{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:4MHMRG2S56XTAVQK57BF2ZHHVL","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":"9a42cb05fbd27342bafff8ef55fb9a5cbcdada296efdd52df8027e98db58295f","cross_cats_sorted":["physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-04-13T09:14:10Z","title_canon_sha256":"89466a897246f01fee1b0ecbc43f553d0ec115cf9fb7b38da64cada3147d67f3"},"schema_version":"1.0","source":{"id":"2204.06262","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2204.06262","created_at":"2026-07-05T05:30:07Z"},{"alias_kind":"arxiv_version","alias_value":"2204.06262v4","created_at":"2026-07-05T05:30:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2204.06262","created_at":"2026-07-05T05:30:07Z"},{"alias_kind":"pith_short_12","alias_value":"4MHMRG2S56XT","created_at":"2026-07-05T05:30:07Z"},{"alias_kind":"pith_short_16","alias_value":"4MHMRG2S56XTAVQK","created_at":"2026-07-05T05:30:07Z"},{"alias_kind":"pith_short_8","alias_value":"4MHMRG2S","created_at":"2026-07-05T05:30:07Z"}],"graph_snapshots":[{"event_id":"sha256:2c36f33cad2b2128ee1984cfb4282d24539378f02429656108c0e18c4357e8d9","target":"graph","created_at":"2026-07-05T05:30:07Z","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/2204.06262/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate the attosecond transient absorption spectroscopy (ATAS) of graphene by numerically solving four-band density-matrix equations, which demonstrates apparent fish bone resonance structures. To gain insight into these interesting structures, we exploit a simplified model that only considers the electrons of $\\Gamma$ and M points in the Brillouin zone. With the help of this model, we can analytically express the ATAS spectrum as the sum of zeroth- and first-order Bessel functions in the variables of the strength and frequency of the infrared pump field as well as the effective mass o","authors_text":"Fulong Dong, Jie Liu","cross_cats":["physics.atom-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-04-13T09:14:10Z","title":"Fishbone resonance structure in the attosecond transient absorption spectroscopy of graphene"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2204.06262","kind":"arxiv","version":4},"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:f487708e95ca38f5ff814bc02ec1da428ac5b2f38151bac759ba3ee86f458b53","target":"record","created_at":"2026-07-05T05:30:07Z","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":"9a42cb05fbd27342bafff8ef55fb9a5cbcdada296efdd52df8027e98db58295f","cross_cats_sorted":["physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-04-13T09:14:10Z","title_canon_sha256":"89466a897246f01fee1b0ecbc43f553d0ec115cf9fb7b38da64cada3147d67f3"},"schema_version":"1.0","source":{"id":"2204.06262","kind":"arxiv","version":4}},"canonical_sha256":"e30ec89b52efaf30560aefc25d64e7aadb04d4d7696aa88097c99169bb692a4b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e30ec89b52efaf30560aefc25d64e7aadb04d4d7696aa88097c99169bb692a4b","first_computed_at":"2026-07-05T05:30:07.284209Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:30:07.284209Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"3HK/GIzpflc0/hb9hc8mAAkPKGpl0zFBbtUuZNzSehQIUJvvpigi4DWgihiT3AVmgWNZinXG1m+oLOj5Nx+zBw==","signature_status":"signed_v1","signed_at":"2026-07-05T05:30:07.284704Z","signed_message":"canonical_sha256_bytes"},"source_id":"2204.06262","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f487708e95ca38f5ff814bc02ec1da428ac5b2f38151bac759ba3ee86f458b53","sha256:2c36f33cad2b2128ee1984cfb4282d24539378f02429656108c0e18c4357e8d9"],"state_sha256":"d3efc0fd3bf77cfd592e4c2b9cbd5e742cef3f1ff6e2b6540cc0994d62e294d5"}