Phonons are quantized collective excitations of a crystal lattice, which are the primary heat carriers in semiconductors and electrical insulators. We study phonon thermal transport in crystalline solids using non-contact laser-based pump-probe techniques.
One such experiment is the transient grating, where a pair of coherent pump laser pulses form an instantaneous sinusoidal thermal excitation on the sample. The temporal decay of this thermal excitation is measured by a low-power probe laser, from which the thermal conductivity of the sample can be obtained. This experiment is well-suited to measure both in-plane and cross-plane thermal conductivity of most materials, and does not suffer from parasitic losses due to contact and interface resistances.
An exciting feature of the transient grating in our lab is that we can measure non-diffusive heat conduction phenomena, where the conventional Fourier's law of heat diffusion no longer holds. The non-diffusive heat conduction regime occurs when the period of the sinusoidal pump excitation, which is the lengthscale of heat transport in this experiment, is systematically reduced to become comparable to, or smaller than, the phonon mean free path (the average distance travelled by phonons before undergoing collision or scattering). In fact, we use the transition from the Fourier-diffusive to non-diffusive heat flow regimes to actually extract phonon-specific mean free paths experimentally.