A unit of energy in the atomic system of units. The unit was proposed in 1926 and named in 1959.² In its rationalized form it is defined as
|m||the rest mass of the electron|
|e||the electron charge|
|h||the Planck constant|
|ε₀||the rationalized permittivity of free space|
According to the 1998 CODATA recommendations, 1 hartree equals 4.359 743 81 × 10⁻¹⁸ joules with a one standard deviation uncertainty of ± 0.000 000 34 × 10⁻¹⁸ joules.³
The hartree is named for D.R. Hartree (1897–1958), who proposed an atomic system of units in 1928.¹
1. D. R. Hartree.
The Wave Mechanics of an Atom with an Non-Coulomb Central Field. Part I. Theory and Methods.
Proceedings of the Cambridge Philosophical Society, volume 24, page 89 (1927).
“Both in order to eliminate various universal constants from the equations and also to avoid high powers of ten in numerical work, it is convenient to express quantities in terms of units, which may be called ‘atomic units,’ defined as follows:
“Unit of length, ,
on the orbital mechanics the radius of the 1-quantum circular orbit of the H-atom with fixed nucleus.
“Unit of charge, e, the magnitude of the charge on the electron.
“Unit of mass, m, the mass of the electron.
“Consistent with these are:
“Unit of action, h⁄2π.
“Unit of energy, e²⁄2 = potential energy of charge e at distance a from an equal charge = 2hcR = twice the ionization energy of the hydrogen atom with fixed nucleus.
“Unit of time, ¼πrcR.”
H. Shull and G. G. Hall.
Nature, volume 184, no. 4698, page 1559 (Nov. 14, 1959).
Since the energy unit in this system is the one most generally needed, it seems appropriate that its name be simplified to the ‘Hartree’ and denoted by H. Thus we define:
The conversion factor from Hartrees to cm.⁻¹ is then precisely twice as large as the infinite Rydberg, R∞.
Peter J. Mohr and Barry N. Taylor.
CODATA recommended values of the fundamental physical constants: 1998.
Journal of Physical and Chemical Reference Data, volume 28, No. 6 (1999).
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Last revised: 26 November 2004.