List of quantum-mechanical systems with analytical solutions

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Much insight in quantum mechanics can be gained from understanding the closed-form solutions to the time-dependent non-relativistic Schrödinger equation. It takes the form

H^ψ(𝐫,t)=[22m2+V(𝐫)]ψ(𝐫,t)=iψ(𝐫,t)t,

where ψ is the wave function of the system, H^ is the Hamiltonian operator, and t is time. Stationary states of this equation are found by solving the time-independent Schrödinger equation,

[22m2+V(𝐫)]ψ(𝐫)=Eψ(𝐫),

which is an eigenvalue equation. Very often, only numerical solutions to the Schrödinger equation can be found for a given physical system and its associated potential energy. However, there exists a subset of physical systems for which the form of the eigenfunctions and their associated energies, or eigenvalues, can be found. These quantum-mechanical systems with analytical solutions are listed below.

Solvable systems

Solutions

System Hamiltonian Energy Remarks
Two-state quantum system αI+𝐫σ^ α±|𝐫|
Free particle 222m 2𝐤22m,𝐤d Massive quantum free particle
Delta potential 22md2dx2+λδ(x) mλ222 Bound state
Symmetric double-well Dirac delta potential 22md2dx2+λ(δ(xR2)+δ(x+R2)) 12R2(λR+W(±λReλR))2 =m=1, W is Lambert W function, for non-symmetric potential see here
Particle in a box 22md2dx2+V(x) V(x)={0,0<x<L,,otherwise π22n22mL2,n=1,2,3, for higher dimensions see here
Particle in a ring 22mR2d2dθ2 2n22mR2,n=0,±1,±2,
Quantum harmonic oscillator 22md2dx2+mω2x22 ω(n+12),n=0,1,2, for higher dimensions see here
Hydrogen atom 22μ2e24πε0r (μe432π2ϵ022)1n2,n=1,2,3,

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See also

References

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Reading materials