Abstract

The energy landscape of a single electron in a triple quantum dot can be tuned such that the energy separation between ground and excited states becomes a flat function of the relevant gate voltages. These so-called sweet spots are beneficial for charge coherence, since the decoherence effects caused by small fluctuations of gate voltages or surrounding charge fluctuators are minimized. We propose a new operation point for a triple quantum dot charge qubit, a so-called $CQ_3$-qubit, having a third order sweet spot. We show strong coupling of the qubit to single photons in a frequency tunable high-impedance SQUID-array resonator. In the dispersive regime we investigate the qubit linewidth in the vicinity of the proposed operating point. In contrast to the expectation for a higher order sweet spot, we there find a local maximum of the linewidth. We find that this is due to a non-negligible contribution of noise on the quadrupolar detuning axis not being in a sweet spot at the proposed operating point. While the original motivation to realize a low-decoherence charge qubit was not fulfilled, our analysis provides insights into charge decoherence mechanisms relevant also for other qubits.

Highlights

  • A single electron occupying two tunnel coupled quantum dots can be operated as a charge qubit [1,2,3,4,5,6,7,8]

  • In order to understand the evolution of the qubit linewidth as a function of δ shown in Fig. 4(b), we investigate the different contributions building up the noise spectrum of the qubit

  • We have proposed and measured a singleelectron qubit hosted in a triple quantum dot with a third-order sweet spot in the detuning parameter δ

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Summary

INTRODUCTION

A single electron occupying two tunnel coupled quantum dots can be operated as a charge qubit [1,2,3,4,5,6,7,8] Control parameters of this qubit are the interdot tunnel coupling t as well as the detuning δ defined as the energy difference between the left and right dot electrochemical potentials. The quadrupole qubit has recently been investigated experimentally [18] by strongly coupling it to a single photon in a superconducting microwave resonator It has a single sweet spot at δ = EM = 0 in both detuning parameters, since at this point ∂E02/∂δ = ∂E02/∂EM = 0. We develop a noise model explaining our experimental findings

THEORY
RESULTS
CONCLUSION
Magnetic noise
Charge noise
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