Sokolov–Ternov effect

An electron in a magnetic field can have its spin oriented in the same ("spin up") or in the opposite ("spin down") direction with respect to the direction of the magnetic field (which is assumed to be oriented "up"). The "spin down" state has a higher energy than "spin up" state. The polarization arises due to the fact that the rate of transition through emission of synchrotron radiation to the "spin down" state is slightly greater than the probability of transition to the "spin up" state. As a result, an initially unpolarized beam of high-energy electrons circulating in a storage ring after sufficiently long time will have spins oriented in the direction opposite to the magnetic field. Saturation is not complete and is explicitly described by the formula[3]

${\displaystyle \xi (t)=A{\Bigl (}1-e^{-{\frac {t}{\tau }}}{\Bigr )}}$

where ${\displaystyle \scriptstyle A\;=\;8{\sqrt {3}}/15\;\approx \;0.924}$ is the limiting degree of polarization (92.4%) and ${\displaystyle \scriptstyle \tau }$ is the relaxation time,

${\displaystyle \tau =A{{{4\pi \epsilon _{0}\hbar }^{2}} \over {mc{e}^{2}}}{\Bigl (}{{mc^{2}} \over {E}}{\Bigr )}^{2}{\Bigl (}{H_{0} \over H}{\Bigr )}^{3}}$

Here ${\displaystyle \scriptstyle A}$ is as before, ${\displaystyle \scriptstyle m}$ and ${\displaystyle \scriptstyle e}$ are the mass and charge of the electron, ${\displaystyle \epsilon _{0}}$ is the vacuum permittivity, ${\displaystyle \scriptstyle c}$ is the speed of light, ${\displaystyle \scriptstyle H_{0}\;\approx \;4.414\,\times \,10^{13}\,{\text{gauss}}}$ is the Schwinger field, ${\displaystyle \scriptstyle H}$ is the magnetic field, and ${\displaystyle \scriptstyle E}$ is the electron energy.

The limiting degree of polarization ${\displaystyle A}$ is less than one due to the existence of spin-orbital energy exchange which allows for transitions to the "spin up" state (with probability 25.25 times less than to the "spin down" state).

Typical relaxation time is on the order of minutes and hours. Thus producing a highly polarized beam requires a long enough time and the use of storage rings.

The self-polarization effect for positrons is similar, with the only difference that positrons will tend to have spins oriented in the direction parallel to the direction of the magnetic field.[4]

The Sokolov–Ternov effect was experimentally observed in the USSR, France, Germany, United States, Japan, and Switzerland in storage rings with electrons of energy 1-50 GeV.[3][5]

• 1971 — Budker Institute of Nuclear Physics (first observation), with the use of 625 MeV storage ring VEPP-2.
• 1971 — Orsay (France), with the use of 536 MeV АСО storage ring.
• 1975 — Stanford (USA), with the use of 2.4 GeV SPEAR storage ring.
• 1980 — DESY, Hamburg (Germany), with the use of 15.2 GeV PETRA.

The effect of radiative polarization provides a unique capability for creating polarized beams of high-energy electrons and positrons that can be used for various experiments.

The effect also has been related to the Unruh effect which, up to now, under experimentally achievable conditions is too small to be observed.

The equilibrium polarization given by the Sokolov and Ternov has corrections when the orbit is not perfectly planar. The formula has been generalized by Derbenev and Kondratenko and others.[6]

• Sokolov A. A. and Ternov I. M. (1973): Award N 131 of 7 August 1973 with priority of 26 June 1963, Byull. Otkr. i Izobr., vol. 47.

• Unruh effect
• Hawking radiation
• Froissart–Stora equation