{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:7JEOQP4RTLUQT2XPIXJNFNHD7I","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":"50b9138654e83bd01a87cd2e40b0d699fdb099b60ca9b9b1a95a4b6de1bf7dda","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2023-11-19T06:05:42Z","title_canon_sha256":"1ad7002fd26f67a280aea02ba6e984cb89f59b87cc25a50c25e4a43dd312bf76"},"schema_version":"1.0","source":{"id":"2311.11242","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2311.11242","created_at":"2026-07-05T09:47:27Z"},{"alias_kind":"arxiv_version","alias_value":"2311.11242v2","created_at":"2026-07-05T09:47:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.11242","created_at":"2026-07-05T09:47:27Z"},{"alias_kind":"pith_short_12","alias_value":"7JEOQP4RTLUQ","created_at":"2026-07-05T09:47:27Z"},{"alias_kind":"pith_short_16","alias_value":"7JEOQP4RTLUQT2XP","created_at":"2026-07-05T09:47:27Z"},{"alias_kind":"pith_short_8","alias_value":"7JEOQP4R","created_at":"2026-07-05T09:47:27Z"}],"graph_snapshots":[{"event_id":"sha256:1a50145065eb135dc488fe7754559ff7880f805de50ecdb39bdffaab7a0057d6","target":"graph","created_at":"2026-07-05T09:47:27Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2311.11242/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Taking N2 and O2 as examples, we theoretically study the post-ionization dynamics of molecules in strong laser fields using a density matrix method for open systems, focusing on the effect of ionization-produced coherence on the dynamics of residual ions. We introduce the adiabatic strong-field approximation (ASFA) method to predict the coherences between ionic states resulting from multiorbital strong-field ionizations. Compared with the standard SFA, the ASFA method can be applied across a wide range of laser intensities due to the consideration of orbital distortion effects. Based on the AS","authors_text":"Anh-Thu Le, Hongchuan Du, PengJi Ding, Ping Li, Shan Xue, Song-Feng Zhao, Wenli Yang, Yuxuan Zhang","cross_cats":["physics.optics","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2023-11-19T06:05:42Z","title":"Coherent postionization dynamics of molecules based on adiabatic strong-field approximation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.11242","kind":"arxiv","version":2},"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":"sha256:44fbbc8a1b5b80303ee4a24958fe4bae456aaf596750bc3594fd8f7a1e21dc42","target":"record","created_at":"2026-07-05T09:47:27Z","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":"50b9138654e83bd01a87cd2e40b0d699fdb099b60ca9b9b1a95a4b6de1bf7dda","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2023-11-19T06:05:42Z","title_canon_sha256":"1ad7002fd26f67a280aea02ba6e984cb89f59b87cc25a50c25e4a43dd312bf76"},"schema_version":"1.0","source":{"id":"2311.11242","kind":"arxiv","version":2}},"canonical_sha256":"fa48e83f919ae909eaef45d2d2b4e3fa200d94926e49796f01a7e0e3c9114b4f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fa48e83f919ae909eaef45d2d2b4e3fa200d94926e49796f01a7e0e3c9114b4f","first_computed_at":"2026-07-05T09:47:27.214661Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:47:27.214661Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"QnGP4uTEOem+gDdLa+Mg+BV8MGAFnAjJCCSn8yXNEROEv+djZId+jadL1PLMxbHtEp3M1wf4z8Rr7RnVMR+lCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T09:47:27.215115Z","signed_message":"canonical_sha256_bytes"},"source_id":"2311.11242","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:44fbbc8a1b5b80303ee4a24958fe4bae456aaf596750bc3594fd8f7a1e21dc42","sha256:1a50145065eb135dc488fe7754559ff7880f805de50ecdb39bdffaab7a0057d6"],"state_sha256":"2f026f893ebbd8e48d6a48b01140c94e2e50a98d0ae163edf50fd5ff3af587a1"}