Spin-exchange interaction

A spin-exchange interaction preserves total angular momentum of the system but may allow other aspects of the system to change. When two spin-polarized atoms in their ground state experience a spin-exchange collision, the total spin of the atoms is preserved yet the orientation of the individual spins may change. For example, if atoms $A$ and $B$ are oppositely polarized, a spin-exchange collision reverses the spins: [cite journal
author=Happer, W. and Tam, A. C.
title=Effect of rapid spin exchange on the magnetic-resonance spectrum of alkali vapors
journal=Physical Review A |year=1977 |volume=16|number=5|pages=1877–1891
doi=10.1103/PhysRevA.16.1877
url=http://link.aps.org/abstract/PRA/v16/p1877] :$A(uparrow)\; +\; B(downarrow)\; ightarrow\; A(downarrow)\; +\; B(uparrow)$In a typical vapor of alkali metal atoms, spin-exchange collisions are the dominant type of interaction between atoms. The collisions happen so rapidly that they only alter the state of the electron spins and do not significantly affect the nuclear spins. Thus, spin-exchange collisions between alkali metal atoms can change the hyperfine state of the atoms while preserving total angular momentum of the colliding pair. As a result, spin-exchange collisions cause decoherence in ensembles of polarized atoms precessing in the presence of a magnetic field.

The time between spin-exchange collisions for a vapor of alkali metal atoms is:where the spin exchange cross section for alkali metals such as K, Rb, and Cs is:$sigma\_\{se\}\; =\; 2\; imes\; 10^\{-14\}\; mathrm\{cm\}^\{2\}$and where $n$ is the vapor density and is the average relative velocity given by the Maxwell-Boltzmann distribution::where $R$ is the ideal gas constant, $T$ is the temperature, and $m$ is the molar mass of the atoms.

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