Approximation methods

adiabatic theorem

The adiabatic theorem says that if a system's conditions are changed slowly enough, a system that began in a particular energy state will stay in the corresponding energy state as the conditions evolve. The energies and the states themselves may drift and reshape, but the system follows its own level faithfully, never jumping across to a neighbour. Slowness, not stillness, is the key: the surroundings can change a great deal, so long as they change gently.

The intuition is that a gradual change gives the system time to readjust at every moment, settling into the new instantaneous version of the state it was in. Picture carrying a bowl of water across a room: walk slowly and the surface stays calm, tracking the bowl's tilt; lurch suddenly and it sloshes into a mess of waves. A slowly tilted quantum system, likewise, rides smoothly along its instantaneous eigenstate without spilling into others.

How slow is slow enough depends on the spacing of the energy levels: the change must be gradual compared with the natural timescale set by the gaps to nearby states. This theorem underlies methods for steering quantum systems gently from one configuration to another, including schemes in adiabatic quantum computing. It also sets the stage for the Berry phase, the subtle geometric twist a state acquires when its conditions are slowly cycled around a loop.

change slow vs. ℏ / (energy gap)² ⇒ stays in the same level

Change conditions slowly relative to the gap timescale and the system rides its own instantaneous eigenstate.

The theorem can fail at an avoided crossing, where two levels approach very closely. There the gap shrinks, the safe-slowness condition becomes brutally strict, and a system can leak into the other level.

Also called
adiabatic approximation绝热近似絕熱近似