4.1 Article

Molecular Optimization for Nuclear Spin State Control via a Single Electron Spin Qubit by Optimal Microwave Pulses: Quantum Control of Molecular Spin Qubits

期刊

APPLIED MAGNETIC RESONANCE
卷 53, 期 3-5, 页码 777-796

出版社

SPRINGER WIEN
DOI: 10.1007/s00723-021-01392-5

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资金

  1. AOARD Scientific Project on Quantum Properties of Molecular Nanomagnets [FA2386-13-4029, 13-4030, 13-4031]
  2. AOARD Project on Molecular Spins for Quantum Technologies [FA2386-17-1-4040]
  3. JSPS
  4. Ministry of Education, Culture, Sports, Science and Technology (Japan) [26400400, 26400422]
  5. JSPS KAKENHI [17H03012, 17K05840]
  6. Ministry of Education, Culture, Sports, Science and Technology (Japan)
  7. FIRST Quantum Information Processing Project, Cabinet Office, Government of Japan
  8. Grants-in-Aid for Scientific Research [17H03012, 17K05840] Funding Source: KAKEN

向作者/读者索取更多资源

Quantum state control is crucial in advanced quantum technology, with molecular open shell entities serving as a testbed for implementing quantum control technology. The control of molecular spin qubits is important for quantum computers, where interactions between different spins play a key role. Indirect control via hyperfine interactions has the advantage of reducing unnecessary interactions with the environment, and optimizing experimental conditions is essential for achieving high-fidelity quantum gates.
Quantum state control is one of the most important concepts in advanced quantum technology, emerging quantum cybernetics and related fields. Molecular open shell entities can be a testing ground for implementing quantum control technology enabling us to manipulate molecular spin quantum bits (molecular spin qubits). In well-designed molecular spins consisting of unpaired electron and nuclear spins, the electrons and nuclear spins can be bus and client qubits, respectively. Full control of molecular spin qubits, in which client spins interact via hyperfine coupling, is a key issue for implementing quantum computers (QCs). In solid-state QCs, there are two approaches to the control of nuclear client qubits, namely, direct control of nuclear spins by radio-wave (RF) pulses and indirect control via hyperfine interactions by microwave pulses applied to electron spin qubits. Although the latter is less popular in the literature, the indirectness has advantage of greatly reducing unnecessary interactions between a qubit system and its environment. In this work, we investigate molecular spin optimization to find optimal experimental conditions which can afford to achieve the high fidelity of quantum gates by the indirect control scheme. In the present quantum systems, one electron is directly controlled by pulsed ESR techniques without manipulating individual hyperfine resonance, but the states of two nuclear client spins are indirectly steered via hyperfine interactions. Single crystals of potassium hydrogen maleate (KHM) radical and C-13-labeled malonyl radical are chosen as typical molecular spin qubits which exemplify the importance of the symmetry of hyperfine tensors and their collinear properties. We have found that both the non-collinearity of the principal axes of hyperfine coupling tensors and the non-distinguishability/non-equivalency between nuclear spins are key issues which extremely reduce the gate fidelity.

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