The thermal conductance of mechanically suspended nanostructures has recent
ly received much attention, in part due to the recent prediction and observ
ation of the quantum limit for thermal conductance, which is observed in lo
ng, thin insulating beams at very low temperatures [D. E. Angelescu, M. C.
Cross, and M. L. Roukes, Superlattices Microstruct. 23, 673 (1998); K. Schw
ab, E. A. Henriksen, J. M. Norlock, and M. L. Roukes, Nature 404, 974 (2000
); I. G. C. Rego and G. Kirczenow, Phys. Rev. Lett. 81. 232 (1998); M. P, B
lencowe. Phys. Rev. B 59. 4992 (1999)]. In this brief report, we describe a
model calculation where the simple beam used to calculate quantum conducta
nce [L. G. C. Rego and G. Kirczenow, Phys. Rev. Lett. 81, 232 (1998)] is re
placed by a beam made from an artificial one-dimensional phononic crystal.
We find that at the lowest temperatures and longest thermal-phonon waveleng
ths, the quantum limit is recovered, while for intermediate temperatures, w
here the dominant phonon wavelength is of the order of the phononic-crystal
repeat distance, a significant suppression of the conductance is predicted
. At higher temperatures the conductance returns to that of a simple beam.