4.7 Article

Coherence of a charge stabilised tin-vacancy spin in diamond

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NPJ QUANTUM INFORMATION
卷 8, 期 1, 页码 -

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NATURE PORTFOLIO
DOI: 10.1038/s41534-022-00552-0

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资金

  1. European Union's Horizon 2020 research and innovation programme [820394]
  2. EMPIR programme
  3. European Union [17FUN06, 20FUN05]
  4. German Federal Ministry of Education and Research (Bundesministerium fur Bildung und Forschung, BMBF) [16KIS0864, 16KISQ001K]
  5. Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) [429529648 - TRR 306]
  6. MEXT Quantum Leap Flagship Program (MEXT Q-LEAP) [JPMXS0118067395]
  7. MEXT Q-LEAP [JPMXS0118068379]
  8. JSPS KAKENHI [JP20K21096]

向作者/读者索取更多资源

This study reveals a charge cycle that can be applied to various group IV-vacancy centers and exploits it to achieve efficient and rapid initialization of the desired negative charge state. It also demonstrates a spin state readout method without the need for aligning a magnetic field.
Quantum information processing (QIP) with solid state spin qubits strongly depends on the efficient initialisation of the qubit's desired charge state. While the negatively charged tin-vacancy (SnV-) centre in diamond has emerged as an excellent platform for realising QIP protocols due to long spin coherence times at liquid helium temperature and lifetime limited optical transitions, its usefulness is severely limited by termination of the fluorescence under resonant excitation. Here, we unveil the underlying charge cycle, potentially applicable to all group IV-vacancy (G4V) centres, and exploit it to demonstrate highly efficient and rapid initialisation of the desired negative charge state of single SnV centres while preserving long term stable optical resonances. In addition to investigating the optical coherence, we all-optically probe the coherence of the ground state spins by means of coherent population trapping and find a spin dephasing time of 5(1) mu s. Furthermore, we demonstrate proof-of-principle single shot spin state readout without the necessity of a magnetic field aligned to the symmetry axis of the defect.

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