Page 77 - Radiochemistry and nuclear chemistry
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66                   Radiochemistry  and  Nuclear  Chemistry


                The last term is approximately the kinetic energy of the particle (2.5)  divided by c 2,  and
               thus

                                            m  ~  m ~  +  Eki n/c 2                 (4.21)

               The  increase  in  mass,  Am  =  m  -  m ~  because of the kinetic energy  of the particle,

                                              Eki n  =  Amc 2                       (4.22)


               was  generalized  by  A.  Einstein  in  the  special  theory  of  relativity,  leading  (after  more
               detailed  calculations)  to  the well known  mass-energy  relationship

                                                E  =  mc 2                         (4.23)

               which  we  already  have applied  in the discussion  of the nuclear binding  energy  (3.3).
                When  a  neutrino  is  ejected  from  the  nucleus  it  carries  away  energy  of  kinetic  nature.
               Thus,  according  to  (4.21)  the neutrino  has  a  relativistic  mass  >  0,  and  obviously  also  a
               momentum p  =  mv.  Recoil  studies  of/3-decay  have proven  this  to be  true.
                In order to correctly apply (4.18) for the calculation of the/3-decay energy, the relativistic
               electron mass must be used; as is seen from Figure 4.2,  already at 0.1  MeV,  the relativistic
               mass of the electron is  15 % larger than the rest mass m o  (In the following  the rest masses
                                                            e"
               of  the  electron,  neutron,  etc.,  will  be  denoted  simply  as  m e,  m n,  etc.;  capital  M  if  in
               universal  mass  units,  u)
                The energy released  in/3-decay  is distributed  between the neutrino,  the electron,  and  the
               recoil  of the daughter nucleus.  This latter will be much smaller than  the  first two and  can
               be neglected  in a  first approximation  (w   Therefore,  the total B-decay energy can be
               considered  to be distributed  between  the neutrino and the electron.  For the decay  137Cs
               137tuBa it can be shown  that the total  decay energy  QB is 0.514  MeV.  This  is also  termed
               Ema x.  The neutrino  energy spectrum is the complement of the/3-particle  energy spectrum.
               If  the  energy  of  the  electron  is  0.400  MeV,  that  of  the  neutrino  is  0.114  MeV.  If  the
               electron  energy  is 0.114  MeV,  the neutrino  energy  is 0.400  MeV.
                In/3--decay  the  average  value  of the/3--particle  energy  is  approximately  0.3 Ema x.  In
               positron  emission,  the average energy of the/3+-particle  is approximately  0.4 Ema x.
                The  assumption  that  the  neutrino  has  a  zero  rest  mass  has  been  questioned  by
               experimentalists and theorists.  A number of experiments have established an upper limit of
               the rest mass as  <  10 eV.  The implications  of a  finite rest mass are broad as the nature  of
               the  neutrino  and  the  theory  of  beta  decay  is  involved.  On  an  even  grander  scale,  the
               expansion  of the universe  depends  on  the neutrino  mass.  If the neutrino  rest  mass  is only
               a  few eV,  this  might result  in  sufficiently  greater gravitational  force that could eventually
               stop  the expansion  and  contraction  will  begin,  see Ch.  17.
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