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Probing relaxation times in graphene quantum dots

机译:探测石墨烯量子点中的弛豫时间

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Graphene quantum dots are attractive candidates for solid-state quantum bits. In fact, thepredicted weak spin-orbit and hyperfine interaction promise spin qubits with long coherencetimes. Graphene quantum dots have been extensively investigated with respect to theirexcitation spectrum, spin-filling sequence and electron-hole crossover. However, theirrelaxation dynamics remain largely unexplored. This is mainly due to challenges in devicefabrication, in particular concerning the control of carrier confinement and the tunability ofthe tunnelling barriers, both crucial to experimentally investigate decoherence times. Here wereport pulsed-gate transient current spectroscopy and relaxation time measurements ofexcited states in graphene quantum dots. This is achieved by an advanced device design thatallows to individually tune the tunnelling barriers down to the low megahertz regime,while monitoring their asymmetry. Measuring transient currents through electronic excitedstates, we estimate a lower bound for charge relaxation times on the order of 60–100 ns.
机译:石墨烯量子点是固态量子位的有吸引力的候选者。实际上,所预测的弱自旋轨道和超精细相互作用承诺了具有长相干时间的自旋量子位。关于石墨烯量子点的激发光谱,自旋填充序列和电子-空穴交换,已经进行了广泛的研究。但是,它们的松弛动力学仍未得到充分探索。这主要归因于器件制造方面的挑战,特别是关于载流子限制的控制和隧穿势垒的可调性,这对于实验研究去相干时间都是至关重要的。在此进行了石墨烯量子点中激发态的脉冲脉冲门瞬态电流光谱和弛豫时间测量。这是通过先进的设备设计实现的,该设备设计可以在监视隧道势垒的不对称性的同时将其单独调节至低兆赫兹范围。通过测量通过电子激发态的瞬态电流,我们估计电荷弛豫时间的下限约为60–100 ns。

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