{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:SW2J5PBC5WUWTV44HW6FIGPGPE","short_pith_number":"pith:SW2J5PBC","schema_version":"1.0","canonical_sha256":"95b49ebc22eda969d79c3dbc5419e67934ab5d748e06f09058c757631774080a","source":{"kind":"arxiv","id":"1409.6364","version":1},"attestation_state":"computed","paper":{"title":"Observation of Kibble-Zurek behavior near the Lifshitz point in ferroelectrics with incommensurate phase","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"A. Kohutych, A. Molnar, J. Banys, K.Z. Rushchanskii, R. Bilanych, R. Yevych, V. Samulionis, Yu.M. Vysochanskii","submitted_at":"2014-09-22T22:39:18Z","abstract_excerpt":"We have investigated non-equilibrium properties of proper uniaxial Sn$_2$P$_2$(Se$_x$S$_{1-x}$)$_6$ ferroelectrics with the Type II incommensurate phase above Lifshitz point $x_{\\rm LP} \\sim 0.28$. We measured dielectric susceptibility with cooling and heating rate ranging 0.002-0.1~K/min, and high-resolution ultrasound experiments and hypersound Brillouin scattering. For samples with $x \\geqslant 0.28$ clear anomalies were observed at incommensurate second order transition ($T_i$) and at first order lock-in transition ($T_c$) in the regime of very slow cooling rate, whereas the intermediate I"},"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":"1409.6364","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-09-22T22:39:18Z","cross_cats_sorted":[],"title_canon_sha256":"0bab2aa161762b49de694afc9813313e878e930e0fb44522c10f9705b48617b1","abstract_canon_sha256":"6a002236afad95e5f6368205693aa1cdcd72e34d01a475d85ee6a9858c9c0b0a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:22:41.881577Z","signature_b64":"Q+3YFE2GhchmEq4QuuiOCvWZUKH0npy45Wt+CA0TPt2egmHKVL9ObAqn+lNbEdQBypXYCqlVIEd1C49UMnvqCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"95b49ebc22eda969d79c3dbc5419e67934ab5d748e06f09058c757631774080a","last_reissued_at":"2026-05-18T01:22:41.881164Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:22:41.881164Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Observation of Kibble-Zurek behavior near the Lifshitz point in ferroelectrics with incommensurate phase","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"A. Kohutych, A. Molnar, J. Banys, K.Z. Rushchanskii, R. Bilanych, R. Yevych, V. Samulionis, Yu.M. Vysochanskii","submitted_at":"2014-09-22T22:39:18Z","abstract_excerpt":"We have investigated non-equilibrium properties of proper uniaxial Sn$_2$P$_2$(Se$_x$S$_{1-x}$)$_6$ ferroelectrics with the Type II incommensurate phase above Lifshitz point $x_{\\rm LP} \\sim 0.28$. We measured dielectric susceptibility with cooling and heating rate ranging 0.002-0.1~K/min, and high-resolution ultrasound experiments and hypersound Brillouin scattering. For samples with $x \\geqslant 0.28$ clear anomalies were observed at incommensurate second order transition ($T_i$) and at first order lock-in transition ($T_c$) in the regime of very slow cooling rate, whereas the intermediate I"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.6364","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":"1409.6364","created_at":"2026-05-18T01:22:41.881221+00:00"},{"alias_kind":"arxiv_version","alias_value":"1409.6364v1","created_at":"2026-05-18T01:22:41.881221+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.6364","created_at":"2026-05-18T01:22:41.881221+00:00"},{"alias_kind":"pith_short_12","alias_value":"SW2J5PBC5WUW","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_16","alias_value":"SW2J5PBC5WUWTV44","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_8","alias_value":"SW2J5PBC","created_at":"2026-05-18T12:28:49.207871+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/SW2J5PBC5WUWTV44HW6FIGPGPE","json":"https://pith.science/pith/SW2J5PBC5WUWTV44HW6FIGPGPE.json","graph_json":"https://pith.science/api/pith-number/SW2J5PBC5WUWTV44HW6FIGPGPE/graph.json","events_json":"https://pith.science/api/pith-number/SW2J5PBC5WUWTV44HW6FIGPGPE/events.json","paper":"https://pith.science/paper/SW2J5PBC"},"agent_actions":{"view_html":"https://pith.science/pith/SW2J5PBC5WUWTV44HW6FIGPGPE","download_json":"https://pith.science/pith/SW2J5PBC5WUWTV44HW6FIGPGPE.json","view_paper":"https://pith.science/paper/SW2J5PBC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1409.6364&json=true","fetch_graph":"https://pith.science/api/pith-number/SW2J5PBC5WUWTV44HW6FIGPGPE/graph.json","fetch_events":"https://pith.science/api/pith-number/SW2J5PBC5WUWTV44HW6FIGPGPE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SW2J5PBC5WUWTV44HW6FIGPGPE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SW2J5PBC5WUWTV44HW6FIGPGPE/action/storage_attestation","attest_author":"https://pith.science/pith/SW2J5PBC5WUWTV44HW6FIGPGPE/action/author_attestation","sign_citation":"https://pith.science/pith/SW2J5PBC5WUWTV44HW6FIGPGPE/action/citation_signature","submit_replication":"https://pith.science/pith/SW2J5PBC5WUWTV44HW6FIGPGPE/action/replication_record"}},"created_at":"2026-05-18T01:22:41.881221+00:00","updated_at":"2026-05-18T01:22:41.881221+00:00"}