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硅晶体管中两个耦合受主原子自旋轨道态的读出与控制。

Readout and control of the spin-orbit states of two coupled acceptor atoms in a silicon transistor.

作者信息

van der Heijden Joost, Kobayashi Takashi, House Matthew G, Salfi Joe, Barraud Sylvain, Laviéville Romain, Simmons Michelle Y, Rogge Sven

机构信息

School of Physics and Australian Centre of Excellence for Quantum Computation and Communication Technology, UNSW, Sydney, Australia.

University of Grenoble Alpes and CEA, LETI, MINATEC, 38000 Grenoble, France.

出版信息

Sci Adv. 2018 Dec 7;4(12):eaat9199. doi: 10.1126/sciadv.aat9199. eCollection 2018 Dec.

DOI:10.1126/sciadv.aat9199
PMID:30539142
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6286166/
Abstract

Coupling spin qubits to electric fields is attractive to simplify qubit manipulation and couple qubits over long distances. Electron spins in silicon offer long lifetimes, but their weak spin-orbit interaction makes electrical coupling challenging. Hole spins bound to acceptor dopants, spin-orbit-coupled = 3/2 systems similar to Si vacancies in SiC and single Co dopants, are an electrically active spin system in silicon. However, = 3/2 systems are much less studied than = 1/2 electrons, and spin readout has not yet been demonstrated for acceptors in silicon. Here, we study acceptor hole spin dynamics by dispersive readout of single-hole tunneling between two coupled acceptors in a nanowire transistor. We identify = ±1/2 and = ±3/2 levels, and we use a magnetic field to overcome the initial heavy-light hole splitting and to tune the = 3/2 energy spectrum. We find regimes of spin-like (+3/2 to -3/2) and charge-like (±1/2 to ±3/2) relaxations, separated by a regime of enhanced relaxation induced by mixing of light and heavy holes. The demonstrated control over the energy level ordering and hybridization are new tools in the = 3/2 system that are crucial to optimize single-atom spin lifetime and electrical coupling.

摘要

将自旋量子比特与电场耦合,对于简化量子比特操作以及实现长距离量子比特耦合很有吸引力。硅中的电子自旋具有较长的寿命,但其较弱的自旋 - 轨道相互作用使得电耦合颇具挑战。与碳化硅中的硅空位和单个钴掺杂剂类似的、与受主掺杂剂束缚的空穴自旋,即自旋 - 轨道耦合的J = 3/2系统,是硅中的一种电活性自旋系统。然而,J = 3/2系统的研究远少于J = 1/2电子,并且尚未证明硅中受主的自旋读出。在此,我们通过对纳米线晶体管中两个耦合受主之间的单空穴隧穿进行色散读出,来研究受主空穴自旋动力学。我们识别出J = ±1/2和J = ±3/2能级,并利用磁场克服初始的重 - 轻空穴分裂,以及调节J = 3/2能谱。我们发现了类自旋(+3/2到 -3/2)和类电荷(±1/2到 ±3/2)弛豫的区域,它们被由轻空穴和重空穴混合引起的增强弛豫区域隔开。所展示的对能级排序和杂化的控制,是J = 3/2系统中的新工具,对于优化单原子自旋寿命和电耦合至关重要。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5744/6286166/b3071f26dc0a/aat9199-F4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5744/6286166/d5cbe2ec2cbe/aat9199-F1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5744/6286166/ddc830a3190a/aat9199-F2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5744/6286166/cdfd1f3a68c2/aat9199-F3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5744/6286166/b3071f26dc0a/aat9199-F4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5744/6286166/d5cbe2ec2cbe/aat9199-F1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5744/6286166/ddc830a3190a/aat9199-F2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5744/6286166/cdfd1f3a68c2/aat9199-F3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5744/6286166/b3071f26dc0a/aat9199-F4.jpg

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Charge-Insensitive Single-Atom Spin-Orbit Qubit in Silicon.硅基电荷不敏感单原子自旋轨道量子比特
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