ADOPTED LEVELS for 104Y
Author: Balraj Singh | Citation: ENSDF | Cutoff date: 10-JUN-2015
Author: Jean Blachot | Citation: Nucl. Data Sheets 108,2035 (2007) | Cutoff date: 30-Mar-2007
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=11670 keV SY | S(n)= 3680 keV SY | S(p)= 13930 keV SY | Q(α)= -9940 keV SY | ||
Reference: 2012WA38 |
E(level) (keV) | T1/2(level) |
0 | 197 ms 4 % β- = 100 % β-2n = ? % β-n = 34 10 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0 | 197 ms 4 % β- = 100 % β-2n = ? % β-n = 34 10 | Theoretical %β-n=3.80, %β-2n=0 (2003Mo09). |
1994Be24, 1998Do08: 104Y produced and identified in Pb(238U,F), E=750 MeV/nucleon reaction, followed by residue separation at at GSI facility and time-of-flight measurement
1999Wa09: IGISOL on-line mass separator facility from 238U(p,F),E=25 MeV and a high efficiency neutron detector and a careful examination of contaminants by γ spectrometry, measured half-life from decay curve for delayed neutrons
2009Pe06: 104Y formed by fragmentation of 136Xe beam at 120 MeV/nucleon at NSCL facility using Coupled Cyclotrons and A1900 fragment separator. The time-of-flight and transversal positions of each particle was measured using two plastic scintillators. The energy loss in a Si PIN detector was measured which, when combined with time-of-flight (tof) and transversal position measurements, allowed for an event-by-event identification of the transmitted nuclei. Transmitted nuclei and their β decays were measured using the β counting system consisting of four Si PIN detectors and a double-sided Si strip detector. β-delayed neutrons were measured in coincidence with β-decay precursor using neutron emission ratio observer (NERO) detector consisting of 60 proportional gas counter tubes embedded in polyethylene moderator matrix. The γ rays were measured with SeGA Ge detectors. Measured isotopic half-lives and delayed neutron emission probabilities Isotopic half-life was measured by 2009Pe06 from least-squares fit and maximum likelihood method of time differences of implantations and correlated β decay events.
2011Ni01: 104Y nuclide produced in Be(238U,F) reactions at E=345 MeV/nucleon produced by the cascade operation of the RBIF complex of accelerators at RIKEN. Target=550 mg/cm2. Identification of 104Y 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 104Y 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: 104Y 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 104Y 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 104Y 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
2013Fa05: calculated half-life, delayed neutron emission probability
Q-value: Estimated uncertainties (2012Wa38): 400 for Q(β-), S(n); 450 for S(p) and Q(α)
Q-value: S(2n)=9030 400, S(2p)=30940 500, Q(β-n)=5690 400 (syst,2012Wa38)