{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:HXNTI6KMZEUD7USK4HNDS4RYXD","short_pith_number":"pith:HXNTI6KM","schema_version":"1.0","canonical_sha256":"3ddb34794cc9283fd24ae1da397238b8c0f098bbb8dab347a45a1eb27e46886b","source":{"kind":"arxiv","id":"0812.1002","version":1},"attestation_state":"computed","paper":{"title":"Formation of ultracold dipolar molecules in the lowest vibrational levels by photoassociation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"A. Grochola, C. Gl\\\"uck, J. Deiglmayr, J. Lange, K. M\\\"ortlbauer, M. Repp, M. Weidem\\\"uller, O. Dulieu, R. Wester","submitted_at":"2008-12-04T18:40:20Z","abstract_excerpt":"We recently reported the formation of ultracold LiCs molecules in the rovibrational ground state X1Sigma+,v''=0,J''=0 [J. Deiglmayr et al., PRL 101, 133004 (2008)]. Here we discuss details of the experimental setup and present a thorough analysis of the photoassociation step including the photoassociation line shape. We predict the distribution of produced ground state molecules using accurate potential nergy curves combined with an ab-initio dipole transition moment and compare this prediction with experimental ionization spectra. Additionally we improve the value of the dissociation energy f"},"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":"0812.1002","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2008-12-04T18:40:20Z","cross_cats_sorted":[],"title_canon_sha256":"63d158fe62aed843782509db8d98c0b683431b51555f4e4ba4dfd104b3d69b39","abstract_canon_sha256":"9db957e515e6f62522d8ddd6666e10027431ada0fee1d0b6b025e7c7803b65c4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:15:11.815651Z","signature_b64":"kSa0S4ElpNrgZ+LonO6Hsek6b113hFsoT7ryP5a8iCITbuB5ppLpylpSD29O9qSalP012YGmbxXJ6go65pjzBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3ddb34794cc9283fd24ae1da397238b8c0f098bbb8dab347a45a1eb27e46886b","last_reissued_at":"2026-05-18T02:15:11.815024Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:15:11.815024Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Formation of ultracold dipolar molecules in the lowest vibrational levels by photoassociation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"A. Grochola, C. Gl\\\"uck, J. Deiglmayr, J. Lange, K. M\\\"ortlbauer, M. Repp, M. Weidem\\\"uller, O. Dulieu, R. Wester","submitted_at":"2008-12-04T18:40:20Z","abstract_excerpt":"We recently reported the formation of ultracold LiCs molecules in the rovibrational ground state X1Sigma+,v''=0,J''=0 [J. Deiglmayr et al., PRL 101, 133004 (2008)]. Here we discuss details of the experimental setup and present a thorough analysis of the photoassociation step including the photoassociation line shape. We predict the distribution of produced ground state molecules using accurate potential nergy curves combined with an ab-initio dipole transition moment and compare this prediction with experimental ionization spectra. Additionally we improve the value of the dissociation energy f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0812.1002","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":"0812.1002","created_at":"2026-05-18T02:15:11.815145+00:00"},{"alias_kind":"arxiv_version","alias_value":"0812.1002v1","created_at":"2026-05-18T02:15:11.815145+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0812.1002","created_at":"2026-05-18T02:15:11.815145+00:00"},{"alias_kind":"pith_short_12","alias_value":"HXNTI6KMZEUD","created_at":"2026-05-18T12:25:57.157939+00:00"},{"alias_kind":"pith_short_16","alias_value":"HXNTI6KMZEUD7USK","created_at":"2026-05-18T12:25:57.157939+00:00"},{"alias_kind":"pith_short_8","alias_value":"HXNTI6KM","created_at":"2026-05-18T12:25:57.157939+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/HXNTI6KMZEUD7USK4HNDS4RYXD","json":"https://pith.science/pith/HXNTI6KMZEUD7USK4HNDS4RYXD.json","graph_json":"https://pith.science/api/pith-number/HXNTI6KMZEUD7USK4HNDS4RYXD/graph.json","events_json":"https://pith.science/api/pith-number/HXNTI6KMZEUD7USK4HNDS4RYXD/events.json","paper":"https://pith.science/paper/HXNTI6KM"},"agent_actions":{"view_html":"https://pith.science/pith/HXNTI6KMZEUD7USK4HNDS4RYXD","download_json":"https://pith.science/pith/HXNTI6KMZEUD7USK4HNDS4RYXD.json","view_paper":"https://pith.science/paper/HXNTI6KM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0812.1002&json=true","fetch_graph":"https://pith.science/api/pith-number/HXNTI6KMZEUD7USK4HNDS4RYXD/graph.json","fetch_events":"https://pith.science/api/pith-number/HXNTI6KMZEUD7USK4HNDS4RYXD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HXNTI6KMZEUD7USK4HNDS4RYXD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HXNTI6KMZEUD7USK4HNDS4RYXD/action/storage_attestation","attest_author":"https://pith.science/pith/HXNTI6KMZEUD7USK4HNDS4RYXD/action/author_attestation","sign_citation":"https://pith.science/pith/HXNTI6KMZEUD7USK4HNDS4RYXD/action/citation_signature","submit_replication":"https://pith.science/pith/HXNTI6KMZEUD7USK4HNDS4RYXD/action/replication_record"}},"created_at":"2026-05-18T02:15:11.815145+00:00","updated_at":"2026-05-18T02:15:11.815145+00:00"}