ADOPTED LEVELS for 165Sm
Authors: Balraj Singh and Jun Chen | Citation: Nucl. Data Sheets 194, 460 (2024) | Cutoff date: 31-Oct-2022
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=7220 keV SY | S(n)= 3660 keV SY | S(p)= 12440 keV SY | Q(α)= -3710 keV SY | ||
Reference: 2021WA16 |
E(level) (keV) | T1/2(level) |
0 | 0.98 s 21 % β- = 100 % β-n = ? |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0 | 0.98 s 21 % β- = 100 % β-n = ? | Production σ (at 1 GeV/nucleon)=7.8 nb 16 (2012Ku26). |
2017Wu04: 165Sm was produced in 9Be(238U,F), E(238U)=345 MeV/nucleon reaction, followed by separation of fragments based on Bρ-ΔE-tof method using the BigRIPS separator at RIBF-RIKEN facility, optimized for the transmission of 158Nd and 170Dy ions. The reaction products were transported through the ZeroDegree spectrometer and implanted into the decay counting system WAS3ABi, surrounded by the EURICA array of 84 HPGe detectors for γ detection. Typical implantation rate was ≈100 ions/s. Measured time distribution of (implanted ion)β-, (implanted ion)β-γ and (implanted ions)γ correlated events, and half-life of decay of 165Sm g.s.
2012Ku26: 165Sm was produced and identified in 9Be(238U,F), E=1 GeV/nucleon reaction using SIS-18 synchrotron facility at GSI. Target was 1.6 g/cm2 9Be placed at the entrance of projectile Fragment Separator (FRS). Particle identification was achieved by event-by-event in-flight analysis of time-of-flight, energy loss measurement, and magnetic rigidity (tof-ΔE’-Bρ). Time-of-flight measured using two plastic scintillation detectors, energy loss or deposit by ionization chambers (MUSIC), and magnetic rigidity by four time-projection chambers (TPC), which also provided energy deposit information. Isomer tagging method for known μs isomers was used to verify event-by-event identification and in-flight separation of new isotopes. Gamma rays from the known isomers were recorded in coincidence with the incoming ions using either the RISING array of Ge detectors at GSI or only two Ge detectors, a stopper foil and a scintillator for veto signal. Measured production cross section. Comparison of measured σ with predictions from ABRABLA model and EPAX-3 model
Q-value: Estimated uncertainties (2021Wa16): ΔQ(β-)=ΔS(n)=400, ΔS(p)=ΔS(α)=570
Q-value: S(2n)=9050 400, S(2p)=24010 640, Q(β-n)=1650 400 (syst, 2021Wa16).