Energetics of an rf SQUID Coupled to Two Thermal Reservoirs
Fig 2
The stationary energy current J2 as a function of the external magnetic flux Φe.
Panel (a) for various temperatures of reservoirs: ({θ1, θ2} = {1, 10}, {1, 5}, {5, 10}. Panel (b) for = 0.1 and various Josephson energy: εJ = 8, 10, 12, 14. Panel (c) for εJ = 14 and various charging energy
= 0.1, 0.15, 0.225, 0.25.