Physics:Nuclear magneton

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Short description: Physical constant
The value of nuclear magneton
System of units Value
SI 5.0507837461(15)×10−27 J⋅T−1[1]
Gaussian 5.05078374×10−24 erg·G−1[2]
eV 3.15245125417(98)×10−8 eV·T−1[3]
MHz/T (per h) 7.6225932188(24) MHz/T[4]

The nuclear magneton (symbol μN) is a physical constant of magnetic moment, defined in SI units by: μN=e2mp and in Gaussian CGS units by: μN=e2mpc where:

Its CODATA recommended value is:

μN = 5.0507837461(15)×10−27 J⋅T−1

In Gaussian CGS units, its value can be given in convenient units as

μN = 0.10515446 efm

The nuclear magneton is the natural unit for expressing magnetic dipole moments of heavy particles such as nucleons and atomic nuclei.

Due to neutrons and protons having internal structure and not being Dirac particles, their magnetic moments differ from μN:

μp = Error in {{val}}: parameter 1 is not a valid number. μN
μn = Error in {{val}}: parameter 1 is not a valid number. μN

The magnetic dipole moment of the electron, which is much larger as a consequence of much larger charge-to-mass ratio, is usually expressed in units of the Bohr magneton, which is calculated in the same fashion using the electron mass. The result is larger than μN by a factor equal to the proton-to-electron mass ratio, about 1836.

See also

References