{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:ND6QQZPDATVH5ZJDHBKJ6OXG67","short_pith_number":"pith:ND6QQZPD","schema_version":"1.0","canonical_sha256":"68fd0865e304ea7ee52338549f3ae6f7dfef618497e16b50daee29b16eb3d262","source":{"kind":"arxiv","id":"cond-mat/9601141","version":1},"attestation_state":"computed","paper":{"title":"Raman continuum in high-$T_c$ superconductors","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"Haranath Ghosh, Manas Sardar","submitted_at":"1996-01-29T15:59:32Z","abstract_excerpt":"Experimentally, Raman continuum for $A_g$ and $B_g$ geometry exhibits peaks far apart from each other (about 80 to 150 $\\rm cm^{-1}$) in frequency. The former is insensitive to doping over a small range where $T_c$ does not vary much whereas the latter shifts towards higher frequencies. We calculate the electronic Raman scattering intensities using the `modified spin bag model'. We show that the calculated results have natural explanation to the observed anamolous peak separation and peculiar doping dependence."},"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":"cond-mat/9601141","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1996-01-29T15:59:32Z","cross_cats_sorted":[],"title_canon_sha256":"ecba054776a111383395c55f92cde1611f952fb220030d0ea93483d9af4126f3","abstract_canon_sha256":"d895c47262eaea1ec6dd791a9d2bafaef10847049f6f24f6e6ff77813ac2672c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:00:27.683975Z","signature_b64":"p6SfbcNbRoN+1VlIV4hlj6A7e1kMzhwzNsuNuZ/cGOjGcoHj/jGJWtsrVR+nyde3tJuEaHJLcaNYrLPHLob0Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"68fd0865e304ea7ee52338549f3ae6f7dfef618497e16b50daee29b16eb3d262","last_reissued_at":"2026-07-04T16:00:27.683589Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:00:27.683589Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Raman continuum in high-$T_c$ superconductors","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"Haranath Ghosh, Manas Sardar","submitted_at":"1996-01-29T15:59:32Z","abstract_excerpt":"Experimentally, Raman continuum for $A_g$ and $B_g$ geometry exhibits peaks far apart from each other (about 80 to 150 $\\rm cm^{-1}$) in frequency. The former is insensitive to doping over a small range where $T_c$ does not vary much whereas the latter shifts towards higher frequencies. We calculate the electronic Raman scattering intensities using the `modified spin bag model'. We show that the calculated results have natural explanation to the observed anamolous peak separation and peculiar doping dependence."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9601141","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/cond-mat/9601141/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"cond-mat/9601141","created_at":"2026-07-04T16:00:27.683650+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9601141v1","created_at":"2026-07-04T16:00:27.683650+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9601141","created_at":"2026-07-04T16:00:27.683650+00:00"},{"alias_kind":"pith_short_12","alias_value":"ND6QQZPDATVH","created_at":"2026-07-04T16:00:27.683650+00:00"},{"alias_kind":"pith_short_16","alias_value":"ND6QQZPDATVH5ZJD","created_at":"2026-07-04T16:00:27.683650+00:00"},{"alias_kind":"pith_short_8","alias_value":"ND6QQZPD","created_at":"2026-07-04T16:00:27.683650+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/ND6QQZPDATVH5ZJDHBKJ6OXG67","json":"https://pith.science/pith/ND6QQZPDATVH5ZJDHBKJ6OXG67.json","graph_json":"https://pith.science/api/pith-number/ND6QQZPDATVH5ZJDHBKJ6OXG67/graph.json","events_json":"https://pith.science/api/pith-number/ND6QQZPDATVH5ZJDHBKJ6OXG67/events.json","paper":"https://pith.science/paper/ND6QQZPD"},"agent_actions":{"view_html":"https://pith.science/pith/ND6QQZPDATVH5ZJDHBKJ6OXG67","download_json":"https://pith.science/pith/ND6QQZPDATVH5ZJDHBKJ6OXG67.json","view_paper":"https://pith.science/paper/ND6QQZPD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9601141&json=true","fetch_graph":"https://pith.science/api/pith-number/ND6QQZPDATVH5ZJDHBKJ6OXG67/graph.json","fetch_events":"https://pith.science/api/pith-number/ND6QQZPDATVH5ZJDHBKJ6OXG67/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ND6QQZPDATVH5ZJDHBKJ6OXG67/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ND6QQZPDATVH5ZJDHBKJ6OXG67/action/storage_attestation","attest_author":"https://pith.science/pith/ND6QQZPDATVH5ZJDHBKJ6OXG67/action/author_attestation","sign_citation":"https://pith.science/pith/ND6QQZPDATVH5ZJDHBKJ6OXG67/action/citation_signature","submit_replication":"https://pith.science/pith/ND6QQZPDATVH5ZJDHBKJ6OXG67/action/replication_record"}},"created_at":"2026-07-04T16:00:27.683650+00:00","updated_at":"2026-07-04T16:00:27.683650+00:00"}