Abstract:We consider the nonlinear effects in Jahn-Teller system of two coupled resonators interacting simultaneously with flux qubit using Circuit QED. Two frequency description of Jahn Teller system that inherits the networked structure of both nonlinear Josephson Junctions and harmonic oscillators is employed to describe the synchronous structures in multifrequency scheme. Emergence of dominating mode is investigated to analyze frequency locking by eigenvalue spectrum. Rabi Supersplitting is tuned for coupled and un… Show more
“…For simulation of our single photon transistor, we use the parameters of two-frequency JT system as a test bed in ref [19,27]. Coupling regimes is considered in weak, strong and ultrastrong regimes of circuit QED.…”
Section: Resultsmentioning
confidence: 99%
“…It is possible to tune the strength of the interaction between qubit and privileged mode in ultrastrong regime when disadvantaged mode interacts with the qubit in strong regime [19,27]. Privileged mode, in which coupling energies concentrated, dominates the system and behaves like the scattering center for the cavity fields.…”
Section: A Circuit Layout and Protocolmentioning
confidence: 99%
“…The thermal occupation number n th = 0.15 is taken as 100 mK [19,27]. D denotes the Lindblad type damping superoperators, κ shows the cavity photon loss rate.…”
Section: A Power Spectrum and Impedance Matchingmentioning
confidence: 99%
“…Different from the generic models [36,37], spontaneous emergence of synchronization [27,52] in the presence of virtual photon conversion [40][41][42][43] makes our model advantageous in coupled cavity systems for switching and sending photons. When the single photon gate field is sent to the coupled cavity system, the incoming field is split into two fields incident both on the left and right cavities by time-reversed process of single-photon generation.…”
Section: B Photon Blockade and Input/output Theorymentioning
confidence: 99%
“…As an electrical analog platform to simulate the nonlinearities [23][24][25][26], photon blockade and localization-delocalization transitions is investigated in coupled Superconducting Quantum Interference Devices (SQUIDS). Population imbalance between coupled resonators is used to synchronize the qubit dephasing in networked JT system wired up to outer circuitry on chip [27].…”
We consider the single photon transistor in coupled cavity system of resonators interacting with multilevel superconducting artificial atom simultaneously. Effective single mode transformation is used for the diagonalization of the hamiltonian and impedance matching in terms of the normal modes. Storage and transmission of the incident field are described by the interactions between the cavities controlling the atomic transitions of lowest lying states. Rabi splitting of vacuum induced multiphoton transitions is considered in input/output relations by the quadrature operators in the absence of the input field. Second order coherence functions are employed to investigate the photon blockade and delocalization-localization transitions of cavity fields. Spontaneous virtual photon conversion into real photons is investigated in localized and oscillating regimes. Reflection and transmission of cavity output fields are investigated in the presence of the multilevel transitions. Accumulation and firing of the reflected and transmitted fields are used to investigate the synchronization of the bunching spike train of transmitted field and population imbalance of cavity fields. In the presence of single photon gate field, gain enhancement is explained for transmitted regime.
“…For simulation of our single photon transistor, we use the parameters of two-frequency JT system as a test bed in ref [19,27]. Coupling regimes is considered in weak, strong and ultrastrong regimes of circuit QED.…”
Section: Resultsmentioning
confidence: 99%
“…It is possible to tune the strength of the interaction between qubit and privileged mode in ultrastrong regime when disadvantaged mode interacts with the qubit in strong regime [19,27]. Privileged mode, in which coupling energies concentrated, dominates the system and behaves like the scattering center for the cavity fields.…”
Section: A Circuit Layout and Protocolmentioning
confidence: 99%
“…The thermal occupation number n th = 0.15 is taken as 100 mK [19,27]. D denotes the Lindblad type damping superoperators, κ shows the cavity photon loss rate.…”
Section: A Power Spectrum and Impedance Matchingmentioning
confidence: 99%
“…Different from the generic models [36,37], spontaneous emergence of synchronization [27,52] in the presence of virtual photon conversion [40][41][42][43] makes our model advantageous in coupled cavity systems for switching and sending photons. When the single photon gate field is sent to the coupled cavity system, the incoming field is split into two fields incident both on the left and right cavities by time-reversed process of single-photon generation.…”
Section: B Photon Blockade and Input/output Theorymentioning
confidence: 99%
“…As an electrical analog platform to simulate the nonlinearities [23][24][25][26], photon blockade and localization-delocalization transitions is investigated in coupled Superconducting Quantum Interference Devices (SQUIDS). Population imbalance between coupled resonators is used to synchronize the qubit dephasing in networked JT system wired up to outer circuitry on chip [27].…”
We consider the single photon transistor in coupled cavity system of resonators interacting with multilevel superconducting artificial atom simultaneously. Effective single mode transformation is used for the diagonalization of the hamiltonian and impedance matching in terms of the normal modes. Storage and transmission of the incident field are described by the interactions between the cavities controlling the atomic transitions of lowest lying states. Rabi splitting of vacuum induced multiphoton transitions is considered in input/output relations by the quadrature operators in the absence of the input field. Second order coherence functions are employed to investigate the photon blockade and delocalization-localization transitions of cavity fields. Spontaneous virtual photon conversion into real photons is investigated in localized and oscillating regimes. Reflection and transmission of cavity output fields are investigated in the presence of the multilevel transitions. Accumulation and firing of the reflected and transmitted fields are used to investigate the synchronization of the bunching spike train of transmitted field and population imbalance of cavity fields. In the presence of single photon gate field, gain enhancement is explained for transmitted regime.
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