In a large-N 1D Yukawa-SYK strange metal, the fermionic second Rényi entropy obeys a CFT-like scaling curve with effective central charge c_eff ≈ 1.6 and a finite fermion-boson entanglement length ℓ0 at T=0.
Quantum Brownian motion and the Third Law of thermodynamics
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abstract
The quantum thermodynamic behavior of small systems is investigated in presence of finite quantum dissipation. We consider the archetype cases of a damped harmonic oscillator and a free quantum Brownian particle. A main finding is that quantum dissipation helps to ensure the validity of the Third Law. For the quantum oscillator, finite damping replaces the zero-coupling result of an exponential suppression of the specific heat at low temperatures by a power-law behavior. Rather intriguing is the behavior of the free quantum Brownian particle. In this case, quantum dissipation is able to restore the Third Law: Instead of being constant down to zero temperature, the specific heat now vanishes proportional to temperature with an amplitude that is inversely proportional to the ohmic dissipation strength. A distinct subtlety of finite quantum dissipation is the result that the various thermodynamic functions of the sub-system do not only depend on the dissipation strength but depend as well on the prescription employed in their definition.
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Entanglement entropy of fermions in a strange metal
In a large-N 1D Yukawa-SYK strange metal, the fermionic second Rényi entropy obeys a CFT-like scaling curve with effective central charge c_eff ≈ 1.6 and a finite fermion-boson entanglement length ℓ0 at T=0.