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136                 Radiochemistry and Nuclear Chemistry

               energy of the/3-particle  is  lost by ionization  and half by excitation.  The  track  formed  is
               further discussed  in  w
                The specific ionization from a B-particle is much lower than that from a heavy ion as can
               be seen in Figure 6.7a.  This is due to the fact that for the same initial energy,  B-particles
               have  much  greater  velocity  than  have  or-particles or  protons  because  their  mass  is  very
               much  smaller  than  the  mass  of  the  heavy  particles.  This  greater  velocity  results  in  a
               correspondingly lower ionization and gives a much longer range to/~-particles.  The erratic
               path observed for/~-particles in Figure 6.5c is a result of the large energy transfer and the
               resulting large deflections involved in the encounters with the orbital electrons.  However,
               at  very high  energies  the/~-particles  have  straight  paths  as a  result  of the  fact  that  very
               energetic  B-particles  have  a  momentum  considerably  in  excess  of  that  of  the  orbital
               electron.


               6.4.2.  Bremsstrahlung


                As a/3-particle  approaches an atomic  nucleus,  it is attracted by the positive  field of the
               nucleus and deflected from its path. The deflection results in an acceleration that, according
               to  classical  electrodynamics,  leads  to  emission  of electromagnetic  radiation  (Fig.  6.8c).
               Therefore  the encounter with the positive charge of the nuclear field decreases the energy
               of the/3-particle  by  an amount  exactly equal  to  the amount  of electromagnetic  radiation
               emitted.  This radiation is known as bremsstrahlung (braking radiation).  The loss of energy
               by emission  of bremsstrahlung  radiation  increases with the/~ energy and with  the atomic
              number of the absorber material (Fig.  6.9).  In aluminum approximately  1% of the energy
               of a  1 MeV electron is lost by bremsstrahlung radiation and 99 % by ionization whereas in
               lead  the  loss  by  radiation  is  about  10%.  For  electrons  of greater  than  10  MeV  energy,





























                      FIG. 6.9. Energy loss of fast electrons by ionization and bremsstrahlung. (From Gentner,
                      Maier-Leibnitz, and Bothe.)
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