Data-driven design of 12-fold quasicrystal nanomechanical resonators achieves Q_m of approximately 10^7 and force sensitivity of 26.4 aN per square root Hz.
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A proposed chip-scale device combines a transmon qubit, SQUID, and nanomechanical resonator to achieve projected gravitational sensitivity of 100-1000 nGal per square root Hz with sub-millisecond interrogation times.
Thin metallic foils mediate dissipative coupling between microwave cavities, producing controllable anti-resonances and enhanced phase response validated by experiment.
In Josephson junction chains, non-resonant two-into-two scattering dominates equilibrium plasmon decay rates while strong driving induces a crossover to a qualitatively different non-equilibrium steady state.
citing papers explorer
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Quasicrystal Architected Nanomechanical Resonators via Data-Driven Design
Data-driven design of 12-fold quasicrystal nanomechanical resonators achieves Q_m of approximately 10^7 and force sensitivity of 26.4 aN per square root Hz.
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Chip-scale superconducting quantum gravimeter combining a SQUID, a transmon, and a nanomechanical resonator
A proposed chip-scale device combines a transmon qubit, SQUID, and nanomechanical resonator to achieve projected gravitational sensitivity of 100-1000 nGal per square root Hz with sub-millisecond interrogation times.
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Equivalent Circuit Modeling of Foil-Mediated Dissipative Coupling in Microwave Cavities with Enhanced Phase Response
Thin metallic foils mediate dissipative coupling between microwave cavities, producing controllable anti-resonances and enhanced phase response validated by experiment.
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Plasmon decay and non-equilibrium steady states in Josephson junction chains
In Josephson junction chains, non-resonant two-into-two scattering dominates equilibrium plasmon decay rates while strong driving induces a crossover to a qualitatively different non-equilibrium steady state.