2020
DOI: 10.1103/physrevlett.124.170502
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Hybrid Quantum Computing with Conditional Beam Splitter Gate in Trapped Ion System

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Cited by 51 publications
(44 citation statements)
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“…Such a operator is used as an entangles of output fields [31,32]. Recently, a conditional beam-splitter quantum gate between the ion's spin states and the two radial modes of single trapped ion was demonstrated [33]. As we see the relevant information of the parameter λ is encoded in the phase θ and thus it can be determined by detecting the phonon state populations e.g., either by detecting axial breathing or radial rocking phonon distributions.…”
Section: B Casementioning
confidence: 88%
“…Such a operator is used as an entangles of output fields [31,32]. Recently, a conditional beam-splitter quantum gate between the ion's spin states and the two radial modes of single trapped ion was demonstrated [33]. As we see the relevant information of the parameter λ is encoded in the phase θ and thus it can be determined by detecting the phonon state populations e.g., either by detecting axial breathing or radial rocking phonon distributions.…”
Section: B Casementioning
confidence: 88%
“…This interaction is useful for CVQC [2,4,53], and can also be used to cool multiple motional modes of trapped ion crystals [57,58]. This interaction was experimentally demonstrated in trapped ions by modulating the voltages of the trap electrodes [57], and with a running optical lat-tice [32]. Instead, we here implement Eq.…”
Section: Beam Splittermentioning
confidence: 99%
“…Existing schemes that generate nonlinear interactions with respect to their motional coupling are ∝ η 2 or higher order, making them significantly weaker than ∝ η interactions. These higher-order interactions include the state-dependent * robert.sutherland@utsa.edu beam splitter and one-or two-mode squeezing operations, and can also be used to generate non-Gaussian states [32][33][34].…”
Section: Introductionmentioning
confidence: 99%
“…While such strategies provide advantages over linear interferometry, these techniques often rely on strong nonlinearities which are difficult to engineer or are applicable only to a specific type of quantum system. In contrast, swap gates provide highly nonlinear interactions and, although challenging, are available in a broad range of experimental platforms [32][33][34][35][36] and are thus ideally suited for nonlinear interferometry. The controlled-swap gate is a particularly attractive gate as it is an essential ingredient of swap tests which are useful for measuring properties of quantum states without full tomography [37], in particular state overlap and purity [38,39], and other verification tasks [40].…”
mentioning
confidence: 99%
“…The second swap test is then used to estimate a phase shift on one of the modes from the probability that an antisymmetric state will be projected onto the symmetric subspace or vice versa. In trappedion and superconducting systems, where the controlledswap gates are readily available [34,36,39], interferometry with NOON states becomes much more straightforward: a NOON state can be both prepared and measured in a single step irrespective of its size. The only resource needed is then an input Fock state |n , for which efficient preparation methods exist in both circuit QED [41][42][43] and trapped-ion systems [44,45].…”
mentioning
confidence: 99%