The photoionization of saturated antimony and bismuth vapors is invest
igated. In antimony, the dominant vapor species is Sb-4. Its photoion
yield curve is similar to those of P-4 and As-4, displaying three auto
ionizing bands and an apparent adiabatic IP of 7.56 eV. The appearance
potential of Sb-3(+)(Sb-4) occurs at 9.75(5-0.04)(+0.01) eV at 830 K,
or 10.22(9-0.04)(+0.01) eV at 0 K. This value, together with Delta (H
10Sb3)-Sb-Theta), yields IP(Sb-3) less than or equal to 6.61 eV. Bismu
th vapor contains approximate to 1% Bi-4 and even less Bi-3. The photo
ion yield curve of Bi-4(+), with an apparent adiabatic IP of 6.81 eV,
also displays three autoionizing bands. An analysis of these bands, an
d comparison with the other Group V tetramers with T-d symmetry enable
s one to estimate vertical IPs of 9.0 eV for (a(1))(-1), 7.5 and 8.9 e
V for the spin-orbit split (t(2))(-1), 7.0 and 7.4 eV for the Jahn-Tel
ler split (e)(-1). The photoion yield curve of Bi-3(+) has an adiabati
c onset of less than or equal to 6.36 eV, corresponding to formation o
f Bi-3(+), X(1)A(1)' in D-3h symmetry. An increase in slope at approxi
mate to 7.4 eV is identified with the configuration... (la(2)'')(2e')(
4)(le''), which may be an E' state. At approximate to 8.8 eV, a pronou
nced increase in slope may indicate a higher excited state, fragmentat
ion of Bi-4, or a near coincidence of the two. The directly or indirec
tly measured IPs of all Group V trimers are in fairly good agreement w
ith ab initio calculations. The heats of formation of the neutral trim
ers can be rationalized by a simple model involving transferability of
sigma and pi bond energies from the corresponding dimers and tetramer
s. The atomization energies of the trimer cations are significantly la
rger than for the corresponding neutrals, which may be related to the
closed shell structure of the cations.