Page 107 - Inorganic Mass Spectrometry : Fundamentals and Applications
P. 107

I~du~tively Coupled Plasma Mass ~pectromet~                   97


         available. The main  advantages  of  TOF-ICP-MS  are  due  to the simultaneous
         sampling of ions of all masses. As a  result,  transient  signals for all elements  and
         isotopes  can  be  monitored  with  high  temporal  resolution.  Because  ions  are  ex-
         tracted  and  injected  into the  TOF-MS  simultaneously,  high-precision  isotope
         ratios  and  analyte/internal  standard  ratios  should  be  attainable.  Ion   trap mass
         spectrometers  have  been  used  in  combination  with  a  quadrupole  mass  filter  and
         alone  with  an ICP ion  source  [ 129- 1331. Initially  the large ratio of Ar+ to analyte
         ions  in  the ICP was  thought  to  make  ion  trap mass  spectrometers  impractical
         because of the limited total number of ions  that can be  stored  in the trap.  However,
         the  number of  Ar+ ions  observed  in the ion trap is orders of magnitude less, on  a
         relative  basis,  than  in  the  ICP itself.
              High-resolution  Fourier  transform  ion  cyclotron  resonance  mass  spectrome-
         ters  have  also  been  used for ICP-MS [ 134,1351.  Quadrupole  mass  spectrometers
                                                                      also
         used in alternate stability  regions  to  obtain  higher  resolution  than  typical  have
         been  used  for ICP-MS  [136,137].




         Several different  detectors  have  been  used  in  ICP-MS inst~ments (Fig.  3.14).  A
         range of ion signals  from less than  1  to lo8 iondsec can be produced.  Counting-
         based  detection is typically  used for signals of about lo6 ionslsec or less.  For  larger







       Ion                                  Ion


                                     ai                                    e
                                                                           al


                  Preamplifier  7                           conversion
                                                             dynode  ,-j-,
                                                        e   scintillator  L
                                                                  >
                                                                  *

                                                                   +
       lo                         I                          photo-
       I on
       0"  0
                                                            multiplier
                                                 Current      tube
                 kV
         Figure 14  Detectors: (a) Discrete dynode electron multiplier. (b) Dual-mode discrete
         dynode electron multiplier detector. (c) Channeltron electron multiplier. (d) Faraday collec-
         tor. (f) Daly detector.
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