{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:YCYHKDG35TFTEBYS5QLGOWYLSY","short_pith_number":"pith:YCYHKDG3","schema_version":"1.0","canonical_sha256":"c0b0750cdbeccb320712ec16675b0b961ca9f574e318064d10e8167b16e0fbe9","source":{"kind":"arxiv","id":"0908.2373","version":1},"attestation_state":"computed","paper":{"title":"Origin of Diffuse Scattering in Relaxor Ferroelectrics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"B. Burton, E. Cockayne, M. Ahart, P. Ganesh, R. E. Cohen, R. J. Hemley, Wenge Yang, Yang Ren, Z-G Ye","submitted_at":"2009-08-17T15:40:46Z","abstract_excerpt":"High-pressure and variable temperature single crystal synchrotron X-ray measurements combined with first-principles based molecular dynamics simulations study diffuse scattering in the relaxor ferroelectric system PSN (PbSc$_{1/2}$Nb$_{1/2}$O$_3$). Constant temperature experiments show pressure induced transition to the relaxor phase at different temperatures characterized by butterfly and rod shaped diffuse scattering around the $\\{$h00$\\}$ and $\\{$hh0$\\}$ Bragg spots, respectively. The simulations reproduce the observed diffuse scattering features as well as their pressure-temperature behavi"},"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":"0908.2373","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2009-08-17T15:40:46Z","cross_cats_sorted":["cond-mat.other"],"title_canon_sha256":"7e6096f1521eef646c8a59fd0cc69d8ad0ec3d8ad565f8be260dcf01eb81c9be","abstract_canon_sha256":"fcb5f4f28d9194a52706db168347e731339cfd644d59017201450ad810c71271"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:12:33.420905Z","signature_b64":"3JQD/KxAw8+8G4K8V+Gguhaqs3ZjZwVokWIiyXXB/pOFDFNGJAn3PBHsG20n+bCieKzDC+qlP/OAizDA+NNjDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c0b0750cdbeccb320712ec16675b0b961ca9f574e318064d10e8167b16e0fbe9","last_reissued_at":"2026-05-18T02:12:33.420221Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:12:33.420221Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Origin of Diffuse Scattering in Relaxor Ferroelectrics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"B. Burton, E. Cockayne, M. Ahart, P. Ganesh, R. E. Cohen, R. J. Hemley, Wenge Yang, Yang Ren, Z-G Ye","submitted_at":"2009-08-17T15:40:46Z","abstract_excerpt":"High-pressure and variable temperature single crystal synchrotron X-ray measurements combined with first-principles based molecular dynamics simulations study diffuse scattering in the relaxor ferroelectric system PSN (PbSc$_{1/2}$Nb$_{1/2}$O$_3$). Constant temperature experiments show pressure induced transition to the relaxor phase at different temperatures characterized by butterfly and rod shaped diffuse scattering around the $\\{$h00$\\}$ and $\\{$hh0$\\}$ Bragg spots, respectively. The simulations reproduce the observed diffuse scattering features as well as their pressure-temperature behavi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0908.2373","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":"0908.2373","created_at":"2026-05-18T02:12:33.420346+00:00"},{"alias_kind":"arxiv_version","alias_value":"0908.2373v1","created_at":"2026-05-18T02:12:33.420346+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0908.2373","created_at":"2026-05-18T02:12:33.420346+00:00"},{"alias_kind":"pith_short_12","alias_value":"YCYHKDG35TFT","created_at":"2026-05-18T12:26:02.257875+00:00"},{"alias_kind":"pith_short_16","alias_value":"YCYHKDG35TFTEBYS","created_at":"2026-05-18T12:26:02.257875+00:00"},{"alias_kind":"pith_short_8","alias_value":"YCYHKDG3","created_at":"2026-05-18T12:26:02.257875+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/YCYHKDG35TFTEBYS5QLGOWYLSY","json":"https://pith.science/pith/YCYHKDG35TFTEBYS5QLGOWYLSY.json","graph_json":"https://pith.science/api/pith-number/YCYHKDG35TFTEBYS5QLGOWYLSY/graph.json","events_json":"https://pith.science/api/pith-number/YCYHKDG35TFTEBYS5QLGOWYLSY/events.json","paper":"https://pith.science/paper/YCYHKDG3"},"agent_actions":{"view_html":"https://pith.science/pith/YCYHKDG35TFTEBYS5QLGOWYLSY","download_json":"https://pith.science/pith/YCYHKDG35TFTEBYS5QLGOWYLSY.json","view_paper":"https://pith.science/paper/YCYHKDG3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0908.2373&json=true","fetch_graph":"https://pith.science/api/pith-number/YCYHKDG35TFTEBYS5QLGOWYLSY/graph.json","fetch_events":"https://pith.science/api/pith-number/YCYHKDG35TFTEBYS5QLGOWYLSY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YCYHKDG35TFTEBYS5QLGOWYLSY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YCYHKDG35TFTEBYS5QLGOWYLSY/action/storage_attestation","attest_author":"https://pith.science/pith/YCYHKDG35TFTEBYS5QLGOWYLSY/action/author_attestation","sign_citation":"https://pith.science/pith/YCYHKDG35TFTEBYS5QLGOWYLSY/action/citation_signature","submit_replication":"https://pith.science/pith/YCYHKDG35TFTEBYS5QLGOWYLSY/action/replication_record"}},"created_at":"2026-05-18T02:12:33.420346+00:00","updated_at":"2026-05-18T02:12:33.420346+00:00"}