{
  "annotation_id": "4d7a1cba-6ad9-4203-9f29-2670b2936f65",
  "date_created": "2026-03-02T18:00:53.469000Z",
  "date_modified": "2026-03-02T18:00:53.469000Z",
  "file_hash": "b80dce83fc020188b727b14971527fa6b63517ca0af76f3cf276ea1e9e14f6f1",
  "private": false,
  "record": {
    "abstract": "Recent advances in the integrated modeling of ELMy H-mode plasmas are\npresented. A model for the H-mode pedestal and for the triggering of ELMs\npredicts the height, width, and shape of the H-mode pedestal and the frequency\nand width of ELMs. Formation of the pedestal and the L-H transition is the\ndirect result of ExB flow shear suppression of anomalous transport. The\nperiodic ELM crashes are triggered by either the ballooning or peeling MHD\ninstabilities. The BALOO, DCON, and ELITE ideal MHD stability codes are used to\nderive a new parametric expression for the peeling-ballooning threshold. The\nnew dependence for the peeling-ballooning threshold is implemented in the ASTRA\ntransport code. Results of integrated modeling of DIII-D like discharges are\npresented and compared with experimental observations. The results from the\nideal MHD stability codes are compared with results from the resistive MHD\nstability code NIMROD.",
    "arxiv_id": "physics/0411086",
    "authors": [
      "A. Y. Pankin",
      "G. Bateman",
      "D. P. Brennan",
      "D. D. Schnack",
      "P. B. Snyder",
      "I. Voitsekhovitch",
      "A. H. Kritz",
      "G. Janeschitz",
      "S. Kruger",
      "T. Onjun",
      "G. W. Pacher",
      "H. D. Pacher"
    ],
    "categories": [
      "physics.plasm-ph"
    ],
    "doi": "10.1007/s10582-005-0048-4",
    "title": "ELM triggering conditions for the integrated modeling of H-mode plasmas",
    "url": "https://arxiv.org/abs/physics/0411086"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "0df85e2e-9491-49d6-8941-0ceff11667f1",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}