Magic number

A proton number $Z$ or neutron number $N$ associated with a pronounced nuclear shell closure. The traditional sequence isThese count either species separately, rather than their sum $A=Z+N$. Calling a number magic summarizes a structural pattern; it does not promise that every isotope at that number is equally stable.

For example, in the chosen scheme the $20$-particle core plus the eight substates of $1f_{7/2}$ gives $28$. The next group contributes $4+6+2+10=22$, giving $50$. The following two groups contribute $8+6+4+2+12=32$ and $10+8+6+4+2+14=44$, giving $82$ and $126$. Counting verifies the capacities once the grouping has been chosen; it does not establish the physical energy gaps that justify that grouping.

Filling the accessible one-species nuclear shell model states below a substantial energy gap. A closed spherical $j$ level has all $m_j$ values occupied, so their sum is zero. In the independent-particle picture, a closed core therefore contributes zero total angular momentum; a single particle outside it, or a single missing particle inside it, supplies the leading spin assignment. Residual interactions can change this simple picture.

The three-dimensional isotropic harmonic oscillator alone has one-species shell capacities $(q+1)(q+2)$ for oscillator index $q=0,1,\dots$, including spin. Summing gives closures $2,8,20,40,70,112,\dots$, rather than the complete traditional magic number sequence. Strong nuclear spin-orbit splitting can separate a high-$j$ level from its former neighbors. Realistic radial potential energies and residual interactions also matter: a chosen oscillator plus an arbitrary single constant is not a demonstrated explanation of every real nuclear gap.

Traditional nuclear shell closures can weaken along isotope chains far from stability, as in neutron-rich magnesium.^[ref]

The relevant test is the actual energy gap and the correlated nuclear quantum states, rather than membership in an immutable numerical list.