ADOPTED LEVELS for 103Sr
Author: Balraj Singh | Citation: ENSDF | Cutoff date: 31-MAY-2015
Author: D. De Frenne | Citation: Nucl. Data Sheets 110, 2081 (2009) | Cutoff date: 1-Mar-2009
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=11040 keV SY | S(n)= 3140 keV SY | S(p)= 17000 keV SY | Q(α)= -11090 keV SY | ||
Reference: 2012WA38 |
E(level) (keV) | T1/2(level) |
0 | 53 ms 10 % β- = 100 % β-n = ? % β-2n = ? |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0 | 53 ms 10 % β- = 100 % β-n = ? % β-2n = ? | Theoretical %β-n=2.2, %β-2n=0.01 (1997Mo25). |
1997Be70, 1995CzZZ: 103Sr produced by Pb(238U,F), E=750 MeV/nucleon, identification by time-of-flight.
2011Ni01: 103Sr nuclide produced in Be(238U,F) reactions at E=345 MeV/nucleon produced by the cascade operation of the RBIF-RIKEN accelerator complex. Target=550 mg/cm2. Identification of 105Sr made on the basis of magnetic rigidity, time-of-flight and energy loss. The separated nuclei were implanted in a nine-layer double-sided silicon-strip detector (DSSSD). Correlations were recorded between the heavy ions and β rays. The half-life of 103Sr isotope was measured from the correlated ion-β decay curves and maximum likelihood analysis technique. In the analysis of the decay curve, β-detection efficiency, background rate, daughter and granddaughter (including those populated in delayed neutron decays) half-lives, and β-delayed neutron emission probabilities were considered. Comparison of measured half-lives with FRDM+QRPA and KTUY+GT2 calculations
2015Lo04: 103Sr 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 103Sr 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 103Sr 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
Theoretical calculations:
2013Fa05: calculated half-lives, delayed neutron emission probabilities
2010Ro27: calculated one-quasineutron levels, J, π
Q-value: Estimated uncertainties (2012Wa38): 200 for Q(β-), 210 for S(n), 360 for S(p), 540 for Q(α)
Q-value: S(2n)=8000 210, S(2p)=32870 540, Q(β-n)=5680 200 (syst,2012Wa38).