Rydberg constant times hc in eV
Atomic & nuclearMeasured
= 13.605 693 122 990(15) eV
- Value
- 13.605 693 122 990 eV
- Standard uncertainty
- 1.5 × 10−11 eV
- Relative uncertainty
- 1.1 × 10−12 (1.1 parts per trillion)
- Status
- Measured
- Symbol
- Source
- CODATA 2022 via NIST · NIST entry
Use in a calculation
# Rydberg constant times hc in eV, CODATA 2022 (NIST)
rydberg_constant_times_hc_in_ev = 1.360569312299e1 # eV, standard uncertainty 1.5e-11
# SciPy: scipy.constants.physical_constants['Rydberg constant times hc in eV']
What it is
The Rydberg energy R∞hc in electronvolts, about 13.6 eV: the ionisation energy of hydrogen in the heavy-nucleus limit.
In other units
| Unit | Value | |
|---|---|---|
| CGS (cm2 g s−2) | 2.179 872 3611 × 10−11 | |
| keV kiloelectronvolt | 0.013 605 693 123 | |
| Eₕ hartree | 0.5 | unit is itself measured |
| Ry rydberg | 1 | unit is itself measured |
Converted with ConstantID's unit table; digits are rounded to the precision of the value, and a long exact value is rounded only for display. The relative uncertainty is unchanged by conversion to an exactly defined unit.
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).
Relative uncertainty
| CODATA | Value (uncertainty) | Relative uncertainty | Change from previous |
|---|---|---|---|
| 2022 | 13.605 693 122 990(15) | 1.1 × 10−12 | −0.2 σ of 2018 |
| 2018 | 13.605 693 122 994(26) | 1.9 × 10−12 | +1.4 σ of 2014 |
| 2014 | 13.605 693 009(84) | 6.2 × 10−9 | +1.6 σ of 2010 |
| 2010 | 13.605 692 53(30) | 2.2 × 10−8 | +1.8 σ of 2006 |
| 2006 | 13.605 691 93(34) | 2.5 × 10−8 | −0.3 σ of 2002 |
| 2002 | 13.605 6923(12) | 8.8 × 10−8 | +1.1 σ of 1998 |
| 1998 | 13.605 691 72(53) | 3.9 × 10−8 |
“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).