Abstract

Atomic spin centers in 2D materials are a highly anticipated building block for quantum technologies. Here, we demonstrate the creation of an effective spin-1/2 system via the atomically controlled generation of magnetic carbon radical ions (CRIs) in synthetic two-dimensional transition metal dichalcogenides. Hydrogenated carbon impurities located at chalcogen sites introduced by chemical doping are activated with atomic precision by hydrogen depassivation using a scanning probe tip. In its anionic state, the carbon impurity is computed to have a magnetic moment of 1 μB resulting from an unpaired electron populating a spin-polarized in-gap orbital. We show that the CRI defect states couple to a small number of local vibrational modes. The vibronic coupling strength critically depends on the spin state and differs for monolayer and bilayer WS2. The carbon radical ion is a surface-bound atomic defect that can be selectively introduced, features a well-understood vibronic spectrum, and is charge state controlled.

Highlights

  • Atomic spin centers in 2D materials are a highly anticipated building block for quantum technologies

  • We demonstrate that the electron-phonon coupling associated with the two discrete electronic carbon radical ions (CRIs) defect states is limited to a only few vibrational modes and exhibits a distinct spin and layer dependence

  • In the following, we discuss our three primary conclusions: the hydrogen depassivation of the CH impurity and formation of the CRI, the two spin-polarized defect states associated with the CRI, and the vibronic coupling of the CRI defect states with the transition metal dichalcogenides (TMDs) host lattice

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Summary

Introduction

Atomic spin centers in 2D materials are a highly anticipated building block for quantum technologies. We precisely characterize the coupling of the spin-polarized local defect states generated by the CRI with its host lattice. We demonstrate that the electron-phonon coupling associated with the two discrete electronic CRI defect states is limited to a only few vibrational modes and exhibits a distinct spin and layer dependence.

Results
Conclusion
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