ConstantID

Electron g factor

Atomic & nuclearMeasured

ge = −2.002 319 304 360 92(36)

Value
−2.002 319 304 360 92
Standard uncertainty
3.6 × 10−13
Relative uncertainty
1.8 × 10−13 (0.18 parts per trillion)
Status
Measured
Symbol
ge
Source
CODATA 2022 via NIST · NIST entry

Use in a calculation

# electron g factor, CODATA 2022 (NIST)
electron_g_factor = -2.00231930436092  # standard uncertainty 3.6e-13

# SciPy: scipy.constants.physical_constants['electron g factor']

What it is

The ratio of the electron's magnetic moment to the value expected from its spin with the Bohr magneton as the unit. Dirac's theory predicts exactly −2; the small excess, the anomaly, comes from quantum electrodynamics and is measured to about a part in 10¹³, the most precise test of a physical theory.

Equations

  • μe=ge2μBrelation to the moment
  • ae=|ge|−22anomaly

How the value changed, 1998–2022

Each point is one CODATA adjustment, plotted as its difference from the 2022 value; the bars show one standard uncertainty (an arrowhead means the bar runs off the chart).

electron g factor: CODATA values 1998–2022 relative to the 2022 value, in parts per trillion, with one-standard-uncertainty bars−10−50+5+10parts per trillion1998200220062010201420182022

Relative uncertainty

electron g factor: relative standard uncertainty in each CODATA adjustment, logarithmic scale10⁻¹³10⁻¹²10⁻¹¹1998200220062010201420182022
CODATAValue (uncertainty)Relative uncertaintyChange from previous
2022−2.002 319 304 360 92(36)1.8 × 10−13 +4.7 σ of 2018
2018−2.002 319 304 362 56(35)1.7 × 10−13 −1.4 σ of 2014
2014−2.002 319 304 361 82(52)2.6 × 10−13 −0.5 σ of 2010
2010−2.002 319 304 361 53(53)2.6 × 10−13 +0.4 σ of 2006
2006−2.002 319 304 3622(15)7.5 × 10−13 +1.3 σ of 2002
2002−2.002 319 304 3718(75)3.7 × 10−12 +0.2 σ of 1998
1998−2.002 319 304 3737(82)4.1 × 10−12

“Change from previous” is the shift in the value divided by the standard uncertainty of the previous adjustment. Earlier values are converted into the current unit where NIST changed it (for example J s to J Hz⁻¹).

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