A. Quentmeier et al., Measurement of uranium isotope ratios in solid samples using laser ablation and diode laser-atomic absorption spectrometry, SPECT ACT B, 56(1), 2001, pp. 45-55
A diode laser was used for the selective detection of U-235 and U-238 in a
laser-induced plasma ignited by a Nd:YAG laser beam focused onto uranium ox
ide samples. The diode laser was sequentially tuned to the absorption lines
of both isotopes (682.6736 nm for U-235, and 682.6913 nm for U-238). The a
bsorption was measured on a pulse-to-pulse basis; the transient absorption
peak was used as an analytical signal. Three samples were used with the rel
ative abundance of the minor isotope U-235 of 0.204%, 0.407% and 0.714%. Op
timal conditions for the detection of the minor isotope were obtained at a
distance of similar to 3 mm from the sample surface, an argon pressure of s
imilar to 3 kPa and for 7.5 mJ pulse energy of the Nd:YAG laser. Absorption
in the wing of the broadened line of the U-238 isotope was found to be the
main source of background for the measurement of the absorption of the min
or isotope. The limit of detection of the minor isotope, evaluated on the b
asis of the 3 sigma criteria was estimated to be 100 mug g(-1). At the opti
mal conditions for the detection of the minor isotope optical thick conditi
ons in the line centre of the main isotope were observed. Therefore, the is
otope ratio measurements were performed by rationing the intensity of the n
et absorption signal measured in the line centre of the minor isotope and t
he absorption signal measured in the wing of the main isotope. This strateg
y was checked by determination of the isotope ratios for the two samples wi
th depleted U-235 concentration using the sample with the natural isotope c
omposition (0.714%) as a standard. The accuracy and precision for this meas
urement strategy was evaluated to approximately 10%. (C) 2001 Elsevier Scie
nce B.V. All rights reserved.