{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:ERDQRO7EGJUUTJGBRDM7CKMVT4","short_pith_number":"pith:ERDQRO7E","schema_version":"1.0","canonical_sha256":"244708bbe4326949a4c188d9f129959f228e73d43adf4ce032a379ed906890fd","source":{"kind":"arxiv","id":"1509.08819","version":2},"attestation_state":"computed","paper":{"title":"Cosmological perturbations in coherent oscillating scalar field models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"astro-ph.CO","authors_text":"A. L. Maroto, J. A. R. Cembranos, S. J. N\\'u\\~nez Jare\\~no","submitted_at":"2015-09-28T13:08:10Z","abstract_excerpt":"The fact that fast oscillating homogeneous scalar fields behave as perfect fluids in average and their intrinsic isotropy have made these models very fruitful in cosmology. In this work we will analyse the perturbations dynamics in these theories assuming general power law potentials $V(\\phi)=\\lambda \\vert\\phi\\vert^{n}/n$. At leading order in the wavenumber expansion, a simple expression for the effective sound speed of perturbations is obtained $c_{\\text{eff}}^2 = \\omega=(n-2)/(n+2)$ with $\\omega$ the effective equation of state. We also obtain the first order correction in $k^2/\\omega_{\\text"},"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":"1509.08819","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2015-09-28T13:08:10Z","cross_cats_sorted":["gr-qc","hep-ph"],"title_canon_sha256":"cb16cbe58b13dee55c20823e28d18dc102a0a9d438a0fd93704ef3c84f3d837e","abstract_canon_sha256":"1903df59d9df900c32a7d30c4fefc06afe82bce7192c4e162505adb89c8922ab"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:18:42.802125Z","signature_b64":"iXbD1dI2Mz2muC++GsTfz0v3zsdW+niDvA5hq8jkhKEqofKjT+KupjorAFSljzyn5Vb52d68IDzCU2cjoJ9NBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"244708bbe4326949a4c188d9f129959f228e73d43adf4ce032a379ed906890fd","last_reissued_at":"2026-05-18T01:18:42.801465Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:18:42.801465Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Cosmological perturbations in coherent oscillating scalar field models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"astro-ph.CO","authors_text":"A. L. Maroto, J. A. R. Cembranos, S. J. N\\'u\\~nez Jare\\~no","submitted_at":"2015-09-28T13:08:10Z","abstract_excerpt":"The fact that fast oscillating homogeneous scalar fields behave as perfect fluids in average and their intrinsic isotropy have made these models very fruitful in cosmology. In this work we will analyse the perturbations dynamics in these theories assuming general power law potentials $V(\\phi)=\\lambda \\vert\\phi\\vert^{n}/n$. At leading order in the wavenumber expansion, a simple expression for the effective sound speed of perturbations is obtained $c_{\\text{eff}}^2 = \\omega=(n-2)/(n+2)$ with $\\omega$ the effective equation of state. We also obtain the first order correction in $k^2/\\omega_{\\text"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.08819","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":"1509.08819","created_at":"2026-05-18T01:18:42.801571+00:00"},{"alias_kind":"arxiv_version","alias_value":"1509.08819v2","created_at":"2026-05-18T01:18:42.801571+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.08819","created_at":"2026-05-18T01:18:42.801571+00:00"},{"alias_kind":"pith_short_12","alias_value":"ERDQRO7EGJUU","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_16","alias_value":"ERDQRO7EGJUUTJGB","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_8","alias_value":"ERDQRO7E","created_at":"2026-05-18T12:29:19.899920+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.00103","citing_title":"Pre-inflationary QCD axion stars after moduli domination","ref_index":97,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ERDQRO7EGJUUTJGBRDM7CKMVT4","json":"https://pith.science/pith/ERDQRO7EGJUUTJGBRDM7CKMVT4.json","graph_json":"https://pith.science/api/pith-number/ERDQRO7EGJUUTJGBRDM7CKMVT4/graph.json","events_json":"https://pith.science/api/pith-number/ERDQRO7EGJUUTJGBRDM7CKMVT4/events.json","paper":"https://pith.science/paper/ERDQRO7E"},"agent_actions":{"view_html":"https://pith.science/pith/ERDQRO7EGJUUTJGBRDM7CKMVT4","download_json":"https://pith.science/pith/ERDQRO7EGJUUTJGBRDM7CKMVT4.json","view_paper":"https://pith.science/paper/ERDQRO7E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1509.08819&json=true","fetch_graph":"https://pith.science/api/pith-number/ERDQRO7EGJUUTJGBRDM7CKMVT4/graph.json","fetch_events":"https://pith.science/api/pith-number/ERDQRO7EGJUUTJGBRDM7CKMVT4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ERDQRO7EGJUUTJGBRDM7CKMVT4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ERDQRO7EGJUUTJGBRDM7CKMVT4/action/storage_attestation","attest_author":"https://pith.science/pith/ERDQRO7EGJUUTJGBRDM7CKMVT4/action/author_attestation","sign_citation":"https://pith.science/pith/ERDQRO7EGJUUTJGBRDM7CKMVT4/action/citation_signature","submit_replication":"https://pith.science/pith/ERDQRO7EGJUUTJGBRDM7CKMVT4/action/replication_record"}},"created_at":"2026-05-18T01:18:42.801571+00:00","updated_at":"2026-05-18T01:18:42.801571+00:00"}