Page 550 - Instrumentation Reference Book 3E
P. 550

532  Nuclear instrumentation technology

             Scintillation  counters  Since alpha  particles  are   either  the zinc sulfide powder  screen or a large-
            very easily absorbed in a very short distance into   area  very  thin  plastic  scintillator  is  used.  The
             any substance, problems  are posed  if  alphas are   latter  is much  cheaper  to produce  than the for-
             to enter a scintillator through a window, however   mer, as the thin layer of zinc sulfide needs a great
             thin, which would also prevent light from enter-   deal  of  labor  to  produce  and  it  is  not  always
             ing and overloading the photomultiplier. The ear-   reproducible.  In health physics applications,  for
             liest scintillation detector using a photomultiplier   monitors  for  hand  and  foot  contamination,  or
             tube had a very thin layer of zinc sulfide powder   bench-top  contamination,  various  combinations
             sprinkled on the glass envelope of a side-viewing   of  plastic scintillator,  zinc sulfide, or sometimes
             photomultiplier  of  the  RCA  931-A  type,  on   anthracene powder scintillators are used.
            which  a  small  layer  of  adhesive  held  the  zinc   If  the  alpha  emitter  of  interest  is mixed  in  a
             sulfide in place. Due to the low light transmission   liquid scintillator the geometrical effect is almost
             of powdered zinc sulfide, a layer 5-10mg/cm2 is   completely  eliminated  and, provided  the  radio-
             the  optimum  thickness.  The  whole  system  was   active  isotope  can  be  dissolved  in  the  liquid
             enclosed in a light-tight box, source and detector   scintillator,  maximum  detection  efficiency  is
             together. Later experimenters used a layer of alu-   obtained.  However,  not  all  radioactive  sources
             minum evaporated onto the zinc sulfide to allow   can  be  introduced  in  a  chemical  form  suitable
             the alphas in but to keep the light out. This was   for  solution,  and  in  such  cases  the  radioactive
             not successful, as an adequate thickness of alumi-   material  can  be  introduced  in  a  finely  divided
             num  to  keep  the  light  out  also  prevented  the   powder  into  a  liquid  scintillator  with  a  gel
             alphas  from  entering  the  zinc  sulfide.  When   matrix-such   a  matrix  would  be  a  very  finely
             photomultipliers  with  flat  entrance  windows   divided extremely pure grade of silica. McDowell
             began  to become available,  the zinc sulfide was   (1980) has written a useful review of alpha liquid
             deposited  on  the  face  of  a  disc  of  transparent   scintillation  counting  from  which  many  refer-
             plastic such as PerspexILucite. This was easier to   ences in the literature may be obtained.
             evaporate  aluminum  on  than  directly  onto  the
             photomultiplier,  but  the  light  problem  was  still
             present,  and even aluminized mylar was not the   22.2.4.2  Detection of beta particles
             answer. Operation in low or zero-light conditions
             was still the only satisfactory solution.   Ionization chainbers  Although ionization cham-
              Thin scintillating plastics were also developed   bers  were  much  used  in  the  early  days  for  the
             to  detect  alphas,  and  in  thin  layers,  generally   detection of beta particles, they are now used only
             cemented by heat to a suitable plastic light guide,   for a few special purposes:
             proved cheaper to use than zinc sulfide detectors.   (1)  The  calibration  of  radioactive  beta  sources
             The  light  output  from plastic  scintillators  was,   for surface dose rate. An extrapolation cham-
             however, less than that from zinc sulfide, but both   ber varies the gap between the two electrodes
             scintillators,  in  their  very  thin  layers,  provide   of a parallel plate ionization chamber. and the
             excellent discrimination  against beta  particles or   ionization current per unit gap versus air gap
             gamma  rays, often present  as background  when   is  plotted  on a  graph as  the gap is  reduced,
             alpha-particle emitters are being measured.  One   and  this  extrapolates  to  zero  gap  with  an
             major  advantage  of  the plastic  scintillator  over   uncertainty  which  is  seldom  as  much  as  1
             the inorganic zinc sulfide detector is its very fast   percent,  giving  a  measure  of  the  absolute
             response, of the order of 4 x   s for the decay   dose from a beta source.
             time of a pulse as compared with 4 - 10 x   s   (2)  Beta dosimetry. Most survey instruments used
             for zinc sulfide.                           to measure dose rate incorporate some sort of
              Another  scintillator  which  has  been  used  for   device to allow beta rays to enter the ioniza-
             alpha detection  is the inorganic crystal CsI (TI).   tion chamber. This can take the form of a thin
             This can be used without any window (but in the   window with a shutter to cut off the betas and
             dark)  as  it  is  non-hygroscopic,  and,  if  suitably   allow gamma rays only to enter when mixed
             beveled  around  the  circumference, will  produce   beta-gamma doses are being measured. How-
             an output proportional to the energy of the ion-   ever,  the  accuracy  of  such  measurements
             izing  particle  incident  on  it,  thus  acting  as  a   leaves a great deal to be desired, and the accu-
             spectrometer.  Extremely thin  CsI  (Tl) detectors   rate measurement of beta dose rates is a field
             have been made by vacuum deposition  and used   where development is needed.
             where the beta and gamma background  must be
             reduced  to very small proportions yet the heavy
             particles of interest must be detected positively.   Proportional counters  Beta particles may origin-
               Inorganic  single  crystals  are  expensive,  and   ate  froin  three  different  positions  in  a  propor-
             when  large  areas  of  detector  must  be  provided   tional  counter;  first,  from  part  of  the  gaseous
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