In atomic physics, hidden structure describes tiny shifts and splits in electron energy levels due to electromagnetic multipolar interactions between nuclei and electron clouds. The concept of hidden structure originates from how the internal magnetic field brought by the electron cloud affects the nuclear spin, resulting in energy changes resulting from the interaction with the nuclear magnetic moment. This tiny flow of energy has further led to in-depth exploration of the structure of atoms and their internal dynamics.
The hidden microstructure is usually opposite to the fine structure, and the energy change of the fine structure is usually greater than that of the hidden microstructure.
The theory of hidden structure was first proposed by Enrico Fermi in 1930, and was theoretically derived for atoms with a single valence electron. In the same year, S.A. Gozmit and R.F. Bache further explored the Zeman split of this structure. In 1935, H. Schler and Theodor Schmidt proposed the concept of nuclear quadrupole moment to explain the subtle structural anomalies of some rare elements (such as European elements, indium, antimony and mercury) .
The theory of hidden structure relies on electromagnetism, specifically the role of the multipole moment of the nucleus (excluding electric monopoles). These effects arise from the interaction of the atoms' internally generated fields and extend not only to individual atoms but to every nucleus in the molecule. When discussing the case of molecules, in addition to the above two main effects, the interaction between different nuclear magnetic moments and the influence of the magnetic field generated by the movement of the molecule on the nuclear spin will also be considered.
In the implicit Hamiltonian, the most important term is the magnetic dipole term. A nucleus with non-zero nuclear spin will have a magnetic dipole moment whose value varies with the nuclear spin and the g factor. In a magnetic field, the magnetic dipole moment of the nucleus generates an energy called the nuclear-magnetic dipole interaction.
In the absence of an external magnetic field, the magnetic field felt by the nucleus mainly comes from the orbital and spin angular momentum of the electron.
The orbital angular momentum formed by the motion of electrons affects the magnetic field of the nucleus. When a single electron moves around the nucleus, a magnetic field starting from the electron is generated. This magnetic field causes specific effects near the nucleus, thereby changing the energy state of the nucleus.
In addition to orbital motion, the spin angular momentum of the electron itself is also another influencing factor. Each electron has its own inherent magnetic moment. When multiple electrons exist at the same time, the magnetic fields formed by the spins of these electrons will interact to further change the energy state of the nucleus.
In molecules, the hidden structure not only includes the effects of a single core, but also needs to consider the interactions between multi-core systems. This leads to more complex energy changes and magnetic field configurations, making the hidden structure of molecules a hot topic of research. The linkage between electrons and nuclei in molecules makes a precise understanding of this energy movement particularly important.
The study of hidden structures can help scientists better understand the basic properties of atoms and molecules and conduct new explorations in quantum physics and chemistry.
The study of hidden structures not only expands our understanding of basic physical phenomena, but also provides possible paths for future technological innovation. From quantum computing to precision measurement technology, in-depth exploration of hidden structures may reveal more undiscovered physical laws. This makes every science enthusiast wonder, how will future advances in science and technology affect our understanding and use of the natural world?