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Gibbs Measure


A Gibbs measure is a probability measure obtained by weighting a reference measure with the exponential of an energy function. For energy H, inverse temperature beta>0, and reference measure nu, its finite-system form is

 dmu(sigma)=Z^(-1)e^(-betaH(sigma))dnu(sigma),

where Z=inte^(-betaH)dnu is finite and positive. The normalizing quantity Z is the statistical-mechanical partition function. Changing from counting measure to uniform probability on {-1,1}^N divides Z by 2^N without changing mu. This lowers the thermodynamic pressure by ln2.

For an infinite lattice with finite-range interactions, a Gibbs measure is specified by requiring its conditional law in every finite region, given the spins outside, to have this form with the corresponding boundary interaction. The Ising model and the O(n) model use discrete and spherical spin reference measures, respectively. Glauber dynamics resamples spins from the conditional probabilities of a Gibbs measure.


See also

Glauber Dynamics, Ising Model, O(n) Model, Thermodynamic Pressure

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References

Friedli, S. and Velenik, Y. Statistical Mechanics of Lattice Systems: A Concrete Mathematical Introduction. Cambridge, England: Cambridge University Press, 2017. https://doi.org/10.1017/9781316882603.

Cite this as:

Weisstein, Eric W. "Gibbs Measure." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/GibbsMeasure.html

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