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General properties of time correlation functions

Define a time correlation function between two quantities tex2html_wrap_inline741 and tex2html_wrap_inline807 by

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The following properties follow immediately from the above definition:

1.

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2.

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Thus, if A=B, then

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known as the autocorrelation function of A, and

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If we define tex2html_wrap_inline813 , then

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which just measures the fluctuations in the quantity A.

3.
A time correlation function may be evaluated as a time average, assuming the system is ergodic. In this case, the phase space average may be equated to a time average, and we have

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which is valid for t;SPMlt;;SPMlt;T. In molecular dynamics simulations, where the phase space trajectory is determined at discrete time steps, the integral is expressed as a sum

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where N is the total number of time steps, tex2html_wrap_inline821 is the time step and tex2html_wrap_inline823 .

4.
Onsager regression hypothesis: In the long time limit, A and B eventually become uncorrelated from each other so that the time correlation function becomes

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For the autocorrelation function of A, this becomes

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Thus, tex2html_wrap_inline831 decays from tex2html_wrap_inline833 at t=0 to tex2html_wrap_inline837 as tex2html_wrap_inline839 .

An example of a signal and its time correlation function appears in the figure below. In this case, the signal is the magnitude of the velocity along the bond of a diatomic molecule interacting with a Lennard-Jones bath. Its time correlation function is shown beneath the signal:

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Figure 1:

Over time, it can be seen that the property being autocorrelated eventually becomes uncorrelated with itself.



Mark Tuckerman
Thu Apr 13 13:07:24 EDT 2000