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A coherent input drive w is applied at one port, and the output field z is monitored at another port.
Therefore, it is possible to maintain the power efficiency at the same maximum level for lower input drive levels.
Most sophisticated test rigs use an iterative algorithm that generates the input drive files that reproduce service environments under laboratory conditions.
A coherent input drive (w) from a widely tunable telecom laser is coupled onto chip from a lensed fiber into port 1.
However, for a strong input drive, low tunneling rates and intermediate to high values of the nonlinearity the Bogoliubov expansion breaks down.
To compensate for such losses, cavity arrays are thus most naturally studied in a regime where an input drive continuously replaces the dissipated excitations.
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For opposite phases of the input drives one finds a destructive interference which suppresses population of the central cavity, whereas for input drives in phase the central cavity is populated with anti-bunched excitations due to its strong nonlinearity.
The oscillation of the excitation number in the central cavity is a result of the interference between the two coherent input drives.
For high input drives however, the theoretical description of the system poses a challenge as conventional numerical methods quickly become computationally infeasible.
Arrays of circuit cavities offer fascinating perspectives for exploring quantum many-body systems in a driven dissipative regime where excitation losses are continuously compensated by coherent input drives.
Δ k = ω k − ω in is the detuning between the input drives and resonance frequency of excitations in the k th transmission line resonator.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com