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57o<br />
In the corresponding region proceeding the shell closure at W equal to<br />
50 no conclusive indications of a similar pattern are found-<br />
The data, however, indicate a small laaxiDBum for nuclei<br />
containing 50 neutrons and a minimum preeeeding that region-<br />
Our adopted values<br />
show this behaviour, although a more regular pattern may also be possible©<br />
A breaJc that cannot be smoothad out by any roeansjoscurs in the abundance<br />
curves at A equal to 120 and 121a<br />
The break, associated with a change in the character<br />
of isotopic abundance distribution occurs at a point where the iranber of<br />
neutrons in Hie nuclei reaches 70o<br />
The break at this nui*er is \ms3qoected, but<br />
the conclusion seems inevitable that tte high spin of the rtsutrons in the 6 hii/2<br />
shell must in scans way t© connected wi.th this irregularityo<br />
At the corresoonding<br />
place for 112 neutrons a slight change in the character of tire abundance<br />
disti^bution mi^t be disscemed, butt a break in the abundance curves, which m5.^t<br />
possibly exist at A. equal to 186 and lfl7, can be smoothed out without difficulty©<br />
Probably the filling of the 7 1 x3/2 neutron shell begins l^fore the nuaiber of<br />
neutrons reaches 112-<br />
Other irregularities in the hi^er mass range are less impressive and not<br />
as firmly established-<br />
Uncertainties in the relative abundamses of the rare<br />
oarth eleu^nts make it impoaalble to recognize in a quantitative way an irregulailty<br />
irtiich apparently exists in the A equal to 170 region, and to see what pattern<br />
may be correlated with the fact that the odd A hafniim isotopes do not show abun-