{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:JGDXA5P27DYLEZXT6BHFV4HIIH","short_pith_number":"pith:JGDXA5P2","schema_version":"1.0","canonical_sha256":"49877075faf8f0b266f3f04e5af0e841c0ee880ea4adde9bdbce97f6b905e64f","source":{"kind":"arxiv","id":"cond-mat/0110394","version":1},"attestation_state":"computed","paper":{"title":"Non-Arrhenius Behavior of Secondary Relaxation in Supercooled Liquids","license":"","headline":"","cross_cats":["cond-mat.soft"],"primary_cat":"cond-mat.dis-nn","authors_text":"Hiroshi Frusawa, Kohzo Ito (Univ. Tokyo), Takuya Fujima","submitted_at":"2001-10-19T01:39:02Z","abstract_excerpt":"Dielectric relaxation spectroscopy (1 Hz - 20 GHz) has been performed on supercooled glass-formers from the temperature of glass transition (T_g) up to that of melting. Precise measurements particularly in the frequencies of MHz-order have revealed that the temperature dependences of secondary beta-relaxation times deviate from the Arrhenius relation in well above T_g. Consequently, our results indicate that the beta-process merges into the primary alpha-mode around the melting temperature, and not at the dynamical transition point T which is approximately equal to 1.2 T_g."},"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/0110394","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.dis-nn","submitted_at":"2001-10-19T01:39:02Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"550aa59a9f9c9730598d4fa946dd94560c46ff1922f84ad11da02c2bab0c0801","abstract_canon_sha256":"f485dc4883573cd5ab6cbd002c5ca0423d5b5ff2884574be5faf013d1cca0869"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:26:25.789093Z","signature_b64":"aT5tBNW4F8LktJ4zgFSWQsklCgn175ZzVax53Nq4/Q9lMhyRt+S/6Y0xGa7zVptkCQYnopGSixf5uYo+yQd7CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"49877075faf8f0b266f3f04e5af0e841c0ee880ea4adde9bdbce97f6b905e64f","last_reissued_at":"2026-07-04T16:26:25.788686Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:26:25.788686Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-Arrhenius Behavior of Secondary Relaxation in Supercooled Liquids","license":"","headline":"","cross_cats":["cond-mat.soft"],"primary_cat":"cond-mat.dis-nn","authors_text":"Hiroshi Frusawa, Kohzo Ito (Univ. Tokyo), Takuya Fujima","submitted_at":"2001-10-19T01:39:02Z","abstract_excerpt":"Dielectric relaxation spectroscopy (1 Hz - 20 GHz) has been performed on supercooled glass-formers from the temperature of glass transition (T_g) up to that of melting. Precise measurements particularly in the frequencies of MHz-order have revealed that the temperature dependences of secondary beta-relaxation times deviate from the Arrhenius relation in well above T_g. Consequently, our results indicate that the beta-process merges into the primary alpha-mode around the melting temperature, and not at the dynamical transition point T which is approximately equal to 1.2 T_g."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0110394","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/0110394/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/0110394","created_at":"2026-07-04T16:26:25.788751+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0110394v1","created_at":"2026-07-04T16:26:25.788751+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0110394","created_at":"2026-07-04T16:26:25.788751+00:00"},{"alias_kind":"pith_short_12","alias_value":"JGDXA5P27DYL","created_at":"2026-07-04T16:26:25.788751+00:00"},{"alias_kind":"pith_short_16","alias_value":"JGDXA5P27DYLEZXT","created_at":"2026-07-04T16:26:25.788751+00:00"},{"alias_kind":"pith_short_8","alias_value":"JGDXA5P2","created_at":"2026-07-04T16:26:25.788751+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/JGDXA5P27DYLEZXT6BHFV4HIIH","json":"https://pith.science/pith/JGDXA5P27DYLEZXT6BHFV4HIIH.json","graph_json":"https://pith.science/api/pith-number/JGDXA5P27DYLEZXT6BHFV4HIIH/graph.json","events_json":"https://pith.science/api/pith-number/JGDXA5P27DYLEZXT6BHFV4HIIH/events.json","paper":"https://pith.science/paper/JGDXA5P2"},"agent_actions":{"view_html":"https://pith.science/pith/JGDXA5P27DYLEZXT6BHFV4HIIH","download_json":"https://pith.science/pith/JGDXA5P27DYLEZXT6BHFV4HIIH.json","view_paper":"https://pith.science/paper/JGDXA5P2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0110394&json=true","fetch_graph":"https://pith.science/api/pith-number/JGDXA5P27DYLEZXT6BHFV4HIIH/graph.json","fetch_events":"https://pith.science/api/pith-number/JGDXA5P27DYLEZXT6BHFV4HIIH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JGDXA5P27DYLEZXT6BHFV4HIIH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JGDXA5P27DYLEZXT6BHFV4HIIH/action/storage_attestation","attest_author":"https://pith.science/pith/JGDXA5P27DYLEZXT6BHFV4HIIH/action/author_attestation","sign_citation":"https://pith.science/pith/JGDXA5P27DYLEZXT6BHFV4HIIH/action/citation_signature","submit_replication":"https://pith.science/pith/JGDXA5P27DYLEZXT6BHFV4HIIH/action/replication_record"}},"created_at":"2026-07-04T16:26:25.788751+00:00","updated_at":"2026-07-04T16:26:25.788751+00:00"}