{
  "annotation_id": "f266832c-b1a6-49e4-8f0e-3daa1bde7c5c",
  "date_created": "2026-02-17T05:53:07.896000Z",
  "date_modified": "2026-02-17T05:53:07.896000Z",
  "file_hash": "be082f067721cfbc3157b517b662e2a0c113616d9c9b69e7d06b8c0a3be5cec0",
  "private": false,
  "record": {
    "abstract": "In this work, we investigate the emergence of higher-spin structure in 2d $\\mathcal{N}=(0,2)$ disordered models. While previous studies focused on the $J$-type model where the $E$-term in the Fermi multiplet was discarded. We extend the discussion to $\\mathcal{N}=(0,2)$ disordered models with $E$-type potential. In terms of (disordered) $\\mathcal{N}=(0,2)$ Landau-Ginzburg theory, we establish a duality between two models. By solving the Schwinger-Dyson equations and the ladder kernel matrix for 4-point functions, we verify that the $E$-type model is dynamically equivalent to the $J$-type model in the IR regime. Furthermore, we demonstrate that the $E$-type model also exhibits emergent higher-spin symmetry in certain limits. Our results reveal a larger region of the moduli space of 2D $\\mathcal{N}=(0,2)$ disordered theories and provides insights into the holographic transition from finite to tensionless strings that can be diagnosed by the emergence of higher-spin symmetries.",
    "arxiv_id": "2601.06923",
    "authors": [
      "Liang Wang",
      "Miao Wang"
    ],
    "categories": [
      "hep-th"
    ],
    "license": "http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
    "title": "$E$ and $J$ type $\\mathcal{N}=(0,2)$ disordered models and higher-spin symmetry",
    "url": "https://arxiv.org/abs/2601.06923",
    "version": "v1"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "e1aa62f7-3202-4d4b-8c7b-a1e3333da702",
    "id": "arXiv Dataset",
    "type": "Model",
    "variant": "snapshot-2026-01-17",
    "version": "0.1.0"
  },
  "user_id": 1000002
}