Green–Kubo relations

Transport coefficients expressed as time integrals of equilibrium current autocorrelation functions (linear response).
Green–Kubo relations

Statement (generic form)

In equilibrium (typically with respect to a ), many linear transport coefficients can be written as time integrals of equilibrium time-correlation functions (a special case of ).

A common template is

Lαβ=0Jα(0)Jβ(t)eqdt, \mathcal{L}_{\alpha\beta} = \int_0^\infty \langle J_\alpha(0)\,J_\beta(t)\rangle_{\mathrm{eq}}\,dt,

up to conventional prefactors (often 1/(kBT)1/(k_B T) and/or volume factors) depending on the definition of the currents and forces.

Here eq\langle \cdot \rangle_{\mathrm{eq}} is an in equilibrium, and Jα(0)Jβ(t)\langle J_\alpha(0)J_\beta(t)\rangle is a .

Standard examples (common conventions)

Electrical conductivity

Let J(t)J(t) be the total electric current in volume VV. Then

σ=1kBTV0J(0)J(t)eqdt. \sigma = \frac{1}{k_B T\,V}\int_0^\infty \langle J(0)\cdot J(t)\rangle_{\mathrm{eq}}\,dt.

Shear viscosity

Let Pxy(t)P_{xy}(t) be the off-diagonal stress tensor component. Then

η=1kBTV0Pxy(0)Pxy(t)eqdt. \eta = \frac{1}{k_B T\,V}\int_0^\infty \langle P_{xy}(0)\,P_{xy}(t)\rangle_{\mathrm{eq}}\,dt.

Diffusion constant (Einstein–Green–Kubo form)

For a tagged particle velocity v(t)v(t) in dd dimensions,

D=1d0v(0)v(t)eqdt. D = \frac{1}{d}\int_0^\infty \langle v(0)\cdot v(t)\rangle_{\mathrm{eq}}\,dt.

Conditions (what is implicitly required)

  • Stationarity: the equilibrium measure is invariant under the dynamics (e.g., Gibbs equilibrium).
  • Decay of correlations / mixing: ensures the integral over t[0,)t\in[0,\infty) converges.
  • Microreversibility: under time-reversal symmetry (or, in stochastic settings, ), one obtains symmetry properties such as Onsager reciprocity.

Relationship to other linear-response statements