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1
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51249163216
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M. I. Dykman, D. G. Luchnsky, R. Mannella, P. V. E. McClintock, N. D. Stein, and N. G. Stocks, Nuovo Cimento D 17, 661 (1995); NIFDAV
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(1995)
Nuovo Cimento D
, vol.17
, pp. 661
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Dykman, M.I.1
Luchnsky, D.G.2
Mannella, R.3
McClintock, P.V.E.4
Stein, N.D.5
Stocks, N.G.6
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2
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85037193034
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other papers in this special issue devoted to stochastic resonance and related phenomena
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and other papers in this special issue devoted to stochastic resonance and related phenomena.
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8
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33646983060
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M. I. Dykman, R. Mannella, P. V. E. McClintock, and N. G. Stocks, Phys. Rev. Lett. 65, 2606 (1990)
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(1990)
Phys. Rev. Lett.
, vol.65
, pp. 2606
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Dykman, M.I.1
Mannella, R.2
McClintock, P.V.E.3
Stocks, N.G.4
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9
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0001336015
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N. G. Stocks, N. D. Stein, S. M. Soskin, and P. V. E. McClintock, J. Phys. A 25, L1119 (1992).
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(1992)
J. Phys. A
, vol.25
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Stocks, N.G.1
Stein, N.D.2
Soskin, S.M.3
McClintock, P.V.E.4
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11
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85037235073
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The authors of a recent paper c11 have claimed the first report of the prediction and discovery of SR in monostable systems. We point out that the phenomenon was originally identified in c8, c9; its observation in a SQUID model was reported in c16
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The authors of a recent paper 11 have claimed the first report of the prediction and discovery of SR in monostable systems. We point out that the phenomenon was originally identified in 89; its observation in a SQUID model was reported in 16.
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16
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0012100029
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P. V. E. McClintock, S. M. Soskin, N. D. Stein, and N. G. Stocks, Phys. Rev. E 48, 147 (1993).
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(1993)
Phys. Rev. E
, vol.48
, pp. 147
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McClintock, P.V.E.1
Soskin, S.M.2
Stein, N.D.3
Stocks, N.G.4
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17
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0001560216
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I. Kh. Kaufman, D. G. Luchinsky, P. V. E. McClintock, S. M. Soskin, and N. D. Stein, Phys. Lett. A 220, 219 (1996)
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(1996)
Phys. Lett. A
, vol.220
, pp. 219
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Kh. Kaufman, I.1
Luchinsky, D.G.2
McClintock, P.V.E.3
Soskin, S.M.4
Stein, N.D.5
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19
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36449006928
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A. D. Hibbs, A. L. Singsaas, E. W. Jacobs, A. R. Bulsara, J. J. Bekkedahl, and F. Moss, J. Appl. Phys. 77, 2582 (1995)
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(1995)
J. Appl. Phys.
, vol.77
, pp. 2582
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Hibbs, A.D.1
Singsaas, A.L.2
Jacobs, E.W.3
Bulsara, A.R.4
Bekkedahl, J.J.5
Moss, F.6
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21
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85037252489
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Strictly, [Formula Presented] also depends on [Formula Presented] because [Formula Presented]. This dependence is much weaker, however, than the activation-law type dependence of [Formula Presented] on [Formula Presented], and therefore has only a minor influence
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Strictly, R([Ω-ωm]/Δω) also depends on T because Δω∝T1/2. This dependence is much weaker, however, than the activation-law type dependence of Cscale on T, and therefore has only a minor influence.
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22
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0000756108
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M. I. Dykman, R. Mannella, P. V. E. McClintock, S. M. Soskin, and N. G. Stocks, Phys. Rev. A 42, 7041 (1990)
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(1990)
Phys. Rev. A
, vol.42
, pp. 7041
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Dykman, M.I.1
Mannella, R.2
McClintock, P.V.E.3
Soskin, S.M.4
Stocks, N.G.5
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24
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85037239006
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This procedure is equivalent to neglecting the nonresonant terms in the original FPE (13), written in an energy-angle representation in accordance with an averaging method c24 (see also c12, c13
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This procedure is equivalent to neglecting the nonresonant terms in the original FPE (13), written in an energy-angle representation in accordance with an averaging method 24 (see also 1213).
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25
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85037209352
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N. N. Bogolyubov and Yu. A. Mitropolsky, Asymptotic Methods in the Theory of Nonlinear Oscillators (Gordon and Breach, New York, 1961)
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N. N. Bogolyubov and Yu. A. Mitropolsky, Asymptotic Methods in the Theory of Nonlinear Oscillators (Gordon and Breach, New York, 1961).
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26
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85037225035
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The case [Formula Presented] requires separate analysis and will be considered elsewhere. Our primary goals in the present paper are the calculations of the susceptibility and the SNR related to a zero-dispersion peak. An evaluation of [Formula Presented] which determines the zero-frequency peak c26 is not necessary for present purposes
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The case n=0 requires separate analysis and will be considered elsewhere. Our primary goals in the present paper are the calculations of the susceptibility and the SNR related to a zero-dispersion peak. An evaluation of W0(j) which determines the zero-frequency peak 26 is not necessary for present purposes.
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27
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0012034944
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M. I. Dykman, R. Mannella, P. V. E. McClintock, S. M. Soskin, and N. G. Stocks, Phys. Rev. A 43, 1701 (1991)
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(1991)
Phys. Rev. A
, vol.43
, pp. 1701
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Dykman, M.I.1
Mannella, R.2
McClintock, P.V.E.3
Soskin, S.M.4
Stocks, N.G.5
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28
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0001475638
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F. Moss, P.V.E. McClintock, Cambridge University Press, Cambridge, England
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L. Fronzoni, in Noise in Nonlinear Dynamical Systems, edited by F. Moss and P.V.E. McClintock (Cambridge University Press, Cambridge, England, 1989), Vol. 3, p. 222.
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(1989)
Noise in Nonlinear Dynamical Systems
, vol.3
, pp. 222
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Fronzoni, L.1
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29
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85037218620
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P. V. E. McClintock and F. Moss, in Ref. c27, p. 243
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P. V. E. McClintock and F. Moss, in Ref. 27, p. 243.
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30
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85037252995
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The AD534LD analog multiplier integrated circuit from Analog Devices, Box 9106, Norwood, MA 02062, USA
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The AD534LD analog multiplier integrated circuit from Analog Devices, Box 9106, Norwood, MA 02062, USA.
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31
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85037185691
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The AD639BD trigonometric integrated circuit from Analog Devices, Box 9106, Norwood, MA 02062, USA
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The AD639BD trigonometric integrated circuit from Analog Devices, Box 9106, Norwood, MA 02062, USA.
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32
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1542679317
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J. Casedemunt, J. I. Jiménez-Acquino, J. M. Sancho, C. J. Lambert, R. Mannella, P. Martano, P. V. E. McClintock, and N. G. Stocks, Phys. Rev. A 40, 5915 (1989)
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(1989)
Phys. Rev. A
, vol.40
, pp. 5915
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Casedemunt, J.1
Jiménez-Acquino, J.I.2
Sancho, J.M.3
Lambert, C.J.4
Mannella, R.5
Martano, P.6
McClintock, P.V.E.7
Stocks, N.G.8
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33
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85037236465
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From Microstar Laboratories Inc., 2265 116th Avenue NE, Bellevue, WA 98004, USA
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From Microstar Laboratories Inc., 2265 116th Avenue NE, Bellevue, WA 98004, USA.
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34
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85037201063
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The numerically calculated frequency dependence of SNR does not reproduce the left wing of the left peak of the experimentally measured dependence because it does not take into account the zero-frequency peak c25. In other frequency ranges the agreement can be considered as quite satisfactory, especially given the exponentially sharp sensitivity of the results to the circuit parameters and noise intensity
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The numerically calculated frequency dependence of SNR does not reproduce the left wing of the left peak of the experimentally measured dependence because it does not take into account the zero-frequency peak 25. In other frequency ranges the agreement can be considered as quite satisfactory, especially given the exponentially sharp sensitivity of the results to the circuit parameters and noise intensity.
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