{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:QNZ76ETRQ3BWORXHUMSCMUEI4Y","short_pith_number":"pith:QNZ76ETR","schema_version":"1.0","canonical_sha256":"8373ff127186c36746e7a324265088e62746b031e043a0152fdbb69ba64abd3d","source":{"kind":"arxiv","id":"1511.02225","version":1},"attestation_state":"computed","paper":{"title":"Doublon dynamics and polar molecule production in an optical lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Ana Maria Rey, Arghavan Safavi-Naini, Deborah S. Jin, Jacob P. Covey, Johannes Schachenmayer, Jun Ye, Martin Garttner, Matthew T. Miecnikowski, Paul S. Julienne, Steven A. Moses, Zhengkun Fu","submitted_at":"2015-11-06T20:52:07Z","abstract_excerpt":"Ultracold polar molecules provide an excellent platform to study quantum many-body spin dynamics, which has become accessible in the recently realized low entropy quantum gas of polar molecules in an optical lattice. To obtain a detailed understanding for the molecular formation process in the lattice, we prepare a density distribution where lattice sites are either empty or occupied by a doublon composed of a bosonic atom interacting with a fermionic atom. By letting this disordered, out-of-equilibrium system evolve from a well-defined initial condition, we observe clear effects on pairing th"},"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":"1511.02225","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-11-06T20:52:07Z","cross_cats_sorted":["physics.atom-ph","quant-ph"],"title_canon_sha256":"8605047e16c2fec9eb592204792df0b9a1b9d2eef888fa684421ff7cecc6fc7a","abstract_canon_sha256":"9dc77549cddd2e3dd9d3921333c26696e89199ebb4bdbd5cd7d3e521ede73fc3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:12:49.514233Z","signature_b64":"4JRiD/OET5KZOmAMd75FH2Vh5LCOApph788jrXZU5KHAiq0EZ02sHBLyt5kAi2CoiOnWrgEmbuuV91/PUvtxDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8373ff127186c36746e7a324265088e62746b031e043a0152fdbb69ba64abd3d","last_reissued_at":"2026-05-18T01:12:49.513899Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:12:49.513899Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Doublon dynamics and polar molecule production in an optical lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Ana Maria Rey, Arghavan Safavi-Naini, Deborah S. Jin, Jacob P. Covey, Johannes Schachenmayer, Jun Ye, Martin Garttner, Matthew T. Miecnikowski, Paul S. Julienne, Steven A. Moses, Zhengkun Fu","submitted_at":"2015-11-06T20:52:07Z","abstract_excerpt":"Ultracold polar molecules provide an excellent platform to study quantum many-body spin dynamics, which has become accessible in the recently realized low entropy quantum gas of polar molecules in an optical lattice. To obtain a detailed understanding for the molecular formation process in the lattice, we prepare a density distribution where lattice sites are either empty or occupied by a doublon composed of a bosonic atom interacting with a fermionic atom. By letting this disordered, out-of-equilibrium system evolve from a well-defined initial condition, we observe clear effects on pairing th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.02225","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":"1511.02225","created_at":"2026-05-18T01:12:49.513953+00:00"},{"alias_kind":"arxiv_version","alias_value":"1511.02225v1","created_at":"2026-05-18T01:12:49.513953+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.02225","created_at":"2026-05-18T01:12:49.513953+00:00"},{"alias_kind":"pith_short_12","alias_value":"QNZ76ETRQ3BW","created_at":"2026-05-18T12:29:37.295048+00:00"},{"alias_kind":"pith_short_16","alias_value":"QNZ76ETRQ3BWORXH","created_at":"2026-05-18T12:29:37.295048+00:00"},{"alias_kind":"pith_short_8","alias_value":"QNZ76ETR","created_at":"2026-05-18T12:29:37.295048+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/QNZ76ETRQ3BWORXHUMSCMUEI4Y","json":"https://pith.science/pith/QNZ76ETRQ3BWORXHUMSCMUEI4Y.json","graph_json":"https://pith.science/api/pith-number/QNZ76ETRQ3BWORXHUMSCMUEI4Y/graph.json","events_json":"https://pith.science/api/pith-number/QNZ76ETRQ3BWORXHUMSCMUEI4Y/events.json","paper":"https://pith.science/paper/QNZ76ETR"},"agent_actions":{"view_html":"https://pith.science/pith/QNZ76ETRQ3BWORXHUMSCMUEI4Y","download_json":"https://pith.science/pith/QNZ76ETRQ3BWORXHUMSCMUEI4Y.json","view_paper":"https://pith.science/paper/QNZ76ETR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1511.02225&json=true","fetch_graph":"https://pith.science/api/pith-number/QNZ76ETRQ3BWORXHUMSCMUEI4Y/graph.json","fetch_events":"https://pith.science/api/pith-number/QNZ76ETRQ3BWORXHUMSCMUEI4Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QNZ76ETRQ3BWORXHUMSCMUEI4Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QNZ76ETRQ3BWORXHUMSCMUEI4Y/action/storage_attestation","attest_author":"https://pith.science/pith/QNZ76ETRQ3BWORXHUMSCMUEI4Y/action/author_attestation","sign_citation":"https://pith.science/pith/QNZ76ETRQ3BWORXHUMSCMUEI4Y/action/citation_signature","submit_replication":"https://pith.science/pith/QNZ76ETRQ3BWORXHUMSCMUEI4Y/action/replication_record"}},"created_at":"2026-05-18T01:12:49.513953+00:00","updated_at":"2026-05-18T01:12:49.513953+00:00"}