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7: CW EPR Spectroscopy

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    • 7.1: Why and how CW EPR spectroscopy is done
    • 7.2: Theoretical description of CW EPR
      All spins in a sample that have the same resonance frequency form a spin packet. In the following we also assume that all spins of a spin packet have the same longitudinal and transverse relaxation times. If the number of spins in the spin packet is sufficiently large, we can assign a magnetization vector to the spin packet. Dynamics of this magnetization vector with equilibrium magnetization M0 during microwave irradiation is described by the Bloch equations in the rotating frame.

    This page titled 7: CW EPR Spectroscopy is shared under a CC BY-NC 4.0 license and was authored, remixed, and/or curated by Gunnar Jeschke via source content that was edited to the style and standards of the LibreTexts platform; a detailed edit history is available upon request.