4.7 Article

X-Band Parallel-Mode and Multifrequency Electron Paramagnetic Resonance Spectroscopy of S=1/2 Bismuth Centers

Journal

INORGANIC CHEMISTRY
Volume 61, Issue 29, Pages 11173-11181

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acs.inorgchem.2c01141

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Funding

  1. Max Planck Society

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Recent successes in isolating and characterizing several bismuth radicals have inspired the development of new spectroscopic approaches. The application of conventional X-band parallel-mode EPR spectroscopy has allowed for the study and analysis of spin systems with S = 1/2, I = 9/2.
The recent successes in the isolation and characterization of several bismuth radicals inspire the development of new spectroscopic approaches for the in-depth analysis of their electronic structure. Electron paramagnetic resonance (EPR) spectroscopy is a powerful tool for the characterization of main group radicals. However, the large electron-nuclear hyperfine interactions of Bi (Bi-209, I = 9/2) have presented difficult challenges to fully interpret the spectral properties for some of these radicals. Parallel-mode EPR (B-1?B-0) is almost exclusively employed for the study of S > 1/2 systems but becomes feasible for S = 1/2 systems with large hyperfine couplings, offering a distinct EPR spectroscopic approach. Herein, we demonstrate the application of conventional X-band parallel-mode EPR for S = 1/2, I = 9/2 spin systems: Bi-doped crystalline silicon (Si:Bi) and the molecular Bi radicals [L(X)Ga](2)Bi-center dot (X = Cl or I) and [L(Cl)GaBi((Me)cAAC)](center dot+) (L = HC[MeCN(2,6-iPr(2)C(6)H(3))](2)). In combination with multifrequency perpendicular-mode EPR (X-, Q-, and W-band frequencies), we were able to fully refine both the anisotropic g- and A-tensors of these molecular radicals. The parallel-mode EPR experiments demonstrated and discussed here have the potential to enable the characterization of other S = 1/2 systems with large hyperfine couplings, which is often challenging by conventional perpendicular-mode EPR techniques. Considerations pertaining to the choice of microwave frequency are discussed for relevant spin-systems.

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