Broken translation symmetry for a 3D continuum particle system
In plain words
Prove that some realistic system of particles in continuous 3D space has, at low temperature, a thermal equilibrium state in which particles keep preferred lattice positions over infinite distances.
Precise statement
For classical particles in $R^3$ with a stable, regular pair potential $V$ (for example Lennard-Jones, or a smooth short-range potential with a crystalline ground state), prove that for large $\beta = 1/T$ at suitable density there is an infinite-volume Gibbs point process that is not translation invariant, with density correlations showing long-range periodic order. One such potential suffices.
What would settle it
A construction, for example by a multiscale or Pirogov-Sinai-type expansion around the crystal, of a non-translation-invariant Gibbs measure for one continuum potential in 3D.
Status in the literature
Unverified note: it names recent work and was partly written without a live literature search; it awaits a check by an editor.
Proved for lattice models via Pirogov-Sinai theory, and positional order is ruled out for 2D continuum systems (Richthammer 2007); as of 2026 no continuum system in $d \ge 3$ has a proof of a crystalline Gibbs state.
Problems built on this one
Special cases
Results
No results have been posted on this problem yet.
Post a result · how results are checked
Sign in to follow or save this problem
Comments (0)
Comments are not records: they are not signed, stamped or logged. How comments work
No comments yet.
Sign in to comment.