2015
DOI: 10.1038/ncomms8681
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Conditional rotation of two strongly coupled semiconductor charge qubits

Abstract: Universal multiple-qubit gates can be implemented by a set of universal single-qubit gates and any one kind of entangling two-qubit gate, such as a controlled-NOT gate. For semiconductor quantum dot qubits, two-qubit gate operations have so far only been demonstrated in individual electron spin-based quantum dot systems. Here we demonstrate the conditional rotation of two capacitively coupled charge qubits, each consisting of an electron confined in a GaAs/AlGaAs double quantum dot. Owing to the strong inter-q… Show more

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Cited by 63 publications
(62 citation statements)
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References 27 publications
(57 reference statements)
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“…So far, short range (∼ 100 nm) qubit-qubit interaction has been realized via capacitive or exchange coupling between charge [4][5][6] and spin qubits [7][8][9][10], which was expanded by making use of interactions mediated by additional qubits (∼ 400 nm) [11] or electronic cavities (∼ 1.7 µm) [12]. However, it is predicted that the range of interaction between semiconductor qubits can be increased significantly using microwave photons [3,13,14].…”
mentioning
confidence: 99%
“…So far, short range (∼ 100 nm) qubit-qubit interaction has been realized via capacitive or exchange coupling between charge [4][5][6] and spin qubits [7][8][9][10], which was expanded by making use of interactions mediated by additional qubits (∼ 400 nm) [11] or electronic cavities (∼ 1.7 µm) [12]. However, it is predicted that the range of interaction between semiconductor qubits can be increased significantly using microwave photons [3,13,14].…”
mentioning
confidence: 99%
“…关于用电荷量子比特构建两量子逻辑门, 研究者们主要利用的是电容耦合. 2009 年, 英国卡文迪 许实验室的 Petersson 等 [67] 和日本电信电话株式会社研究所的 Shinkai 等 [68] 都实现了两个电荷量 子比特的电容耦合, 但是均没有实现逻辑门操控, 直到 2015 年, 中国科学技术大学的郭国平教授研究 组利用电容耦合的两个电荷量子比特首次实现了两电荷量子比特的控制非 (Control-NOT, CNOT) 的 逻辑操作 [29] , 测量保真度达到 68%, 操作速度达到 6 GHz. 如图 11 为两电荷量子比特实验装置示意 图.…”
Section: 空穴编码的自旋量子比特unclassified
“…In the same way, the abrupt energy shift around the anti-crossing points ( 1 = 0 and  3 = 0) tells the value of their coupling strength: J 13 approximately equals 135 μeV. These large coupling strengths will enable us to implement three-qubit operations [18,24]. For instance, the coherent rotations of the target qubit, such as Larmor procession [8], Landau-Zener-Stütckelberg (LZS) interferences [9], and Rabi oscillations [10], usually occur when the qubit is brought from an initial state to its detuning anti-crossing point.…”
mentioning
confidence: 95%