ConstantID

Shielded proton gyromagnetic ratio in MHz/T

Atomic & nuclearMeasured

γp′/2π = 42.576 385 43(17) MHz T−1

Value
42.576 385 43 MHz T−1
Standard uncertainty
1.7 × 10−7 MHz T−1
Relative uncertainty
4.0 × 10−9 (4 parts per billion)
Status
Measured
Symbol
γp′/2π
Source
CODATA 2022 via NIST · NIST entry

Use in a calculation

# shielded proton gyromagnetic ratio in MHz/T, CODATA 2022 (NIST)
shielded_proton_gyromagnetic_ratio_in_mh = 4.257638543e1  # MHz T^-1, standard uncertainty 1.7e-7

# SciPy: scipy.constants.physical_constants['shielded proton gyromag. ratio in MHz/T']

What it is

The precession frequency, per tesla of magnetic field, of a proton in a spherical sample of pure water at 25 °C, whose magnetic field is partly screened by the surrounding electrons: the gyromagnetic ratio divided by 2π. Magnetic resonance spectroscopists use this form.

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).

shielded proton gyromagnetic ratio in MHz/T: CODATA values 1998–2022 relative to the 2022 value, in parts per billion, with one-standard-uncertainty bars−150−100−500+50+100+150parts per billion1998200220062010201420182022

Relative uncertainty

shielded proton gyromagnetic ratio in MHz/T: relative standard uncertainty in each CODATA adjustment, logarithmic scale10⁻⁹10⁻⁸10⁻⁷1998200220062010201420182022
CODATAValue (uncertainty)Relative uncertaintyChange from previous
202242.576 385 43(17)4.0 × 10−9 +1.5 σ of 2018
201842.576 384 74(46)1.1 × 10−8 −0.6 σ of 2014
201442.576 385 07(53)1.2 × 10−8 −1.5 σ of 2010
201042.576 3866(10)2.3 × 10−8 −1.2 σ of 2006
200642.576 3881(12)2.8 × 10−8 +0.2 σ of 2002
200242.576 3875(37)8.7 × 10−8 −0.7 σ of 1998
199842.576 3888(18)4.2 × 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).

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