{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:QOUOBFD7NESX5YU5GUA2UP2CXO","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":"dfb5892098ec4a6aa242a04f1b015245fea9ad384f5f5c36615da09318ded4d3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-08-15T01:21:43Z","title_canon_sha256":"5462bc6c4ef69aa33865e199cf9c320af7c60a18ba7b9124150e6cb362fd9729"},"schema_version":"1.0","source":{"id":"1708.04374","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.04374","created_at":"2026-05-18T00:01:00Z"},{"alias_kind":"arxiv_version","alias_value":"1708.04374v3","created_at":"2026-05-18T00:01:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.04374","created_at":"2026-05-18T00:01:00Z"},{"alias_kind":"pith_short_12","alias_value":"QOUOBFD7NESX","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_16","alias_value":"QOUOBFD7NESX5YU5","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_8","alias_value":"QOUOBFD7","created_at":"2026-05-18T12:31:39Z"}],"graph_snapshots":[{"event_id":"sha256:c57b6ca37b3fee48694af5afcf09e262a7b51e0df1b917a783fcdbc40ef233a1","target":"graph","created_at":"2026-05-18T00:01:00Z","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":"During the ionization of atoms irradiated by linearly polarized intense laser fields, we find for the first time that the transverse momentum distribution of photoelectrons can be well fitted by a squared zeroth-order Bessel function because of the quantum interference effect of Glory rescattering. The characteristic of the Bessel function is determined by the common angular momentum of a bunch of semiclassical paths termed as Glory trajectories, which are launched with different nonzero initial transverse momenta distributed on a specific circle in the momentum plane and finally deflected to ","authors_text":"J. Cai, J. F. Tao, J. Liu, L. B. Fu, Q. Z. Xia","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-08-15T01:21:43Z","title":"Quantum Interference of Glory Rescattering in Strong-Field Atomic Ionization"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.04374","kind":"arxiv","version":3},"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":"sha256:8a4f17bb38f384930a812d0d3f542d64b42dfc8122483d9c9e4138206d85483c","target":"record","created_at":"2026-05-18T00:01:00Z","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":"dfb5892098ec4a6aa242a04f1b015245fea9ad384f5f5c36615da09318ded4d3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-08-15T01:21:43Z","title_canon_sha256":"5462bc6c4ef69aa33865e199cf9c320af7c60a18ba7b9124150e6cb362fd9729"},"schema_version":"1.0","source":{"id":"1708.04374","kind":"arxiv","version":3}},"canonical_sha256":"83a8e0947f69257ee29d3501aa3f42bb8897809a47cbe981405e9d8b43e147a2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"83a8e0947f69257ee29d3501aa3f42bb8897809a47cbe981405e9d8b43e147a2","first_computed_at":"2026-05-18T00:01:00.384378Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:01:00.384378Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qK/YJW4RihAYrsGJRPOAV4wGX3xc23u0HlrAE1uXgqewDVUKKEKojQuY621Uo23bs3sxI+VIvp+vYaKR1QvgAA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:01:00.384890Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.04374","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8a4f17bb38f384930a812d0d3f542d64b42dfc8122483d9c9e4138206d85483c","sha256:c57b6ca37b3fee48694af5afcf09e262a7b51e0df1b917a783fcdbc40ef233a1"],"state_sha256":"950737bac736325d11ca020912862d148a1d0a6f9b18c7adede146899d609d32"}