{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:BPECKREER6KW33KTCM3TOTKQ3J","short_pith_number":"pith:BPECKREE","schema_version":"1.0","canonical_sha256":"0bc82544848f956ded531337374d50da57f5007d1e9716396e7592d03a6db13e","source":{"kind":"arxiv","id":"1306.0838","version":1},"attestation_state":"computed","paper":{"title":"Dipole transitions in the bound rotational-vibrational spectrum of the heteronuclear molecular ion HD$^+$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"physics.atm-clus","authors_text":"Daniel Baye, Horacio Olivares Pil\\'on","submitted_at":"2013-06-04T15:57:07Z","abstract_excerpt":"The non-relativistic three-body Schr\\\"odinger equation of the heteronuclear molecular ion HD$^+$ is solved in perimetric coordinates using the Lagrange-mesh method. Energies and wave functions of the four lowest vibrational bound or quasibound states $v=0-3$ are calculated for total orbital momenta from 0 to 47. Energies are given with an accuracy from about 12 digits for the lowest vibrational level to at least 9 digits for the third vibrational excited level. With a simple calculation using the corresponding wave functions, accurate dipole transition probabilities per time unit between those"},"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":"1306.0838","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atm-clus","submitted_at":"2013-06-04T15:57:07Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"b99410f95d3ef7f0837afc7b3f97f63b37df8fe34c29a759567602d00176a520","abstract_canon_sha256":"d41dcaa8aedb58c7802c8fc61e3313281356cf78a0202dcbd4f7b97adf56e95b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:49:33.000851Z","signature_b64":"Uy9NXix5Q3smCsBhnFco74e9ugFVZ/YGJM5JFaNuqj7NGTLoQOWyEBx2EJHgbnV8jTk0HK5v/gsayeMvHu3SAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0bc82544848f956ded531337374d50da57f5007d1e9716396e7592d03a6db13e","last_reissued_at":"2026-05-18T01:49:33.000351Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:49:33.000351Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dipole transitions in the bound rotational-vibrational spectrum of the heteronuclear molecular ion HD$^+$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"physics.atm-clus","authors_text":"Daniel Baye, Horacio Olivares Pil\\'on","submitted_at":"2013-06-04T15:57:07Z","abstract_excerpt":"The non-relativistic three-body Schr\\\"odinger equation of the heteronuclear molecular ion HD$^+$ is solved in perimetric coordinates using the Lagrange-mesh method. Energies and wave functions of the four lowest vibrational bound or quasibound states $v=0-3$ are calculated for total orbital momenta from 0 to 47. Energies are given with an accuracy from about 12 digits for the lowest vibrational level to at least 9 digits for the third vibrational excited level. With a simple calculation using the corresponding wave functions, accurate dipole transition probabilities per time unit between those"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.0838","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":"1306.0838","created_at":"2026-05-18T01:49:33.000448+00:00"},{"alias_kind":"arxiv_version","alias_value":"1306.0838v1","created_at":"2026-05-18T01:49:33.000448+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.0838","created_at":"2026-05-18T01:49:33.000448+00:00"},{"alias_kind":"pith_short_12","alias_value":"BPECKREER6KW","created_at":"2026-05-18T12:27:40.988391+00:00"},{"alias_kind":"pith_short_16","alias_value":"BPECKREER6KW33KT","created_at":"2026-05-18T12:27:40.988391+00:00"},{"alias_kind":"pith_short_8","alias_value":"BPECKREE","created_at":"2026-05-18T12:27:40.988391+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/BPECKREER6KW33KTCM3TOTKQ3J","json":"https://pith.science/pith/BPECKREER6KW33KTCM3TOTKQ3J.json","graph_json":"https://pith.science/api/pith-number/BPECKREER6KW33KTCM3TOTKQ3J/graph.json","events_json":"https://pith.science/api/pith-number/BPECKREER6KW33KTCM3TOTKQ3J/events.json","paper":"https://pith.science/paper/BPECKREE"},"agent_actions":{"view_html":"https://pith.science/pith/BPECKREER6KW33KTCM3TOTKQ3J","download_json":"https://pith.science/pith/BPECKREER6KW33KTCM3TOTKQ3J.json","view_paper":"https://pith.science/paper/BPECKREE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1306.0838&json=true","fetch_graph":"https://pith.science/api/pith-number/BPECKREER6KW33KTCM3TOTKQ3J/graph.json","fetch_events":"https://pith.science/api/pith-number/BPECKREER6KW33KTCM3TOTKQ3J/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BPECKREER6KW33KTCM3TOTKQ3J/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BPECKREER6KW33KTCM3TOTKQ3J/action/storage_attestation","attest_author":"https://pith.science/pith/BPECKREER6KW33KTCM3TOTKQ3J/action/author_attestation","sign_citation":"https://pith.science/pith/BPECKREER6KW33KTCM3TOTKQ3J/action/citation_signature","submit_replication":"https://pith.science/pith/BPECKREER6KW33KTCM3TOTKQ3J/action/replication_record"}},"created_at":"2026-05-18T01:49:33.000448+00:00","updated_at":"2026-05-18T01:49:33.000448+00:00"}