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2021
DOI: 10.21468/scipostphys.10.6.127
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Visibility of noisy quantum dot-based measurements of Majorana qubits

Abstract: Measurement schemes of Majorana zero modes (MZMs) based on quantum dots (QDs) are of current interest as they provide a scalable platform for topological quantum computation. In a coupled qubit-QD setup we calculate the dependence of the charge of the QD and its differential capacitance on experimentally tunable parameters for both 2-MZM and 4-MZM measurements. We quantify the effect of noise on the measurement visibility by considering 1/f noise in detuning, tunneling amplitudes or phase. We find that on- or… Show more

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Cited by 9 publications
(5 citation statements)
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“…In our dephasing calculation, we have chosen the quasistatic approximation also for its conceptual simplicity and widespread use in the literature 49,51 . In real devices, classical or quantum noise often follows a characteristic noise spectrum, e.g., 1/f noise 35,40,46,47,[55][56][57][68][69][70] , Johnson-Nyquist noise, quantum noise of phonons 35,36 , gate-voltage fluctuations 31,35,39,40 , etc. Going beyond the quasistatic approximation by incorporating these frequency-dependent noise features would be an important addition to this work.…”
Section: Discussionmentioning
confidence: 99%
“…In our dephasing calculation, we have chosen the quasistatic approximation also for its conceptual simplicity and widespread use in the literature 49,51 . In real devices, classical or quantum noise often follows a characteristic noise spectrum, e.g., 1/f noise 35,40,46,47,[55][56][57][68][69][70] , Johnson-Nyquist noise, quantum noise of phonons 35,36 , gate-voltage fluctuations 31,35,39,40 , etc. Going beyond the quasistatic approximation by incorporating these frequency-dependent noise features would be an important addition to this work.…”
Section: Discussionmentioning
confidence: 99%
“…In our dephasing calculation, we have chosen the quasistatic approximation also for its conceptual simplicity and widespread use in the literature 49,51 . In real devices, classical or quantum noise often follows a characteristic noise spectrum, e.g., 1/f noise 35,40,46,47,[55][56][57][67][68][69] , Johnson-Nyquist noise, quantum noise of phonons 35,36 , gate-voltage fluctuations 31,35,39,40 , etc. Going beyond the quasistatic approximation by incorporating these frequency-dependent noise features would be an important addition to this work.…”
Section: Discussionmentioning
confidence: 99%
“…The key difference to previous works [23,31,32,34,69] is that here, we do not assume the dot to be described by a single electronic level. We instead consider a more realistic multi-orbital scenario with M dot states j entering the dynamics.…”
Section: A Model and Readout Principlementioning
confidence: 93%
“…2(f), or when noise sources such as quasiparticle poisoning limit the measurement time. We emphasize, however, that this requires a challenging tuning of the phase φ with low parameter noise [69], as well as a good control of the initial dot state. The latter also involves gate operations faster than the typical decay rate Γ = gλ, as needs to be varied from some large initial detuning | | λ that strongly favors an empty or fully occupied dot level.…”
Section: Visibility In the Presence Of Charge Sensormentioning
confidence: 99%