Elementary excitations in weakly interacting quantum fluids have a correlated
particle-hole nature that leads to spectacular macroscopic quantum phenomena
such as superfluidity. This many-body character was established in the context
of cold-atom condensates at thermal equilibrium in the framework of
Bogoliubov's celebrated theory of the weakly interacting Bose gas. Bogoliubov
excitations were also found to be highly relevant to driven-dissipative quantum
fluid of light, with certain resulting phenomena strikingly analogue to their
equilibrium counterparts, but also genuine out-of-equilibrium aspects. In this
work, we investigate both theoretically and experimentally a regime in which
the elementary excitations in a quantum fluid of light result dominantly from
their interaction with thermal lattice phonons, namely the elementary
vibrations of the crystal. By an accurate comparison with the theoretically
predicted spectral function of the driven-dissipative quantum fluid we achieve
a quantitative understanding of the particle-hole nature of the elementary
excitations, and unveil a remarkable decoupling from thermal excitations which
is expected to be relevant in equilibrium quantum fluids as well. Finally, we
exploit this quantitative understanding to identify a crossover temperature
around 1K, below which the lattice phonons are sufficiently quieted down
for the quantum fluctuations to take over in the generation of Bogoliubov
excitations. This regime is highly desired as it is characterized by strong
quantum correlations between Bogoliubov excitations.Comment: Main text: 22 pages 6 figures, Supplementary Information : 4 pages, 3
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