Optoelectronic devices are increasingly important in communication and info
rmation technology. To achieve the necessary manipulation of light (which c
arries information in optoelectronic devices), considerable efforts are dir
ected at the development of photonic crystals-periodic dielectric materials
that have so-called photonic bandgaps, which prohibit the propagation of p
hotons having energies within the bandgap region. Straightforward applicati
on of the bandgap concept is generally thought to require three-dimensional
(3D) photonic crystals(1-5); their two-dimensional (2D) counterparts confi
ne light in the crystal plane(6,7), but not in the perpendicular z directio
n, which inevitably leads to diffraction losses. Nonetheless, 2D photonic c
rystals still attract interest(8-15) because they are potentially more amen
able to fabrication by existing techniques and diffraction losses need not
seriously impair utility. Here we report the fabrication of a waveguide-cou
pled photonic crystal slab (essentially a free-standing 2D photonic crystal
) with a strong 2D bandgap at wavelengths of about 1.5 mum, yet which is ca
pable of fully controlling light in all three dimensions. These features co
nfirm theoretical calculations(16,17) on the possibility of achieving 3D li
ght control using 2D bandgaps, with index guiding providing control in the
third dimension, and raise the prospect of being able to realize unusual ph
otonic-crystal devices, such as thresholdless lasers(1).