# G-factor (physics)

A g-factor (also called g value) is a dimensionless quantity that characterizes the magnetic moment and angular momentum of an atom, a particle or the nucleus. It is the ratio of the magnetic moment (or, equivalently, the gyromagnetic ratio) of a particle to that expected of a classical particle of the same charge and angular momentum. In nuclear physics, the nuclear magneton replaces the classically expected magnetic moment (or gyromagnetic ratio) in the definition. The two definitions coincide for the proton.

## Definition
### Dirac particle

The spin magnetic moment of a charged, spin-1/2 particle that does not possess any internal structure (a Dirac particle) is given by ${\boldsymbol {\mu }}=g{e \over 2m}\mathbf {S} ,$ where μ is the spin magnetic moment of the particle, g is the g-factor of the particle, e is the elementary charge, m is the mass of the particle, and S is the spin angular momentum of the particle (with magnitude ħ/2 for Dirac particles).

### Baryon or nucleus

Protons, neutrons, nuclei, and other composite baryonic particles have magnetic moments arising from their spin (both the spin and magnetic moment may be zero, in which case the g-factor is undefined). Conventionally, the associated g-factors are defined using the nuclear magneton, and thus implicitly using the proton's mass rather than the particle's mass as for a Dirac particle. The formula used under this convention is ${\boldsymbol {\mu }}=g{\mu _{\text{N}} \over \hbar }{\mathbf {I} }=g{e \over 2m_{\text{p}}}\mathbf {I} ,$ where μ is the magnetic moment of the nucleon or nucleus resulting from its spin, g is the effective g-factor, I is its spin angular momentum, μ$_N$ is the nuclear magneton, e is the elementary charge, and m$_p$ is the proton rest mass.

## Calculation
### 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 known of these is the electron spin g-factor (more often called simply the electron g-factor) g$_e$, defined by ${\boldsymbol {\mu }}_{\text{s}}=g_{\text{e}}{\frac {\mu _{\text{B}}}{\hbar }}\mathbf {S} ,$ where μ$_s$ is the magnetic moment resulting from the spin of an electron, S is its spin angular momentum, and μ$_B$ = eħ/2m$_e$ is the Bohr magneton. In atomic physics, the electron spin g-factor is often defined as the absolute value of g$_e$: $g_{\text{s}}=|g_{\text{e}}|=-g_{\text{e}}.$
The z component of the magnetic moment then becomes $\mu _{\text{z}}=-g_{\text{s}}\mu _{\text{B}}m_{\text{s}},$ where $\hbar m_{\text{s}}$ are the eigenvalues of the S$_z$ operator, meaning that m$_s$ can take on values $\pm 1/2$.
The value g$_s$ is roughly equal to 2.002319 and is known to extraordinary precision – one part in 10$^{13}$. The reason it is not precisely two is explained by quantum electrodynamics calculation of the anomalous magnetic dipole moment.

#### Electron orbital g-factor

Secondly, the electron orbital g-factor g$_L$ is defined by ${\boldsymbol {\mu }}_{L}=-g_{L}{\frac {\mu _{\text{B}}}{\hbar }}\mathbf {L} ,$ where μ$_L$ is the magnetic moment resulting from the orbital angular momentum of an electron, L is its orbital angular momentum, and μ$_B$ is the Bohr magneton. For an infinite-mass nucleus, the value of g$_L$ 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 m$_l$, the z component of the orbital magnetic moment is $\mu _{z}=-g_{L}\mu _{\text{B}}m_{l},$ which, since g$_L$ = 1, is −μ$_B$m$_l$.
For a finite-mass nucleus, there is an effective g value $g_{L}=1-{\frac {1}{M}},$ where M is the ratio of the nuclear mass to the electron mass.

#### Total angular momentum (Landé) g-factor

Thirdly, the Landé g-factor g$_J$ is defined by $|{\boldsymbol {\mu }}_{J}|=g_{J}{\frac {\mu _{\text{B}}}{\hbar }}|\mathbf {J} |,$ where μ$_J$ 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 g$_J$ is related to g$_L$ and g$_s$ by a quantum-mechanical argument; see the article Landé g-factor. μ$_J$ and J vectors are not collinear, so only their magnitudes can be compared.

### Muon g-factor

The muon, like the electron, has a g-factor associated with its spin, given by the equation ${\boldsymbol {\mu }}=g{e \over 2m_{\mu }}\mathbf {S} ,$ where μ is the magnetic moment resulting from the muon's spin, S is the spin angular momentum, and m$_μ$ is the muon mass.
That the muon g-factor is not quite the same as the electron g-factor is mostly explained by quantum electrodynamics and its calculation of the anomalous magnetic dipole moment. Almost all of the small difference between the two values (99.96% of it) is due to a well-understood lack of heavy-particle diagrams contributing to the probability for emission of a photon representing the magnetic dipole field, which are present for muons, but not electrons, in QED theory. These are entirely a result of the mass difference between the particles.
However, not all of the difference between the g-factors for electrons and muons is exactly explained by the Standard Model. The muon g-factor can, in theory, be affected by physics beyond the Standard Model, so it has been measured very precisely, in particular at the Brookhaven National Laboratory. In the E821 collaboration final report in November 2006, the experimental measured value is 2.0023318416(13), compared to the theoretical prediction of 2.00233183620(86). This is a difference of 3.4 standard deviations, suggesting that beyond-the-Standard-Model physics may be a contributory factor. The Brookhaven muon storage ring was transported to Fermilab where the Muon g–2 experiment used it to make more precise measurements of muon g-factor. On April 7, 2021, the Fermilab Muon g−2 collaboration presented and published a new measurement of the muon magnetic anomaly. When the Brookhaven and Fermilab measurements are combined, the new world average differs from the theory prediction by 4.2 standard deviations.

## Measured g-factor values

CODATA recommended g-factor values :
| Particle | Symbol | g-factor | Relative standard uncertainty |
| electron | g$_e$ | −2.00231930436092(36) | 1.8×10$^{−13}$‍ |
| muon | g$_μ$ | −2.00233184123(82) | 4.1×10$^{−10}$‍ |
| proton | g$_p$ | +5.5856946893(16) | 2.9×10$^{−10}$‍ |
| neutron | g$_n$ | −3.82608552(90) | 2.4×10$^{−7}$‍ |
The electron g-factor is one of the most precisely measured values in physics.