A quantum dot traps its electron and hole in a finite 3D box of size L. Solving the particle-in-a-box Schrödinger equation gives discrete, quantized energy levels rather than a continuum:
E_n = n²π²ℏ² / (2·m*·L²)
E_gap(L) = E_bulk + E_e,1 + E_h,1
λ_emit = 1240 / E_gap(eV) [nm]
- Dot size L — the physical confinement length. Because E_n scales as 1/L², halving the dot roughly quadruples each confinement energy — shrink it and the ladder rungs spread apart, the gap widens and the emitted photon shifts toward blue; grow it and the ladder compresses toward the bulk gap and the photon reddens.
- Transition n — which confined electron/hole rung pair recombines. Higher-n transitions carry more confinement energy on top of the same bandgap, so they emit a bluer photon than the ground-state (n=1) transition at the same dot size.
- Material — sets the bulk bandgap E_bulk and the electron/hole effective masses (m*), which control how strongly confinement responds to size for that semiconductor (lighter effective mass → stronger size sensitivity).
Real-world relevance: this is the exact size-tunable bandgap effect that lets QLED TVs and quantum-dot biolabels emit a precise, saturated color from one chemistry, just by controlling nanocrystal diameter during synthesis — no dye or filter needed.