Page 120 - Inorganic Mass Spectrometry : Fundamentals and Applications
P. 120

110                                                        Olesik


            have  been  obtained for elements  that  suffer  from  extensive  molecular  ion  spectral
            overlaps [ 1531.
                 The multico~ponent spectral  fitting  approach  has  been  the  most  successful
            for a broad  range of sample  types  [ 153,1541. A linear  combination of spectra of all
            of  the individual  components  (elemental  ions  and  polyatomic  ions) is optimized
            for best  fit  of  the  experimental  spectrum.  “Model” spectra  are  determined  from
            the  natural  abundances  of  the  elements  and  polyatomic   “model”  spectra  are
                                            of
            calculated  from  the  isotopic  abundances the  individual  element  isotopes.  There-
            fore, experimental “model” spectra  are  not  required.
                 Several  problems  can  be  encountered  with  multicomponent spectral fitting.
            If the signal is too large to be measured  directly at some  masses,  those  masses  must
            not  be  included.  An   initial mass  scan  can  be  used  to  identify  regions   of  the
            spectrum that should be skipped [ 1531. The initial mass  scan  might also be used to
            determine  whether  certain  molecular  ions  can  be  excluded  from  the  model  be-
            cause  they are at  insignificantly  low  levels.  If  there  are  more  individual  compo-
            nents  in  a segment of  the spectrum  than  masses,  there  are  more  variables  than
            unknowns  and a unique  solution to multicomponent  fitting is not  found.  This  can
            be  dealt  with by establishing  relationships  between  components  and  constraining
            the  signals  due  to  certain  ions  in  order  to  have  at  least  as  many  equations  as
            unknowns  (independent  variables).  Ions  such  as  oxides  and  hydroxides  containing
            a co~mon element (e.g., CaO+ and CaOH+) should  maintain a relatively  constant
            relationship  [154]. Blank spectra  can  be  used  to  establish limits for ArN+ com-
            pared  to  the  signal  at  mass   54, ArO+ compared  to  the  signal  at  mass   56, and
            ArOH+ compared  to  the  signal  at  mass 57. A lower limit for Kr in  relation  to  the
            signal  at  mass  84  and value for the “continuum” background  (measured at mass
                             a
            220)  can  also  be set from  the  blank  spectrum.  Mass  bias  must be determined  and
            included.  Experimental  spectra form Ca and sulfate standard  solutions  can  be  used
            to  establish  limits for the CaO+-to-CaOH+ ratio  and the ratios for S species [S,+/
            SO,+,  SO,H+/(S,+  + SO2+), and S03+/(S2+ + SO2+)] [154]. An Excel based
            spreadsheet  template  is  available  for  download  from  a  S~ectroc~i~ic~ Acta
            ~lectro~ica
                      article by DeBoer [ 1541 at http://www.elsevier.nl:8O/inc~omepa~e/
            saalsabl  (download  file 520389197).




            Many  experimental  parameters  and  components  affect  sensitivity,  including  the
            analyte  transport  efficiency of the  sample  introduction  system  and the mean size
            and size distribution of the  aerosol  entering  the IC€? The  plasma  torch  design,  rf
            generator,  load  coil, interface  between  the  atmospheric  pressure  ICP and  mass
            spectrometer,  ion  optics,  mass  spectrometer itself, and  detector  also  affect  sensi-
            tivity.
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