2018
DOI: 10.1103/physrevlett.120.150504
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Realization of a Λ System with Metastable States of a Capacitively Shunted Fluxonium

Abstract: We realize a Λ system in a superconducting circuit, with metastable states exhibiting lifetimes up to 8 ms. We exponentially suppress the tunneling matrix elements involved in spontaneous energy relaxation by creating a "heavy" fluxonium, realized by adding a capacitive shunt to the original circuit design. The device allows for both cavity-assisted and direct fluorescent readouts, as well as state preparation schemes akin to optical pumping. Since direct transitions between the metastable states are strongly … Show more

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Cited by 118 publications
(115 citation statements)
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“…Accordingly, we adopt a baseline superconducting noise model, labeled as SC, corresponding to a superconducting device which has 10x lower gate errors and 10x longer T 1 duration than the current IBM hardware. This range of parameters has already been achieved experimentally in superconducting devices for gate errors [55,56] and for T 1 duration [57,58] independently. Faster gates Noise Model 3p 1 15p 2 T 1 SC 10 −4 10 −3 1 ms SC+T1 10 −4 10 −3 10 ms SC+GATES 10 −5 10 −4 1 ms SC+T1+GATES 10 −5 10 −4 10 ms Table 2: Noise models simulated for superconducting devices.…”
Section: Superconducting Qcmentioning
confidence: 53%
“…Accordingly, we adopt a baseline superconducting noise model, labeled as SC, corresponding to a superconducting device which has 10x lower gate errors and 10x longer T 1 duration than the current IBM hardware. This range of parameters has already been achieved experimentally in superconducting devices for gate errors [55,56] and for T 1 duration [57,58] independently. Faster gates Noise Model 3p 1 15p 2 T 1 SC 10 −4 10 −3 1 ms SC+T1 10 −4 10 −3 10 ms SC+GATES 10 −5 10 −4 1 ms SC+T1+GATES 10 −5 10 −4 10 ms Table 2: Noise models simulated for superconducting devices.…”
Section: Superconducting Qcmentioning
confidence: 53%
“…The simplest manifestations involve improving quality factors associated with coupling to different thermal baths [42,48,49] and reducing noise spectral densities for different Hamiltonian parameters [13,50,51]. At a higher level, a popular approach to suppressing qubit relaxation has been to localize wavefunctions in disparate regions of phase space to lessen transition matrix elements [28,30,36,52]. On the other hand, delocalization of the same wavefunctions has been shown to mitigate dephasing effects by reducing qubit sensitivity to Hamiltonian parameters [10,18,43,[53][54][55].…”
Section: A Protectionmentioning
confidence: 99%
“…In contrast to the transmon, heavy fluxonium combines strong Josephson non-linearity with T 1 protection due to disjoint support of its lowest-lying localized wave functions. Heavy fluxonium devices utilize a decreased capacitive energy E C , which emphasizes the localization of states [28,30]. Moreover, fluxonium eigenenergies are intrinsically insensitive to slow offset charge variations [47].…”
Section: A Single-qubit Gatesmentioning
confidence: 99%
“…Experimentally, gates for heavy fluxonium have been realized by driving Raman transitions [28,29], which utilize intermediary higher-energy states to assist indirect transitions between the protected states. We will demonstrate a similar approach, exploiting the availability of intermediary state transitions using optimal control theory.…”
Section: A Single-qubit Gatesmentioning
confidence: 99%