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单电子石墨烯量子点中的自旋弛豫

Spin relaxation in a single-electron graphene quantum dot.

作者信息

Banszerus L, Hecker K, Möller S, Icking E, Watanabe K, Taniguchi T, Volk C, Stampfer C

机构信息

JARA-FIT and 2nd Institute of Physics, RWTH Aachen University, Aachen, Germany.

Peter Grünberg Institute (PGI-9), Forschungszentrum Jülich, Jülich, Germany.

出版信息

Nat Commun. 2022 Jun 25;13(1):3637. doi: 10.1038/s41467-022-31231-5.

Abstract

The relaxation time of a single-electron spin is an important parameter for solid-state spin qubits, as it directly limits the lifetime of the encoded information. Thanks to the low spin-orbit interaction and low hyperfine coupling, graphene and bilayer graphene (BLG) have long been considered promising platforms for spin qubits. Only recently, it has become possible to control single-electrons in BLG quantum dots (QDs) and to understand their spin-valley texture, while the relaxation dynamics have remained mostly unexplored. Here, we report spin relaxation times (T) of single-electron states in BLG QDs. Using pulsed-gate spectroscopy, we extract relaxation times exceeding 200 μs at a magnetic field of 1.9 T. The T values show a strong dependence on the spin splitting, promising even longer T at lower magnetic fields, where our measurements are limited by the signal-to-noise ratio. The relaxation times are more than two orders of magnitude larger than those previously reported for carbon-based QDs, suggesting that graphene is a potentially promising host material for scalable spin qubits.

摘要

单电子自旋的弛豫时间是固态自旋量子比特的一个重要参数,因为它直接限制了编码信息的寿命。由于低自旋 - 轨道相互作用和低超精细耦合,石墨烯和双层石墨烯(BLG)长期以来一直被认为是自旋量子比特的有前景的平台。直到最近,才能够在BLG量子点(QD)中控制单电子并了解它们的自旋 - 谷纹理,而弛豫动力学大多仍未被探索。在这里,我们报告了BLG量子点中单电子态的自旋弛豫时间(T)。使用脉冲栅极光谱,我们在1.9 T的磁场中提取出超过200μs的弛豫时间。T值显示出对自旋分裂的强烈依赖性,在较低磁场下有望获得更长的T值,在那里我们的测量受信噪比限制。这些弛豫时间比先前报道的基于碳的量子点的弛豫时间大两个数量级以上,这表明石墨烯是用于可扩展自旋量子比特的潜在有前景的主体材料。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6e63/9233672/861c3d3825bd/41467_2022_31231_Fig1_HTML.jpg

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