{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:4ZEO7ACVU5OF2PGUSI2WZXSC3F","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":"98ca3d59c679704755a47e3658b701f8a2c7fa5739e3557d026bc12893e50290","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-06-09T13:25:08Z","title_canon_sha256":"74dc937537228868f6637f6206b277abe865e7cd3b2d3093f77b3e59efb6e842"},"schema_version":"1.0","source":{"id":"2606.10837","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.10837","created_at":"2026-06-10T01:10:43Z"},{"alias_kind":"arxiv_version","alias_value":"2606.10837v1","created_at":"2026-06-10T01:10:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.10837","created_at":"2026-06-10T01:10:43Z"},{"alias_kind":"pith_short_12","alias_value":"4ZEO7ACVU5OF","created_at":"2026-06-10T01:10:43Z"},{"alias_kind":"pith_short_16","alias_value":"4ZEO7ACVU5OF2PGU","created_at":"2026-06-10T01:10:43Z"},{"alias_kind":"pith_short_8","alias_value":"4ZEO7ACV","created_at":"2026-06-10T01:10:43Z"}],"graph_snapshots":[{"event_id":"sha256:6d484f5702906664daee0d2aa44191f13bcf4135cf9f65febf6319b73ae98c7a","target":"graph","created_at":"2026-06-10T01:10:43Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2606.10837/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate the dependence on wavelength of nondipole effects in triple ionization of Ne driven by intense infrared and mid-infrared laser pulses using a three-dimensional semiclassical model that fully accounts for nondipole effects and the Coulomb singularity in the electron-core interaction. We find in triple ionization of strongly driven Ne a large positive average momentum offset along the direction of laser propagation, which vanishes in the dipole approximation. This positive momentum offset significantly increases with increasing wavelength of the laser pulse. This increase is prese","authors_text":"Agapi Emmanouilidou, Daria Romero Torres, Georgios Petros Katsoulis, Samuel James Praill","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-06-09T13:25:08Z","title":"Enhanced nondipole momentum offsets in triple ionization of atoms driven by mid-infrared laser fields"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.10837","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:a64e43b53820a8bfdb6d59c19c36f5ef664d0750bb26de1811cc01843cb94697","target":"record","created_at":"2026-06-10T01:10:43Z","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":"98ca3d59c679704755a47e3658b701f8a2c7fa5739e3557d026bc12893e50290","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-06-09T13:25:08Z","title_canon_sha256":"74dc937537228868f6637f6206b277abe865e7cd3b2d3093f77b3e59efb6e842"},"schema_version":"1.0","source":{"id":"2606.10837","kind":"arxiv","version":1}},"canonical_sha256":"e648ef8055a75c5d3cd492356cde42d96198313fd7a170599e81a53291a14291","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e648ef8055a75c5d3cd492356cde42d96198313fd7a170599e81a53291a14291","first_computed_at":"2026-06-10T01:10:43.222280Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-10T01:10:43.222280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"k2HIC5sLaH/s3HBW6s9kvWjnSs+ZVLH/hcLw+EYT8dCPpkcVbgPD12dhmybKvOIloLTWDI/NrnrmpWsMIwhZAg==","signature_status":"signed_v1","signed_at":"2026-06-10T01:10:43.223158Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.10837","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a64e43b53820a8bfdb6d59c19c36f5ef664d0750bb26de1811cc01843cb94697","sha256:6d484f5702906664daee0d2aa44191f13bcf4135cf9f65febf6319b73ae98c7a"],"state_sha256":"6365c2789993dfee9b944ad89c6649819fb4943cd7af03a1f64b4dc68e1e19ce"}