{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:AGU6URTOHNTVDSXSPQEFCWZVFW","short_pith_number":"pith:AGU6URTO","schema_version":"1.0","canonical_sha256":"01a9ea466e3b6751caf27c08515b352da71f419e4d35d857dae3934685f16d01","source":{"kind":"arxiv","id":"1307.6383","version":1},"attestation_state":"computed","paper":{"title":"Analytical transformed harmonic oscillator basis for three-body nuclei of astrophysical interest: Application to 6He","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"J. Casal, J. M. Arias, M. Rodr\\'iguez-Gallardo","submitted_at":"2013-07-24T11:07:50Z","abstract_excerpt":"Recently, a square-integrable discrete basis, obtained performing a simple analytical local scale transformation to the harmonic oscillator basis, has been proposed and successfully applied to study the properties of two-body systems. Here, the method is generalized to study three-body systems. To test the goodness of the formalism and establish its applicability and limitations, the capture reaction rate for the nucleosynthesis of the Borromean nucleus 6He (4He + n + n) is addressed. Results are compared with previous publications and with calculations based on actual three-body continuum wav"},"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":"1307.6383","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-07-24T11:07:50Z","cross_cats_sorted":[],"title_canon_sha256":"d81e004e2738976ca9d04858d224d8347108b5884f10bf4f2c06b2b9ba1475d5","abstract_canon_sha256":"c10675f1f1996525e572a7cc15b0f93ae60ad63ff9b77f026b4a5ec8752398c2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:16:26.888249Z","signature_b64":"4VlqXCs5ruRGe8EPsBDfxHMFsDMeeMi08T+80iv5AyZUYK98h1vdizxhJp+roKD7ng/9zrC93/t1T2+qlWu4BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"01a9ea466e3b6751caf27c08515b352da71f419e4d35d857dae3934685f16d01","last_reissued_at":"2026-05-18T01:16:26.887802Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:16:26.887802Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analytical transformed harmonic oscillator basis for three-body nuclei of astrophysical interest: Application to 6He","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"J. Casal, J. M. Arias, M. Rodr\\'iguez-Gallardo","submitted_at":"2013-07-24T11:07:50Z","abstract_excerpt":"Recently, a square-integrable discrete basis, obtained performing a simple analytical local scale transformation to the harmonic oscillator basis, has been proposed and successfully applied to study the properties of two-body systems. Here, the method is generalized to study three-body systems. To test the goodness of the formalism and establish its applicability and limitations, the capture reaction rate for the nucleosynthesis of the Borromean nucleus 6He (4He + n + n) is addressed. Results are compared with previous publications and with calculations based on actual three-body continuum wav"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.6383","kind":"arxiv","version":1},"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":"1307.6383","created_at":"2026-05-18T01:16:26.887874+00:00"},{"alias_kind":"arxiv_version","alias_value":"1307.6383v1","created_at":"2026-05-18T01:16:26.887874+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.6383","created_at":"2026-05-18T01:16:26.887874+00:00"},{"alias_kind":"pith_short_12","alias_value":"AGU6URTOHNTV","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_16","alias_value":"AGU6URTOHNTVDSXS","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_8","alias_value":"AGU6URTO","created_at":"2026-05-18T12:27:38.830355+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/AGU6URTOHNTVDSXSPQEFCWZVFW","json":"https://pith.science/pith/AGU6URTOHNTVDSXSPQEFCWZVFW.json","graph_json":"https://pith.science/api/pith-number/AGU6URTOHNTVDSXSPQEFCWZVFW/graph.json","events_json":"https://pith.science/api/pith-number/AGU6URTOHNTVDSXSPQEFCWZVFW/events.json","paper":"https://pith.science/paper/AGU6URTO"},"agent_actions":{"view_html":"https://pith.science/pith/AGU6URTOHNTVDSXSPQEFCWZVFW","download_json":"https://pith.science/pith/AGU6URTOHNTVDSXSPQEFCWZVFW.json","view_paper":"https://pith.science/paper/AGU6URTO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1307.6383&json=true","fetch_graph":"https://pith.science/api/pith-number/AGU6URTOHNTVDSXSPQEFCWZVFW/graph.json","fetch_events":"https://pith.science/api/pith-number/AGU6URTOHNTVDSXSPQEFCWZVFW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AGU6URTOHNTVDSXSPQEFCWZVFW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AGU6URTOHNTVDSXSPQEFCWZVFW/action/storage_attestation","attest_author":"https://pith.science/pith/AGU6URTOHNTVDSXSPQEFCWZVFW/action/author_attestation","sign_citation":"https://pith.science/pith/AGU6URTOHNTVDSXSPQEFCWZVFW/action/citation_signature","submit_replication":"https://pith.science/pith/AGU6URTOHNTVDSXSPQEFCWZVFW/action/replication_record"}},"created_at":"2026-05-18T01:16:26.887874+00:00","updated_at":"2026-05-18T01:16:26.887874+00:00"}