{
  "annotation_id": "549834f7-7c18-4b2f-8e40-a6bffefc706b",
  "date_created": "2026-02-17T05:53:24.333000Z",
  "date_modified": "2026-02-17T05:53:24.333000Z",
  "file_hash": "be7aea9ba93826fc2f7c5826670a1a69f25c17ff2adc008bf7027193e5b3be17",
  "private": false,
  "record": {
    "abstract": "We introduce and study finite lattice kinetic equations for bosons, fermions, and discrete NLS. For each model this closed evolution equation provides an approximate description for the evolution of the appropriate covariance function in the system. It is obtained by truncating the cumulant hierarchy and dropping the higher order cumulants in the usual manner. To have such a reference solution should simplify controlling the full hierarchy and thus allow estimating the error from the truncation. The harmonic part is given by nearest neighbour hopping, with arbitrary symmetric interaction potential of coupling strength $\\lambda\u003e0$. We consider the well-posedness of the resulting evolution equation up to finite kinetic times on a finite but large enough lattice. We obtain decay of the solutions and upper bounds that are independent of $\\lambda$ and depend on the lattice size only via some Sobolev type norms of the interaction potential and initial data. We prove that the solutions are not sensitive to how the energy conservation delta function is approximated.",
    "arxiv_id": "2601.10486",
    "authors": [
      "Jani Lukkarinen",
      "Sakari Pirnes",
      "Aleksis Vuoksenmaa"
    ],
    "categories": [
      "math-ph",
      "math.MP"
    ],
    "license": "http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
    "title": "Finite lattice kinetic equations for bosons, fermions, and discrete NLS",
    "url": "https://arxiv.org/abs/2601.10486",
    "version": "v1"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "1a82fe25-8f7b-47a8-abb2-69c59a98c213",
    "id": "arXiv Dataset",
    "type": "Model",
    "variant": "snapshot-2026-01-17",
    "version": "0.1.0"
  },
  "user_id": 1000002
}