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Interplay between positive feedbacks in the generalized CEV process

Author

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  • Reimann, St.
  • Gontis, V.
  • Alaburda, M.

Abstract

The dynamics of the generalized CEV process dXt=aXtndt+bXtmdWt(gCEV) is due to an interplay of two feedback mechanisms: State-to-Drift and State-to-Diffusion, whose degrees are n and m respectively. We particularly show that the gCEV, in which both feedback mechanisms are positive, i.e. n,m>1, admits a stationary probability distribution P provided that n<2m−1. In this case the stationary pdf asymptotically decays as a power law P(x)∼1xμ with tail exponent μ=2m>2. Furthermore the power spectral density obeys S(f)∼1fβ, where β=2−1+ϵ2(m−1), ϵ>0. The tail behavior of the stationary pdf as well as of the power-spectral density thus are both independent of the drift feedback degree n but governed by the diffusion feedback degree m. Bursting behavior of the gCEV is investigated numerically. Burst intensity S and burst duration T are shown to be related by S∼T2.

Suggested Citation

  • Reimann, St. & Gontis, V. & Alaburda, M., 2011. "Interplay between positive feedbacks in the generalized CEV process," Physica A: Statistical Mechanics and its Applications, Elsevier, vol. 390(8), pages 1393-1401.
  • Handle: RePEc:eee:phsmap:v:390:y:2011:i:8:p:1393-1401
    DOI: 10.1016/j.physa.2010.11.043
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    Citations

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    Cited by:

    1. Kononovicius, A. & Gontis, V., 2012. "Agent based reasoning for the non-linear stochastic models of long-range memory," Physica A: Statistical Mechanics and its Applications, Elsevier, vol. 391(4), pages 1309-1314.
    2. Vygintas Gontis & Aleksejus Kononovicius & Stefan Reimann, 2012. "The class of nonlinear stochastic models as a background for the bursty behavior in financial markets," Papers 1201.3083, arXiv.org, revised May 2012.

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