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The steady-state frequency shifts due to
ionizing radiation are due to radiation caused changes at impurity
defects. The defect of major concern
in quartz is the substitutional Al3+ defect with its associated
interstitial charge compensator, which can be an H+, Li+,
or Na+ ion, or a hole. This
defect substitutes for a Si4+ in the quartz lattice (see chapter
5). Radiation can result in a change
in the position of weakly bound compensators, which changes the elastic
constants of quartz and thereby leads to a frequency change. The movement of ions also results in
a decrease in the crystal's Q, i.e., in an increase in the crystal's
equivalent series resistance, especially upon exposure to a pulse of ionizing
radiation. If the oscillator's gain
margin is insufficient, the increased resistance can stop the oscillation for
periods lasting many seconds.
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B. R. Capone, A.
Kahan, R. N. Brown, and J. R. Buckmelter, "Quartz Crystal Radiation
Effects," IEEE Trans. Nuclear Sci., NS-17, pp. 217-221, 1970.
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J. C. King and D. R.
Koehler, Radiation Effects on Resonators. In: Precision Frequency Control,
Vol. 2 (E. A. Gerber and A. Ballato, eds.), Academic Press, New York,
pp. 147-159, 1985.
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J. J. Suter, et al.,
“The Effects of Ionizing and Particle Radiation on Precision Frequency
Sources,” Proc. 1992 IEEE Frequency Control Symposium, IEEE Cat. No.
92CH3083-3, 1992.
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J. C. King and H. H.
Sander, “Rapid Annealing of Frequency Change in High Frequency Crystal
Resonators Following Pulsed X-irradiation at Room Temperature,” Proc. 27th
Ann. Symp. Frequency Control, pp. 117-119, NTIS Accession No. AD-771042,
1973.
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R. E. Paradysz, and
W. L. Smith, “Crystal Controlled Oscillators for Radiation Environments,” Proc.
27th Ann. Symp. Frequency Control, pp. 120-123, NTIS Accession No.
AD-771042, 1973.
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