Lattice Vibrations & Phonons

normal mode

Push a child on a swing at just the right rhythm and the whole swing settles into one clean, repeating motion. A normal mode is the equivalent for a whole crowd of connected atoms: a special pattern in which every atom oscillates back and forth at one single, shared frequency, all keeping perfect time with each other.

A real solid jiggles in a hopelessly complicated way, with every atom seeming to do something different. The deep trick of physics is that any such tangled motion, however messy, can always be split into a sum of simple normal modes laid on top of one another. Each mode has its own fixed shape (which atoms move and in which direction) and its own frequency, and once set going it keeps that pattern forever without help. A crystal with many atoms has a huge number of these modes, and together they form a complete 'vocabulary' for describing every possible vibration.

Normal modes matter because they turn an impossible many-body problem into many simple, independent oscillators we already understand. The honest subtlety is that this clean independence relies on the springs being ideally springy; real forces are slightly imperfect, so in truth the modes leak a little energy into one another, which is what eventually lets heat spread and settle.

Sprinkle sand on a metal plate and stroke its edge with a violin bow: the sand jumps away from the moving parts and gathers along the still lines, drawing a beautiful pattern. Each pattern is one normal mode of the plate made visible, and a different bowing rhythm picks out a different mode.

Chladni figures: sand reveals the still lines of a plate's normal modes.

One phonon is exactly one quantum of energy added to one normal mode. So normal modes are the modes; phonons are the countable lumps of energy you put into them.

Also called
normal mode of vibration本征振动模式