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

Ĥψ(𝐫,t)=[−ℏ22m∇2+V(𝐫)]ψ(𝐫,t)=iℏ∂ψ(𝐫,t)∂t,

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

[−ℏ22m∇2+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+𝐫𝝈̂ α±|𝐫|
Free particle −ℏ2∇22m ℏ2𝐤22m,𝐤∈ℝd Massive quantum free particle
Delta potential −ℏ22md2dx2+λδ(x) −mλ22ℏ2 Bound state
Symmetric double-well Dirac delta potential −ℏ22md2dx2+λ(δ(x−R2)+δ(x+R2)) −12R2(λR+W(±λRe−λR))2 ℏ=m=1, W is Lambert W function, for non-symmetric potential see here
Particle in a box −ℏ22md2dx2+V(x) V(x)={0,0<x<L,∞,otherwise π2ℏ2n22mL2,n=1,2,3,… for higher dimensions see here
Particle in a ring −ℏ22mR2d2dθ2 ℏ2n22mR2,n=0,±1,±2,…
Quantum harmonic oscillator −ℏ22md2dx2+mω2x22 ℏω(n+12),n=0,1,2,… for higher dimensions see here
Hydrogen atom −ℏ22μ∇2−e24πε0r −(μe432π2ϵ02ℏ2)1n2,n=1,2,3,…

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See also

References

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Reading materials