{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:UCQPDSJTSCXBSUT6CL5VEWYFYC","short_pith_number":"pith:UCQPDSJT","schema_version":"1.0","canonical_sha256":"a0a0f1c93390ae19527e12fb525b05c0bc8beb5ea5d4d94822fa95ddc8e13a70","source":{"kind":"arxiv","id":"cond-mat/0008101","version":1},"attestation_state":"computed","paper":{"title":"Optical mode crossings and the low temperature anomalies of SrTiO3","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"A.K. Tagantsev, B. Hehlen, E. Courtens, E. Farhi","submitted_at":"2000-08-07T09:19:22Z","abstract_excerpt":"Optical mode crossing is not a plausible explanation for the new broad Brillouin doublet nor for the strong acoustic anomalies observed at low temperatures in SrTiO3. Data presented to support that explanation are also inconclusive."},"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/0008101","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2000-08-07T09:19:22Z","cross_cats_sorted":[],"title_canon_sha256":"9fc9c679999a4e9f84980e0710b9f26969aeaaacf931ece526228c29311d9f1c","abstract_canon_sha256":"4b20880e7a1fc91d452499e0783967acc5376260832df243a4bf8d3f5a7e0ed8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:40:08.206591Z","signature_b64":"joi2zyZow+VriYUdrWaSCW4BTJXxuz2EPTU+nax3RI700fbrJijPgGsnRhYz1rHWs56DEM9ogvcp7wp7PMTzCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a0a0f1c93390ae19527e12fb525b05c0bc8beb5ea5d4d94822fa95ddc8e13a70","last_reissued_at":"2026-05-18T01:40:08.205823Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:40:08.205823Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Optical mode crossings and the low temperature anomalies of SrTiO3","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"A.K. Tagantsev, B. Hehlen, E. Courtens, E. Farhi","submitted_at":"2000-08-07T09:19:22Z","abstract_excerpt":"Optical mode crossing is not a plausible explanation for the new broad Brillouin doublet nor for the strong acoustic anomalies observed at low temperatures in SrTiO3. Data presented to support that explanation are also inconclusive."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0008101","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":"cond-mat/0008101","created_at":"2026-05-18T01:40:08.205951+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0008101v1","created_at":"2026-05-18T01:40:08.205951+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0008101","created_at":"2026-05-18T01:40:08.205951+00:00"},{"alias_kind":"pith_short_12","alias_value":"UCQPDSJTSCXB","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_16","alias_value":"UCQPDSJTSCXBSUT6","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_8","alias_value":"UCQPDSJT","created_at":"2026-05-18T12:25:50.254431+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/UCQPDSJTSCXBSUT6CL5VEWYFYC","json":"https://pith.science/pith/UCQPDSJTSCXBSUT6CL5VEWYFYC.json","graph_json":"https://pith.science/api/pith-number/UCQPDSJTSCXBSUT6CL5VEWYFYC/graph.json","events_json":"https://pith.science/api/pith-number/UCQPDSJTSCXBSUT6CL5VEWYFYC/events.json","paper":"https://pith.science/paper/UCQPDSJT"},"agent_actions":{"view_html":"https://pith.science/pith/UCQPDSJTSCXBSUT6CL5VEWYFYC","download_json":"https://pith.science/pith/UCQPDSJTSCXBSUT6CL5VEWYFYC.json","view_paper":"https://pith.science/paper/UCQPDSJT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0008101&json=true","fetch_graph":"https://pith.science/api/pith-number/UCQPDSJTSCXBSUT6CL5VEWYFYC/graph.json","fetch_events":"https://pith.science/api/pith-number/UCQPDSJTSCXBSUT6CL5VEWYFYC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UCQPDSJTSCXBSUT6CL5VEWYFYC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UCQPDSJTSCXBSUT6CL5VEWYFYC/action/storage_attestation","attest_author":"https://pith.science/pith/UCQPDSJTSCXBSUT6CL5VEWYFYC/action/author_attestation","sign_citation":"https://pith.science/pith/UCQPDSJTSCXBSUT6CL5VEWYFYC/action/citation_signature","submit_replication":"https://pith.science/pith/UCQPDSJTSCXBSUT6CL5VEWYFYC/action/replication_record"}},"created_at":"2026-05-18T01:40:08.205951+00:00","updated_at":"2026-05-18T01:40:08.205951+00:00"}