DETECTION OF TITANIUM IN ELECTROTHERMAL ATOMIZERS BY LASER-INDUCED FLUORESCENCE .2. INVESTIGATION OF VARIOUS TYPES OF ATOMIZERS

Citation
P. Ljung et al., DETECTION OF TITANIUM IN ELECTROTHERMAL ATOMIZERS BY LASER-INDUCED FLUORESCENCE .2. INVESTIGATION OF VARIOUS TYPES OF ATOMIZERS, Spectrochimica acta, Part B: Atomic spectroscopy, 52(6), 1997, pp. 703-716
Citations number
57
Categorie Soggetti
Spectroscopy
ISSN journal
05848547
Volume
52
Issue
6
Year of publication
1997
Pages
703 - 716
Database
ISI
SICI code
0584-8547(1997)52:6<703:DOTIEA>2.0.ZU;2-C
Abstract
Different types of electrothermal atomizers (graphite and tungsten fur naces) have been studied for the determination of Ti by laser-induced fluorescence (LIF). It was found that all graphite furnaces suffer fro m both bulk contamination by Ti, corresponding to tens of pg per firin g, and significant memory effects in such a way that the high sensitiv ity of the LIF technique could not be fully utilized. The detectabilit y of Ti by the LIF technique was limited by fluctuations of the atomiz er blank signals and therefore depended mainly on the Ti history of th e furnaces. The detection limit of Ti was found to be similar for all graphite furnaces: around 1 pg for furnaces not exposed to any substan tial amounts of Ti, and a few pg for those which had been exposed to a few hundreds of pg of Ti (or more). It was found that the transversel y heated graphite atomizer (THGA) from Perkin-Elmer gives the most rep roducible atomization of Ti. The tungsten furnace showed no memory eff ects and therefore no empty firings (bum-outs) between determinations are needed. The tungsten furnace, however, afforded significantly weak er signals (approximately 250-fold) than the graphite furnaces; this w as attributed to incomplete atomization processes. The Ti signal from the tungsten furnace could be increased by the addition of H-2 in the buffer gas. For 20% of H-2 added, however, the analyte signal was stil l weaker by a factor of 8 than that seen in a graphite furnace shielde d with Ar (the remaining difference is primarily attributed to fluores cence quenching from H-2) In addition, the precision of the measuremen ts was poorer than that obtained from graphite furnaces. (C) 1997 Else vier Science B.V.