{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:OXE7M6V3OXO3SICJFDMMMFN3UX","short_pith_number":"pith:OXE7M6V3","canonical_record":{"source":{"id":"1504.04761","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2015-04-18T21:09:13Z","cross_cats_sorted":[],"title_canon_sha256":"66a7a84aa8db40fa0189117e4eabb796c1ac07630da20ebd1cd969007aa09ad0","abstract_canon_sha256":"aab2c4ddec06a5432ec0293e13a09e57a49f0cab1d7bb3c5eb3cdf15830d9321"},"schema_version":"1.0"},"canonical_sha256":"75c9f67abb75ddb9204928d8c615bba5ec60907a2680a7afebcc6ea20f329c01","source":{"kind":"arxiv","id":"1504.04761","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1504.04761","created_at":"2026-05-18T02:18:24Z"},{"alias_kind":"arxiv_version","alias_value":"1504.04761v1","created_at":"2026-05-18T02:18:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.04761","created_at":"2026-05-18T02:18:24Z"},{"alias_kind":"pith_short_12","alias_value":"OXE7M6V3OXO3","created_at":"2026-05-18T12:29:34Z"},{"alias_kind":"pith_short_16","alias_value":"OXE7M6V3OXO3SICJ","created_at":"2026-05-18T12:29:34Z"},{"alias_kind":"pith_short_8","alias_value":"OXE7M6V3","created_at":"2026-05-18T12:29:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:OXE7M6V3OXO3SICJFDMMMFN3UX","target":"record","payload":{"canonical_record":{"source":{"id":"1504.04761","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2015-04-18T21:09:13Z","cross_cats_sorted":[],"title_canon_sha256":"66a7a84aa8db40fa0189117e4eabb796c1ac07630da20ebd1cd969007aa09ad0","abstract_canon_sha256":"aab2c4ddec06a5432ec0293e13a09e57a49f0cab1d7bb3c5eb3cdf15830d9321"},"schema_version":"1.0"},"canonical_sha256":"75c9f67abb75ddb9204928d8c615bba5ec60907a2680a7afebcc6ea20f329c01","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:18:24.843421Z","signature_b64":"uC0AVieWRNVwyHRq6MHtWaCP1sfEE4RR0KhLUi8BeZissogPN3wFUwE5PsEf0DfGltHsiAVDoUO97p+tEVu8Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"75c9f67abb75ddb9204928d8c615bba5ec60907a2680a7afebcc6ea20f329c01","last_reissued_at":"2026-05-18T02:18:24.842716Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:18:24.842716Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1504.04761","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":"2026-05-18T02:18:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gmW5LGWUpI4ilem59Szs+7n1jtcgx8GKzjkT10Ui/mXNE6aO8rELZ8JfY2sZjhDSjpz/fREx2lE5NVQP1QNiAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T18:54:00.416600Z"},"content_sha256":"1612375729a7bfc7db86b7ecbbdf36cc7c69d631623c552dac843ca48fba55fa","schema_version":"1.0","event_id":"sha256:1612375729a7bfc7db86b7ecbbdf36cc7c69d631623c552dac843ca48fba55fa"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:OXE7M6V3OXO3SICJFDMMMFN3UX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"All-band Bragg solitons and cw eigenmodes","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"A. E. Kaplan","submitted_at":"2015-04-18T21:09:13Z","abstract_excerpt":"We found an amazingly simple general \"all-band\" intensity profile of bandgap (Bragg) solitons for arbitrary parameters of spatially-periodic nonlinear systems, similar to those of multi-frequency stimulated Raman scattering, in particular the so called Lorentzian-profile solitons. We also found nonlinear eigen-modes of such system that propagate without energy exchange between waves."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.04761","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":"2026-05-18T02:18:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JrxaOX0L9iKUhTPrQLcJzqFxB+CaTraUuxSylmdbzFLQJO1T1JR6ZLpNVIX12lg5+jZeKkWTdZa+RT7xupjVCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T18:54:00.416977Z"},"content_sha256":"b0faeab2369586a7c7e3c65724d7212840f068044cc828d3de7b8195a3a30b24","schema_version":"1.0","event_id":"sha256:b0faeab2369586a7c7e3c65724d7212840f068044cc828d3de7b8195a3a30b24"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OXE7M6V3OXO3SICJFDMMMFN3UX/bundle.json","state_url":"https://pith.science/pith/OXE7M6V3OXO3SICJFDMMMFN3UX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OXE7M6V3OXO3SICJFDMMMFN3UX/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":"2026-06-27T18:54:00Z","links":{"resolver":"https://pith.science/pith/OXE7M6V3OXO3SICJFDMMMFN3UX","bundle":"https://pith.science/pith/OXE7M6V3OXO3SICJFDMMMFN3UX/bundle.json","state":"https://pith.science/pith/OXE7M6V3OXO3SICJFDMMMFN3UX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OXE7M6V3OXO3SICJFDMMMFN3UX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:OXE7M6V3OXO3SICJFDMMMFN3UX","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":"aab2c4ddec06a5432ec0293e13a09e57a49f0cab1d7bb3c5eb3cdf15830d9321","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2015-04-18T21:09:13Z","title_canon_sha256":"66a7a84aa8db40fa0189117e4eabb796c1ac07630da20ebd1cd969007aa09ad0"},"schema_version":"1.0","source":{"id":"1504.04761","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1504.04761","created_at":"2026-05-18T02:18:24Z"},{"alias_kind":"arxiv_version","alias_value":"1504.04761v1","created_at":"2026-05-18T02:18:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.04761","created_at":"2026-05-18T02:18:24Z"},{"alias_kind":"pith_short_12","alias_value":"OXE7M6V3OXO3","created_at":"2026-05-18T12:29:34Z"},{"alias_kind":"pith_short_16","alias_value":"OXE7M6V3OXO3SICJ","created_at":"2026-05-18T12:29:34Z"},{"alias_kind":"pith_short_8","alias_value":"OXE7M6V3","created_at":"2026-05-18T12:29:34Z"}],"graph_snapshots":[{"event_id":"sha256:b0faeab2369586a7c7e3c65724d7212840f068044cc828d3de7b8195a3a30b24","target":"graph","created_at":"2026-05-18T02:18:24Z","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 found an amazingly simple general \"all-band\" intensity profile of bandgap (Bragg) solitons for arbitrary parameters of spatially-periodic nonlinear systems, similar to those of multi-frequency stimulated Raman scattering, in particular the so called Lorentzian-profile solitons. We also found nonlinear eigen-modes of such system that propagate without energy exchange between waves.","authors_text":"A. E. Kaplan","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2015-04-18T21:09:13Z","title":"All-band Bragg solitons and cw eigenmodes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.04761","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":"sha256:1612375729a7bfc7db86b7ecbbdf36cc7c69d631623c552dac843ca48fba55fa","target":"record","created_at":"2026-05-18T02:18:24Z","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":"aab2c4ddec06a5432ec0293e13a09e57a49f0cab1d7bb3c5eb3cdf15830d9321","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2015-04-18T21:09:13Z","title_canon_sha256":"66a7a84aa8db40fa0189117e4eabb796c1ac07630da20ebd1cd969007aa09ad0"},"schema_version":"1.0","source":{"id":"1504.04761","kind":"arxiv","version":1}},"canonical_sha256":"75c9f67abb75ddb9204928d8c615bba5ec60907a2680a7afebcc6ea20f329c01","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"75c9f67abb75ddb9204928d8c615bba5ec60907a2680a7afebcc6ea20f329c01","first_computed_at":"2026-05-18T02:18:24.842716Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:18:24.842716Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"uC0AVieWRNVwyHRq6MHtWaCP1sfEE4RR0KhLUi8BeZissogPN3wFUwE5PsEf0DfGltHsiAVDoUO97p+tEVu8Cg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:18:24.843421Z","signed_message":"canonical_sha256_bytes"},"source_id":"1504.04761","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1612375729a7bfc7db86b7ecbbdf36cc7c69d631623c552dac843ca48fba55fa","sha256:b0faeab2369586a7c7e3c65724d7212840f068044cc828d3de7b8195a3a30b24"],"state_sha256":"e48a21213609605261808d60b018d0164152a86fe82e0494a0b9b501f6516952"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SqR/LlHRHycn3XfpI+HzoCUKkLDTB7gpcwvKiSPoVHJtnoMTK96Q+9zQWhi2Ry+yraV28Luuz+tV0ExNVKIKCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-27T18:54:00.418821Z","bundle_sha256":"efbad543962411e8ef170444b202393400da61d163f2efc89ca00938f65b5230"}}