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the Odd p Even n Nuclides from Iodine (53) to Berkelium (97) |
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The magnetic moment of a nucleus is due to the spinning of its charges. One part comes from the net sum of the intrinsic spins of its nucleons. The other part is due to the rotation of the positively charged protons in the nuclear structure.
However nucleons form spin pairs with other nucleons of the same type but opposite spin. Therefore for an odd p, even n nucleus there should be the net magnetic moment due to the intrinsic spin of one proton. The magnetic dipole moment of a proton, measured in magneton units, is 2.79285.
The magnetic moment of a nucleus μ due to the rotation of its charges is proportional to ωr²Q, where ω is the rotation rate of the nucleus, Q is its total charge and r is an average radius of the charges' orbits. The angular momentum L of a nucleus is equal to ωr²M, where M is the total mass of the nucleus. The average radii could be different but they would be correlated. Thus the magnetic moment of a nucleus could be computed by dividing its angular momentum by its mass and multiplying by it charge; i.e.,
where α is a constant of proportionality, possibly unity. Angular momentum may be quantized. This would make μ directly proportional to Q and inversely proportional to M. But Q and M can be expected to be proportional to each other. That means that if L is quantized then μ is quantized. This means means that μ should approximately be a constant independent of the scale of the nucleus.
There could be a slight variation in μ with the neutron number n because of its effect on the ratio (Q/M).
Here is the graph of the data for the magnetic moments of the odd p, even n nuclides from Iodine (53) to Berkelium (97): .
The data themselves are:
Magnetic Moments of the Even n, Odd p Nuclides from Iodine (53) to Berkelium (97) |
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53 | 64 | 3.1 |
53 | 66 | 2.9 |
53 | 68 | 2.3 |
53 | 70 | 2.818 |
53 | 72 | 2.821 |
53 | 74 | 2.81327 |
53 | 76 | 2.621 |
53 | 78 | 2.742 |
53 | 80 | 2.856 |
55 | 64 | 5.46 |
55 | 66 | 0.77 |
55 | 68 | 1.377 |
55 | 70 | 1.409 |
55 | 72 | 1.459 |
55 | 74 | 1.491 |
55 | 76 | 3.53 |
55 | 78 | 2.582025 |
55 | 80 | 2.7324 |
55 | 82 | 2.8513 |
55 | 84 | 2.696 |
55 | 86 | 2.438 |
55 | 88 | 0.87 |
55 | 90 | 0.784 |
57 | 76 | 7.5 |
57 | 78 | 0 |
57 | 80 | 2.695 |
57 | 82 | 2.7830455 |
59 | 80 | 6.6 |
59 | 82 | 4.2754 |
59 | 84 | 2.701 |
61 | 82 | 3.8 |
61 | 84 | 3.8 |
61 | 86 | 2.58 |
61 | 88 | 3.3 |
61 | 90 | 1.8 |
63 | 76 | 6.1 |
63 | 78 | 3.494 |
63 | 80 | 3.673 |
63 | 82 | 3.999 |
63 | 84 | 3.736 |
63 | 86 | 3.576 |
63 | 88 | 3.4717 |
63 | 90 | 1.5324 |
63 | 92 | 1.52 |
63 | 94 | 1.5 |
63 | 96 | 1.38 |
65 | 82 | 1.7 |
65 | 84 | 1.35 |
65 | 86 | 0.919 |
65 | 88 | 3.44 |
65 | 90 | 2.01 |
65 | 92 | 2.01 |
65 | 94 | 2.014 |
67 | 86 | 6.81 |
67 | 88 | 3.51 |
67 | 90 | 4.35 |
67 | 92 | 4.28 |
67 | 94 | 4.25 |
67 | 96 | 4.23 |
67 | 98 | 4.17 |
69 | 88 | 0.476 |
69 | 90 | 3.42 |
69 | 92 | 2.4 |
69 | 94 | -0.082 |
69 | 96 | -0.139 |
69 | 98 | -0.197 |
69 | 100 | -0.231 |
69 | 102 | -0.228 |
71 | 98 | 2.297 |
71 | 100 | 2.305 |
71 | 102 | 2.28 |
71 | 104 | 2.2323 |
71 | 106 | 2.239 |
73 | 100 | 1.7 |
73 | 102 | 2.27 |
73 | 104 | 2.25 |
73 | 106 | 2.289 |
73 | 108 | 2.3705 |
73 | 110 | 2.36 |
75 | 104 | 2.8 |
75 | 106 | 3.19 |
75 | 108 | 3.168 |
75 | 110 | 3.187 |
77 | 106 | 2.36 |
77 | 108 | 2.605 |
77 | 112 | 0.13 |
77 | 114 | 0.1507 |
77 | 116 | 0.1637 |
79 | 104 | 1.97 |
79 | 106 | 2.17 |
79 | 108 | 0.535 |
79 | 110 | 0.494 |
79 | 112 | 0.1369 |
79 | 114 | 0.1396 |
79 | 116 | 0.1487 |
79 | 118 | 0.145746 |
79 | 120 | 0.261 |
81 | 106 | 1.55 |
81 | 108 | 3.878 |
81 | 110 | 1.588 |
81 | 112 | 1.591 |
81 | 114 | 1.58 |
81 | 116 | 1.58 |
81 | 118 | 1.6 |
81 | 120 | 1.605 |
81 | 122 | 1.62225787 |
81 | 124 | 1.63821461 |
81 | 126 | 1.876 |
83 | 116 | 4.6 |
83 | 118 | 4.8 |
83 | 120 | 4.017 |
83 | 122 | 4.605 |
83 | 124 | 4.081 |
83 | 126 | 4.1103 |
83 | 128 | 4.5 |
83 | 130 | 3.89 |
85 | 122 | 3.75 |
85 | 124 | 10 |
85 | 126 | 9.56 |
85 | 128 | 3.8 |
87 | 120 | 3.89 |
87 | 122 | 3.95 |
87 | 124 | 4 |
87 | 126 | 4.02 |
87 | 134 | 1.58 |
87 | 136 | 1.17 |
87 | 138 | 1.07 |
87 | 140 | 1.5 |
89 | 126 | 7.82 |
89 | 128 | 3.83 |
89 | 138 | 1.1 |
91 | 140 | 2.01 |
91 | 142 | 4 |
93 | 144 | 3.14 |
93 | 146 | 2 |
95 | 144 | 2.6 |
95 | 146 | 1.58 |
95 | 148 | 0.951 |
97 | 152 | 2 |
The graph of magnetic moments versus neutron numbers does reveal critical values at 126 and 82.
The criticality of neutron numbers near 126 shows up in the data.
p | n | μ (magnetons) |
81 | 126 | 1.876 |
83 | 116 | 4.6 |
83 | 118 | 4.8 |
83 | 120 | 4.017 |
83 | 122 | 4.605 |
83 | 124 | 4.081 |
83 | 126 | 4.1103 |
83 | 128 | 4.5 |
83 | 130 | 3.89 |
85 | 122 | 3.75 |
85 | 124 | 10 |
85 | 126 | 9.56 |
85 | 128 | 3.8 |
87 | 120 | 3.89 |
87 | 122 | 3.95 |
87 | 124 | 4 |
87 | 126 | 4.02 |
It just happens that when n is near 126 the proton number is near 82.
A similar criticality is found near a neutron number of 82.
There does not seem to be a criticality of proton numbers near 82.
There is not an appearance of the constancy of the magnetic moment for proton and neutron numbers not near a critical number.
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