
A change in the topological properties of a physical system, often marked by a phase transition.A topological transition is a change in a physical system where its global, 'topological' properties—such as the number of holes, twists, or winding numbers—shift, often accompanied by a phase transition. Unlike ordinary phase changes (like melting), these transitions are not driven by local order parameters but by global invariants that remain unchanged under smooth deformations. They explain phenomena like the quantum Hall effect and the behavior of certain exotic materials.
The concept emerged from the 1980s work on the quantum Hall effect, where Thouless, Kohmoto, Nightingale, and den Nijs (1982) linked the quantized Hall conductance to a topological invariant.
Topological transitions occur when the system's energy landscape or band structure changes such that a topological invariant (e.g., Chern number) jumps from one integer to another. This typically happens when a gap in the energy spectrum closes and reopens, allowing the system to change its global topology. The transition is robust against small perturbations, making the resulting states—like edge currents or surface states—highly stable.
Topological transitions underpin the design of topological insulators and superconductors, which are explored for fault-tolerant quantum computing and spintronics.
During a topological transition, the system often exhibits a 'critical' state where excitations become massless, akin to particles in high-energy physics.






