Page 232 - Radiochemistry and nuclear chemistry
P. 232

216                 Radiochemistry and Nuclear Chemistry

               crystal  adjusts  itself during  the drifting process  so that the lithium atoms compensate  the
               impurities.  This is, however, not a stable situation when the drifting operation is stopped.
               Hence,  the  final  state  is  "frozen"  by  cooling  of  the  drifted  crystal  to  liquid  nitrogen
               temperature. Accidental heat-up will destroy the lithium compensation and the detector must
               be redrifled.
                When  a  potential  is  applied  over  such  a  crystal,  with  the positive  terminal  at  the  high
               lithium  side,  three volumes  are created,  one  of p-type,  a  middle  "intrinsic"  one,  and  an
               n-type one (p-i-n detectors).  In the intrinsic volume the lithium donor electrons neutralize
               any  original  impurities,  which  are  of  acceptor  p-type.  The  intrinsic  volume  becomes
               depleted and thereby sensitive to nuclear radiation, and detectors with depleted volumes up
               to more  than  100 cm 3 are commercially available.  Figure  8.14  shows the arrangement of
               the Dewar vessel with liquid N 2,  cold-finger,  detector,  and preamplifier.
                Lithium-drifted  detectors  are  made  either  from  silicon  (Si(Li)  detectors)  or  from
               germanium  (Ge(Li)  detectors).  The  latter  has  a  higher  atomic  number  and  density  than
               silicon and  is  therefore preferable  for "y-spectrometry.  For 60 keV  X-rays,  the efficiency
               of a Si(Li)  detector may be 5 %, while for a comparable Ge(Li) detector it may be  100%.
               At lower energy the $i(Li) detector is preferable, especially if the measurements are carried
               out  in  a  high  "),-background.  Si(Li)  detectors  are  of  particular  importance  in  X-ray
               fluorescence analysis  (of.  w
                Both types give excellent resolution,  for a good Si(Li) X-ray detector about  160 eV at 5.9
               keV  and  for  a  good  Ge(Li)  detector  about  1.75  keV  FWHM  for  1.33  MeV  ~.  Energy
               resolution  of Ge detectors  varies with energy below  1.5  MeV  according  to  the empirical





                                                                     PopTop TM  Doqlsctor
                                                     To Electronics    Capsule
                                                     (power supply,   ~'q'~ Shroud
                                                     amplifier, eta:.)
               LN 2 Fill lind                                    Filter
               Vent Tubes                                                 C
                                                                           Pick       ]
                                                                              Germanium Crystal


                                                    O-Ring Seal
                                         LkluM Nitrogen
                                          Fill Collar
                                                          Preamplifier
                                            Flange
                                                                 /   Cooled FET
                                         Cooling Rod         Cooling Rod   Assembly   End Cap
                                         '(copper)           Stabilizer     /   Mounting
                                                                            /   Cup
                                           Charcoal                      Contact Pin
                                         (to maintain vacuum)






                      FIG.  8.14.  Cut-away view of a Ge-detector showing Dewar, cold-finger, preamplifier and
                      germanium crystal.  (Acc.  to ORTEC.)
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