{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:WB3YQY4B2QBS2OSJQHUZS3FSFX","short_pith_number":"pith:WB3YQY4B","schema_version":"1.0","canonical_sha256":"b077886381d4032d3a4981e9996cb22dcaf65f132c6d465609bb35ea840b1512","source":{"kind":"arxiv","id":"1411.1255","version":1},"attestation_state":"computed","paper":{"title":"On the flow and thermal characteristics of high Reynolds numbers (2800-17000) dye cell: simulation and experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Abhay Kumar, G. K. Mishra, O. Prakash, R. Biswal, S. K. Dixit, S. V. Nakhe","submitted_at":"2014-11-05T12:36:09Z","abstract_excerpt":"This paper presents computational and experimental studies on wavelength/frequency fluctuation characteristics of high pulse repetition rate (PRR: 18 kHz) dye laser pumped by frequency doubled Nd:YAG laser (532 nm). The temperature gradient in the dye solution is found to be responsible for wavelength fluctuations of the dye laser at low flow rates (2800<Red<5600). The turbulence Reynolds number (ReT) and the range of eddy sizes present in the turbulent flow are found to be responsible for the fluctuations at high flow rates (8400<Red<17000). A new dimensionless parameter, dimensionless eddy s"},"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":"1411.1255","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-11-05T12:36:09Z","cross_cats_sorted":[],"title_canon_sha256":"4f71367a21ed7fe5fa7d972d9fb2b9179627c3a836989869bba0234222ea408f","abstract_canon_sha256":"73fc9725da44b4e4657b98b29c0ec1d3a6968f38f20e611e10d8ce28b9f25f10"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:18:13.501808Z","signature_b64":"G8aBnz6jcFXJ8PKWa8cez+CzOzUyPq+Y+2WMp7dN+Sd+Wf3zQLvvqfld79aiNXw1qAGV9BY7OoM8ccb4kFeeDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b077886381d4032d3a4981e9996cb22dcaf65f132c6d465609bb35ea840b1512","last_reissued_at":"2026-05-18T02:18:13.501421Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:18:13.501421Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the flow and thermal characteristics of high Reynolds numbers (2800-17000) dye cell: simulation and experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Abhay Kumar, G. K. Mishra, O. Prakash, R. Biswal, S. K. Dixit, S. V. Nakhe","submitted_at":"2014-11-05T12:36:09Z","abstract_excerpt":"This paper presents computational and experimental studies on wavelength/frequency fluctuation characteristics of high pulse repetition rate (PRR: 18 kHz) dye laser pumped by frequency doubled Nd:YAG laser (532 nm). The temperature gradient in the dye solution is found to be responsible for wavelength fluctuations of the dye laser at low flow rates (2800<Red<5600). The turbulence Reynolds number (ReT) and the range of eddy sizes present in the turbulent flow are found to be responsible for the fluctuations at high flow rates (8400<Red<17000). A new dimensionless parameter, dimensionless eddy s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.1255","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":"1411.1255","created_at":"2026-05-18T02:18:13.501475+00:00"},{"alias_kind":"arxiv_version","alias_value":"1411.1255v1","created_at":"2026-05-18T02:18:13.501475+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.1255","created_at":"2026-05-18T02:18:13.501475+00:00"},{"alias_kind":"pith_short_12","alias_value":"WB3YQY4B2QBS","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_16","alias_value":"WB3YQY4B2QBS2OSJ","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_8","alias_value":"WB3YQY4B","created_at":"2026-05-18T12:28:54.890064+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/WB3YQY4B2QBS2OSJQHUZS3FSFX","json":"https://pith.science/pith/WB3YQY4B2QBS2OSJQHUZS3FSFX.json","graph_json":"https://pith.science/api/pith-number/WB3YQY4B2QBS2OSJQHUZS3FSFX/graph.json","events_json":"https://pith.science/api/pith-number/WB3YQY4B2QBS2OSJQHUZS3FSFX/events.json","paper":"https://pith.science/paper/WB3YQY4B"},"agent_actions":{"view_html":"https://pith.science/pith/WB3YQY4B2QBS2OSJQHUZS3FSFX","download_json":"https://pith.science/pith/WB3YQY4B2QBS2OSJQHUZS3FSFX.json","view_paper":"https://pith.science/paper/WB3YQY4B","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1411.1255&json=true","fetch_graph":"https://pith.science/api/pith-number/WB3YQY4B2QBS2OSJQHUZS3FSFX/graph.json","fetch_events":"https://pith.science/api/pith-number/WB3YQY4B2QBS2OSJQHUZS3FSFX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WB3YQY4B2QBS2OSJQHUZS3FSFX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WB3YQY4B2QBS2OSJQHUZS3FSFX/action/storage_attestation","attest_author":"https://pith.science/pith/WB3YQY4B2QBS2OSJQHUZS3FSFX/action/author_attestation","sign_citation":"https://pith.science/pith/WB3YQY4B2QBS2OSJQHUZS3FSFX/action/citation_signature","submit_replication":"https://pith.science/pith/WB3YQY4B2QBS2OSJQHUZS3FSFX/action/replication_record"}},"created_at":"2026-05-18T02:18:13.501475+00:00","updated_at":"2026-05-18T02:18:13.501475+00:00"}