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Extra info for NMR and EPR Spectroscopy. Papers Presented at Varian(s Third Annual Workshop on Nuclear Magnetic Resonance and Electron Paramagnetic Resonance, Held at Palo Alto, California
7. H . MISRA, Rev. Sei. Instr. 29, 590 (1958). 8. A. ABRAGAM and M. H . L. P R Y C E , Proc. Roy. Soc. A205, 135 (1951); B . B L E A N E Y and K. W . H . STEVENS, Rep. Progr. Phys. 16, 108 (1953); K . D . BOWERS and J . OWEN, Rep. Progr. , 18, 304 (1955). 9. J . E . , Proc. Roy. Soc. A240, 67 (1957). 10. R . H . SANDS, Phys. Rev. 99, 1222 (1955). 11. A. W. OVERHAUSER, Phys. Rev. 91, 476 (1953); Phys. Rev. 92, 411 (1953). 12. A. L. M C W H O R T E R a n d J . W. M E Y E R , Phys. Rev. 109, 312 (1958).
Block diagram of X-band E P R spectrometer. tion microwave impedance bridge system employing a crystal detector. 8026 Mc/gauss of applied static magnetic field, it is convenient to use X-band microwave equipment which operates between 8000 and 12,000 Mc/s and to use applied magnetic fields in the neighborhood of 3000 gauss. With a source of 300 mW of microwave power and using low audio-frequency magnetic field modula tion one obtains in practice the theoretical signal-to-noise ratio and may detect 5 x 10~ 12 Δ// moles of electron spins where Δ/7 is the full width of the absorption line in gauss.
7) The linear sweep provides a linear sawtooth modulation of the mag netic field while simultaneously driving the X-axis of the oscilloscope. This modulation produces a small change in t h e static magnetic field (Ho) a t the sample position, t h u s sweeping the field through the reson ance value. c. current to the coils of the electromagnet.
NMR and EPR Spectroscopy. Papers Presented at Varian(s Third Annual Workshop on Nuclear Magnetic Resonance and Electron Paramagnetic Resonance, Held at Palo Alto, California