{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:XXXV4NH3A3CGMLLEAIC4Z76KFW","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":"e7fd4a121f887e06b74bd1262cb407b052793edeba09cbfa32f44168c048e3f1","cross_cats_sorted":["nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2019-04-05T08:28:59Z","title_canon_sha256":"f37c68d229bb355f6c68e62162d5293234e03e65af2696c7a3c4cbd38afb5f52"},"schema_version":"1.0","source":{"id":"1904.02933","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1904.02933","created_at":"2026-07-05T03:30:49Z"},{"alias_kind":"arxiv_version","alias_value":"1904.02933v2","created_at":"2026-07-05T03:30:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1904.02933","created_at":"2026-07-05T03:30:49Z"},{"alias_kind":"pith_short_12","alias_value":"XXXV4NH3A3CG","created_at":"2026-07-05T03:30:49Z"},{"alias_kind":"pith_short_16","alias_value":"XXXV4NH3A3CGMLLE","created_at":"2026-07-05T03:30:49Z"},{"alias_kind":"pith_short_8","alias_value":"XXXV4NH3","created_at":"2026-07-05T03:30:49Z"}],"graph_snapshots":[{"event_id":"sha256:24f98b47466306a84d57ee26ad71b6142358d2421540c10a55169eaaf974a7a2","target":"graph","created_at":"2026-07-05T03:30:49Z","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/1904.02933/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Over the last dozen of years, the area of accelerating waves has made considerable advances not only in terms of fundamentals and experimental demonstrations but also in connection to a wide range of applications. Starting from the prototypical Airy beam that was proposed and observed in 2007, new families of accelerating waves have been identified in the paraxial and nonparaxial domains in space and/or time, with different methods developed to control at will their trajectory, amplitude, and beam width. Accelerating optical waves exhibit a number of highly desirable attributes. They move alon","authors_text":"Demetrios N. Christodoulides, Mordechai Segev, Nikolaos K. Efremidis, Zhigang Chen","cross_cats":["nlin.PS"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2019-04-05T08:28:59Z","title":"Airy beams and accelerating waves: An overview of recent advances"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1904.02933","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:e2f8ddc4f6354d245fe5af38a2e6b4d46dd7cbb4b51347901af719dd78d00a92","target":"record","created_at":"2026-07-05T03:30:49Z","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":"e7fd4a121f887e06b74bd1262cb407b052793edeba09cbfa32f44168c048e3f1","cross_cats_sorted":["nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2019-04-05T08:28:59Z","title_canon_sha256":"f37c68d229bb355f6c68e62162d5293234e03e65af2696c7a3c4cbd38afb5f52"},"schema_version":"1.0","source":{"id":"1904.02933","kind":"arxiv","version":2}},"canonical_sha256":"bdef5e34fb06c4662d640205ccffca2da33f53d66e9e5695d8e0a2470a71d622","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bdef5e34fb06c4662d640205ccffca2da33f53d66e9e5695d8e0a2470a71d622","first_computed_at":"2026-07-05T03:30:49.296344Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T03:30:49.296344Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xRmpLn2aNO3i3o1/RaBSFTnHBjr0gu16RBryRN2yfukicUdbHOLFQzEMv8bvR50B/Stx5kR1WHhcuEojL8trBA==","signature_status":"signed_v1","signed_at":"2026-07-05T03:30:49.296867Z","signed_message":"canonical_sha256_bytes"},"source_id":"1904.02933","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e2f8ddc4f6354d245fe5af38a2e6b4d46dd7cbb4b51347901af719dd78d00a92","sha256:24f98b47466306a84d57ee26ad71b6142358d2421540c10a55169eaaf974a7a2"],"state_sha256":"a36de925ed950bd0944f72824b8ef5b36b1f4ac6d78734b7b4ea5bf230a9eb02"}