Page 263 - Inorganic Mass Spectrometry - Fundamentals and Applications
P. 263

The  mission of  Ions                                         249


         face of the emitter. An interesting feature is the enhanced  ion  emission  from the
         cracks  in the face of the emitter  in  Fig.  6.4a. These appear to be due  to  enhanced
         migration of ions  along  the  surfaces  within the cracks.  This  information  by  itself
                                                         to emission.  Another
         provides  the insight that  ions  can  migrate  along  surfaces  prior
         possible inte~retation of the  enhanced  ion  emission from the cracks is that the
         edges  may  provide  an  enhancement eEect, possibly due to electrostatic field gra-
                           at
         dients  that  are  stronger an  edge. The fourth  image is Bi+ from a molten  glass  ion
         emitter.  Although the image  does  not  show  any  surface  topographical features, the
         majority of the ions  are  originating  from  the face of the bulk  of the deposit. The
         ions  forming  the  ring  around  the  main  area of ion  emission are thought to origi-
                                            of
         nate  from  sample  residing  on  the  outer  rim the tube  source. The intensity  was
         su~ciently low  that  an  exposure of several  minutes  would  have  been  required  to
         obtain a good  photograph. The features changed  with  time  rapidly  enough  that  this
         was  not  practical,  hence  the  image  in Fig, 6.4d is from the  video  camera. An in-
         teresting  topographical feature of the molten  ion  emitter,  which  unfortunately  can-
         not be demonstrated to the  reader,  was the fashion in  which  bubbles  could  be  ob-
         served  forming  and  bursting  on the surface.  If  such  a bubble  were to occur  in a
         sample for which  an isotope ratio were  being  measured it would be impossible to
         get  accurate  results since the  beam  intensity  would  fluctuate  excessively. This may
         be  the  reason why  many  analytical  procedures  that  use  silica gel require the use  of
         very  small  loadings.
              It is recognized  that there may be other ion  emitting  condensed  phase  mate-
         rials for which  ions  originate  from a region other than from the bulk of the mate-
                                             to
         rial, but since these  have  not  been  identified date, the  remainder of this  chapter
         deals  with  those  systems  emitting  ions  from bulk  of  the  deposit.
                                             the



         Material  volatilizing  from the surface of most  condensed  phases at high  tempera-
                                                       a
         tures  consists  predominantly of neutral  species,  with  only few  materials  emitting
                                                    in
         ions to an  appreciable  extent.  Ion  emitters  are  unique this  regard.  In an eEort to
         understand  the  mechanisms  responsible for this  phenomenon  better  an  instrument
         was  constructed to measure  the  ions  and  the  neutrals  volatilizing  from a  single
         specimen of an emitter sequentially, The purpose is to gain  better  understanding
         of the  types  and  quantities of neutrals  volatilizing from the materials  along  with
         the ions so as to  gain  new  insights into the processes  governing  ion  emission.
              "his instrument [7] measures  three  types of ions  in a sequential  mode:  the
         positive  and  negative  ions  emitted from the  surface of the ion  emitter,  and the neu-
         tral  species  volatilizing  from  the  surface  and  ionized by electron impact (EI). A
         commercially  available  quadrupole  mass  spectrometer  equipped  with  an source
                                                                   E1
         was  modified to allot a specially  designed  thermal emitter to be  just barely  inserted
         into the ionization  chamber. The chamber is much  cooler than. the emitter; there-
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