2018
DOI: 10.1103/physrevx.8.041032
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Single-Shot Single-Gate rf Spin Readout in Silicon

Abstract: For solid-state spin qubits, single-gate RF readout can help minimise the number of gates required for scale-up to many qubits since the readout sensor can integrate into the existing gates required to manipulate the qubits [1,2]. However, a key requirement for a scalable quantum computer is that we must be capable of resolving the qubit state within single-shot, that is, a single measurement [3].Here we demonstrate single-gate, single-shot readout of a singlet-triplet spin state in silicon, with an average re… Show more

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Cited by 88 publications
(72 citation statements)
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References 35 publications
(54 reference statements)
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“…In summary, we have characterised a gate-based approach for spin-qubit measurements in a future silicon quantum processor.The signal-to-noise ratio obtained with a simple resonant circuit is sufficient to read out the electronic spin state in a single shot. Our results, together with contemporaneous results in several other silicon quantum dot architectures [31][32][33], open a path to the readout of many spin qubits in parallel, using a compact gate design that will be needed for large-scale quantum processors of the future. SET current (left) and dispersive response (right) measured after initialising either via A1 → A2, to initialise S, or via B1 → B2 to initialise a mixed state between S and the three triplets (pulse sequence is shown in inset).…”
mentioning
confidence: 59%
“…In summary, we have characterised a gate-based approach for spin-qubit measurements in a future silicon quantum processor.The signal-to-noise ratio obtained with a simple resonant circuit is sufficient to read out the electronic spin state in a single shot. Our results, together with contemporaneous results in several other silicon quantum dot architectures [31][32][33], open a path to the readout of many spin qubits in parallel, using a compact gate design that will be needed for large-scale quantum processors of the future. SET current (left) and dispersive response (right) measured after initialising either via A1 → A2, to initialise S, or via B1 → B2 to initialise a mixed state between S and the three triplets (pulse sequence is shown in inset).…”
mentioning
confidence: 59%
“…They ensure that the operators appearing in Eq. (16) are expressed in a basis that is close to the true eigenbasis of the full system Hamiltonian H. If the transition term becomes resonant, the resulting change of basis enables probe photons to generate new transitions between the system eigenstates.…”
Section: A Dispersive Limitmentioning
confidence: 99%
“…1(b), resulting in a large gate-coupling factor, α = 0.95±0.06, similar to previously reported values 11,12 . The results presented in this paper are performed in a cryo-free dilution refrigerator using gate-based reflectometry and homodyne detection [13][14][15][16][17] .For the typically large impedances of nanoelectronic devices at radio-frequencies, the circuit's resonant frequency is f 0 ≈ 1/(2π √ LC tot ) where C tot = C t +C d +C p . The equivalent impedance at resonance is arXiv:1807.07842v2 [cond-mat.mes-hall]…”
mentioning
confidence: 99%
“…1(b), resulting in a large gate-coupling factor, α = 0.95±0.06, similar to previously reported values 11,12 . The results presented in this paper are performed in a cryo-free dilution refrigerator using gate-based reflectometry and homodyne detection [13][14][15][16][17] .…”
mentioning
confidence: 99%