ADOPTED LEVELS for 211Tl
Author: Balraj Singh | Citation: Nucl. Data Sheets 114, 661 (2013) | Cutoff date: 28-FEB-2013
Full ENSDF file | Adopted Levels (PDF version)
| Q(β-)=4410 keV 40 | S(n)= 4900 keV 40 | S(p)= 8000 keV SY | Q(α)= 2300 keV SY | ||
| Reference: 2012WA38 |
| E(level) (keV) | T1/2(level) |
| 0 | 88 s +46-29 % β- = 100 % β-n = ? |
Additional Level Data and Comments:
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 0 | 88 s +46-29 % β- = 100 % β-n = ? | Production cross section measured in 2010Al24, values are given in figure 2, plot of σ versus mass number for Tl isotopes. Statistical uncertainty=10%, systematic uncertainty=20%. Production σ=82 nb (from e-mail reply of Oct 29, 2010 from H. Alvarez-Pol, which also stated that further analysis was in progress. From α/Z plot (figure 1 in 2010Al24), a large number of events is assigned to 211Tl. |
211Tl evaluated by B. Singh
1998Pf02: 211Tl was produced by fragmentation of a 1-GeV/nucleon 238U beam on a beryllium target. Isotope was identified by a measurement of mass-to-charge ratio.
2010Al24: 211Tl nuclide identified in 9Be(238U,X) reaction with a beam energy of 1 GeV/nucleon produced by the SIS synchrotron at GSI facility. Target=2500 mg/cm2. The fragment residues were analyzed with the high resolving power magnetic spectrometer fragment separator (FRS). The identification of nuclei was made on the basis of magnetic rigidity, velocity, time-of-flight, energy loss and atomic number of the fragments using two plastic scintillators and two multisampling ionization chambers. The FRS magnet was tuned to center on 210Au, 216Pb, 219Pb, 227At and 229At nuclei along the central trajectory of FRS.
Unambiguous identification of nuclides required the separation of different charge states of the nuclei passing through the FRS. At 1 GeV/nucleon incident energy of 238U, fraction of fully stripped 226Po nuclei was about 89%. Through the measurement of difference in magnetic rigidity in the two sections of the FRS and the difference in energy loss in the two ionization chambers, the charge state of the transmitted nuclei was determined, especially, that of the singly charged (hydrogen-like) nuclei which preserved their charge in the current experimental setup. Measured production cross sections with 10% statistical and 20% systematic uncertainties
Criterion established in 2010Al24 for acceptance of identification of a new nuclide: 1. number of events should be compatible with the corresponding mass and atomic number located in the expected range of positions at both image planes of the FRS spectrometer; 2. number of events should be compatible with >95% probability that at least one of the counts does not correspond to a charge-state contaminant. Comparisons of measured σ with model predictions using the computer codes COFRA and EPAX.
2012Be28: see 2010Al24 above for method of production at GSI facility. In this work half-life of the isotope is measured from an implant of 3503 events
Q-value: Estimated uncertainties (2012Wa38): 200 for S(p); 300 for Q(α)
Q-value: Q(β-n)=580 40, S(2n)=8580 40, S(2p)=18190 400 (syst) (2012Wa38)