{
  "annotation_id": "7ef7bbcd-782f-4ee1-8def-7b23cac3d437",
  "date_created": "2026-02-17T05:53:16.279000Z",
  "date_modified": "2026-02-17T05:53:16.279000Z",
  "file_hash": "f32d4ab71ce2fc7239bdeeae642122d75491972bf6b8b7b5e1723a05010783e3",
  "private": false,
  "record": {
    "abstract": "Motivated by the discovery of exotic superconductivity in rhombohedral graphene, we study the two-body problem in electronic bands endowed with Berry curvature and show that it supports chiral, non-$s$-wave bound states with nonzero angular momentum. In the presence of a Fermi sea, these interactions give rise to a chiral pairing problem featuring multiple superconducting phases that break time-reversal symmetry. These phases form a cascade of chiral topological states with different angular momenta, where the order-parameter phase winds by $2\\pi m$ around the Fermi surface, with $m = 1,3,5,\\ldots$, and the succession of phases is governed by the Berry-curvature flux through the Fermi surface area, $\\Phi = b k_F^2/2$. As $\\Phi$ increases, the system undergoes a sequence of first-order phase transitions between distinct chiral phases, occurring whenever $\\Phi$ crosses integer values. This realizes a quantum-geometry analog of the Little--Parks effect -- oscillations in $T_c$ that provide a clear and experimentally accessible hallmark of chiral superconducting order.",
    "arxiv_id": "2601.08055",
    "authors": [
      "Daniil Karuzin",
      "Leonid Levitov"
    ],
    "categories": [
      "cond-mat.mes-hall"
    ],
    "license": "http://creativecommons.org/licenses/by/4.0/",
    "title": "Chiral Two-Body Bound States from Berry Curvature and Chiral Superconductivity",
    "url": "https://arxiv.org/abs/2601.08055",
    "version": "v1"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "1103f6c1-836b-445e-97c0-a06fd69ed3be",
    "id": "arXiv Dataset",
    "type": "Model",
    "variant": "snapshot-2026-01-17",
    "version": "0.1.0"
  },
  "user_id": 1000002
}