
A state of matter characterized by global topological invariants that are robust against local perturbations.Topological phases are states of matter whose defining properties are global, geometric features that remain unchanged under smooth deformations. Unlike ordinary phases distinguished by local order parameters like density or magnetization, topological phases are characterized by invariants such as the Chern number or winding number. These invariants are quantized and robust against local perturbations, meaning that small disturbances like impurities or defects cannot easily alter them. This robustness makes topological phases fundamentally different from conventional states and opens pathways for applications where stability is critical.
The concept emerged in the 1980s with the discovery of the integer quantum Hall effect by Klaus von Klitzing, who found that the Hall conductance is quantized to extraordinary precision. The theoretical explanation by David Thouless and collaborators in 1982 linked this quantization to topological invariants. Later, the idea expanded to topological insulators and superconductors in the 2000s.
The mechanism relies on the mathematical concept of topology, where objects are classified by properties preserved under continuous transformations. In a topological phase, the quantum wavefunction of the system acquires a global structure—like a twist or a hole—that cannot be undone without crossing an energy gap. For example, in the quantum Hall effect, electrons in a magnetic field form edge states that conduct without dissipation because the bulk has a nonzero Chern number. The edge states are a direct consequence of the bulk's topology, a principle known as bulk-boundary correspondence.
Topological phases are used in quantum computing research, particularly for topologically protected qubits that are resilient to decoherence, and in the design of dissipationless electronic devices.
The 2016 Nobel Prize in Physics was awarded for theoretical discoveries of topological phase transitions and topological phases of matter.






