S(2p)=35040 (1997Mo25,theory)