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Glow Discharge  Mass Spectro~et~                              61

                 Bias  Corrected  Isotope  Ratio ~easurements in  the  Unspiked
         Sample,  Isotopically  Enriched  Spike,  and  Spiked  Sample  for  Three  Oil
         Leachate  Samples  as  Determined  by  Glow  Discharge  Mass  Spectroscopy
         Sol~tion Residue  Method
                     R,           R,           RM
                 zo7Pb+PPbf  207Pb+P~Pb+   207Pb+/z04Pb+  Concentration
         Sample  (sample)  (spike)  (mixture)  (PPm)
         A        14.9 4 0.5   0.029 4 0.001  0.192 4 0.004   2.69  4 0.05
         B         7.5 4 0.2   0.029 4 0.001  0.130 4 0.001   3.5 4 0.1
         c1       15.2 It: 0.2   0.029 5 0.001   1.44 4 0.01   82.5 4 0.7
         c2       15.9 4 0.3   0.029 4 0.001   1.46 It: 0.02   83.2 4 0.8
         c3       15.1 4 0.2   0.029 4 0.001   1.41 4 0.02   80.2 4 0.8

         Source: Ref. 64.


         deleterious  effect  on  the  resulting  mass  spectrum.  This  effect   is multiplied by
         several  orders  of  magnitude  because  the  support  gas  is far and  away  the most
         abundant  constituent  of  the discharge.  Complicating  this  effect   further is  the
         production of polyato~c species  such  as CO+, Arc+, ArN+, and ArO+. Several
         methods  have  been  used  to  reduce  interferences  in  the  glow  discharge  to  accept-
         able  levels.  One is to dissociate  the  molecular  ions into their  component  elements
         through  the  use  of  gas-phase  collisions  [ 109-  1  1 l], a  second  is to resolve  the
                                                    [ 1 121, and  a  third is to used
         interferences  with  a  high-resolution  mass  spectrometer
         gated  detection  with  a  pulsed  discharge
                                         [ 1 13,1141.  None of these  methods,  how-
                                                      0). Among  the  methods
         ever,  reduces  the cont~butions of residual  gases  (C,  N,  or
         specifically  designed to remove cont~nants, heating  the  gas  to  drive  them out,
         cryocooling  to  condense  them  from  the  gas  phase  [ 1 151, using  getters  as  a
         conductive  binder  [ 1 161, and  using  a  high-purity  support  gas [ 1 171 hold  the  most
         promise.  Mykytiuk et al. 1691 and  Valiga et al. [ 1 181 have  used  a  combination of
         approaches  to  analyze  C, N,  and 0 at the tens of part  per  million  level  and  lower  in
         samples, In  particular,  Valiga's  work  was  impressive  because  he  used  a  low-
         resolution  quadrupole  mass  spectrometer,  an  inherently  less  expensive  instrument
         than  a  sector.  Table  2.5  shows  these  results for the analysis of a  National Institute




                   Thee glow  discharge  mass  spectra  taken  over  the  mass range mlz 200-210
                                           pL of
         for  three  different  cathodes  doped  with  (a)  500  a 40.9-ppm  2oQPb  spike,  (b)  500 pL
         of an unknown  waste  oil  sample,  and  (c) 500 pL of a mixture  consisting  of 1 .O nk of  the
         u~own and  100 pL of  the  40.9-ppm  z04Pb  spike.  The  discharge  conditions  of  all  three
         cathodes  were -1000  V dc,  2.0  mA,  and  133.3  Pa  argon.
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