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Davidovich M.V.

Noise-switched tunnel diod amplifier on microwave
M.V. Davidovich
Saratov Technical University,
Saratov, Russia

The tunnel diod amplifier of small modulated signal switched by noise of big intensity was investigated in the microwave frequency range. As the tunnel diod have the cubic nonlinearity in the static current per voltage characteristic, noise switching over the two extremal points on this characteristic can cause the amplification of the small regular signal. This amplification and signal to noise ratio (SNR) increase when stochastic resonance (SR) occur or when the frequency of switching is equal to the main frequency of the modulated signal [1,2]. In this work the amplification of amplitude- modulated and frequency-modulated signals have explored for diod included in transmission line by use of two impedance transformers.

For the pass band of these tramsformers we can approximately use the following equation to describe the SR phenomenon:

equation443

where R is the transmission line wave impedance, C is the shunt diod capacitance, L is the series inductance, J(U) is the current per voltage diod characteristic function which can be taken by cubic polynomial in the explored range of U, S(t) is the modulated signal function and N(t) is the white noise. For solving (1) the procedure based upon pertubation method for two follow from (1) integral equations was elaborated. For each time realization of the solution of equation (1) the spectrum have been computed by use the fast Fourier integral tramsform based upon pulse-constant time discreditation of this solution. The such transform for solitary pulse between moments tex2html_wrap_inline2768 and tex2html_wrap_inline2770 with amplitude V and duration tex2html_wrap_inline2774 is

equation448

To compute the SNR the stochastic averaging by use the several tens of the spectral realizations have used.

The investigations show the following results: 1) there is strong (in order of several tens of decibel) wide band signal and noise amplification for frequencies more less then own resonant frequency; 2) the pass band without perceptible signal distortion is about 20%; 3) the SNR increase when SR occur and decrease with frequency.

  1. R. Benzi, S. Sutera, A. Vulpiani, J. Phys. A. 14 (1981) 453.
  2. J.Stat.Phys., Special issue. 70 (1993) No. 1/2.


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Next: Davidovich M.V. Up: Book of Abstracts Previous: David P.J. and Tripathi D.N.

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