{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:HF4BXYW6O26BL4F73ZRDDWKUL6","short_pith_number":"pith:HF4BXYW6","schema_version":"1.0","canonical_sha256":"39781be2de76bc15f0bfde6231d9545fbfe4672fff2343373752a318443c4c47","source":{"kind":"arxiv","id":"1506.05265","version":1},"attestation_state":"computed","paper":{"title":"Ginzburg-Landau turbulence in quasi-CW Raman fiber lasers","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Dmitry V. Churkin, Nikita Tarasov, Srikanth Sugavanam, Stefan Wabnitz","submitted_at":"2015-06-17T10:10:54Z","abstract_excerpt":"Fiber lasers operating via Raman gain or based on rare-earth doped active fibers are widely used as sources of CW radiation. However these lasers are only quasi-CW: their intensity fluctuates strongly on short time-scales. Here the framework of the complex Ginzburg-Landau equations, that are well known as an efficient model of mode-locked fiber lasers, is applied for the description of quasi-CW fiber lasers as well. The first ever vector model of a Raman fiber laser describes the experimentally observed turbulent-like intensity dynamics, as well as polarization rogue waves. Our results open de"},"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":"1506.05265","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2015-06-17T10:10:54Z","cross_cats_sorted":[],"title_canon_sha256":"eee327c9063381a4657f855d21bd9fadc38a37ab19219be11ee5978c3c1f7e9e","abstract_canon_sha256":"a723ceea218c578afbc34fb3dfb70f05cd606f7028b53f55ca11a121f4540e1b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:46:12.634654Z","signature_b64":"pB07znED7qM7rPuFTNMuKv4pTdKG1gxKdUPjhDKGp+sqYc1s//NdZL6bvnSGaLjJZ8LV77pKCnLcaFAZa7qWBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"39781be2de76bc15f0bfde6231d9545fbfe4672fff2343373752a318443c4c47","last_reissued_at":"2026-05-18T01:46:12.634136Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:46:12.634136Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Ginzburg-Landau turbulence in quasi-CW Raman fiber lasers","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Dmitry V. Churkin, Nikita Tarasov, Srikanth Sugavanam, Stefan Wabnitz","submitted_at":"2015-06-17T10:10:54Z","abstract_excerpt":"Fiber lasers operating via Raman gain or based on rare-earth doped active fibers are widely used as sources of CW radiation. However these lasers are only quasi-CW: their intensity fluctuates strongly on short time-scales. Here the framework of the complex Ginzburg-Landau equations, that are well known as an efficient model of mode-locked fiber lasers, is applied for the description of quasi-CW fiber lasers as well. The first ever vector model of a Raman fiber laser describes the experimentally observed turbulent-like intensity dynamics, as well as polarization rogue waves. Our results open de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.05265","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":"1506.05265","created_at":"2026-05-18T01:46:12.634227+00:00"},{"alias_kind":"arxiv_version","alias_value":"1506.05265v1","created_at":"2026-05-18T01:46:12.634227+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.05265","created_at":"2026-05-18T01:46:12.634227+00:00"},{"alias_kind":"pith_short_12","alias_value":"HF4BXYW6O26B","created_at":"2026-05-18T12:29:25.134429+00:00"},{"alias_kind":"pith_short_16","alias_value":"HF4BXYW6O26BL4F7","created_at":"2026-05-18T12:29:25.134429+00:00"},{"alias_kind":"pith_short_8","alias_value":"HF4BXYW6","created_at":"2026-05-18T12:29:25.134429+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/HF4BXYW6O26BL4F73ZRDDWKUL6","json":"https://pith.science/pith/HF4BXYW6O26BL4F73ZRDDWKUL6.json","graph_json":"https://pith.science/api/pith-number/HF4BXYW6O26BL4F73ZRDDWKUL6/graph.json","events_json":"https://pith.science/api/pith-number/HF4BXYW6O26BL4F73ZRDDWKUL6/events.json","paper":"https://pith.science/paper/HF4BXYW6"},"agent_actions":{"view_html":"https://pith.science/pith/HF4BXYW6O26BL4F73ZRDDWKUL6","download_json":"https://pith.science/pith/HF4BXYW6O26BL4F73ZRDDWKUL6.json","view_paper":"https://pith.science/paper/HF4BXYW6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1506.05265&json=true","fetch_graph":"https://pith.science/api/pith-number/HF4BXYW6O26BL4F73ZRDDWKUL6/graph.json","fetch_events":"https://pith.science/api/pith-number/HF4BXYW6O26BL4F73ZRDDWKUL6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HF4BXYW6O26BL4F73ZRDDWKUL6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HF4BXYW6O26BL4F73ZRDDWKUL6/action/storage_attestation","attest_author":"https://pith.science/pith/HF4BXYW6O26BL4F73ZRDDWKUL6/action/author_attestation","sign_citation":"https://pith.science/pith/HF4BXYW6O26BL4F73ZRDDWKUL6/action/citation_signature","submit_replication":"https://pith.science/pith/HF4BXYW6O26BL4F73ZRDDWKUL6/action/replication_record"}},"created_at":"2026-05-18T01:46:12.634227+00:00","updated_at":"2026-05-18T01:46:12.634227+00:00"}