Bound states & barriers

particle in a box

The particle in a box is the simplest worked example in quantum mechanics: a single particle confined to a one-dimensional stretch of space, free to move inside but unable to leave. It is the quantum version of a bead sliding on a short wire with hard stops at each end. Stripped of every complication, it shows the essential consequences of confinement with arithmetic clean enough to do by hand.

Solving it reveals that the particle cannot have just any energy. Its wavefunction must be zero at both walls, like a guitar string pinned at its ends, and only standing waves that fit a whole number of half-wavelengths into the box satisfy this. Each allowed standing wave carries its own definite energy, so the energies form a discrete ladder rather than a continuous range. The energies grow as the square of a counting number: the second level is four times the first, the third nine times, and so on.

Despite its toy-like simplicity, the model captures real physics. It explains roughly why electrons confined to tiny semiconductor structures, dye molecules, or quantum dots glow at particular colours, since the spacing of the energy rungs sets the energy of light the system can absorb or emit. Almost every textbook uses it as the first place where quantization stops being mysterious and becomes a direct result of fitting waves into a confined space.

Eₙ = n²·h² / (8·m·L²), n = 1, 2, 3, …

The energy of each level grows with the square of the counting number n and shrinks as the box L widens.

The 'box' is an idealization: real traps have walls of finite height, so a real particle's wavefunction leaks a little beyond the edges. The box model assumes infinitely high walls to keep the maths clean.

Also called
particle in a wellbox model一维势阱模型