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Atomic Units

Atomic units are tuned to electron-scale Coulomb problems. They are common in atomic physics, quantum chemistry, and electronic-structure calculations.

For versioned conversion factors, dimensional restoration, and Hartree–Rydberg code diagnostics, use the AMO Atomic Units reference. The present entry is the short cross-volume convention translator.

The usual Hartree atomic-unit convention sets

ℏ=1,me=1,e=1,4πϵ0=1.\hbar=1, \qquad m_e=1, \qquad e=1, \qquad 4\pi\epsilon_0=1.

Then the Coulomb potential between charges q1q_1 and q2q_2 is written without the SI prefactor:

V(r)=q1q2r.V(r)=\frac{q_1q_2}{r}.
QuantityAtomic UnitSI Meaning
LengthBohr radius a0a_0see Constants
EnergyHartree EhE_hEh≈27.211386246 eVE_h\approx27.211386246\ \mathrm{eV} using 2022 CODATA
Chargeelementary charge magnitude eepositive charge unit
Masselectron mass mem_eelectron mass unit
Angular momentumℏ\hbaraction unit

In atomic units, the nonrelativistic hydrogen Hamiltonian for an infinitely heavy nucleus is often written

H=−12∇2−1r.H=-\frac12\nabla^2-\frac{1}{r}.

The simplicity is convention-dependent. Restoring SI units brings back ℏ\hbar, mem_e, ee, and 4πϵ04\pi\epsilon_0.

  • Treating e=1e=1 as meaning the electron charge is +1+1; the electron charge is still negative.
  • Mixing atomic-unit Coulomb expressions with SI electromagnetic fields.
  • Forgetting that energies in Hartree are twice energies in Rydberg units.
  • Comparing code outputs without checking whether the code uses Hartree, Rydberg, or electron volt units.