By Sandra S. Eaton
Pt. A. loose radicals, metals, drugs, and body structure -- Pt. B. technique, instrumentation, and dynamics
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And Venkataraman, B. (1974a) Study of molecular motions in liquids by electron spin lattice relaxation measurements. I. Semiquinone ions in hydrogen bonding solvents. Pramana 3, 95-121. Rengen, S. , Khakhar, M. , and Venkataraman, B. (1974b) Study of molecular motions in liquids by electron spin lattice relaxation measurements. II. 2,5-Ditert-butylsemiquinone Ion in Acetonitrile and Tetrahydrofuran. J. Magn. Reson. 16, 35-43. Rengen, S. , Bhagat, V. R. Sastry, V. S. , and Venkataraman, B. (1979).
Therefore, a coupling circuit is required between the resonator and the line to transform the very low or very high resistance into 50 ohms (Figure 4). Coupling (matching) a resonator to the microwave/RF transmission line is an important design and construction feature. Various types of transformers and electric probes have been used. , 1989). 30 GEORGE A. RINARD AND GARETH R. EATON Figure 4. A resonator (R, L, C) is coupled to a microwave source via a matching network, where is the spin system voltage and is the magnetic resonance signal voltage sensed at the detector side of the impedance matching network.
It has a maximum value of one. In practice, the filling factor is usually much less than 1. d. tube (ca. 01, while that for a LGR can be more than an order of magnitude larger. A LGR inherently has a larger filling factor than does a cavity resonator at the same frequency, and the filling factor can be increased by making the return flux cross section large relative to the sample loop cross section. The filling factor of a LGR is limited by the wall thickness of the sample tube. d. tube and the sample is 3 mm od, and long relative to the resonator so that the length can be ignored, the filling factor is reduced relative to that for a completely full loop by a factor of The parameters and depend on resonator geometry.
Biomedical EPR by Sandra S. Eaton