
The Berry phase is a geometric phase acquired by a quantum system when its parameters are cycled adiabatically.In 1984, British physicist Michael Berry generalized an old idea about a phase accumulated during adiabatic (slow) changes of parameters. It turned out this phase is geometric: its magnitude is determined not by time or speed but by the curvature of parameter space. Earlier partial manifestations had been noticed before Berry, but he showed their universality and connection to gauge fields.
Predecessors: in 1956, S. Pancharatnam studied the phase of light under cyclic polarization changes. In 1984, Michael Berry gave a rigorous quantum-mechanical formulation for general adiabatic processes. Later, Frank Wilczek and others generalized the Berry phase to non-adiabatic processes and degenerate states, linking it to topological invariants.
The Berry phase is widely used to describe quantum transport, topological insulators (materials conducting only on the surface), molecular dynamics (e.g., predicting forbidden transitions), and quantum computing (topological qubits). Limits of applicability: adiabatic approximation—the rate of parameter change must be small compared to the energy gap between levels.
Explains electron behavior in crystals and is used to create topological quantum computers resistant to noise.
The famous Foucault pendulum, which rotates its swing plane due to Earth's rotation, is a classical analogue of the Berry phase: the pendulum 'senses' geometry, not just forces.
| \Omega | variable | Berry curvature — berry curvature square metre |
| m | variable | electron mass — mass kilogram |
| c | variable | speed of light in vacuum — speed metre per second |












