In physics, Larmor precession (named after Joseph Larmor) is the precession of the magnetic moments of electrons, muons, and all leptons with magnetic moments, which are quantum effects of particle spin, atomic nuclei, and atoms about an external magnetic field. The magnetic field exerts a torque on the magnetic moment,
where is the torque, is the magnetic dipole moment, is the angular momentum vector, is the external magnetic field, symbolizes the cross product, and is the gyromagnetic ratio which gives the proportionality constant between the magnetic moment and the angular momentum.
The angular momentum vector precesses about the external field axis with an angular frequency known as the Larmor frequency,
where is the angular frequency, and is the magnitude of the applied magnetic field. is (for a particle of charge ) the gyromagnetic ratio, equal to , where is the mass of the precessing system, while is the g-factor of the system. The g-factor is the unit-less proportionality factor relating the system's angular momentum to the intrinsic magnetic moment; in classical physics it is just 1.
In nuclear physics the g-factor of a given system includes the effect of the nucleon spins, their orbital angular momenta, and their couplings. Generally, the g-factors are very difficult to calculate for such many-body systems, but they have been measured to high precision for most nuclei. The Larmor frequency is important in NMR spectroscopy. The gyromagnetic ratios, which give the Larmor frequencies at a given magnetic field strength, have been measured and tabulated here.
Crucially, the Larmor frequency is independent of the polar angle between the applied magnetic field and the magnetic moment direction. This is what makes it a key concept in fields such as nuclear magnetic resonance (NMR) and electron paramagnetic resonance (EPR), since the precession rate does not depend on the spatial orientation of the spins.
Including Thomas precession
where is the relativistic Lorentz factor (not to be confused with the gyromagnetic ratio above). Notably, for the electron g is very close to 2 (2.002..), so if one sets g=2, one arrives at
The spin precession of an electron in an external electromagnetic field is described by the Bargmann–Michel–Telegdi (BMT) equation 
where , , , and are polarization four-vector, charge, mass, and magnetic moment, is four-velocity of electron, , , and is electromagnetic field-strength tensor. Using equations of motion,
one can rewrite the first term in the right side of the BMT equation as , where is four-acceleration. This term describes Fermi–Walker transport and leads to Thomas precession. The second term is associated with Larmor precession.
When electromagnetic fields are uniform in space or when gradient forces like can be neglected, the particle's translational motion is described by
The BMT equation is then written as 
A 1935 paper published by Lev Landau and Evgeny Lifshitz predicted the existence of ferromagnetic resonance of the Larmor precession, which was independently verified in experiments by J. H. E. Griffiths (UK) and E. K. Zavoiskij (USSR) in 1946.
Larmor precession is important in nuclear magnetic resonance, magnetic resonance imaging, electron paramagnetic resonance and muon spin resonance. It is also important for the alignment of cosmic dust grains, which is a cause of the polarization of starlight.
To calculate the spin of a particle in a magnetic field, one must also take into account Thomas precession.
The spin angular momentum of an electron precesses counter-clockwise about the direction of the magnetic field. An electron has a negative charge, so the direction of magnetic moment is opposite to that of its spin.
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