{
  "annotation_id": "850d2f5b-6af2-498b-b39d-facf81a5c755",
  "date_created": "2026-03-02T18:00:03.743000Z",
  "date_modified": "2026-03-02T18:00:03.743000Z",
  "file_hash": "56eaa0a51318284c403e357c1d8501638098f7b77e90e226faf6b42678ad7148",
  "private": false,
  "record": {
    "abstract": "We show that the so-called more effective effective field theory (MEEFT) is\nessentially equivalent to the proper nuclear effective field theory (NEFT) in\ndescribing low-energy electroweak processes in nuclei. A key to understanding\ntheir equivalence is the relation between a NEFT-based NN-potential and a\nphenomenological potential through the Wilsonian renormalization group\nequation.We also discuss an important advantage of MEEFT.",
    "arxiv_id": "nucl-th/0411109",
    "authors": [
      "Satoshi X. Nakamura"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "doi": "10.1143/PTP.114.713",
    "journal_ref": "Prog.Theor.Phys. 114 (2005) 713-717",
    "title": "Explanation of more effective effective field theory",
    "url": "https://arxiv.org/abs/nucl-th/0411109"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "46aaf58c-8f51-4947-ba21-57a2a8253eb7",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}