Quantum mechanical model describing interacting spins with exchange coupling between neighboring sites.The Heisenberg model is a mathematical framework used in condensed matter physics to describe how magnetic moments (spins) on a lattice interact with their immediate neighbors. It treats each atom as having a tiny quantum magnet, and the model specifies how the orientation of one magnet influences the ones next to it. This interaction is captured by an exchange coupling constant, which determines whether neighboring spins prefer to align parallel (ferromagnetic) or antiparallel (antiferromagnetic).
Introduced by Werner Heisenberg in 1928 to explain ferromagnetism, building on earlier ideas of exchange interaction from quantum mechanics.
In the model, each lattice site carries a spin operator, and the total energy is the sum of pairwise interactions between adjacent spins, weighted by the coupling constant. The quantum nature means spins are not classical arrows but obey commutation relations, leading to phenomena like spin waves (magnons) and entanglement. Solving the model for one-dimensional chains is exact, while higher dimensions require approximations or numerical methods.
It is used to model magnetic materials, from simple insulators to high-temperature superconductors, and to design spintronic devices.
The one-dimensional Heisenberg model is exactly solvable using the Bethe ansatz, a rare example of an integrable quantum system.


