{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:BT2CBXY7WPB4HHO4XDSVCV64PH","short_pith_number":"pith:BT2CBXY7","schema_version":"1.0","canonical_sha256":"0cf420df1fb3c3c39ddcb8e55157dc79ce8be6b7f028978d4b5c484a47474549","source":{"kind":"arxiv","id":"1501.03793","version":2},"attestation_state":"computed","paper":{"title":"Polarizability of ultracold $\\textrm{Rb}_2$ molecules in the rovibrational ground state of $\\mathrm{a}^3\\Sigma_u^+$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas"],"primary_cat":"physics.atom-ph","authors_text":"Bj\\\"orn Drews, Johannes Hecker Denschlag, Markus Dei{\\ss}, Nadia Bouloufa-Maafa, Olivier Dulieu, Romain Vexiau","submitted_at":"2015-01-15T19:53:56Z","abstract_excerpt":"We study, both theoretically and experimentally, the dynamical polarizability $\\alpha(\\omega)$ of $\\textrm{Rb}_2$ molecules in the rovibrational ground state of $\\mathrm{a}^3\\Sigma_u^+$. Taking all relevant excited molecular bound states into account, we compute the complex-valued polarizability $\\alpha(\\omega)$ for wave numbers up to $20000\\:\\textrm{cm}^{-1}$. Our calculations are compared to experimental results at $1064.5\\:\\textrm{nm}$ ($\\sim9400\\:\\textrm{cm}^{-1}$) as well as at $830.4\\:\\textrm{nm}$ ($\\sim12000\\:\\textrm{cm}^{-1}$). Here, we discuss the measurements at $1064.5\\:\\textrm{nm}$"},"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":"1501.03793","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-01-15T19:53:56Z","cross_cats_sorted":["cond-mat.quant-gas"],"title_canon_sha256":"d32ada9e48d567b1fc1dbff58c00755a596daae4f94ea1b25d23daf105f2c574","abstract_canon_sha256":"c21922eb90c8e23b49eedbf64a4d2426ac90c84116dc8e2a2bf2fbe3ebc73fea"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:55:52.352206Z","signature_b64":"aBnf4/whfWu77irkG7kOePT+11610Y+ruPL15nsmevQ1uujMrvE3C3XTPdWwUtr5MllhZTwVP8o8ZuZk+rHbCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0cf420df1fb3c3c39ddcb8e55157dc79ce8be6b7f028978d4b5c484a47474549","last_reissued_at":"2026-05-18T00:55:52.351551Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:55:52.351551Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Polarizability of ultracold $\\textrm{Rb}_2$ molecules in the rovibrational ground state of $\\mathrm{a}^3\\Sigma_u^+$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas"],"primary_cat":"physics.atom-ph","authors_text":"Bj\\\"orn Drews, Johannes Hecker Denschlag, Markus Dei{\\ss}, Nadia Bouloufa-Maafa, Olivier Dulieu, Romain Vexiau","submitted_at":"2015-01-15T19:53:56Z","abstract_excerpt":"We study, both theoretically and experimentally, the dynamical polarizability $\\alpha(\\omega)$ of $\\textrm{Rb}_2$ molecules in the rovibrational ground state of $\\mathrm{a}^3\\Sigma_u^+$. Taking all relevant excited molecular bound states into account, we compute the complex-valued polarizability $\\alpha(\\omega)$ for wave numbers up to $20000\\:\\textrm{cm}^{-1}$. Our calculations are compared to experimental results at $1064.5\\:\\textrm{nm}$ ($\\sim9400\\:\\textrm{cm}^{-1}$) as well as at $830.4\\:\\textrm{nm}$ ($\\sim12000\\:\\textrm{cm}^{-1}$). Here, we discuss the measurements at $1064.5\\:\\textrm{nm}$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.03793","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":"1501.03793","created_at":"2026-05-18T00:55:52.351655+00:00"},{"alias_kind":"arxiv_version","alias_value":"1501.03793v2","created_at":"2026-05-18T00:55:52.351655+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.03793","created_at":"2026-05-18T00:55:52.351655+00:00"},{"alias_kind":"pith_short_12","alias_value":"BT2CBXY7WPB4","created_at":"2026-05-18T12:29:14.074870+00:00"},{"alias_kind":"pith_short_16","alias_value":"BT2CBXY7WPB4HHO4","created_at":"2026-05-18T12:29:14.074870+00:00"},{"alias_kind":"pith_short_8","alias_value":"BT2CBXY7","created_at":"2026-05-18T12:29:14.074870+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/BT2CBXY7WPB4HHO4XDSVCV64PH","json":"https://pith.science/pith/BT2CBXY7WPB4HHO4XDSVCV64PH.json","graph_json":"https://pith.science/api/pith-number/BT2CBXY7WPB4HHO4XDSVCV64PH/graph.json","events_json":"https://pith.science/api/pith-number/BT2CBXY7WPB4HHO4XDSVCV64PH/events.json","paper":"https://pith.science/paper/BT2CBXY7"},"agent_actions":{"view_html":"https://pith.science/pith/BT2CBXY7WPB4HHO4XDSVCV64PH","download_json":"https://pith.science/pith/BT2CBXY7WPB4HHO4XDSVCV64PH.json","view_paper":"https://pith.science/paper/BT2CBXY7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1501.03793&json=true","fetch_graph":"https://pith.science/api/pith-number/BT2CBXY7WPB4HHO4XDSVCV64PH/graph.json","fetch_events":"https://pith.science/api/pith-number/BT2CBXY7WPB4HHO4XDSVCV64PH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BT2CBXY7WPB4HHO4XDSVCV64PH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BT2CBXY7WPB4HHO4XDSVCV64PH/action/storage_attestation","attest_author":"https://pith.science/pith/BT2CBXY7WPB4HHO4XDSVCV64PH/action/author_attestation","sign_citation":"https://pith.science/pith/BT2CBXY7WPB4HHO4XDSVCV64PH/action/citation_signature","submit_replication":"https://pith.science/pith/BT2CBXY7WPB4HHO4XDSVCV64PH/action/replication_record"}},"created_at":"2026-05-18T00:55:52.351655+00:00","updated_at":"2026-05-18T00:55:52.351655+00:00"}