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SPONTANEOUS SELF‐PULSING AND CAVITY DUMPING IN A CO2 LASER WITH ELECTRO‐OPTIC Q‐SWITCHING
1.O. R. Wood and S. E. Schwarz, Appl. Phys. Letters 12, 263 (1968).
2.P. W. Smith, IEEE J. Quantum Electron. QE‐3, 627 (1967).
3.W. R. Hook, R. P. Hilberg, and R. H. Dishington, Proc. IEEE 54, 1954 (1966);
3.R. N. Zitter, W. H. Steier, and R. Rosenberg, IEEE J. Quantum Electron. QE‐3, 614 (1967).
4.Supplied by Argonne National Laboratory, Argonne, Ill. See R. N. Lewis, E. A. Jung, G. L. Chapman, L. S. VanLoon, and T. A. Romanowski, IEEE Trans. Nucl. Sci. NS13, 84 (1966).
5.Following a trigger pulse to the unit, the dc voltage is removed after a delay of Pulse repetition rates are limited to ≈60 pulses per sec by the spark‐gap type pulser.
6.P. K. Cheo and R. L. Abrams, Appl. Phys. Letters 14, 47 (1969).
7.A. G. Fox and P. W. Smith, Phys. Rev. Letters 18, 826 (1967).
8.T. J. Bridges, H. A. Haus, and P. W. Hoff, Appl. Phys. Letters 13, 316 (1968).
9.J. A. Armstrong and Eric Courtens, IEEE J. Quantum Electron. QE‐4, 411 (1968).
9.We use the Slowly Varying Envelope Approximation which would apply to all gas lasers (comparatively narrow bandwidth).
10.For circular polarization, the right‐hand side should be multiplied by two.
11.E. T. Gerry and D. A. Leonard, Appl. Phys. Letters 8, 227 (1966).
12.The theory is one‐dimensional and therefore neglects diffraction and variation of field strength across the beam. It also takes no account of degeneracies of the levels or any pumping of levels during the pulse.
13.J. A. Fleck, Phys. Rev. Letters 21, 131 (1968).
14.H. Risken and K. Nummedal, J. Appl. Phys. 39, 4662 (1968).
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