G-FACTOR


A '''g''-factor' (also called '''g'' value' or 'dimensionless magnetic moment') is a dimensionless quantity which characterizes the magnetic moment and gyromagnetic ratio of a particle or nucleus. It is essentially a proportionality constant that relates the observed magnetic moment μ of a particle to the appropriate angular momentum quantum number and the fundamental quantum unit of magnetism, the Bohr magneton.

Contents
Electron ''g''-factors
Electron spin ''g''-factor
Electron orbital ''g''-factor
Landé ''g''-factor
Nucleon and Nucleus ''g''-factors
Muon ''g''-factor
Measured ''g''-factor Values
Notes and references
See also

Electron ''g''-factors


There are three magnetic moments associated with an electron: One from its spin angular momentum, one from its orbital angular momentum, and one from its total angular momentum (the quantum-mechanical sum of those two components). Corresponding to these three moments are three different ''g''-factors:
Electron spin ''g''-factor

The most famous of these is the ''electron spin g-factor'', ''gS'' (more often called simply the ''electron g-factor'', ''g''e), defined by
: oldsymbol{mu}_S=-g_S mu_mathrm{B} (oldsymbol{S}/hbar)
where '''μS''' is the total magnetic moment resulting from the spin of an electron, '''S''' is the magnitude of its spin angular momentum, and '''μ''B' is the Bohr magneton. The ''z''-component of the magnetic moment then becomes
: oldsymbol{mu}_z=-g_S mu_mathrm{B} m_s
The value ''gS'' is roughly equal to two, and is known to extraordinary accuracy ([1]). The reason it is not ''precisely'' two is explained by quantum electrodynamics.
Electron orbital ''g''-factor

Secondly, the ''electron orbital g-factor'', ''gL'', is defined by
: oldsymbol{mu}_L=g_L mu_mathrm{B} (oldsymbol{L}/hbar)
where '''μL''' is the total magnetic moment resulting from the orbital angular momentum of an electron, '''L''' is the magnitude of its orbital angular momentum, and '''μ''B' is the Bohr magneton. The value of ''gL'' is exactly equal to one, by a quantum-mechanical argument analogous to the derivation of the classical magnetogyric ratio. For an electron in an orbital with a magnetic quantum number ml, the ''z''-component of the orbital angular momentum is
: oldsymbol{mu}_z=g_L mu_mathrm{B} m_l
which, since ''gL'' = 1, is just ''μ''Bml
Landé ''g''-factor

Thirdly, the ''Landé g-factor'', ''gJ'', is defined by
: oldsymbol{mu}=g_J mu_mathrm{B} (oldsymbol{J}/hbar)
where '''μ''' is the total magnetic moment resulting from both spin and orbital angular momentum of an electron, '''J''' = '''L'''+'''S''' is its total angular momentum, and '''μ''B' is the Bohr magneton. The value of ''gJ'' is related to ''gL'' and ''gS'' by a quantum-mechanical argument; see the article Landé g-factor.

Nucleon and Nucleus ''g''-factors


Protons, neutrons, and many nuclei have spin and magnetic moments, and therefore associated ''g''-factors. The formula conventionally used is
: oldsymbol{mu}=g mu_mathrm{p} (oldsymbol{I}/hbar)
where '''μ''' is the magnetic moment resulting from the nuclear spin, '''I''' is the nuclear spin angular momentum, and '''μ''p' is the nuclear magneton.

Muon ''g''-factor


The muon, like the electron has a ''g''-factor from its spin, given by the equation
: mathbf{mu}=g (ehbar/(2m_mu)) (mathbf{S}/hbar)
where '''μ''' is the magnetic moment resulting from the muon’s spin, '''S''' is the spin angular momentum, and '''mμ''' is the muon mass.
One-loop MSSM corrections to the muon g-2 involving a neutralino and a smuon, and a chargino and a muon sneutrino respectively.

The muon ''g''-factor can be affected by physics beyond the Standard Model, so has been measured very precisely, in particular at the Brookhaven National Laboratory. As of November 2006, the experimentally measured value is 2.0023318416 with an uncertainy of 0.0000000013, compared to the theoretical prediction of 2.0023318361 with an uncertainty of 0.0000000010[1]. This is a difference of 3.4 standard deviations, suggesting beyond-the-Standard-Model physics may be having an effect.

Measured ''g''-factor Values


{| class="wikitable" style="text-align:center"
|-
! Elementary Particle !! ''g''-factor !! Uncertainty
|-
! Electron g_mathrm{e}
| 2.002 319 304 3622 || 0.000 000 000 0015
|-
! Neutron g_mathrm{n}
| 3.826 085 46 || 0.000 000 90
|-
! Proton g_mathrm{p}
| 5.585 694 701 || 0.000 000 056
|-
! Muon g_{mu}
| 2.002 331 8396 || 0.000 000 0012
|-
|+Currently accepted NIST ''g''-factor values[2]
|}
It should be noted that the electron g-factor is one of the most precisely measured values in physics, with its uncertainty beginning at the twelfth decimal place.

Notes and references


1.
Improved predictions for g-2 of the muon and alpha(QED)(M(Z)

★ 2), , K., Hagiwara, ,



See also



anomalous magnetic dipole moment

Electron magnetic dipole moment

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