Memoryless nonlinear response: A simple mechanism for the 1/f noise

Author: Chand Yadav Avinash   Ramaswamy Ramakrishna   Dhar Deepak  

Publisher: Edp Sciences

E-ISSN: 1286-4854|103|6|60004-60004

ISSN: 0295-5075

Source: EPL (EUROPHYSICS LETTERS), Vol.103, Iss.6, 2013-10, pp. : 60004-60004

Disclaimer: Any content in publications that violate the sovereignty, the constitution or regulations of the PRC is not accepted or approved by CNPIEC.

Previous Menu Next

Abstract

Discovering the mechanism underlying the ubiquity of “$1/f^{\alpha}$ ” noise has been a long-standing problem. The wide range of systems in which the fluctuations show the implied long-time correlations suggests the existence of some simple and general mechanism that is independent of the details of any specific system. We argue here that a memoryless nonlinear response suffices to explain the observed nontrivial values of α: a random input noisy signal S(t) with a power spectrum varying as $1/f^{\alpha'}$ , when fed to an element with such a response function R, gives an output $R(S(t))$ that can have a power spectrum $1/f^{\alpha}$ with $\alpha < \alpha$ '. As an illustrative example, we show that an input Brownian noise $(\alpha'=2)$ acting on a device with a sigmoidal response function $R(S)= \text{sgn}(S)|S|^x$ , with x < 1, produces an output with $\alpha = 3/2 +x$ , for $0 \leq x \leq 1/2$ . Our discussion is easily extended to more general types of input noise as well as more general response functions.