Page 225 - Radiochemistry and nuclear chemistry
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Detection  and Measurement  Techniques             209


               90%  At"  +  10%  CH 4 ("P-gas") and 96 % He  +  4 % i-C4Hlo ("Q-gas").  Many other pure
               gases or  combinations are possible,  but molecules which readily attach  electrons  must be
               avoided.  Figure  8.8(b)  shows  a  proportional  counter  tube  using  pure  CH~ and  the  tube
               characteristics (i.e.  count rate versus voltage) for 239pu cr   and for "roSe B-particles
               entering  through the thin aluminized mylar window.
                The gas mixture and electrodes may be separated by a thin window from the radioactive
               sample,  or  the  counter  may  be  operated  windowless.  For  windowless  operation,  after
               insertion of the sample the chamber must be  flushed with gas  to eliminate all the  oxygen
               and water vapor as these molecules absorb electrons readily to form negative ions and,  by
               so  doing  reduce  the  pulse  size.  For  cr  and  ~-particles  whose  ranges  do  not  exceeA the
               dimensions of the chamber, windowless counters are often referred to as 27r counters since
               a  solid  angle of 2r  is  subtended  above the  sample.  In  these cases,  with proper  care,  the
               measured count rate is very close to 50 % of the true disintegration rate.  Such windowless
               proportional  counters  are  very  useful  for  measuring  low  energy  radiation  such  as  the  ~-
               emissions of 14C and 3H, and for absolute counting.  Figure 8.10 shows a 47r proportional
               counter  in  which  the  sample  is  inserted  in  the  middle  between  the  two  half-domes
               (cathodes).
                Proportional  counters  can  be used also  for neutron  detection  by using  a  gas containing
               nuclei that capture neutrons and in the nuclear reaction produce charged particles,  e.g.  10B
               or 3He.  In BF3-counter the gas is BF 3, usually enriched in  10B. With neutrons the reaction


                                 10B  +  n~7Li  +  4He   (Q  =  2.78  MeV)

               occurs (cf.  Ch.  14).  The ionization of the two products produces a heavy pulse,  which  is
               easy  to  discriminate  against  an intense  ~-background.  Some properties  of a  BF 3 neutron
               detector  are  given  in  Table  8.2.  From Figure  14.4  it  is clear  that  the  BF 3 counter  has  a
              higher efficiency  for thermal  than  for fast neutrons.



                                  UPPER          UPPER GAS
                                A  IUI/'~I'~I  tA/IDI=   CONNECTION
                       SC
                    RING
                                                  9 .'h"~ i


                                                                           SLIDE



                                                                  HIGH VOLTAGE
                                                                  CONNECTORS

                                                         D r



                      FIG. 8.10. A 4a" proportional counter for  measuring absolute decay rates. (Acc. to
                      O'Kelley.)
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