{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:IK7C5UWYBLFXKMXW5CC4KIP63X","short_pith_number":"pith:IK7C5UWY","schema_version":"1.0","canonical_sha256":"42be2ed2d80acb7532f6e885c521fedde6bf6a5fe4c1c4319a1801e6dc2b2f1d","source":{"kind":"arxiv","id":"2607.26747","version":1},"attestation_state":"computed","paper":{"title":"Fluctuation force induced by quenched random polarizations","license":"http://creativecommons.org/licenses/by-sa/4.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.mtrl-sci","physics.atom-ph"],"primary_cat":"cond-mat.dis-nn","authors_text":"Bing-Sui Lu","submitted_at":"2026-07-29T10:38:42Z","abstract_excerpt":"We investigate the zero-temperature behavior of the fluctuation force induced by random electric dipoles that are frozen into a material and incapable of fluctuating thermally. Examples of such materials are relaxor ferroelectrics. In terms of the setup and geometry, we focus on a layered system comprising two coplanar semi-infinite slabs separated by a distance $\\ell$ as well as a system comprising a neutral atom in the vacuum located at a distance $\\ell$ above the surface of a semi-infinite slab. For both systems, we consider the cases where the quenched random dipolar disorder occurs inside"},"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":"2607.26747","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2026-07-29T10:38:42Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci","physics.atom-ph"],"title_canon_sha256":"eb041d2b0d973316641f7cf5e90777eca52fe4fefb5d58dbb923bd43c6147ae1","abstract_canon_sha256":"7c528db93ab60bcd9b47220812a7cd84447d72d993d43b72018c7e124df59fde"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"42be2ed2d80acb7532f6e885c521fedde6bf6a5fe4c1c4319a1801e6dc2b2f1d","last_reissued_at":"2026-07-30T01:22:10.555962Z","signature_status":"unsigned_v0","first_computed_at":"2026-07-30T01:22:10.555962Z"},"graph_snapshot":{"paper":{"title":"Fluctuation force induced by quenched random polarizations","license":"http://creativecommons.org/licenses/by-sa/4.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.mtrl-sci","physics.atom-ph"],"primary_cat":"cond-mat.dis-nn","authors_text":"Bing-Sui Lu","submitted_at":"2026-07-29T10:38:42Z","abstract_excerpt":"We investigate the zero-temperature behavior of the fluctuation force induced by random electric dipoles that are frozen into a material and incapable of fluctuating thermally. Examples of such materials are relaxor ferroelectrics. In terms of the setup and geometry, we focus on a layered system comprising two coplanar semi-infinite slabs separated by a distance $\\ell$ as well as a system comprising a neutral atom in the vacuum located at a distance $\\ell$ above the surface of a semi-infinite slab. For both systems, we consider the cases where the quenched random dipolar disorder occurs inside"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.26747","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/2607.26747/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":"2607.26747","created_at":"2026-07-30T01:22:10.561561+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.26747v1","created_at":"2026-07-30T01:22:10.561561+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.26747","created_at":"2026-07-30T01:22:10.561561+00:00"},{"alias_kind":"pith_short_12","alias_value":"IK7C5UWYBLFX","created_at":"2026-07-30T01:22:10.561561+00:00"},{"alias_kind":"pith_short_16","alias_value":"IK7C5UWYBLFXKMXW","created_at":"2026-07-30T01:22:10.561561+00:00"},{"alias_kind":"pith_short_8","alias_value":"IK7C5UWY","created_at":"2026-07-30T01:22:10.561561+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/IK7C5UWYBLFXKMXW5CC4KIP63X","json":"https://pith.science/pith/IK7C5UWYBLFXKMXW5CC4KIP63X.json","graph_json":"https://pith.science/api/pith-number/IK7C5UWYBLFXKMXW5CC4KIP63X/graph.json","events_json":"https://pith.science/api/pith-number/IK7C5UWYBLFXKMXW5CC4KIP63X/events.json","paper":"https://pith.science/paper/IK7C5UWY"},"agent_actions":{"view_html":"https://pith.science/pith/IK7C5UWYBLFXKMXW5CC4KIP63X","download_json":"https://pith.science/pith/IK7C5UWYBLFXKMXW5CC4KIP63X.json","view_paper":"https://pith.science/paper/IK7C5UWY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.26747&json=true","fetch_graph":"https://pith.science/api/pith-number/IK7C5UWYBLFXKMXW5CC4KIP63X/graph.json","fetch_events":"https://pith.science/api/pith-number/IK7C5UWYBLFXKMXW5CC4KIP63X/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IK7C5UWYBLFXKMXW5CC4KIP63X/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IK7C5UWYBLFXKMXW5CC4KIP63X/action/storage_attestation","attest_author":"https://pith.science/pith/IK7C5UWYBLFXKMXW5CC4KIP63X/action/author_attestation","sign_citation":"https://pith.science/pith/IK7C5UWYBLFXKMXW5CC4KIP63X/action/citation_signature","submit_replication":"https://pith.science/pith/IK7C5UWYBLFXKMXW5CC4KIP63X/action/replication_record"}},"created_at":"2026-07-30T01:22:10.561561+00:00","updated_at":"2026-07-30T01:22:10.561561+00:00"}