{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:TPBVZUHWXY64SPRNQUZWBS5HNV","short_pith_number":"pith:TPBVZUHW","canonical_record":{"source":{"id":"1708.05002","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-08-16T17:58:06Z","cross_cats_sorted":["nlin.PS"],"title_canon_sha256":"135bd5932a00ca16861e6d59c36748ab5c635e038c3821d31932c957cc415c55","abstract_canon_sha256":"e444e5cfdffab3b8d78798bcd623cd1ff5df40f2a86eb9cac59666ed85eb3344"},"schema_version":"1.0"},"canonical_sha256":"9bc35cd0f6be3dc93e2d853360cba76d5ed7f850db3c99a3ca7a4248b1b39b73","source":{"kind":"arxiv","id":"1708.05002","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.05002","created_at":"2026-05-18T00:24:16Z"},{"alias_kind":"arxiv_version","alias_value":"1708.05002v1","created_at":"2026-05-18T00:24:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.05002","created_at":"2026-05-18T00:24:16Z"},{"alias_kind":"pith_short_12","alias_value":"TPBVZUHWXY64","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_16","alias_value":"TPBVZUHWXY64SPRN","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_8","alias_value":"TPBVZUHW","created_at":"2026-05-18T12:31:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:TPBVZUHWXY64SPRNQUZWBS5HNV","target":"record","payload":{"canonical_record":{"source":{"id":"1708.05002","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-08-16T17:58:06Z","cross_cats_sorted":["nlin.PS"],"title_canon_sha256":"135bd5932a00ca16861e6d59c36748ab5c635e038c3821d31932c957cc415c55","abstract_canon_sha256":"e444e5cfdffab3b8d78798bcd623cd1ff5df40f2a86eb9cac59666ed85eb3344"},"schema_version":"1.0"},"canonical_sha256":"9bc35cd0f6be3dc93e2d853360cba76d5ed7f850db3c99a3ca7a4248b1b39b73","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:24:16.686953Z","signature_b64":"1e+CQDZF/TchGG/qhALqqx9HtGG2i9dQn98y21MNwuVSykdcGUR2TdrPUeAeuAs3r2PwUQ8GOxi3I8UcHQy2Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9bc35cd0f6be3dc93e2d853360cba76d5ed7f850db3c99a3ca7a4248b1b39b73","last_reissued_at":"2026-05-18T00:24:16.686358Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:24:16.686358Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1708.05002","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":"2026-05-18T00:24:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KbqFifM1/hi3+d+0qf/rFPUe1u5zMIIjKcU5AfcJZlr8U8ISk1IyFPygJxCMOl9c3/D2yn4XleigdDJ62NXJBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T10:56:59.081501Z"},"content_sha256":"8e16271a69d8cc489f07fe19a2b31ffb9bfdc319acf5b5d0d809fcada9c55010","schema_version":"1.0","event_id":"sha256:8e16271a69d8cc489f07fe19a2b31ffb9bfdc319acf5b5d0d809fcada9c55010"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:TPBVZUHWXY64SPRNQUZWBS5HNV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Stimulated Raman Scattering Imposes Fundamental Limits to the Duration and Bandwidth of Temporal Cavity Solitons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.PS"],"primary_cat":"physics.optics","authors_text":"Miles Anderson, Miro Erkintalo, St\\'ephane Coen, Stuart G. Murdoch, Yadong Wang","submitted_at":"2017-08-16T17:58:06Z","abstract_excerpt":"Temporal cavity solitons (CS) are optical pulses that can persist in passive resonators, and they play a key role in the generation of coherent microresonator frequency combs. In resonators made of amorphous materials, such as fused silica, they can exhibit a spectral red-shift due to stimulated Raman scattering. Here we show that this Raman-induced self-frequency-shift imposes a fundamental limit on the duration and bandwidth of temporal CSs. Specifically, we theoretically predict that stimulated Raman scattering introduces a previously unidentified Hopf bifurcation that leads to destabilizat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.05002","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":"2026-05-18T00:24:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2zIfKfO3+zmTt/QR7HS2qTWFmF4No6tNvjzpt0oZ5tYXeQZqHNH2K6IAKi/lGRMMVpwnniRinLQOvIcm/1nyDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T10:56:59.081943Z"},"content_sha256":"7b95e4298a9ed98f90bdd457c9f920a7ec621cefb798f7bb83cd5d4bc4953bce","schema_version":"1.0","event_id":"sha256:7b95e4298a9ed98f90bdd457c9f920a7ec621cefb798f7bb83cd5d4bc4953bce"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TPBVZUHWXY64SPRNQUZWBS5HNV/bundle.json","state_url":"https://pith.science/pith/TPBVZUHWXY64SPRNQUZWBS5HNV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TPBVZUHWXY64SPRNQUZWBS5HNV/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":"2026-05-27T10:56:59Z","links":{"resolver":"https://pith.science/pith/TPBVZUHWXY64SPRNQUZWBS5HNV","bundle":"https://pith.science/pith/TPBVZUHWXY64SPRNQUZWBS5HNV/bundle.json","state":"https://pith.science/pith/TPBVZUHWXY64SPRNQUZWBS5HNV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TPBVZUHWXY64SPRNQUZWBS5HNV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:TPBVZUHWXY64SPRNQUZWBS5HNV","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":"e444e5cfdffab3b8d78798bcd623cd1ff5df40f2a86eb9cac59666ed85eb3344","cross_cats_sorted":["nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-08-16T17:58:06Z","title_canon_sha256":"135bd5932a00ca16861e6d59c36748ab5c635e038c3821d31932c957cc415c55"},"schema_version":"1.0","source":{"id":"1708.05002","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.05002","created_at":"2026-05-18T00:24:16Z"},{"alias_kind":"arxiv_version","alias_value":"1708.05002v1","created_at":"2026-05-18T00:24:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.05002","created_at":"2026-05-18T00:24:16Z"},{"alias_kind":"pith_short_12","alias_value":"TPBVZUHWXY64","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_16","alias_value":"TPBVZUHWXY64SPRN","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_8","alias_value":"TPBVZUHW","created_at":"2026-05-18T12:31:46Z"}],"graph_snapshots":[{"event_id":"sha256:7b95e4298a9ed98f90bdd457c9f920a7ec621cefb798f7bb83cd5d4bc4953bce","target":"graph","created_at":"2026-05-18T00:24:16Z","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":"Temporal cavity solitons (CS) are optical pulses that can persist in passive resonators, and they play a key role in the generation of coherent microresonator frequency combs. In resonators made of amorphous materials, such as fused silica, they can exhibit a spectral red-shift due to stimulated Raman scattering. Here we show that this Raman-induced self-frequency-shift imposes a fundamental limit on the duration and bandwidth of temporal CSs. Specifically, we theoretically predict that stimulated Raman scattering introduces a previously unidentified Hopf bifurcation that leads to destabilizat","authors_text":"Miles Anderson, Miro Erkintalo, St\\'ephane Coen, Stuart G. Murdoch, Yadong Wang","cross_cats":["nlin.PS"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-08-16T17:58:06Z","title":"Stimulated Raman Scattering Imposes Fundamental Limits to the Duration and Bandwidth of Temporal Cavity Solitons"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.05002","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":"sha256:8e16271a69d8cc489f07fe19a2b31ffb9bfdc319acf5b5d0d809fcada9c55010","target":"record","created_at":"2026-05-18T00:24:16Z","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":"e444e5cfdffab3b8d78798bcd623cd1ff5df40f2a86eb9cac59666ed85eb3344","cross_cats_sorted":["nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-08-16T17:58:06Z","title_canon_sha256":"135bd5932a00ca16861e6d59c36748ab5c635e038c3821d31932c957cc415c55"},"schema_version":"1.0","source":{"id":"1708.05002","kind":"arxiv","version":1}},"canonical_sha256":"9bc35cd0f6be3dc93e2d853360cba76d5ed7f850db3c99a3ca7a4248b1b39b73","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9bc35cd0f6be3dc93e2d853360cba76d5ed7f850db3c99a3ca7a4248b1b39b73","first_computed_at":"2026-05-18T00:24:16.686358Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:24:16.686358Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1e+CQDZF/TchGG/qhALqqx9HtGG2i9dQn98y21MNwuVSykdcGUR2TdrPUeAeuAs3r2PwUQ8GOxi3I8UcHQy2Cw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:24:16.686953Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.05002","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8e16271a69d8cc489f07fe19a2b31ffb9bfdc319acf5b5d0d809fcada9c55010","sha256:7b95e4298a9ed98f90bdd457c9f920a7ec621cefb798f7bb83cd5d4bc4953bce"],"state_sha256":"3a20c74d5d8fa5aaa83ae4da75fb48fbf214dc55a48d161aa0e41319da5be263"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QP4X161vl58VbGjes7ScS4cFHaJIOIkDzixWJDCbIahuNQo8M9R9nrJ6wxj6soZrQduCAu+1z6ZZQWBgpw5bBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T10:56:59.084301Z","bundle_sha256":"72438e0254c8290bc374638f3bb8c1462199069cd97bf7eb4df15c2684a791be"}}