{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:2D2NL2RZDVASR4VKEQVIPB7IEV","short_pith_number":"pith:2D2NL2RZ","canonical_record":{"source":{"id":"1303.7078","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2013-03-28T09:40:32Z","cross_cats_sorted":[],"title_canon_sha256":"69c825eb651973bbaa545b166d131b7c142a8ce8680a0678b646f6b24c9247f3","abstract_canon_sha256":"3f19a3c4a23d7dfadc558721e7dd02671ca3a1384d0049842534faccea2cd543"},"schema_version":"1.0"},"canonical_sha256":"d0f4d5ea391d4128f2aa242a8787e82554c8e55d201cedb3b88f4332d10182d7","source":{"kind":"arxiv","id":"1303.7078","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.7078","created_at":"2026-05-18T03:09:48Z"},{"alias_kind":"arxiv_version","alias_value":"1303.7078v1","created_at":"2026-05-18T03:09:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.7078","created_at":"2026-05-18T03:09:48Z"},{"alias_kind":"pith_short_12","alias_value":"2D2NL2RZDVAS","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"2D2NL2RZDVASR4VK","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"2D2NL2RZ","created_at":"2026-05-18T12:27:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:2D2NL2RZDVASR4VKEQVIPB7IEV","target":"record","payload":{"canonical_record":{"source":{"id":"1303.7078","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2013-03-28T09:40:32Z","cross_cats_sorted":[],"title_canon_sha256":"69c825eb651973bbaa545b166d131b7c142a8ce8680a0678b646f6b24c9247f3","abstract_canon_sha256":"3f19a3c4a23d7dfadc558721e7dd02671ca3a1384d0049842534faccea2cd543"},"schema_version":"1.0"},"canonical_sha256":"d0f4d5ea391d4128f2aa242a8787e82554c8e55d201cedb3b88f4332d10182d7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:09:48.823346Z","signature_b64":"q7ezDZZeX6MTu2Cg0/ObwzvJOT02hKqI5O5Mxtsk4k/LzLxI9MG7FMDXzG8ziuWtnKtdGqSP16FQD8/1DfMuCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d0f4d5ea391d4128f2aa242a8787e82554c8e55d201cedb3b88f4332d10182d7","last_reissued_at":"2026-05-18T03:09:48.822641Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:09:48.822641Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1303.7078","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":"2026-05-18T03:09:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"U02Ue98FghVCJkTE7YatpgsTeDmEQuEwlXAfgyn5E/Cw/emEX36YcLTfG6mKXgfuS2P/MDHIMWDJk2c/bLi7AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T05:31:19.612249Z"},"content_sha256":"da5a605ecb270f71a6bf585df799aa6449397e42c457eac94ff6344b62d6f4a8","schema_version":"1.0","event_id":"sha256:da5a605ecb270f71a6bf585df799aa6449397e42c457eac94ff6344b62d6f4a8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:2D2NL2RZDVASR4VKEQVIPB7IEV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Universal scaling laws of Kerr frequency combs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Miro Erkintalo, Stephane Coen","submitted_at":"2013-03-28T09:40:32Z","abstract_excerpt":"Using the known solutions of the Lugiato-Lefever equation, we derive universal trends of Kerr frequency combs. In particular, normalized properties of temporal cavity soliton solutions lead us to a simple analytic estimate of the maximum attainable bandwidth for given pump-resonator parameters. The result is validated via comparison with past experiments encompassing a diverse range of resonator configurations and parameters."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.7078","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":"2026-05-18T03:09:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kkwm0PoEskioastW9AR3Bun2pwnxUSAL+9yRQaE4rRCt9/xahyOp4KEoNR/HqUgEJnLUql/c+wXIaplRWS/0Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T05:31:19.612939Z"},"content_sha256":"e468401bd8ad770f6bd71e4550c85ab73d85ce58e2768e3f5b298937ae7962f6","schema_version":"1.0","event_id":"sha256:e468401bd8ad770f6bd71e4550c85ab73d85ce58e2768e3f5b298937ae7962f6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2D2NL2RZDVASR4VKEQVIPB7IEV/bundle.json","state_url":"https://pith.science/pith/2D2NL2RZDVASR4VKEQVIPB7IEV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2D2NL2RZDVASR4VKEQVIPB7IEV/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":"2026-05-27T05:31:19Z","links":{"resolver":"https://pith.science/pith/2D2NL2RZDVASR4VKEQVIPB7IEV","bundle":"https://pith.science/pith/2D2NL2RZDVASR4VKEQVIPB7IEV/bundle.json","state":"https://pith.science/pith/2D2NL2RZDVASR4VKEQVIPB7IEV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2D2NL2RZDVASR4VKEQVIPB7IEV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:2D2NL2RZDVASR4VKEQVIPB7IEV","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":"3f19a3c4a23d7dfadc558721e7dd02671ca3a1384d0049842534faccea2cd543","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2013-03-28T09:40:32Z","title_canon_sha256":"69c825eb651973bbaa545b166d131b7c142a8ce8680a0678b646f6b24c9247f3"},"schema_version":"1.0","source":{"id":"1303.7078","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.7078","created_at":"2026-05-18T03:09:48Z"},{"alias_kind":"arxiv_version","alias_value":"1303.7078v1","created_at":"2026-05-18T03:09:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.7078","created_at":"2026-05-18T03:09:48Z"},{"alias_kind":"pith_short_12","alias_value":"2D2NL2RZDVAS","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"2D2NL2RZDVASR4VK","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"2D2NL2RZ","created_at":"2026-05-18T12:27:30Z"}],"graph_snapshots":[{"event_id":"sha256:e468401bd8ad770f6bd71e4550c85ab73d85ce58e2768e3f5b298937ae7962f6","target":"graph","created_at":"2026-05-18T03:09:48Z","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":"Using the known solutions of the Lugiato-Lefever equation, we derive universal trends of Kerr frequency combs. In particular, normalized properties of temporal cavity soliton solutions lead us to a simple analytic estimate of the maximum attainable bandwidth for given pump-resonator parameters. The result is validated via comparison with past experiments encompassing a diverse range of resonator configurations and parameters.","authors_text":"Miro Erkintalo, Stephane Coen","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2013-03-28T09:40:32Z","title":"Universal scaling laws of Kerr frequency combs"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.7078","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:da5a605ecb270f71a6bf585df799aa6449397e42c457eac94ff6344b62d6f4a8","target":"record","created_at":"2026-05-18T03:09:48Z","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":"3f19a3c4a23d7dfadc558721e7dd02671ca3a1384d0049842534faccea2cd543","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2013-03-28T09:40:32Z","title_canon_sha256":"69c825eb651973bbaa545b166d131b7c142a8ce8680a0678b646f6b24c9247f3"},"schema_version":"1.0","source":{"id":"1303.7078","kind":"arxiv","version":1}},"canonical_sha256":"d0f4d5ea391d4128f2aa242a8787e82554c8e55d201cedb3b88f4332d10182d7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d0f4d5ea391d4128f2aa242a8787e82554c8e55d201cedb3b88f4332d10182d7","first_computed_at":"2026-05-18T03:09:48.822641Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:09:48.822641Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"q7ezDZZeX6MTu2Cg0/ObwzvJOT02hKqI5O5Mxtsk4k/LzLxI9MG7FMDXzG8ziuWtnKtdGqSP16FQD8/1DfMuCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:09:48.823346Z","signed_message":"canonical_sha256_bytes"},"source_id":"1303.7078","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:da5a605ecb270f71a6bf585df799aa6449397e42c457eac94ff6344b62d6f4a8","sha256:e468401bd8ad770f6bd71e4550c85ab73d85ce58e2768e3f5b298937ae7962f6"],"state_sha256":"fc28e44e24e89e9351301915e3171e354d6fad235d5d9179dc784833da53ae24"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lh6D6gRFJmPMNkUeslD8Ehp7Z0MAvsTiiXBuDamhzWwyG+B6UhLQOoYR4+6P4PRtPzDWGI6wxDkLm8yskvpwBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T05:31:19.616533Z","bundle_sha256":"0d8493d27cb0b71b820a1c90828fc86de75b418ab486de993ba6634ae327d453"}}