The cooling of hot electrons in graphene is the critical process underlying
the operation of exciting new graphene-based optoelectronic and plasmonic
devices, but the nature of this cooling is controversial. We extract the hot
electron cooling rate near the Fermi level by using graphene as novel
photothermal thermometer that measures the electron temperature (T(t)) as it
cools dynamically. We find the photocurrent generated from graphene p−n
junctions is well described by the energy dissipation rate CdT/dt=−A(T3−Tl3), where the heat capacity is C=αT and Tl is the
base lattice temperature. These results are in disagreement with predictions of
electron-phonon emission in a disorder-free graphene system, but in excellent
quantitative agreement with recent predictions of a disorder-enhanced
supercollision (SC) cooling mechanism. We find that the SC model provides a
complete and unified picture of energy loss near the Fermi level over the wide
range of electronic (15 to ∼3000 K) and lattice (10 to 295 K) temperatures
investigated.Comment: 7pages, 5 figure