101SN 105TE A DECAY (0.62 US) 2006LI41,2006SE08 ENSDF 200710
101SN H TYP=ERR$AUT=J. Tuli$DAT=14-Dec-2007$COM=Fixed typos noted by PNPI group
101SN H TYP=FUL$AUT=BALRAJ SINGH$CUT=15-OCT-2007$CIT=ENSDF$
101SN c 2006Li41: {+105}Te produced in |a decay chain of {+109}Xe.
101SN2c {+109}Xe was produced and identified in {+54}Fe({+58}Ni,3n) reaction
101SN3c at E({+58}Ni)=220,225 MeV in a fusion-evaporation reaction, followed
101SN4c by mass separation of A=109 products were using Recoil Mass
101SN5c Spectrometer at the Holifield Radioactive Ion Beam facility.
101SN6c The fragments were separated according to the ratio of atomic mass
101SN7c and ionic charge. The separated ion beam passed through the mylar
101SN8c film of a microchannel plate counter and then implanted into
101SN9c (at an energy of |?60 MeV) into a double-sided silicon strip detector
101SNAc (DSSD). Sequence of |a-|a decay events with a certain time selection
101SNBc with the implanted events were recorded, from which {+109}Xe was
101SNCc unambiguously identified. Measured isotopic half-life, E|a, I|a.
101SN c 2006Se08: {+105}Te isotope produced and identified in
101SN2c {+50}Cr({+58}Ni,3n) reaction at E=2224, 214 and 204 MeV. The reaction
101SN3c products were separated from the beam according to mass/charge ratio in
101SN4c the Fragment Mass Analyzer (FMA) at Argonne. The recoils were implanted
101SN5c in a double-sided Si strip detector (DSSD). Measured |a decay
101SN6c spectrum and isotopic half-life. A total of 13 counts were observed in
101SN7c the |a spectrum from A=105 just above 4500 keV. The corresponding
101SN8c cross section is |? 10 nb for beam energies of 204 and 214 MeV. No
101SN9c events were seen for beam energy of 224 MeV.
105TE P 0.0 (5/2+) 0.62 US 7 4889 6
105TE cP T$ from 2006Li41. Other: 0.70 |ms {I+25-17} (2006Se08) from 13 events
105TE2cP in |a spectrum
105TE cP QP$ deduced from E|a=4703 {I5} (2006Li41). Other: 4900 {I50} from
105TE2cP E|a=4720 {I50} (2006Se08). 2003Au03 give 4640 {I590} from systematics
101SN N 1 AP
101SN cN BR$ |a decay branching is not known, 2006Se08 assumed 100% |a branch
101SN2cN in the calculation of reduced |a decay width
101SN L 0 (5/2+)
101SN cL J$ from 'adopted levels'
101SN A 4703 5 100 AP
101SN cA E$ from 2006Li41. Other: 4720 {I50} (2006Se08)
101SN cA $Reduced |a-decay width: |d{+2}/(|d{+2} for {+212}Po)=2.0 {I3}
101SN2cA (2006Li41)
101SN cA $ Assuming 100% |a branch for {+105}Te, reduced width
101SN2cA |d{+2}=0.23 MeV {+10-14} (2006Se08)