Geometric phase curvature in momentum space that acts as an effective magnetic field for electron motion.Berry curvature is a geometric property of quantum states that describes how the phase of a wavefunction changes as the system's parameters (like momentum) are varied adiabatically. In momentum space, it acts as an effective magnetic field for electrons, influencing their motion even in the absence of a real magnetic field. This curvature is the local manifestation of the Berry phase, a global geometric phase acquired by a quantum state during a closed loop in parameter space.
The concept of the Berry phase was introduced by Michael Berry in 1984, building on earlier work by Pancharatnam (1956) in optics and the adiabatic theorem of Born and Fock (1928). The Berry curvature as a momentum-space field was later developed in the context of condensed matter physics.
When an electron moves through a crystal, its wavefunction acquires a phase that depends on the path taken in momentum space. The Berry curvature is the curl of the Berry connection, analogous to how a magnetic field is the curl of the vector potential. This effective magnetic field can deflect electrons, leading to phenomena like the anomalous Hall effect and the quantum Hall effect. The total Berry flux through a closed surface in momentum space is quantized, giving rise to topological invariants that classify materials.
Berry curvature is fundamental to the physics of topological insulators and Weyl semimetals, and it is exploited in spintronics and quantum computing for robust, topologically protected states.
The Berry curvature of a black hole's spacetime can shift the quantum phase of particles, effectively 'twisting' their wavefunctions as they pass near the event horizon.
| \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 |














