{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:4Y3FYGHCVMQICXVJHM2TZPRMPP","short_pith_number":"pith:4Y3FYGHC","schema_version":"1.0","canonical_sha256":"e6365c18e2ab20815ea93b353cbe2c7bc0630760a92f1dc93a05db09098338c4","source":{"kind":"arxiv","id":"hep-ph/0009222","version":2},"attestation_state":"computed","paper":{"title":"Quantum Dissipative Effects and Neutrinos : current constraints and future perspectives","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.M. Gago, E.M. Moura, R. Zukanovich Funchal, W.J.C. Teves","submitted_at":"2000-09-19T16:12:30Z","abstract_excerpt":"We establish the most stringent experimental constraints coming from recent terrestrial neutrino experiments on quantum mechanical decoherence effects in neutrino systems. Taking a completely phenomenological approach, we probe vacuum oscillations plus quantum decoherence between two neutrino species in the channels $\\nu_\\mu \\to \\nu_\\tau$, $\\nu_\\mu \\to \\nu_e$ and $\\nu_e \\to \\nu_\\tau$, admitting that the quantum decoherence parameter $\\gamma$ is related to the neutrino energy $E_\\nu$ as : $\\gamma=\\gamma_0 (E_\\nu/\\text{GeV})^{n}$, with $n=-1,0,1$ and 2. Our bounds are valid for a neutrino mass s"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-ph/0009222","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2000-09-19T16:12:30Z","cross_cats_sorted":[],"title_canon_sha256":"c34b05c7048f94c99a9cadc8bbaa89d4edc7c2714a963721f99682680add6273","abstract_canon_sha256":"a5a9de221467e6458ce182aff642f0ebab445bb3cfc1dcd8c37f557f26c48599"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T23:57:30.686306Z","signature_b64":"NBwCtFbZsrdcxyn794AU8OwTYgWkF1MjBdq7RkHRhbkZsiCGpUrpo6F283aNGMQgTxFRcjrIzHaVRJr/EiREBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e6365c18e2ab20815ea93b353cbe2c7bc0630760a92f1dc93a05db09098338c4","last_reissued_at":"2026-07-04T23:57:30.685856Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T23:57:30.685856Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum Dissipative Effects and Neutrinos : current constraints and future perspectives","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.M. Gago, E.M. Moura, R. Zukanovich Funchal, W.J.C. Teves","submitted_at":"2000-09-19T16:12:30Z","abstract_excerpt":"We establish the most stringent experimental constraints coming from recent terrestrial neutrino experiments on quantum mechanical decoherence effects in neutrino systems. Taking a completely phenomenological approach, we probe vacuum oscillations plus quantum decoherence between two neutrino species in the channels $\\nu_\\mu \\to \\nu_\\tau$, $\\nu_\\mu \\to \\nu_e$ and $\\nu_e \\to \\nu_\\tau$, admitting that the quantum decoherence parameter $\\gamma$ is related to the neutrino energy $E_\\nu$ as : $\\gamma=\\gamma_0 (E_\\nu/\\text{GeV})^{n}$, with $n=-1,0,1$ and 2. Our bounds are valid for a neutrino mass s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0009222","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0009222/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0009222","created_at":"2026-07-04T23:57:30.685912+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0009222v2","created_at":"2026-07-04T23:57:30.685912+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0009222","created_at":"2026-07-04T23:57:30.685912+00:00"},{"alias_kind":"pith_short_12","alias_value":"4Y3FYGHCVMQI","created_at":"2026-07-04T23:57:30.685912+00:00"},{"alias_kind":"pith_short_16","alias_value":"4Y3FYGHCVMQICXVJ","created_at":"2026-07-04T23:57:30.685912+00:00"},{"alias_kind":"pith_short_8","alias_value":"4Y3FYGHC","created_at":"2026-07-04T23:57:30.685912+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.13362","citing_title":"Probing damping effects in neutrino oscillations with the first JUNO data","ref_index":43,"is_internal_anchor":false},{"citing_arxiv_id":"2604.09776","citing_title":"Visible Neutrino Decay As An Open Quantum System","ref_index":47,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4Y3FYGHCVMQICXVJHM2TZPRMPP","json":"https://pith.science/pith/4Y3FYGHCVMQICXVJHM2TZPRMPP.json","graph_json":"https://pith.science/api/pith-number/4Y3FYGHCVMQICXVJHM2TZPRMPP/graph.json","events_json":"https://pith.science/api/pith-number/4Y3FYGHCVMQICXVJHM2TZPRMPP/events.json","paper":"https://pith.science/paper/4Y3FYGHC"},"agent_actions":{"view_html":"https://pith.science/pith/4Y3FYGHCVMQICXVJHM2TZPRMPP","download_json":"https://pith.science/pith/4Y3FYGHCVMQICXVJHM2TZPRMPP.json","view_paper":"https://pith.science/paper/4Y3FYGHC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0009222&json=true","fetch_graph":"https://pith.science/api/pith-number/4Y3FYGHCVMQICXVJHM2TZPRMPP/graph.json","fetch_events":"https://pith.science/api/pith-number/4Y3FYGHCVMQICXVJHM2TZPRMPP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4Y3FYGHCVMQICXVJHM2TZPRMPP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4Y3FYGHCVMQICXVJHM2TZPRMPP/action/storage_attestation","attest_author":"https://pith.science/pith/4Y3FYGHCVMQICXVJHM2TZPRMPP/action/author_attestation","sign_citation":"https://pith.science/pith/4Y3FYGHCVMQICXVJHM2TZPRMPP/action/citation_signature","submit_replication":"https://pith.science/pith/4Y3FYGHCVMQICXVJHM2TZPRMPP/action/replication_record"}},"created_at":"2026-07-04T23:57:30.685912+00:00","updated_at":"2026-07-04T23:57:30.685912+00:00"}