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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-

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