{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:5IZVZ5YYJRQSRTDRMFMORLKAE6","short_pith_number":"pith:5IZVZ5YY","schema_version":"1.0","canonical_sha256":"ea335cf7184c6128cc716158e8ad4027a1af16de200b9d44901cce250716af87","source":{"kind":"arxiv","id":"0802.4449","version":2},"attestation_state":"computed","paper":{"title":"Stationary condition in a perturbative approach for mass varying neutrinos","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alex E. Bernardini, O. Bertolami","submitted_at":"2008-02-29T19:01:39Z","abstract_excerpt":"A perturbative approach for arbitrary choices of the equation of state of the universe is introduced in order to treat scenarios for mass varying neutrinos (MaVaN's) coupled to the dark sector. The generalized criterion for the applicability of such an approach is expressed through a constraint on the coefficient of the linear perturbation on the dark sector scalar field. This coefficient depends on the ratio between the variation of the neutrino energy and the scalar field potential. Upon certain conditions, the usual {\\em stationary condition} found in the context of MaVaN models together wi"},"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":"0802.4449","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2008-02-29T19:01:39Z","cross_cats_sorted":[],"title_canon_sha256":"f055975d4389f6d53a8563a3f8d79167f9f00be226a7b947c1a41d766a758bea","abstract_canon_sha256":"d0cb5e7330afc1161241900e40b23ee6ce464a1bebf666a2f2807a331dfd953c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:35:23.225506Z","signature_b64":"7oKZARZLKvpJ7u6/27JgexrP2rtJs2nyZj1s6rgz5En8vr8KTqhbSD0MXllMD7p7Wpqmf0zFlSfPAWOooRGSAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ea335cf7184c6128cc716158e8ad4027a1af16de200b9d44901cce250716af87","last_reissued_at":"2026-05-18T02:35:23.224943Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:35:23.224943Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Stationary condition in a perturbative approach for mass varying neutrinos","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alex E. Bernardini, O. Bertolami","submitted_at":"2008-02-29T19:01:39Z","abstract_excerpt":"A perturbative approach for arbitrary choices of the equation of state of the universe is introduced in order to treat scenarios for mass varying neutrinos (MaVaN's) coupled to the dark sector. The generalized criterion for the applicability of such an approach is expressed through a constraint on the coefficient of the linear perturbation on the dark sector scalar field. This coefficient depends on the ratio between the variation of the neutrino energy and the scalar field potential. Upon certain conditions, the usual {\\em stationary condition} found in the context of MaVaN models together wi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0802.4449","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":""},"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":"0802.4449","created_at":"2026-05-18T02:35:23.225044+00:00"},{"alias_kind":"arxiv_version","alias_value":"0802.4449v2","created_at":"2026-05-18T02:35:23.225044+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0802.4449","created_at":"2026-05-18T02:35:23.225044+00:00"},{"alias_kind":"pith_short_12","alias_value":"5IZVZ5YYJRQS","created_at":"2026-05-18T12:25:56.245647+00:00"},{"alias_kind":"pith_short_16","alias_value":"5IZVZ5YYJRQSRTDR","created_at":"2026-05-18T12:25:56.245647+00:00"},{"alias_kind":"pith_short_8","alias_value":"5IZVZ5YY","created_at":"2026-05-18T12:25:56.245647+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5IZVZ5YYJRQSRTDRMFMORLKAE6","json":"https://pith.science/pith/5IZVZ5YYJRQSRTDRMFMORLKAE6.json","graph_json":"https://pith.science/api/pith-number/5IZVZ5YYJRQSRTDRMFMORLKAE6/graph.json","events_json":"https://pith.science/api/pith-number/5IZVZ5YYJRQSRTDRMFMORLKAE6/events.json","paper":"https://pith.science/paper/5IZVZ5YY"},"agent_actions":{"view_html":"https://pith.science/pith/5IZVZ5YYJRQSRTDRMFMORLKAE6","download_json":"https://pith.science/pith/5IZVZ5YYJRQSRTDRMFMORLKAE6.json","view_paper":"https://pith.science/paper/5IZVZ5YY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0802.4449&json=true","fetch_graph":"https://pith.science/api/pith-number/5IZVZ5YYJRQSRTDRMFMORLKAE6/graph.json","fetch_events":"https://pith.science/api/pith-number/5IZVZ5YYJRQSRTDRMFMORLKAE6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5IZVZ5YYJRQSRTDRMFMORLKAE6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5IZVZ5YYJRQSRTDRMFMORLKAE6/action/storage_attestation","attest_author":"https://pith.science/pith/5IZVZ5YYJRQSRTDRMFMORLKAE6/action/author_attestation","sign_citation":"https://pith.science/pith/5IZVZ5YYJRQSRTDRMFMORLKAE6/action/citation_signature","submit_replication":"https://pith.science/pith/5IZVZ5YYJRQSRTDRMFMORLKAE6/action/replication_record"}},"created_at":"2026-05-18T02:35:23.225044+00:00","updated_at":"2026-05-18T02:35:23.225044+00:00"}