Comment on “Monostable array-enhanced stochastic resonance”

Physical Review E - Statistical Physics, Plasmas, Fluids, and Related Interdisciplinary Topics

Volumn 66, Issue 1, 2002, Pages

  Soskin, S M ^a,b   McClintock, P V E ^b  

^a INSTITUTE OF SEMICONDUCTOR PHYSICS   (Ukraine)

^b LANCASTER UNIVERSITY   (United Kingdom)

Author keywords

[No Author keywords available]

Indexed keywords

APPROXIMATION THEORY; COMPUTER SIMULATION; INDUCTANCE; NATURAL FREQUENCIES; NONLINEAR SYSTEMS; OSCILLATORS (ELECTRONIC); RESONANCE; SIGNAL TO NOISE RATIO; SPURIOUS SIGNAL NOISE; SYNCHRONIZATION;

DUFFING OSCILLATORS; KRAMERS-KRÖNIG RELATIONS; NONLINEAR OSCILLATORS; STOCHASTIC RESONANCES (SR);

RANDOM PROCESSES;

EID: 85036249549     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.66.013101     Document Type: Letter

References (16)

1. J.F. Lindner, B.J. Breen, M.E. Wills, A.R. Bulsara, and W.L. Ditto, Phys. Rev. E 63, 051107 (2001).
2. N.G. Stocks, N.D. Stein, and P.V.E. McClintock, J. Phys. A 26, L385 (1993).
3. N.G. Stocks, N.D. Stein, S.M. Soskin, and P.V.E. McClintock, J. Phys. A 25, L1119 (1992).
4. A.R. Bulsara and G. Schmera, Phys. Rev. E 47, 3734 (1993).
5. L. D. Landau and E. M. Lifshitz, Statistical Physics (Pergamon, New York, 1980).
6. M.I. Dykman, R. Mannella, P.V.E. McClintock, and N.G. Stocks, JETP Lett. 52, 141 (1990);
7. M.I. DykmanR. MannellaP.V.E. McClintockN.G. StocksPhys. Rev. Lett. 65, 2606 (1990).
8. B. McNamara, K. Wiesenfeld, and R. Roy, Phys. Rev. Lett. 60, 2626 (1988);
9. B. McNamara and K. Wiesenfeld, Phys. Rev. A 39, 4854 (1989).
10. M.I. Dykman and M.A. Krivoglaz, Physica A 104, 495 (1980).
11. L. D. Landau and E. M. Lifshitz, Mechanics (Pergamon, London, 1976).
12. S.M. Soskin, Physica A 155, 401 (1989);
13. Physica AS.M. Soskin180, 386 (1992).
14. D.G. Luchinsky, P.V.E. McClintock, S.M. Soskin, and R. Mannella, Phys. Rev. Lett. 76, 4453 (1996).
15. I.K. Kaufman, D.G. Luchinsky, P.V.E. McClintock, S.M. Soskin, and N.D. Stein, Phys. Rev. E 57, 78 (1998).
16. Note that even a single ZD oscillator may possess more than one local maximum in SNR (cf. 12), provided that (Formula presented) possesses more than one extremum and that the extrema are sufficiently separated in frequency.