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inattention<br />

will be drawn to any evidence which might serve as a<br />

basis for future work along these lines and some tentative<br />

suggestions which may be helpful for further work will be<br />

included.<br />

f<br />

?^^g3 for the Relative Abundance of Nuclides<br />

All species of stable nuclei occur In nature. Their<br />

relative abundance, however, shows a variation by a factor of the<br />

order of lO-'-^, Harklns (1917) was the first to attempt a systematic<br />

classification of the stable nuclear species or nuclides<br />

based upon our knowledge of atomic number as a proper<br />

designation of an element and of the Isotopes as the ultimate<br />

constituents of these elements, and Harkins* rules represent<br />

important regularities in the abundances of the nuclides.<br />

Mattauch introduced additional rules. Such rules are now in<br />

general understood in teiras of binding energies, in particular<br />

from the point of view of the nuclear shell model as discovered<br />

and developed by Mayer (19^, 19*^9) and by Baxel, Jensen and<br />

Suess {19^*9).<br />

In a previous paper (Suess, 19^7) certain rules regarding<br />

the abundances of the stable nuclides were presented as follows:<br />

(1) Odd mass number nuclides: The abundances of odd mass numbered<br />

nuclear species with A>'v50 change steadily with the mass number»<br />

When Isobars occur, the sum of the abundances of the isobars must be<br />

used instead of the individual abundances.<br />

(2) Even mass number nuclides: (a) In the region of the heavier

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