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
“…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.…”
Quantum bits based on Majorana zero modes are expected to be robust against certain noise types, and hence provide a quantum computing platform that is superior to conventional qubits. This robustness is not complete though: imperfections can still lead to qubit decoherence and hence to information loss. In this work, we theoretically study Majorana-qubit dephasing in a minimal model: in a Kitaev chain with quasistatic disorder. Our approach, based on numerics as well as first-order non-degenerate perturbation theory, provides a conceptually simple physical picture and predicts Gaussian dephasing. We show that, as system parameters are varied, the dephasing rate due to disorder oscillates out-of-phase with respect to the oscillating Majorana splitting of the clean system. In our model, first-order dephasing sweet spots are absent if disorder is uncorrelated. We describe the crossover between uncorrelated and highly correlated disorder, and show that dephasing measurements can be used to characterize the disorder correlation length. We expect that our results will be utilized for the design and interpretation of future Majorana-qubit experiments.
“…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.…”
Quantum bits based on Majorana zero modes are expected to be robust against certain noise types, and hence provide a quantum computing platform that is superior to conventional qubits. This robustness is not complete though: imperfections can still lead to qubit decoherence and hence to information loss. In this work, we theoretically study Majorana-qubit dephasing in a minimal model: in a Kitaev chain with quasistatic disorder. Our approach, based on numerics as well as first-order non-degenerate perturbation theory, provides a conceptually simple physical picture and predicts Gaussian dephasing. We show that, as system parameters are varied, the dephasing rate due to disorder oscillates out-of-phase with respect to the oscillating Majorana splitting of the clean system. In our model, first-order dephasing sweet spots are absent if disorder is uncorrelated. We describe the crossover between uncorrelated and highly correlated disorder, and show that dephasing measurements can be used to characterize the disorder correlation length. We expect that our results will be utilized for the design and interpretation of future Majorana-qubit experiments.
“…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.…”
Quantum bits based on Majorana zero modes are expected to be robust against certain noise types, and hence provide a quantum computing platform that is superior to conventional qubits. This robustness is not complete though: imperfections can still lead to qubit decoherence and hence to information loss. In this work, we theoretically study Majorana-qubit dephasing in a minimal model: in a Kitaev chain with quasistatic disorder. Our approach, based on numerics as well as first-order non-degenerate perturbation theory, provides a conceptually simple physical picture and predicts Gaussian dephasing. We show that, as system parameters are varied, the dephasing rate due to disorder oscillates out-of-phase with respect to the oscillating minigap of the clean system. In our model, first-order dephasing sweet spots are absent, a feature that can be used to characterize the spatial structure of noise in a dephasing experiment. We expect that our results will be utilized for the design and interpretation of future Majorana-qubit experiments.
“…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
Quantum-dot based parity-to-charge conversion is a promising method for reading out quantum information encoded nonlocally into pairs of Majorana zero modes. To obtain a sizable parity-tocharge visibility, it is crucial to tune the relative phase of the tunnel couplings between the dot and the Majorana modes appropriately. However, in the presence of multiple quasi-degenerate dot orbitals, it is in general not experimentally feasible to tune all couplings individually. This paper shows that such configurations could make it difficult to avoid a destructive multi-orbital interference effect that substantially reduces the read-out visibility. We analyze this effect using a Lindblad quantum master equation. This exposes how the experimentally relevant system parameters enhance or suppress the visibility when strong charging energy, measurement dissipation and, most importantly, multi-orbital interference is accounted for. In particular, we find that an intermediate-time readout could mitigate some of the interference-related visibility reductions affecting the stationary limit.
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