{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:QMCAIRV3VRJBAMBGNNBCWVIIMR","short_pith_number":"pith:QMCAIRV3","schema_version":"1.0","canonical_sha256":"83040446bbac521030266b422b5508646e05bdca10524ea69081b2b7848fd3f8","source":{"kind":"arxiv","id":"2406.13157","version":2},"attestation_state":"computed","paper":{"title":"Genetics-based deperturbation analysis for the spin-orbit coupled ${\\rm A}^1\\Sigma^+$ and ${\\rm b}^3\\Pi_{0^+}$ states of LiRb","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.comp-ph"],"primary_cat":"physics.atom-ph","authors_text":"Gaoren Wang, Jie Yu, Xin-Yu Luo, Xuechun Li, Xuhui Bai, Yide Yin, Yongchang Han","submitted_at":"2024-06-19T02:20:05Z","abstract_excerpt":"We present a deperturbation analysis of the spin-orbit coupled $\\rm A^1\\Sigma^+$ and $\\rm b^3\\Pi_{0^+}$ states of LiRb based on the rovibrational energy levels observed previously by photoassociation spectroscopy in bosonic $^7$Li$^{85}$Rb molecule. Using the genetic algorithm, we fit the potential energy curves of the $\\rm A^1\\Sigma^+$ state and the $\\rm b^3\\Pi$ state into point-wise form. We then fit these point-wise potentials along with the spin-orbit coupling into expanded Morse oscillator functional form and optimise analytical parameters based on the experimental data. From the fitted r"},"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":"2406.13157","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2024-06-19T02:20:05Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"960272217bc4666fb04fd2a627b76096763d6a295aa640e7b0af7785e475ed48","abstract_canon_sha256":"8be4fe3739737814cfdfc680014a47c3cf3150733ce9801656ed4276c5982da4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:19:29.447235Z","signature_b64":"KfLbsGRmlopLI4CDJnsxfqIThBGPG9SpjHFM8o8PvAspFGVpf3CTTHqTaKuO1RmeefEfrcdukMF9weNKeIYKCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"83040446bbac521030266b422b5508646e05bdca10524ea69081b2b7848fd3f8","last_reissued_at":"2026-07-05T09:19:29.446792Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:19:29.446792Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Genetics-based deperturbation analysis for the spin-orbit coupled ${\\rm A}^1\\Sigma^+$ and ${\\rm b}^3\\Pi_{0^+}$ states of LiRb","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.comp-ph"],"primary_cat":"physics.atom-ph","authors_text":"Gaoren Wang, Jie Yu, Xin-Yu Luo, Xuechun Li, Xuhui Bai, Yide Yin, Yongchang Han","submitted_at":"2024-06-19T02:20:05Z","abstract_excerpt":"We present a deperturbation analysis of the spin-orbit coupled $\\rm A^1\\Sigma^+$ and $\\rm b^3\\Pi_{0^+}$ states of LiRb based on the rovibrational energy levels observed previously by photoassociation spectroscopy in bosonic $^7$Li$^{85}$Rb molecule. Using the genetic algorithm, we fit the potential energy curves of the $\\rm A^1\\Sigma^+$ state and the $\\rm b^3\\Pi$ state into point-wise form. We then fit these point-wise potentials along with the spin-orbit coupling into expanded Morse oscillator functional form and optimise analytical parameters based on the experimental data. From the fitted r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.13157","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2406.13157/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2406.13157","created_at":"2026-07-05T09:19:29.446846+00:00"},{"alias_kind":"arxiv_version","alias_value":"2406.13157v2","created_at":"2026-07-05T09:19:29.446846+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.13157","created_at":"2026-07-05T09:19:29.446846+00:00"},{"alias_kind":"pith_short_12","alias_value":"QMCAIRV3VRJB","created_at":"2026-07-05T09:19:29.446846+00:00"},{"alias_kind":"pith_short_16","alias_value":"QMCAIRV3VRJBAMBG","created_at":"2026-07-05T09:19:29.446846+00:00"},{"alias_kind":"pith_short_8","alias_value":"QMCAIRV3","created_at":"2026-07-05T09:19:29.446846+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/QMCAIRV3VRJBAMBGNNBCWVIIMR","json":"https://pith.science/pith/QMCAIRV3VRJBAMBGNNBCWVIIMR.json","graph_json":"https://pith.science/api/pith-number/QMCAIRV3VRJBAMBGNNBCWVIIMR/graph.json","events_json":"https://pith.science/api/pith-number/QMCAIRV3VRJBAMBGNNBCWVIIMR/events.json","paper":"https://pith.science/paper/QMCAIRV3"},"agent_actions":{"view_html":"https://pith.science/pith/QMCAIRV3VRJBAMBGNNBCWVIIMR","download_json":"https://pith.science/pith/QMCAIRV3VRJBAMBGNNBCWVIIMR.json","view_paper":"https://pith.science/paper/QMCAIRV3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2406.13157&json=true","fetch_graph":"https://pith.science/api/pith-number/QMCAIRV3VRJBAMBGNNBCWVIIMR/graph.json","fetch_events":"https://pith.science/api/pith-number/QMCAIRV3VRJBAMBGNNBCWVIIMR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QMCAIRV3VRJBAMBGNNBCWVIIMR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QMCAIRV3VRJBAMBGNNBCWVIIMR/action/storage_attestation","attest_author":"https://pith.science/pith/QMCAIRV3VRJBAMBGNNBCWVIIMR/action/author_attestation","sign_citation":"https://pith.science/pith/QMCAIRV3VRJBAMBGNNBCWVIIMR/action/citation_signature","submit_replication":"https://pith.science/pith/QMCAIRV3VRJBAMBGNNBCWVIIMR/action/replication_record"}},"created_at":"2026-07-05T09:19:29.446846+00:00","updated_at":"2026-07-05T09:19:29.446846+00:00"}