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EPR Parameters Experimental and Calculated

EPR spectra of organic radicals recorded in fluid solution present two principal parameters The g factor and the isotropic hyperfine coupling constant, hfc. The g factor characterizes the center of the EPR signal and spin orbit coupling leads to specific deviations from the value of the free electron, 2.0023. [Pg.143]

The hfc represents the orientation-independent interaction between the free electron and a magnetic nucleus (e.g., H, C, F, etc.). It reflects the spin density and the spin population at the magnetic nucleus and the orbital character of the spincarrying atom (Fermi contact). [Pg.143]

In most cases, carbon-centered radicals carry the unpaired electron in p(7t)-type orbitals. Since C isotopes are present at a very low percentage (natural abundance, 1.11%), the spin distribution is monitored by adjacent H nuclei. The spin from the p-type orbital of the C atom is transferred to the adjacent H atom (H ) via n- y spin polarization (Fig. 7.2a) however, spin transfer to more distant protons follows the model of a hyperconjugation mechanism illustrated in Fig. 7.2b. The closer the Cp-Hp is oriented toward the z-axis of the C p orbital, (0 = 0°) the bigger becomes the Hp hfc. When 0 is equal to 90°, the Hp hfc reaches its minimum value. This behavior is described by an empirical formula  [Pg.143]

A third arrangement for a rather efficient long-range spin transfer is a W-plane-like arrangement between the z-axis of the C p orbital and a Cy-H bond (Fig. 7.2c). [Pg.143]

Obviously, the interactions sketched in Fig. 7.2 are very helpful, yet rough, empirical models for efficient spin transfer. Substantially more precise hfc values [Pg.143]


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