Pattern formation, energy landscapes, and scaling laws

Head:
Felix Otto

Contact: Email
Phone:
+49 (0) 341 - 9959 - 950

Address:
Inselstr. 22
04103 Leipzig

Administrative Assistant:
Katja Heid
Email, Phone/Fax:
+49 (0) 341 - 9959
- 951
- 658

Hydrodynamic Limit

Microscopic evolution with thermal fluctuations on a discrete space...

On the microscopic scale, one considers an atomistic or mesoscopic model. There is a lot of freedom to choose the model, but to have an application in mind let us think of a spin system on a lattice. The microscopic evolution is usually governed by two mechanisms:

  • an equilibration mechanism tries to minimize the energy of the microscopic system, and
  • the thermal noise prevents the system of freezing in a local minimizer of the energy.

Because of the noise, the microscopic system may approach a statistical equilibrium state.

...lead to a macroscopic evolution without noise on a continuous space

Now, let's have a look at the microscopic system at a coarse scale. In our example this means looking at averages of spins gathered in blocks. By considering coarser and coarser scales, one observes two phenomena:

  • The discrete lattice space approximates a continuous space, and
  • the noise is getting smaller by an averaging effect. The stochastic evolution becomes more and more deterministic.

We want to answer the following questions:

  • Is there a deterministic evolution on the continuous space that is approximated by the coarse-grained microscopic evolution?
  • How is the deterministic evolution linked to the microscopic energy?
  • How fast is the approximation?
  • What are the statistics of the fluctuations around the deterministic evolution?

A two-scale approach

The two-scale approach [1] represents a general strategy to answer the questions from above. The main idea of the two-scale approach is to gain better understanding by considering the atomistic or mesoscopic system at two scales:

  • the microscopic scale describes the fluctuation of the system around a macroscopic state,
  • the macroscopic scale describes the coarsened macroscopic system.

An important ingredient is the fast equilibration on the microscopic scale; this means that the statistical equilibrium of the fluctuations is attained very fast. The fast equilibration allows to further neglect the microscopic scale.

By averaging, one can already assume that the evolution on the macroscopic scale is already deterministic. Now, one only has to identify the limit of the evolution on a discrete space that becomes more and more continuous.

Equilibration in high dimensions - the logarithmic Sobolev inequality

As outlined in the last section, it is very important to show that on the microscopic scale there is a fast equilibration. In the hydrodynamic limit, the system size goes to infinity. Therefore, it is important to measure the equilibration with a tool that is able to handle high dimensions. For that reason, we measure the equilibration with the help of the relative entropy, which is closely connected to the logarithmic Sobolev inequality. To have a sufficiently good equilibration, it is sufficient to show that the statistical equilibrium state of the microscopic system satisfies the logarithmic Sobolev inequality uniformly in the system size. This motivates our interest in deducing the logarithmic Sobolev inequality for several systems.

References and further reading

For a general introduction to the two-scale approach we recommend to read the article:

  1. Natalie Grunewald ; Felix Otto ; Cédric Villani and Maria G. Westdickenberg: A two-scale approach to logarithmic Sobolev inequalities and the hydrodynamic limit
    In: Annales de l'Institut Henri Poincaré / B, 45 (2009) 2, p. 302-351
    DOI: 10.1214/07-AIHP200

For a general introduction to hydrodynamic limits, we recommend to read [1] and:

  • S. R. S. Varadhan.
    Relative entropy and hydrodynamic limits.
    Stochastic processes, 329-336, Springer, New York, 1993.

For a general introduction to logarithmic Sobolev inequalities, we recommend to read:

  • M. Ledoux.
    Logarithmic Sobolev inequalities for unbounded spin systems revisited.
    Sem. Probab. XXXV, Lecture Notes in Math., Springer 1755:167-194, 2011.
  • G. Royer.
    Une initiation aux inégalités de Sobolev logarithmiques.
    Cours Spécialisés, Soc. Math. de France, 1999.

Works of our research group connected to this research topic:

  • Georg Menz.
    LSI for Kawasaki dynamics with weak interaction.
    Commun. Math. Phys. 307, 817-860, 2011.
    MPI MIS preprint 31/2010
  • Georg Menz.
    Equilibrium dynamics of continuous unbounded spin systems.
    Dissertation, University of Bonn, 2011.
  • Georg Menz and Felix Otto.
    Uniform logarithmic Sobolev inequalities for conservative spin systems with super-quadratic single-site potential.
    MPI MIS Preprint 5/2011, accepted by Ann. Probab.
  • Felix Otto and Maria G. Reznikoff.
    A new criterion for the logarithmic Sobolev inequality and two applications.
    J. Funct. Anal., 243(1):121-157, 2007.
    download (PDF, 281 kbyte)

Presentations

  • Criteria for Logarithmic Sobolev Inequalities, Application to hydrodynamic limit (see PDF, 140 Kbyte)
14.11.2019, 12:30