We describe a procedure for measuring the contribution of relativistic
positrons to radio synchrotron radiation. The method relies on the fa
ct that synchrotron radiation from particles of one sign (e.g., electr
ons) is circularly polarized by a small but measurable amount. If, on
the other hand, there are equal numbers of relativistic positrons and
electrons, the net circular polarization is zero. The method is illust
rated through high-accuracy mapping of the circular polarization of th
e Crab Nebula at 610 MHz. No significant circular polarization was det
ected: a very conservative limit is 0.05%, and a more realistic one is
0.03%. We calculate the degree of circular polarization expected if o
nly electrons are present, allowing for the reduction in polarization
resulting from nonuniformities in the magnetic held along the line of
sight and across the telescope beam. This reduction due to held nonuni
formity is estimated from measurements of the degree of linear polariz
ation at optical and high radio frequencies with similar angular resol
ution to the circular polarization measurements. We find that the obse
rved upper limit on the degree of circular polarization is comparable
to or below that expected if only electrons radiate. Various explanati
ons of this result are discussed, including (1) a weaker than assumed
magnetic field, (2) a held preferentially nearly perpendicular to the
line of sight, (3) a held structure of such a type that nonuniformitie
s reduce the degree of circular polarization by more than they reduce
the degree of linear polarization, and (4) the presence of relativisti
c positrons. Although explanation 1 is implausible, possibilities 2 an
d 3 cannot be excluded. If future observations establish that the degr
ee of circular polarization at 610 MHz is less than 0.01%, a contribut
ion from positrons would be strongly favored.