pith. sign in

(E1) is α(t) =Ce −κt/2 −ie −iϕd ε κ ,(E2) whereCis an integral constant depending on the initial condition

Linear resonator, three-segment pulse For a linear resonator (K r = 0) under a constant resonant drive [ε(t) =ε, ∆ = 0], the solution of Eq · 2000

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Probing excited-state dynamics of transmon ionization

quant-ph · 2025-05-01 · unverdicted · novelty 5.0

Experimental verification that transmon ionization under strong readout drives is a controllable Landau-Zener transition, with quantitative measurements of critical photon numbers and population transfer matching a semiclassical model.

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  • Probing excited-state dynamics of transmon ionization quant-ph · 2025-05-01 · unverdicted · none · ref 5

    Experimental verification that transmon ionization under strong readout drives is a controllable Landau-Zener transition, with quantitative measurements of critical photon numbers and population transfer matching a semiclassical model.