aiqbench analysis
This research establishes a fundamental quantum-geometric bound linking the Fubini-Study speed of state distinguishability to instantaneous symplectic stretching in driven bosonic systems. By proving that classical stability estimates can be converted into sharp quantum bounds, the study clarifies the relationship between dynamical instability and geometric rates even for exactly solvable multimode quadratic dynamics. The findings are significant for understanding limits in parametric amplifiers and other resonant pure squeezer configurations where these two natural system rates interact non-invertibly.
Quantum-Geometric Bound on Dynamical Instability in Bosonic Systems
arXiv:2608.12406v2 Announce Type: replace-cross Abstract: Quantum-geometric speed and dynamical instability are two natural rates for a driven quantum system, and their relation is unsettled even for exactly solvable dynamics. Here we show that for any multimode quadratic bosonic system referred to the bare-mode vacuum the Fubini-Study speed v_FS is the Frobenius norm of the symmetric, stretching part of the flow: the rate at which the vacuum becomes distinguishable from itself measures instantaneous symplectic stretching. That identity turns a classical stability estimate into a quantum-geometric bound, lambda_max <= sqrt(2) v_FS, sharp at every mode number and saturated by a resonant pure squeezer. The bound is not invertible: in a detuned parametric amplifier we hold either rate fixed while varying the other.
arXiv:2608.12406 (cond-mat)
Abstract:Quantum-geometric speed and dynamical instability are two natural rates for a driven quantum system, and their relation is unsettled even for exactly solvable dynamics. Here we show that for any multimode quadratic bosonic system referred to the bare-mode vacuum the Fubini-Study speed v_FS is the Frobenius norm of the symmetric, stretching part of the flow: the rate at which the vacuum becomes distinguishable from itself measures instantaneous symplectic stretching. That identity turns a classical stability estimate into a quantum-geometric bound, lambda_max <= sqrt(2) v_FS, sharp at every mode number and saturated by a resonant pure squeezer. The bound is not invertible: in a detuned parametric amplifier we hold either rate fixed while varying the other.
Mesoscale and Nanoscale Physics (cond-mat.mes-hall); Quantum Physics (quant-ph)
arXiv:2608.12406 [cond-mat.mes-hall]
(or arXiv:2608.12406v2 [cond-mat.mes-hall] for this version)
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Full text under the publisher's open licence · 205 words
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