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Program - Brookhaven National Laboratory

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good timing characteristics.Examples of recent precision measurements using a combined LaBr3-HpGe<br />

array based at the tandem van de Graaff accelerator, Bucharest, Romania will be presented [1,2]. The<br />

presentation will also discuss the development of a multidetector array based on LaBr3 detectors for future<br />

studies of very exotic nuclei produced at the upcoming Facility for Anti-Proton and Ion Research (FAIR)<br />

[3]. ∗ This work is supported by grants from the Engineering and Physical Sciences Research Council<br />

(EPSRC-UK) and the Science and Technology Facilities Council (STFC-UK).<br />

[1] P.J.Mason et al., Phys. Rev. C 85, 064303 (2012) [2]T.Alharbi et al., App. Rad. Isotopes 70, 1337<br />

(2012) [3] P.H. Regan App. Rad. Isotopes 70, 1125 (2012)<br />

HD 4 4:40 PM<br />

Further Test of Internal-Conversion Theory with a Measurement in 119 Sn m<br />

N. Nica, J. C. Hardy, V. E. Iacob<br />

Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA<br />

Internal conversion is a general property of the atomic nucleus and its electronic shells, which has become of<br />

increased interest, particularly in the last decade. In order to balance decay schemes, one needs to know the<br />

internal conversion contribution to each transition as expressed by its internal conversion coefficients (ICC).<br />

For some transitions used in critical applications or basic nuclear science, very precise and accurate values<br />

of ICC’s are crucial. However, ICC’s are only rarely measured and are instead taken from calculations,<br />

so for decades people have relied on tabulated ICC’s. Unfortunately the tabulated values can differ quite<br />

significantly from calculation to calculation so precision is hard to guarantee. Thus one must seek guidance<br />

from very precisely measured ICC’s, which can distinguish among the various calculations. But in 2002,<br />

when a survey of measured ICC’s was made [1], only about 20 out of hundreds of published measured values<br />

were found with a reported precision of 2% or better, so an extended set of 100 ICC values of precision not<br />

worse than 6% was finally adopted for comparison with theories. Of particular importance for calculations<br />

is the treatment of the electronic vacancy, which is known to survive long enough after the electronic<br />

conversion takes place that it should really be taken into account in determining the potential seen by<br />

the outgoing conversion electron. However the 2002 survey showed better agreement with calculations<br />

that ignored the electronic vacancy and, as a result, the most recent published tables [2] were deliberately<br />

calculated without the inclusion of the vacancy. This apparent contradiction prompted us 2003 to begin a<br />

series of ICC measurements aimed at high precision ( 1%) that focuses on transitions that are particularly<br />

sensitive to the theoretic treatment of the atomic vacancy. Our method consists of measuring αK ICC’s<br />

based on the ratio of the intensity of the K x rays produced as a result of internal conversion, and<br />

the corresponding gamma-ray intensity. This is possible using an HPGe detector whose high-precision<br />

calibration of the detection efficiency has been reported in [3]. The method is suitable for radioactive<br />

sources with a single transition that converts in the K shell. We use neutron activated sources, which<br />

introduces some impurities that need to be dealt with. For energies below 50 keV there are also important<br />

contributions from the scattered radiation that contribute to the K x-rays peaks, which we characterize<br />

specifically from case to case. We use redundancy checks and simulation calculations to address these<br />

issues. With this method we have measured [4] αK’s in 134 Cs, 137 Ba, 193 Ir, and 197 Pt. Here we report on a<br />

new ICC measurement, the 65.7-keV, M4 transition in 119 Sn for which we find αK = 1604(30). This is in<br />

agreement with the calculated value that includes the vacancy (by the so-called ”frozen-orbital” method),<br />

1618, and differs from the calculated value that ignores the vacancy, 1544. The same conclusion resulted<br />

from all the cases we have measured previously, thus demonstrating that the calculations including the<br />

atomic vacancy should be used for tabulated values.<br />

[1] S. Raman et al., Phys. Rev. C bf 66 (2002) 044312. [2] I.M. Band et al., At. Data Nucl. Data Tables,<br />

122

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