By James A. Barnes
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00. Superconducting Devices and Materials. A literature s u r v e y issued quarterly. 00. 02) Boulder, Colorado 80302.
1966). [30] Doob, J . L . , The Brownian movement and stochastic equations, Annals of Mathematics, vol. 43, No. 2 (April 1942). [31] Barnes, J . , Atomic timekeeping and the s t a t i s t i c s of precision signal generat o r s , Proc. IEEE, vol. 54, pp. 207-220 (Feb. 1966). [32] Allan, D. W . , S t a t i s t i c s o f atomic frequency standards, Proc. IEEE, vol. 54, pp. 221-230 (Feb. 1966). [33] Atkinson, W . R . , Fey, L . , Newman, J . , Spectrum analysis of extremely low f r e quency variations of quartz o s c i l l a t o r s , Proc.
B-2). Correspondingly, one chooses a MA f i l t e r when t h e f u n c t i o n t u r n s upward as i n F i g . (B-1). 001 Fig. O1 Frequency Fig. 01 Frequency F i g . 1 Frequency Fig. (B-4) Bode P l o t o f Filter Cascade 30 where at i s the i n p u t t o the cascade and zt is the o u t p u t . 6381 (B-11) . Making use of equation ( 4 . 2 ) one can obtain t h e spectrum corresponding t o (B-10). Figure (B-5) i s a p l o t of t h e spectrum superimposed on the Bode p l o t of Figure (B-3). 319 was s e l e c t e d t o make the spectrum f i t the Bode p l o t i n amplia tude.
Models for the Interpretation of Frequency Stability Measurements by James A. Barnes
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