{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:AVIP76VWQAX6MHIQJAQVXQHI6G","short_pith_number":"pith:AVIP76VW","schema_version":"1.0","canonical_sha256":"0550fffab6802fe61d1048215bc0e8f1a39c69af5b71506917b58ee83755bbed","source":{"kind":"arxiv","id":"1704.06083","version":1},"attestation_state":"computed","paper":{"title":"Characteristics and stability of soliton crystals in optical fibres for the purpose of optical frequency comb generation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"nlin.PS","authors_text":"A. A. Rieznik, D. Bodenm\\\"uller, J. M. Chavez Boggio, K. Blow, M. B\\\"ohm, M. M. Roth, M. Zajnulina","submitted_at":"2017-04-20T10:37:47Z","abstract_excerpt":"We study the properties of a soliton crystal, an bound state of several optical pulses that propagate with a fixed temporal separation through the optical fibres of the proposed approach for generation of optical frequency combs (OFC) for astronomical spectrograph calibration. This approach - also being suitable for subpicosecond pulse generation for other applications - consists of a conventional single-mode fibre and a suitably pumped Erbium-doped fibre. Two continuous-wave lasers are used as light source. The soliton crystal arises out of the initial deeply modulated laser field at low inpu"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1704.06083","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.PS","submitted_at":"2017-04-20T10:37:47Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"99d4db1dd550455c76181ec18ca0715656aaf56c947e3fb6f003bf157633f6a5","abstract_canon_sha256":"883d6a7f04d99a712b39c00f206773569a5a73ef13f127a2facaa2f18b639d39"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:46:03.360827Z","signature_b64":"RSAxuwdtgnrgOeQYw1+P4w2lKS3Lay3VvAkPYtg1KAE60dQ70taMwZx9ua/FAZnnUsZccNNqvGC2xqw6Ev0iBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0550fffab6802fe61d1048215bc0e8f1a39c69af5b71506917b58ee83755bbed","last_reissued_at":"2026-05-18T00:46:03.360155Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:46:03.360155Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Characteristics and stability of soliton crystals in optical fibres for the purpose of optical frequency comb generation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"nlin.PS","authors_text":"A. A. Rieznik, D. Bodenm\\\"uller, J. M. Chavez Boggio, K. Blow, M. B\\\"ohm, M. M. Roth, M. Zajnulina","submitted_at":"2017-04-20T10:37:47Z","abstract_excerpt":"We study the properties of a soliton crystal, an bound state of several optical pulses that propagate with a fixed temporal separation through the optical fibres of the proposed approach for generation of optical frequency combs (OFC) for astronomical spectrograph calibration. This approach - also being suitable for subpicosecond pulse generation for other applications - consists of a conventional single-mode fibre and a suitably pumped Erbium-doped fibre. Two continuous-wave lasers are used as light source. The soliton crystal arises out of the initial deeply modulated laser field at low inpu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.06083","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1704.06083","created_at":"2026-05-18T00:46:03.360260+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.06083v1","created_at":"2026-05-18T00:46:03.360260+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.06083","created_at":"2026-05-18T00:46:03.360260+00:00"},{"alias_kind":"pith_short_12","alias_value":"AVIP76VWQAX6","created_at":"2026-05-18T12:31:08.081275+00:00"},{"alias_kind":"pith_short_16","alias_value":"AVIP76VWQAX6MHIQ","created_at":"2026-05-18T12:31:08.081275+00:00"},{"alias_kind":"pith_short_8","alias_value":"AVIP76VW","created_at":"2026-05-18T12:31:08.081275+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/AVIP76VWQAX6MHIQJAQVXQHI6G","json":"https://pith.science/pith/AVIP76VWQAX6MHIQJAQVXQHI6G.json","graph_json":"https://pith.science/api/pith-number/AVIP76VWQAX6MHIQJAQVXQHI6G/graph.json","events_json":"https://pith.science/api/pith-number/AVIP76VWQAX6MHIQJAQVXQHI6G/events.json","paper":"https://pith.science/paper/AVIP76VW"},"agent_actions":{"view_html":"https://pith.science/pith/AVIP76VWQAX6MHIQJAQVXQHI6G","download_json":"https://pith.science/pith/AVIP76VWQAX6MHIQJAQVXQHI6G.json","view_paper":"https://pith.science/paper/AVIP76VW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.06083&json=true","fetch_graph":"https://pith.science/api/pith-number/AVIP76VWQAX6MHIQJAQVXQHI6G/graph.json","fetch_events":"https://pith.science/api/pith-number/AVIP76VWQAX6MHIQJAQVXQHI6G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AVIP76VWQAX6MHIQJAQVXQHI6G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AVIP76VWQAX6MHIQJAQVXQHI6G/action/storage_attestation","attest_author":"https://pith.science/pith/AVIP76VWQAX6MHIQJAQVXQHI6G/action/author_attestation","sign_citation":"https://pith.science/pith/AVIP76VWQAX6MHIQJAQVXQHI6G/action/citation_signature","submit_replication":"https://pith.science/pith/AVIP76VWQAX6MHIQJAQVXQHI6G/action/replication_record"}},"created_at":"2026-05-18T00:46:03.360260+00:00","updated_at":"2026-05-18T00:46:03.360260+00:00"}