System 01

Infinite Potential Well

Governing equations
ψn(x)= 2L sin(nπxL)
En= n2π2ℏ22mL2
The interactive model uses ℏ = 1.

Wavefunction ψ(x)

Amplitude can be positive or negative.

ψ

Probability density |ψ(x)|²

Higher curve values indicate greater detection probability density.

|ψ|²
01

Increasing n adds nodes and shortens the wavelength inside the well.

02

Increasing L spreads the state across a wider region and lowers the energy.

03

Increasing m lowers the energy because the kinetic term becomes smaller.

Governing equations
En=ℏω (n+12)
ψn(x) ∝ Hn(u) e−u2/2
Here u = √(mω/ℏ) x; the interactive model uses ℏ = 1.

Wavefunction ψ(x)

Higher states develop more nodes and oscillations.

ψ

Probability density |ψ(x)|²

Classically forbidden regions remain visible through the quantum tails.

|ψ|²