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lYoblems of interpreting the imclaar abundance distribution<br />
Theories of the origin of the eletitents<br />
The nuclear abundance distribution as derivfxi from the discussion above,<br />
supplies a basis for comparison of empirical data with the various theories of<br />
the origin of the nuclear specieSo<br />
No such comparison will be given here,<br />
and the reader is referred to thrcaexcellent review articles by Alpher and<br />
^Herman (1950/1953) on the theory of the origin and relative abtmdance<br />
distribution of the elements dealing with this subject, in which sone IBO<br />
papers are critically discussed-<br />
It is shown there that none of the existing<br />
theories can account for all of the empirical facts, even in a crude way©<br />
Hence, It seems hopeless to attempt to explain the finer details presented<br />
here by any of these theories in their present form.<br />
It seems possible, however, that a modification of one theory or the other,<br />
in pairticular through assun^xtions regarding secondary and subsequent reactions,<br />
may load to a satisfactory agreement.<br />
We hope that tl» following discussion will<br />
be helpful for the study of the nature of such reactions»<br />
ISie nuclear abundance values obtained in the way described above differ<br />
in son© mass regions quite noticeably frcwi orevlous estimates (Suess 19U9).<br />
A comparison, howe^^r, of figure I with the corresponding figure published<br />
previously shows that the main features of the abundance distribution have<br />
been retaii»do<br />
TI»se features are essentially independent of the choice of the<br />
element abundance and constitute well-defined probleraSi, which will be discussed<br />
in the followingo<br />
This discussion will not be a complets one, and it will be left<br />
to the reader to detect many more features in figure 1 "srtiich might ssrve<br />
as evidence<br />
for or against the prevailing of a certain mechanism of element forraationo<br />
An impressive difference exists between the character of the region of the<br />
lighter (A 90) nucleio<br />
In the lower A region the line