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双层石墨烯中自旋-谷保护的克莱默斯对。

Spin-valley protected Kramers pair in bilayer graphene.

作者信息

Denisov Artem O, Reckova Veronika, Cances Solenn, Ruckriegel Max J, Masseroni Michele, Adam Christoph, Tong Chuyao, Gerber Jonas D, Huang Wei Wister, Watanabe Kenji, Taniguchi Takashi, Ihn Thomas, Ensslin Klaus, Duprez Hadrien

机构信息

Laboratory for Solid State Physics, ETH Zurich, Zurich, Switzerland.

Research Center for Functional Materials, National Institute for Materials Science, Tsukuba, Japan.

出版信息

Nat Nanotechnol. 2025 Apr;20(4):494-499. doi: 10.1038/s41565-025-01858-8. Epub 2025 Feb 10.

DOI:10.1038/s41565-025-01858-8
PMID:39930102
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC12015173/
Abstract

The intrinsic valley degree of freedom makes bilayer graphene (BLG) a unique platform for semiconductor qubits. The single-carrier quantum dot (QD) ground state exhibits a twofold degeneracy, where the two states that constitute a Kramers pair have opposite spin and valley quantum numbers. Because of the valley-dependent Berry curvature, an out-of-plane magnetic field breaks the time-reversal symmetry of this ground state and a qubit can be encoded in the spin-valley subspace. The Kramers states are protected against known spin- and valley-mixing mechanisms because mixing requires a simultaneous change of the two quantum numbers. Here, we fabricate a tunable QD device in Bernal BLG and measure a spin-valley relaxation time for the Kramers states of 38 s at 30 mK, which is two orders of magnitude longer than the 0.4 s measured for purely spin-blocked states. We also show that the intrinsic Kane-Mele spin-orbit splitting enables a Kramers doublet single-shot readout even at zero magnetic field with a fidelity above 99%. If these long-lived Kramers states also possess long coherence times and can be effectively manipulated, electrostatically defined QDs in BLG may serve as long-lived semiconductor qubits, extending beyond the spin qubit paradigm.

摘要

本征谷自由度使双层石墨烯(BLG)成为半导体量子比特的独特平台。单载流子量子点(QD)基态呈现双重简并,构成克莱默斯对的两个态具有相反的自旋和谷量子数。由于谷依赖的贝里曲率,面外磁场打破了该基态的时间反演对称性,并且量子比特可以编码在自旋 - 谷子空间中。克莱默斯态受到已知的自旋和谷混合机制的保护,因为混合需要两个量子数同时改变。在这里,我们在伯纳尔双层石墨烯中制造了一个可调谐量子点器件,并在30 mK温度下测量了克莱默斯态的自旋 - 谷弛豫时间为38 s,这比纯自旋阻塞态测量的0.4 s长两个数量级。我们还表明,本征的凯恩 - 梅勒自旋 - 轨道分裂即使在零磁场下也能实现克莱默斯二重态的单次读出,保真度超过99%。如果这些长寿命的克莱默斯态也具有长相干时间并且能够被有效操纵,双层石墨烯中静电定义的量子点可能用作长寿命半导体量子比特,超越自旋量子比特范式。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1f5a/12015173/3a1a80e86683/41565_2025_1858_Fig7_ESM.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1f5a/12015173/a1835837840c/41565_2025_1858_Fig1_HTML.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1f5a/12015173/b8717a52efd3/41565_2025_1858_Fig4_ESM.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1f5a/12015173/7994fd469cd4/41565_2025_1858_Fig5_ESM.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1f5a/12015173/6edd55fbf66e/41565_2025_1858_Fig6_ESM.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1f5a/12015173/3a1a80e86683/41565_2025_1858_Fig7_ESM.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1f5a/12015173/a1835837840c/41565_2025_1858_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1f5a/12015173/d5ba9a927c65/41565_2025_1858_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1f5a/12015173/b856348aa1e3/41565_2025_1858_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1f5a/12015173/b8717a52efd3/41565_2025_1858_Fig4_ESM.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1f5a/12015173/7994fd469cd4/41565_2025_1858_Fig5_ESM.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1f5a/12015173/6edd55fbf66e/41565_2025_1858_Fig6_ESM.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1f5a/12015173/3a1a80e86683/41565_2025_1858_Fig7_ESM.jpg

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Nano Lett. 2023 Jul 12;23(13):6171-6177. doi: 10.1021/acs.nanolett.3c01779. Epub 2023 Jun 26.
3
Particle-hole symmetry protects spin-valley blockade in graphene quantum dots.粒子-空穴对称性保护石墨烯量子点中的自旋-谷阻塞。
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