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Mikhail Fistul

Publications and source records attributed to Mikhail Fistul.

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Bose condensation and Bogoliubov excitation in resonator-embedded superconducting qubit network

Superconducting qubit networks (SQNs) embedded in a low-dissipative resonator is a promising device allowing one not only to establish the collective quantum dynamics on a macroscopic scale but also to greatly enhance the sensitivity of detectors of microwave photons. A quantum ac Stark effect provided by coupling between an SQN and microwave photons of a resonator, leads to a strong nonlinear interaction between photons. Here, we present a two-tone spectroscopy experiment in which a set of 10 superconducting flux qubits is coupled to the input R- resonator and the output T- transmission line. An external microwave pump field close to the resonance frequency populates macroscopically the resonator mode as a Bose-Einstein condensate, while a second probe beam scans the resonances referred also as Bogoliubov-like excitations. The corresponding excitation frequency measured from the transmission coefficient, |S21(f)| displays an abrupt change of the resonant dip position once the power of the pump field overcomes a critical value Pcr. This sharp shift occurs in a narrow region of pump frequencies, and can be tuned by an applied magnetic field. It is a signature of bistability of the photon number inside the resonator, in agreement with theory.

quant-ph

Floquet Anderson Localization of Two Interacting Discrete Time Quantum Walks

We study the interplay of two interacting discrete time quantum walks in the presence of disorder. Each walk is described by a Floquet unitary map defined on a chain of two-level systems. Strong disorder induces a novel Anderson localization phase with a gapless Floquet spectrum and one unique localization length $ξ_1$ for all eigenstates for noninteracting walks. We add a local contact interaction which is parametrized by a phase shift $γ$. A wave packet is spreading subdiffusively beyond the bounds set by $ξ_1$ and saturates at a new length scale $ξ_2 \gg ξ_1$. In particular we find $ξ_2 \sim ξ_1^{1.2}$ for $γ=π$. We observe a nontrivial dependence of $ξ_2$ on $γ$, with a maximum value observed for $γ$-values which are shifted away from the expected strongest interaction case $γ=π$. The novel Anderson localization regime violates single parameter scaling for both interacting and noninteracting walks.

cond-mat.dis-nn