Page 224 - Inorganic Mass Spectrometry - Fundamentals and Applications
P. 224

Secondary Ion   ass Spectrometry                              209


























                   High-resolution  secondary ion mass  spectrometry (SMS) images on. silver
         halide microcrystals. Large crystal at top is 6.5 prn across. Crystals have four alte~ating
         layers of AgBr  and Ag13ro~910~l on a AgBr core. A, Br” image; b, I” after -3  nm  removed;
         c, 1-  after -24  nm  removed; d, I-  after -46  nm  removed. (From Ref. 133.)



         are  3 to 7 pm across  and c0.3 pm  thick. The high  resolving  power of  SIMS  al-
         lowed  the  photographic  materials  engineers to study  directly  the  effects of con-
         trolled  physical  and  chemical  conditions  on  composition  and mo~hological char-
         acteristics.
              The capability of SIMS to  record  all  elements  and  isotopes  with  high spatial
         resolution in three  dimensions is making it popular  in  solid-state  science.  Three-
                                                                to
         dimensional  (3-D)  imaging is done  retrospectively,  using  a  computer stack  a  se-
         ries of 2-D  images.  A good  example of the  visualization  that  may  be  done  using
         3-D data is shown  in  Fig.  4.42  [134]. The l60- image of a  separation by implanted
         oxygen (SIMOX) structure is 150 pm in  diameter  and  2.5 pm deep. The upper left
         shows  a “pie slice’’ to reveal  some  inner  structure  that  includes  an  oxide  defect  ex-
         tending  from the surface to a  depth of about  2  pm. The bottom left is a ho~zontal
                                       4 pm in  diameter.  At the right  are 0” depth
         slice showing  the  oxygen  defect  to  be
         profiles  from  the  defect at position A (top)  and  a  typical  region at positio
         tom). To show  internal  structure  better,  a  “volume  rendering,”  as illustrate
         4.43 [ 1341,  may  be done.  In  this  technique  a  gray  and a partial ~~sparency value
         for each  voxel(3-D volume element)  are calculated.  Regions of low inte~sity are
         made   an spa rent to maximize  the  visibility of internal structure. Since sputtering
         rates  may  not be unifo~ over  the  area  viewed, topo~aphical corrections of the 3-
         D images  may be made  by  making  maps of the surface  before  and  after  sputtering
         using  atomic force microscopy [ 134,1351.
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