Page 300 - Radiochemistry and nuclear chemistry
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284                 Radiochemistry and Nuclear Chemistry
                           FROM   THE   SUN          FROM   GALAXIES
                           Non-isotrop~  padicle flux   I~tmpic  I~dicle flux
                           Flux dependent on solar activity   Flux independent  of solar activity
                           All masses (mainly  1H, also 3H))   All masses (mainly  1H, no  3H)
                           Energies  < 10 4 GeV      Energies  10 4 - 1010 GeV
                           Minor fraction            Major fraction

                                 ~
                              ~176
                                              "~
                                  .R~,
                                       oO
                                      ~
                         9 ~149 ~176176176 ~176176176 "~176176176176 ~176176149 o'.~ ~176176176176 ~176149176176176176176176176176176 ~176176176 ~176176 ".~176 ". ~149176
                                        ~
                                              "~176
                                                                  o.
                                                                 ~
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                                                                     ~176
                                                                        ~
                                                                           ".
                                                                              "~
                                                         o
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                                                                Oo
                                                               ~
                                                           9176176149
                            .
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                        ~  12:::2:::  .  .  .  .  .  .  .  .  .  .  .  .  .   9   .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  ,   .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  ~   .
                         ~
                          .
                                                                         ........
                        i:i-i:i:i:i:i:i:i:  ...E~. T.H.'.S .A..T~...SP.HE.R.E !N2.,.O2o,.Ar: et?! AT...A~. ?T " 2.5..KIM...:i:i:i:!:!:i:i:!: .........
                        o.~   .  .  .  .  .  .  .  .  .  .  .  .  ~  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  ~   .  .  .  .  o   .  .  .  .  .  .  .  .  .  .  .  .  .  .  ~
                        ::::::  Neutrinos   Formation of pions   Direct ionization   Spallation reactions  ":"
                        ...............................................................    9 ."
                                   .
                        .  .  .  .  .  .  .  .  .  .  . .  .  .  .  .  o  .  .  .  ~176176  .  .  .  .  . .  . .  . .  . .  .  .~176  . .  .  . .  . .  .  .  .  .  .  .   .  .  .  .  .  .  .  .  .  .  .  ~  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .
                                    .
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                        ~   .  .  .  .  .  .  .  0   ~  1  7  6  1  7  6  1 .  7.  6.  1 .  7 .  6 .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  ~  1  7  6  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .  .
                             v      ff+   n-    ~o       e"          n     p
                             1Jl           t  I
                             v      p+    p-
                                                                       Y
                                                    ~_.   e-  I Allen   Nuclear reactions
                                                            9 belts   producing
                                                                 3H, 2500 m-2 s-1
                                      Hard         Soft          10Be, 300 m-2 s-1
                                           component             14C, 22000 m-2 s-1
                                     (50-80%)     (-10%)              etc
                          1011 m-2 s-1   2 - 3 ion pairs cm-3 s-1
                       ---  -   "  ---':""  -  --'-  ---'-~"  Rapidly absorbed  -~   2
                       "~   Very liffie absorption  .  --'-=-~  =  "----- -  .  .  .  .  .  .  .  .  .
               FIG.  ]0.1.  Cosmic  radiation  consists  of  atoms  and  photons  which  react  with  the  atmosphere  leading  to  the
               formation  of numerous  secondary  particles,  some  (but  not  all)  detectable  at  the  earth's  surface.
               and intensities of this radiation have been of great importance to development of models of
               the formation and composition of the universe.
                The  major  part  of  the  cosmic  radiation  is  nuclear  particles  with  very  high  energy:
               approximately  70%  protons,  20%  a-particles,  0.7 % lithium,  beryllium,  and boron  ions,
               1.7% carbon, nitrogen, and oxygen ions, the residual 0.6%  ions ofZ  >  10. These ions are
               bare nuclei prior to interaction since their kinetic energies exceed the binding energies of
               all  of the orbital  electrons.
                The cosmic particle radiation can be divided by energy into two major groups (Fig.  10.1).
               One group has energies mainly below 1 GeV and consists primarily of protons.  This group
               originates mainly from the sun. Its intensity varies in relation to solar eruptions since at the
               time of such an eruption  a large amount of solar material,  primarily hydrogen,  is ejected
               into space.
                The  second  group  has energies  up  to  10 l~ GeV,  although  the  intensity  of the particles
               decreases with increasing energy,  following the relation N(E)  oc E -1.6  where N(E) is the
               number  of  particles  with  energies  in  excess  of E.  Thus  particles  of  10 3  GeV  have  an
               intensity of about  101] higher than particles of  10 l~ GeV.  Within this high energy group
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