{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:EC5G6WFF2EM6XIP7BYDCSEPYHF","short_pith_number":"pith:EC5G6WFF","canonical_record":{"source":{"id":"1705.06536","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-05-18T11:47:38Z","cross_cats_sorted":["nlin.PS"],"title_canon_sha256":"cdb22ed9f1347d2fd815f1a8c51069447f4fa0a937d59e8d3e788ce2b7eeba25","abstract_canon_sha256":"c2d488e262f447c3b7c45312d3a76e43fb25ab7b2f963a97b8c53e1c64bcc187"},"schema_version":"1.0"},"canonical_sha256":"20ba6f58a5d119eba1ff0e062911f83970f3fad771905a7a6c0114a38ef6da68","source":{"kind":"arxiv","id":"1705.06536","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.06536","created_at":"2026-05-18T00:38:52Z"},{"alias_kind":"arxiv_version","alias_value":"1705.06536v1","created_at":"2026-05-18T00:38:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.06536","created_at":"2026-05-18T00:38:52Z"},{"alias_kind":"pith_short_12","alias_value":"EC5G6WFF2EM6","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_16","alias_value":"EC5G6WFF2EM6XIP7","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_8","alias_value":"EC5G6WFF","created_at":"2026-05-18T12:31:12Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:EC5G6WFF2EM6XIP7BYDCSEPYHF","target":"record","payload":{"canonical_record":{"source":{"id":"1705.06536","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-05-18T11:47:38Z","cross_cats_sorted":["nlin.PS"],"title_canon_sha256":"cdb22ed9f1347d2fd815f1a8c51069447f4fa0a937d59e8d3e788ce2b7eeba25","abstract_canon_sha256":"c2d488e262f447c3b7c45312d3a76e43fb25ab7b2f963a97b8c53e1c64bcc187"},"schema_version":"1.0"},"canonical_sha256":"20ba6f58a5d119eba1ff0e062911f83970f3fad771905a7a6c0114a38ef6da68","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:52.404757Z","signature_b64":"ceZ+0gE/2XlIxD3Po1sbW7e74TGtLDLWXW6dbnw6nANOYH+TqNg5G657h4DG8O6Q1Hsyibkj3A/QIBhEmM77Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"20ba6f58a5d119eba1ff0e062911f83970f3fad771905a7a6c0114a38ef6da68","last_reissued_at":"2026-05-18T00:38:52.404220Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:52.404220Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1705.06536","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:38:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"B07b65GoJ/vWHwJITDGuziClgSXsfbyemp/v5hVl/AFfkoRRJ0tAef3fPd2Ek3e3CcVMmLk4Y7iDhQx1noFkDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T23:14:18.744748Z"},"content_sha256":"93b20b03c0dd74a5beb6df9273e11f925c25837bdb388df02a40ac3a60c33eba","schema_version":"1.0","event_id":"sha256:93b20b03c0dd74a5beb6df9273e11f925c25837bdb388df02a40ac3a60c33eba"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:EC5G6WFF2EM6XIP7BYDCSEPYHF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The interaction of Airy waves and solitons in the three-wave system","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.PS"],"primary_cat":"physics.optics","authors_text":"Boris A. Malomed, Thawatchai Mayteevarunyoo","submitted_at":"2017-05-18T11:47:38Z","abstract_excerpt":"We employ the generic three-wave system, with the $\\chi ^{(2)}$ interaction between two components of the fundamental-frequency (FF) wave and second-harmonic (SH) one, to consider collisions of truncated Airy waves (TAWs) and three-wave solitons in a setting which is not available in other nonlinear systems. The advantage is that the single-wave TAWs, carried by either one of the FF component, are not distorted by the nonlinearity and are stable, three-wave solitons being stable too in the same system. The collision between mutually symmetric TAWs, carried by the different FF components, trans"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.06536","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:38:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"E9NFPa8mikIHS8m8J6dTzmezYX0795zmoOGhTQN1UXce4xFLdVhmOFfhJrPiTqrGuEo3HjK7NlN6/3VWmIyZBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T23:14:18.745518Z"},"content_sha256":"d48883f5c27d0c6cc5a378a99d243f49bccf79ba3ea3711f1d434f6ea38d9048","schema_version":"1.0","event_id":"sha256:d48883f5c27d0c6cc5a378a99d243f49bccf79ba3ea3711f1d434f6ea38d9048"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EC5G6WFF2EM6XIP7BYDCSEPYHF/bundle.json","state_url":"https://pith.science/pith/EC5G6WFF2EM6XIP7BYDCSEPYHF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EC5G6WFF2EM6XIP7BYDCSEPYHF/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-30T23:14:18Z","links":{"resolver":"https://pith.science/pith/EC5G6WFF2EM6XIP7BYDCSEPYHF","bundle":"https://pith.science/pith/EC5G6WFF2EM6XIP7BYDCSEPYHF/bundle.json","state":"https://pith.science/pith/EC5G6WFF2EM6XIP7BYDCSEPYHF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EC5G6WFF2EM6XIP7BYDCSEPYHF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:EC5G6WFF2EM6XIP7BYDCSEPYHF","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":"c2d488e262f447c3b7c45312d3a76e43fb25ab7b2f963a97b8c53e1c64bcc187","cross_cats_sorted":["nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-05-18T11:47:38Z","title_canon_sha256":"cdb22ed9f1347d2fd815f1a8c51069447f4fa0a937d59e8d3e788ce2b7eeba25"},"schema_version":"1.0","source":{"id":"1705.06536","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.06536","created_at":"2026-05-18T00:38:52Z"},{"alias_kind":"arxiv_version","alias_value":"1705.06536v1","created_at":"2026-05-18T00:38:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.06536","created_at":"2026-05-18T00:38:52Z"},{"alias_kind":"pith_short_12","alias_value":"EC5G6WFF2EM6","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_16","alias_value":"EC5G6WFF2EM6XIP7","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_8","alias_value":"EC5G6WFF","created_at":"2026-05-18T12:31:12Z"}],"graph_snapshots":[{"event_id":"sha256:d48883f5c27d0c6cc5a378a99d243f49bccf79ba3ea3711f1d434f6ea38d9048","target":"graph","created_at":"2026-05-18T00:38:52Z","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":"We employ the generic three-wave system, with the $\\chi ^{(2)}$ interaction between two components of the fundamental-frequency (FF) wave and second-harmonic (SH) one, to consider collisions of truncated Airy waves (TAWs) and three-wave solitons in a setting which is not available in other nonlinear systems. The advantage is that the single-wave TAWs, carried by either one of the FF component, are not distorted by the nonlinearity and are stable, three-wave solitons being stable too in the same system. The collision between mutually symmetric TAWs, carried by the different FF components, trans","authors_text":"Boris A. Malomed, Thawatchai Mayteevarunyoo","cross_cats":["nlin.PS"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-05-18T11:47:38Z","title":"The interaction of Airy waves and solitons in the three-wave system"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.06536","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":"sha256:93b20b03c0dd74a5beb6df9273e11f925c25837bdb388df02a40ac3a60c33eba","target":"record","created_at":"2026-05-18T00:38:52Z","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":"c2d488e262f447c3b7c45312d3a76e43fb25ab7b2f963a97b8c53e1c64bcc187","cross_cats_sorted":["nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-05-18T11:47:38Z","title_canon_sha256":"cdb22ed9f1347d2fd815f1a8c51069447f4fa0a937d59e8d3e788ce2b7eeba25"},"schema_version":"1.0","source":{"id":"1705.06536","kind":"arxiv","version":1}},"canonical_sha256":"20ba6f58a5d119eba1ff0e062911f83970f3fad771905a7a6c0114a38ef6da68","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"20ba6f58a5d119eba1ff0e062911f83970f3fad771905a7a6c0114a38ef6da68","first_computed_at":"2026-05-18T00:38:52.404220Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:38:52.404220Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ceZ+0gE/2XlIxD3Po1sbW7e74TGtLDLWXW6dbnw6nANOYH+TqNg5G657h4DG8O6Q1Hsyibkj3A/QIBhEmM77Dw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:38:52.404757Z","signed_message":"canonical_sha256_bytes"},"source_id":"1705.06536","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:93b20b03c0dd74a5beb6df9273e11f925c25837bdb388df02a40ac3a60c33eba","sha256:d48883f5c27d0c6cc5a378a99d243f49bccf79ba3ea3711f1d434f6ea38d9048"],"state_sha256":"7019f4de6770e1fe008efef36e5b97e9facd399f0cde2dc40d523608da936b7c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"18BMmOxUIpwGL3MqC+KpWAy6WZIwCro++3+6oaCrnkCc+ILi7TtLmUykvWg86R4FQ4iSfQsRgn8xlDyznHDKAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T23:14:18.749391Z","bundle_sha256":"cd063d7c4a2f25f5dfbc15602b45d7122608f0e332cb3885519d97d1669e1728"}}