Linear response function Information & Linear response function Links at HealthHaven.com

A linear response function describes the input-output relationship of a signal transducer such as a radio turning electromagnetic waves into music or a neuron turning synaptic input into a response. Because of its many applications in information theory, physics and engineering there exist alternative names for specific linear response functions such as susceptibility or impedance. The concept of a Green's function or fundamental solution of an ordinary differential equation is closely related.

[edit] Mathematical definition

Denote the input of a system by $h (t)$ , and the response of the system by $o (t)$ . Generally, the value of $o (t)$ will depend not only on the present value of $h (t)$ , but also on past values. Approximately $o (t)$ is a weighted sum of the previous values of $h (t')$ , with the weights given by the linear response function $χ(t - t')$ :

$o(t)\approx\int_{-\infty}^{t} dt'\, \chi(t-t')h(t')\,.$

This expression is the leading order term of a Volterra-expansion. If the system in question is highly non-linear, higher order terms become important and the signal transducer can not adequately be described just by its linear response function.

The Fourier transform $\tilde{\chi}(\omega)$ of the linear response function is very useful as it describes the output of the system if the input is a sine wave $i (t) = i 0 sin(ω t)$ with frequency $ω$ . The output reads

$o(t)=|\tilde{\chi}(\omega)| i_0 \sin(\omega t+\arg\tilde{\chi}(\omega))\,,$

with amplitude gain $|\tilde{\chi}(\omega)|$ and phase shift $\arg\tilde{\chi}(\omega)$ .

[edit] Example

Consider the damped harmonic oscillator, which gets an external driving by the input $i (t)$

$\ddot{o}(t)+\gamma \dot{o}(t)+\omega_0^2 o(t)=i(t)\,.$

The Fourier transform of the linear response function is given as

$\tilde{\chi}(\omega) = \frac{1}{\omega_0^2-\omega^2+i\gamma\omega}\,.$

From this representation, we see that the Fourier transform $\tilde{\chi}(\omega)$ of the linear response function attains a maximum for $\omega\approx\omega_0$ : The damped harmonic oscillator acts as a band pass filter.

[edit] References

The exposition of linear response theory can be found in the seminal paper by Ryogo Kubo.^[1]

^ Kubo, R., Statistical Mechanical Theory of Irreversible Processes I, Journal of the Physical Society of Japan, vol. 12, pp. 570 - 586 (1957).

[edit] See also

[0] Kubo, R., Statistical Mechanical Theory of Irreversible Processes I, Journal of the Physical Society of Japan, vol. 12, pp. 570 - 586 (1957).

[1]

Contents

[edit] Mathematical definition

[edit] Example

[edit] References

[edit] See also