Quantum confinement in a 1D infinite square-well potential of width L: Schrödinger equation −(ℏ²/2m)·d²ψ/dx² = Eψ with boundary conditions ψ(0) = ψ(L) = 0 yields stationary eigenstates ψ_n(x) = √(2/L)·sin(nπx/L) and eigenenergies E_n =…
Quantum confinement in a 1D infinite square-well potential of width L: Schrödinger equation −(ℏ²/2m)·d²ψ/dx² = Eψ with boundary conditions ψ(0) = ψ(L) = 0 yields stationary eigenstates ψ_n(x) = √(2/L)·sin(nπx/L) and eigenenergies E_n =…