Larmor precession

 In physics, Larmor precession (named after Joseph Larmor) is the precession of the magnetic moment of an object about an external magnetic field. Objects with a magnetic moment also have angular momentum and effective internal electric current proportional to their angular momentum; these include electrons, protons, other fermions, many atomic and nuclear systems, as well as classical macroscopic systems. The external magnetic field exerts a torque on the magnetic moment,
where formula_2 is the torque, formula_3 is the magnetic dipole moment, formula_4 is the angular momentum vector, formula_5 is the external magnetic field, formula_6 symbolizes the cross product, and formula_7 is the gyromagnetic ratio which gives the proportionality constant between the magnetic moment and the angular momentum. The phenomenon is similar to the precession of a tilted classical gyroscope in an external torque-exerting gravitational field.
The angular momentum vector formula_4 precesses about the external field axis with an angular frequency known as the Larmor frequency,
where formula_10 is the angular frequency, and
formula_11 is the magnitude of the applied magnetic field.
formula_7 is (for a particle of charge formula_13) the gyromagnetic ratio, equal to formula_14, where formula_15 is the mass of the precessing system, while formula_16 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.
The above equation is the one that is used in most applications. However, a full treatment must include the effects of Thomas precession, yielding the equation (in CGS units) (The CGS units are used so that E has the same units as B):
where formula_7 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
Bargmann–Michel–Telegdi equation.
The spin precession of an electron in an external electromagnetic field is described by the Bargmann–Michel–Telegdi (BMT) equation 
where formula_21, formula_22, formula_15, and formula_24 are polarization four-vector, charge, mass, and magnetic moment, formula_25 is four-velocity of electron, formula_26, formula_27, and formula_28 is electromagnetic field-strength tensor. Using equations of motion,
one can rewrite the first term on the right side of the BMT equation as formula_30, where formula_31 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 formula_32 can be neglected, the particle's translational motion is described by
The BMT equation is then written as 
The Beam-Optical version of the Thomas-BMT, from the "Quantum Theory of Charged-Particle Beam Optics", applicable in accelerator optics
Applications.
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.
Precession direction.
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 its magnetic moment is opposite to that of its spin.