{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:35WI6UUJLCDZX2BBAMVWM2BQ66","short_pith_number":"pith:35WI6UUJ","schema_version":"1.0","canonical_sha256":"df6c8f528958879be821032b666830f7b35765b26ce8c391e9e01b1a830a2e58","source":{"kind":"arxiv","id":"1004.0112","version":1},"attestation_state":"computed","paper":{"title":"Crossover of Critical Casimir forces between different surface universality classes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"A. Macio{\\l}ek, S. Dietrich, T. F. Mohry","submitted_at":"2010-04-01T11:36:51Z","abstract_excerpt":"In confined systems near a continuous phase transition the long-ranged fluctuations of the corresponding order parameter are subject to boundary conditions. These constraints result in so-called critical Casimir forces acting as effective forces on the confining surfaces. For systems belonging to the Ising bulk universality class corresponding to a scalar order parameter the critical Casimir force is studied for the film geometry in the crossover regime characterized by different surface fields at the two surfaces. The scaling function of the critical Casimir force is calculated within mean fi"},"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":"1004.0112","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-04-01T11:36:51Z","cross_cats_sorted":[],"title_canon_sha256":"35313534d36f3084474b7a05808d6f0c4415072e0fd5618ffcee2e3938a4dddd","abstract_canon_sha256":"79df71db63486c37e39efe129ef9fd6375f6c7359820e659714dd243f8c4b527"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:08:15.068613Z","signature_b64":"ltTctEE2RDT92ddzPJG5W9EkIiifloRPCdkk10mrXapwPtmM6bfogrpREJ6adQMRH9vuw3osOQUd1YDKrq6xBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"df6c8f528958879be821032b666830f7b35765b26ce8c391e9e01b1a830a2e58","last_reissued_at":"2026-05-18T02:08:15.068096Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:08:15.068096Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Crossover of Critical Casimir forces between different surface universality classes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"A. Macio{\\l}ek, S. Dietrich, T. F. Mohry","submitted_at":"2010-04-01T11:36:51Z","abstract_excerpt":"In confined systems near a continuous phase transition the long-ranged fluctuations of the corresponding order parameter are subject to boundary conditions. These constraints result in so-called critical Casimir forces acting as effective forces on the confining surfaces. For systems belonging to the Ising bulk universality class corresponding to a scalar order parameter the critical Casimir force is studied for the film geometry in the crossover regime characterized by different surface fields at the two surfaces. The scaling function of the critical Casimir force is calculated within mean fi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.0112","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":"1004.0112","created_at":"2026-05-18T02:08:15.068186+00:00"},{"alias_kind":"arxiv_version","alias_value":"1004.0112v1","created_at":"2026-05-18T02:08:15.068186+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.0112","created_at":"2026-05-18T02:08:15.068186+00:00"},{"alias_kind":"pith_short_12","alias_value":"35WI6UUJLCDZ","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_16","alias_value":"35WI6UUJLCDZX2BB","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_8","alias_value":"35WI6UUJ","created_at":"2026-05-18T12:26:03.138858+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/35WI6UUJLCDZX2BBAMVWM2BQ66","json":"https://pith.science/pith/35WI6UUJLCDZX2BBAMVWM2BQ66.json","graph_json":"https://pith.science/api/pith-number/35WI6UUJLCDZX2BBAMVWM2BQ66/graph.json","events_json":"https://pith.science/api/pith-number/35WI6UUJLCDZX2BBAMVWM2BQ66/events.json","paper":"https://pith.science/paper/35WI6UUJ"},"agent_actions":{"view_html":"https://pith.science/pith/35WI6UUJLCDZX2BBAMVWM2BQ66","download_json":"https://pith.science/pith/35WI6UUJLCDZX2BBAMVWM2BQ66.json","view_paper":"https://pith.science/paper/35WI6UUJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1004.0112&json=true","fetch_graph":"https://pith.science/api/pith-number/35WI6UUJLCDZX2BBAMVWM2BQ66/graph.json","fetch_events":"https://pith.science/api/pith-number/35WI6UUJLCDZX2BBAMVWM2BQ66/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/35WI6UUJLCDZX2BBAMVWM2BQ66/action/timestamp_anchor","attest_storage":"https://pith.science/pith/35WI6UUJLCDZX2BBAMVWM2BQ66/action/storage_attestation","attest_author":"https://pith.science/pith/35WI6UUJLCDZX2BBAMVWM2BQ66/action/author_attestation","sign_citation":"https://pith.science/pith/35WI6UUJLCDZX2BBAMVWM2BQ66/action/citation_signature","submit_replication":"https://pith.science/pith/35WI6UUJLCDZX2BBAMVWM2BQ66/action/replication_record"}},"created_at":"2026-05-18T02:08:15.068186+00:00","updated_at":"2026-05-18T02:08:15.068186+00:00"}