KAHIBARO
Table of Contents
Shell closures in nuclei
In nuclear physics, some numbers of protons or neutrons appear again and again as especially stable. These special values are called magic numbers. The most important magic numbers are
$$2,\ 8,\ 20,\ 28,\ 50,\ 82,\ 126$$
A nucleus with one of these numbers of protons, or one of these numbers of neutrons, tends to be more tightly bound and more stable than nearby nuclei.
The idea of magic numbers comes from the nuclear shell model. In that model, protons and neutrons occupy discrete energy levels inside the nucleus, somewhat like electrons in atomic shells. When a shell is completely filled, the arrangement is especially stable. That closed shell gives rise to a magic number.
Magic numbers are numbers of protons or neutrons that correspond to closed nuclear shells.
Common magic numbers are
$$2,\ 8,\ 20,\ 28,\ 50,\ 82,\ 126$$
Why closed shells are special
A closed shell means that all available states in a certain energy group are filled. If a nucleus has a closed shell, the next proton or neutron would have to go into a higher energy level. Because of this, nuclei with closed shells are unusually stable.
This extra stability shows up in several ways. Such nuclei often have higher binding energy than expected, lower tendency to undergo certain reactions, and characteristic patterns in separation energies and excited states. The detailed discussion of binding energy belongs elsewhere, but here the main point is simple: closed shells are energetically favorable.
A nucleus can be magic in proton number, neutron number, or both. If both proton number $Z$ and neutron number $N$ are magic, the nucleus is called doubly magic. Doubly magic nuclei are especially stable and important in nuclear structure.
Examples of magic nuclei
Some well known examples help make the idea concrete.
| Nucleus | Proton number $Z$ | Neutron number $N$ | Type |
|---|---|---|---|
| $^4\text{He}$ | 2 | 2 | Doubly magic |
| $^{16}\text{O}$ | 8 | 8 | Doubly magic |
| $^{40}\text{Ca}$ | 20 | 20 | Doubly magic |
| $^{48}\text{Ca}$ | 20 | 28 | Doubly magic |
| $^{132}\text{Sn}$ | 50 | 82 | Doubly magic |
| $^{208}\text{Pb}$ | 82 | 126 | Doubly magic |
For example, lead 208 is especially important because both its proton number and neutron number are magic. This helps explain why it is one of the most stable heavy nuclei.
Experimental signs of magic numbers
Magic numbers were not invented first and then observed later. They were inferred from patterns seen in nuclear data. Several experimental clues point to shell closures.
One clue is unusual stability. Nuclei with magic numbers are often more abundant or longer lived than nearby nuclei.
Another clue is the energy needed to remove a nucleon. If a shell is closed, removing a proton or neutron usually requires relatively large energy. But once the shell is filled, adding one more nucleon places it in a new shell, and that nucleon is less tightly bound. This creates sudden changes in separation energies.
A third clue comes from nuclear size and shape. Many closed shell nuclei are close to spherical, because filled shells tend to produce a more symmetric distribution.
A fourth clue comes from excited states. Closed shell nuclei often have their first excited state at relatively high energy, because exciting a nucleon requires crossing a shell gap.
A magic number is associated with a shell gap, an energy jump between a filled shell and the next available shell.
Large shell gap, greater stability.
Relation to the shell model
The shell model explains magic numbers by arranging nucleons into quantized energy levels. At first, a simple model of nucleons in a central potential predicts some shell structure, but it does not produce all the observed magic numbers correctly. In particular, numbers like $28$, $50$, $82$, and $126$ need an additional effect.
The key improvement is spin orbit coupling. In the nucleus, the interaction between a nucleon's spin and its orbital motion splits energy levels strongly. This rearrangement of levels creates large shell gaps at exactly the observed magic numbers.
So magic numbers are one of the strongest successes of the nuclear shell model. They show that the nucleus is not just a random collection of protons and neutrons, but has an organized quantum structure.
A simple shell filling picture
It is useful to think of shells as containers with limited capacity. As protons or neutrons are added, they fill lower energy levels first. When a shell is full, the system reaches a particularly stable configuration.
The exact labeling of levels belongs to the shell model discussion as a whole, but the central idea for magic numbers is that stability peaks when a shell is completed.
This drawing is only schematic. The important feature is the gap between one filled group of levels and the next higher level. That gap is what gives a magic number its special stability.
Doubly magic nuclei
If only the proton number is magic, the proton configuration is especially stable. If only the neutron number is magic, the neutron configuration is especially stable. If both are magic, the whole nucleus gains extra stability from both sides.
Doubly magic nuclei are often used as benchmarks in nuclear physics because their structure is relatively simple compared with many open shell nuclei. Their properties can often be described as a closed core plus possible excitations across shell gaps.
If both $Z$ and $N$ are magic, the nucleus is called doubly magic.
Doubly magic nuclei are especially stable and often nearly spherical.
Limits and modern view
The classic magic numbers work very well for many stable nuclei, but nuclear physics has shown that shell structure can change in exotic nuclei, especially those far from stability. In some regions, traditional magic numbers may weaken, and new ones may appear. This means magic numbers are not just fixed arithmetic facts, but consequences of the underlying nuclear forces and level structure.
Still, for an introductory course, the standard magic numbers remain fundamental because they explain many of the most important patterns in nuclear stability.
Summary
Magic numbers are special proton or neutron numbers that correspond to closed shells in the nucleus. The main magic numbers are $2$, $8$, $20$, $28$, $50$, $82$, and $126$. Nuclei with these numbers are unusually stable, often have larger shell gaps, and show characteristic experimental signatures. The concept is one of the clearest pieces of evidence for the nuclear shell model.