{
  "annotation_id": "7378ced8-6cdc-445c-8226-41eac5f0e045",
  "date_created": "2026-03-02T18:00:43.425000Z",
  "date_modified": "2026-03-02T18:00:43.425000Z",
  "file_hash": "03b40802bfd7007dee99e84ff50e79793094fefbfed56a642d7381c4ce3eb5fa",
  "private": false,
  "record": {
    "abstract": "It is considered the detection of neutrinos moving from the opposite\ndirections. The states of the particle of the detector interacting with the\nneutrinos are connected with the P-transformation. Hence only a half of\nneutrinos gives contribution into the superposition of the neutrino states.\nTaking into account the effect of the opposite neutrino directions the total\nneutrino flux from several sources are in the range 0.5--1 of that without the\neffect. The neutrino flux from nuclear reactors measured in the KamLAND\nexperiment is $0.611\\pm 0.085 {\\rm (stat)} \\pm 0.041 {\\rm (syst)} $ of the\nexpected flux. Calculations for the conditions of the KamLAND experiment yield\nthe neutrino flux taking into account the effect of the opposite neutrino\ndirections, 0.555, of that without the effect that may account for the neutrino\nflux observed in the KamLAND experiment.",
    "arxiv_id": "physics/0302066",
    "authors": [
      "D. L. Khokhlov"
    ],
    "categories": [
      "physics.gen-ph"
    ],
    "title": "Detection of the Neutrino Fluxes from Several Sources",
    "url": "https://arxiv.org/abs/physics/0302066"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "347b6db6-427d-46fd-8c93-bce5ad998eb7",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}