{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:SLXLL4UI7ETTIOLX55JVWSUCGN","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"cac9e88db7450ff9e32676bb84084bf8d0aa02e3fa1ed9983808e544ea5dcf2c","cross_cats_sorted":["cond-mat.quant-gas"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-06-14T01:01:26Z","title_canon_sha256":"93749119b42d100f6f928d4c44f407cbca7b3eed8e71845ebabe7aa4fc891602"},"schema_version":"1.0","source":{"id":"1906.05974","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1906.05974","created_at":"2026-05-17T23:39:43Z"},{"alias_kind":"arxiv_version","alias_value":"1906.05974v1","created_at":"2026-05-17T23:39:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1906.05974","created_at":"2026-05-17T23:39:43Z"},{"alias_kind":"pith_short_12","alias_value":"SLXLL4UI7ETT","created_at":"2026-05-18T12:33:27Z"},{"alias_kind":"pith_short_16","alias_value":"SLXLL4UI7ETTIOLX","created_at":"2026-05-18T12:33:27Z"},{"alias_kind":"pith_short_8","alias_value":"SLXLL4UI","created_at":"2026-05-18T12:33:27Z"}],"graph_snapshots":[{"event_id":"sha256:e6f11b8cd0da96144586970c5cc94d71a6dcd03f02fbcce28a98d4e86cb43c3f","target":"graph","created_at":"2026-05-17T23:39:43Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Stimulated Raman adiabatic passage (STIRAP) allows to efficiently transferring the populations between two discrete quantum states and has been used to prepare molecules in their rovibrational ground state. In realistic molecules, a well-resolved intermediate state is usually selected to implement the resonant STIRAP. Due to the complex molecular level structures, the detuned STIRAP always coexists with the resonant STIRAP and may cause unexpected interference phenomenon. However, it is generally accepted that the detuned STIRAP can be neglected if compared with the resonant STIRAP. Here we re","authors_text":"Bo Zhao, De-Chao Zhang, Huan Yang, Jian-Wei Pan, Jue Nan, Jun Rui, Lan Liu, Ya-Xiong Liu","cross_cats":["cond-mat.quant-gas"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-06-14T01:01:26Z","title":"Observation of interference between resonant and detuned STIRAP in the adiabatic creation of $^{23}$Na$^{40}$K molecules"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1906.05974","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:7f7482ad5d6b5ecfa6825baa047ff9962283894130a3182c7058389bdf120e50","target":"record","created_at":"2026-05-17T23:39:43Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"cac9e88db7450ff9e32676bb84084bf8d0aa02e3fa1ed9983808e544ea5dcf2c","cross_cats_sorted":["cond-mat.quant-gas"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-06-14T01:01:26Z","title_canon_sha256":"93749119b42d100f6f928d4c44f407cbca7b3eed8e71845ebabe7aa4fc891602"},"schema_version":"1.0","source":{"id":"1906.05974","kind":"arxiv","version":1}},"canonical_sha256":"92eeb5f288f927343977ef535b4a82337479ac196973b8a47950f18e0e7a1afc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"92eeb5f288f927343977ef535b4a82337479ac196973b8a47950f18e0e7a1afc","first_computed_at":"2026-05-17T23:39:43.106987Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:39:43.106987Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/iJzGSE03NGA8eHGoNAN77wAJncAY5AANcdtu4LphZn19+czg3+AyqKh7ehCFxUtwr21z3ahVVuZmw0kn4ZDDg==","signature_status":"signed_v1","signed_at":"2026-05-17T23:39:43.107618Z","signed_message":"canonical_sha256_bytes"},"source_id":"1906.05974","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7f7482ad5d6b5ecfa6825baa047ff9962283894130a3182c7058389bdf120e50","sha256:e6f11b8cd0da96144586970c5cc94d71a6dcd03f02fbcce28a98d4e86cb43c3f"],"state_sha256":"c5fc887fedfea01f59eee0545def2781de0324f9adef670d693597d3a6d12b9f"}