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18.4. One-Particle Motion in Deformed Nuclei (Nilsson Model) 557<br />

A state is consequently denoted<br />

by K π . Actually, three<br />

partially conserved quantum<br />

numbers are used to describe<br />

a given level further. We<br />

shall not need these asymptotic<br />

quantum numbers here.<br />

As an application of the<br />

Nilsson model, we consider<br />

the ground states of some nuclides<br />

with a neutron or proton<br />

number around 11. Figure<br />

18.1 shows that these nuclides<br />

are expected to have<br />

a deformation of the order<br />

of 0.1, and consequently the<br />

Nilsson model should be applicable.<br />

Figure 18.10: In a nonspherical nucleus, the total angular<br />

momentum, j, of a nucleon is no longer a conserved quantity.<br />

Only its component, K, along the nuclear symmetry<br />

axis is conserved. A nucleon with spin j (in the spherical<br />

case) gives rise to K values j, j − 1,..., 1<br />

. States K and<br />

2<br />

−K have the same energy.<br />

The relevant properties of a number of nuclides are summarized in Table 18.2.<br />

If it is assumed that the nuclides are described by the single-particle spherical shell<br />

model, their ground-state spin-parity assignment can be read from Fig. 17.9: only<br />

the last odd nucleon is assumed to determine the moments. The listed nuclides<br />

have one or three nucleons outside the closed shell 8: According to Fig. 17.9, they<br />

should all have an assignment ( 5<br />

2 )+ . In reality, the spins are different, even for<br />

19F, which has only one proton outside the magic number 8. The quadrupole<br />

moment has been measured for two of the listed nuclides, and 〈r2 〉 can be taken<br />

from Eq. (6.26); Eq. (18.31) then provides the value of the deformation parameter<br />

δ(≈ ɛ). In agreement with the estimate from Fig. 18.1, δ is of the order of 0.1. The<br />

value δ =0.1 is indicated in Fig. 18.9. Following this line the predicted assignments<br />

can be read: for one nucleon outside the closed shell 8, ( 1<br />

2 )+ is predicted. Three<br />

nucleons outside the shell lead to an assignment ( 3<br />

2 )+ . As Table 18.2 shows, these<br />

values agree with experiment and demonstrate that the Nilsson model can explain<br />

at least some of the properties of deformed nuclei. (In all these assignments it is<br />

assumed that the even number of nucleons, for instance, the 10 neutrons in 19F, remain coupled to zero.)<br />

The prediction of ground-state moments is only one of the successes of the<br />

Nilsson model. It is also able to correlate a great many other observed properties<br />

of deformed nuclei. (16,17)<br />

16B.R. Mottelson and S.G. Nilsson, Kgl. Danske Videnskab. Selskab, Mat-fys. Medd. 1, No.8<br />

(1959).<br />

17M.E. Bunker and C.W. Reich, Rev. Mod. Phys. 43, 348 (1971).

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