Heat transport in the quantum Rabi model at weak interaction with the heat baths is controlled by the qubit-oscillator coupling. Universality of the linear conductance versus the temperature is found for , with a coupling-dependent Kondo-like temperature. At low temperature, coherent heat transfer via virtual processes yields a behavior with destructive interference in the presence of quasi-degeneracies in the spectrum. As the temperature increases, incoherent emission and absorption dominate and a maximum is reached at . In the presence of a bias on the qubit, the conductance makes a transition from a resonant to a broad, zero-bias peak regime. Parallels and differences are found compared to the spin-boson model in [K. Saito and T. Kato, Phys. Rev. Lett. , 214301 (2013)], where the qubit-bath coupling instead of the internal qubit-oscillator coupling rules thermal transport.

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