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Quantum Confinement in Nanostructures

Confine a particle in an infinite square well of side LL and its energy is quantised, En=2π2n2/(2mL2)E_n=\hbar^2\pi^2 n^2/(2mL^2): the levels go as n2n^2, so E2E1=3E1E_2-E_1=3E_1, and the ground-state confinement energy (the gap) scales as 1/L21/L^2, growing as the box shrinks and vanishing in the bulk limit. The left panel shows the well, its levels and the wavefunctions ψn(x)=sin(nπx/L)\psi_n(x)=\sin(n\pi x/L). Which directions are confined sets the dimensionality, and the density of states takes a qualitatively different shape in each case: g(E)E1/2g(E)\propto E^{1/2} for the 3D bulk, a staircase for the 2D quantum well, (EEc)1/2(E-E_c)^{-1/2} van Hove spikes for the 1D wire, and discrete delta peaks for the 0D dot. The right panel is that DOS with the optical-absorption onset (the effective gap) marked. Everything is closed form (gate-tested).

Figure 1. Left: the infinite-square-well levels Enn2E_n\propto n^2 and wavefunctions. Right: the density of states, E1/2E^{1/2} (3D bulk), step (2D well), (EEc)1/2(E-E_c)^{-1/2} (1D wire) or delta peaks (0D dot), with the absorption onset marked. Method: closed-form particle-in-a-box energies and dimensionality-resolved DOS (gate-tested sim.js), Canvas2D; the live readouts are E1E_1, E2E1E_2-E_1, the gap and the absorption onset.
dimensionality
box size L2.00
eff. mass m1.00

WHAT TO TRY

  • Vary each control and watch the rail readouts respond.
  • Compare the diagnostic plot against the live scene.