Substitutional boron impurities in diamond exhibit characteristic Lyman tra
nsitions, originating in the lower 1s(p(3/2)): Gamma(8) ground state and te
rminating in its spin-orbit split 1s(p(1/2)): Gamma(7) counterpart. In addi
tion to the Lyman spectrum observed in the infrared having p-like final sta
tes, the 1S(P-3/2) --> 1S(p(1/2)) transition (Delta') appears as an electro
nic Raman line. We have investigated the Zeeman effect bf the Delta' Raman
line for magnetic field B along different crystallographic directions, for
a variety of scattering geometries. The Zeeman components for B parallel to
[001], corresponding to pseudo-angular momentum change of 0, +/-2 (+/-1),
with incident light polarized perpendicular (parallel) to B, occur with rel
ative intensities proportional to the squares of the Luttinger parameters,
taking account of thermal depopulation effects. In addition, Raman transiti
ons within the 1s(p(3/2)) Zeeman multiplet, i.e. Raman electron-paramagneti
c-resonance (EPR) lines, are observed. Measurements yield g-factors for the
orbital and spin contributions to the Zeeman energy and are g(1) = -0.39 /- 0.04 and g(2) = -2.04 +/- 0.10, respectively, which characterize the Gam
ma(8) and Gamma(7) multiplets.