Page 31 - Inorganic Mass Spectrometry : Fundamentals and Applications
P. 31

The~al Ionization Mass Spectrometry                            21


     layer of platinum over the sample. The sample atoms are thus forced to migrate
     through the platinum layer before leaving the filament. In this manner, the ad-
     vantages of using rhenium as a filament material (high melting point, ductility)
     were  retained  while  the  higher  work  function  of  platinum  was  exploited  to
     enhance ionization efficiency. A mean ionization efficiency of  0.34% for plu-
     tonium was reported; that efficiency is a substantial improvement when compared
     to analyzing samples loaded as solutions, which is generally an order of magni-
     tude lower.
          Similar  reasoning led  Smith  and  Carter  to  develop  a  method  using  an
     overlayer of pure rhenium powder slurried with a source of carbon, such as starch
     solution [19]. Rhenium and carbon do not form a stoichiometric compound, but
     carbon dissolves in the metal to form a composite surface that has higher work
     function than pure polycrystalline rhenium; this has been measured as 5.8 eV,
     about the same as the work function of platinum [Xi]. Rhenium powder, when
     heated to the operating temperatures required for many elements  (> 1SOO0C),
     sinters to  form  a  barrier  to  evaporation that  forces  analyte  atoms to  migrate
     through it before leaving the filament. Thus, in a manner similar to the platinum
     overcoat electrolytically deposited, the advantages of rhenium as a filament mate-
     rial and an emitting surface of high work function are both exploited. The higher
     work function explains in part the benefits derived from loading samples on resin
     beads; the carbon skeleton of the bead that remains after its thermal decomposition
     dissolves in the rhenium substrate, forming a local surface with a higher work
     function than that of the surrounding metal [ 171.
          It  is  not  clear  which  of  the  two  overcoating methods provides  greater
     enhancement in ionization efficiency. Smith et al. report ion collection efficiencies
     of  4%-9%  for plutonium [76], but this was for an experiment specifically de-
     signed to  evaluate  this  ability;  Perrin  et  al.  [18] were  more  concerned  with
     improving the stability of their ion beam (and hence precision) than they were
     with determining ionization efficiency. Substaritially improved ion beam stability
     and reduced isotopic fractionation were noted by both sets of authors as a signifi-
     cant benefit of both methods of  overcoating.






     Thermal ionization has widespread application in areas where measurement of
     isotope ratios is the goal of the analysis. Each area has its unique problems and
     challenges, and there is considerable cro~s-fe~lization among disciplines. Ex-
     haustive treatment would require a book of its own; no attempt has been made here
     to cover all areas addressed by thermal ionization, Rather, a few areas of current
     and historical interest have been selected; these should give the reader a good idea
     of the versatility of the technique.
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