@prefix this: . @prefix sub: . @prefix np: . @prefix rdf: . @prefix prov: . @prefix npx: . @prefix dc: . @prefix xsd: . sub:Head { this: a np:Nanopublication; np:hasAssertion sub:assertion; np:hasProvenance sub:provenance; np:hasPublicationInfo sub:pubinfo . } sub:assertion { a prov:SoftwareAgent; "delphisci dataset-resolvability assessor (Gemini 4 Argon)"; prov:actedOnBehalfOf ; . a ; dc:description "Curie's claim that ferromagnets heated well above their transformation point (specifically magnetite from 850 to 1370 °C) obey an asymptotic inverse-temperature susceptibility law of paramagnetic magnitude is directly testable using Curie's own 1895 data and modern high-temperature susceptibility tables in Landolt-Börnstein/SpringerMaterials. Furthermore, modern data distinguish the asymptotic linear 1/χ(T) Curie-Weiss regime from Néel ferrimagnetic curvature closer to T_C."; dc:subject ; "Proposed test with existing data: For magnetite (Fe3O4) in the high-temperature paramagnetic regime (850 to 1370 °C, i.e., 1123 to 1643 K, well above T_C ≈ 853 K) and other ferromagnets far above T_C, plot inverse susceptibility 1/χ against T. Evaluate whether χ(T) approaches the asymptotic Curie-Weiss / inverse-temperature scaling χ = C/(T - θ) (with ∂(1/χ)/∂T → constant and log-log slope approaching -1 at T >> T_C) and has magnitude comparable to standard paramagnetic salts."; "Gemini 4 Argon on curie1895-07: resolvable-now, resolvability 0.83"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0"; "Because magnetite is a two-sublattice ferrimagnet, its exact inverse susceptibility above T_C follows Néel's hyperbolic law 1/χ = (T - θ_a)/C - σ/(T - θ'), which only asymptotically approaches a straight line at temperatures well above T_C"; "0.85"^^xsd:double; ; "0.828"^^xsd:double; "resolvable-now" . a ; dc:isPartOf ; dc:subject ; "Analysis feasibility of curie1895-07 by Gemini 4 Argon: 0.85"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/analysis-feasibility"; "0.85"^^xsd:double . a ; dc:isPartOf ; dc:subject ; "Data adequacy of curie1895-07 by Gemini 4 Argon: 0.75"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/data-adequacy"; "0.75"^^xsd:double . a ; dc:isPartOf ; dc:subject ; "Data existence of curie1895-07 by Gemini 4 Argon: 0.8"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/data-existence"; "0.8"^^xsd:double . a ; dc:isPartOf ; dc:subject ; "Discriminating power of curie1895-07 by Gemini 4 Argon: 0.85"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/discriminating-power"; "0.85"^^xsd:double . a ; dc:isPartOf ; dc:subject ; "Operationalizability of curie1895-07 by Gemini 4 Argon: 0.9"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/operationalizability"; "0.9"^^xsd:double . , , , , , . a ; dc:description "Contains high-temperature paramagnetic susceptibility data 1/χ(T) above T_C for Fe3O4 and ferromagnetic metals."; "Candidate dataset: SpringerMaterials (Landolt-Börnstein)"; prov:wasDerivedFrom . a ; dc:identifier "gemini-4-argon-medium"; "Gemini 4 Argon" . } sub:provenance { sub:assertion prov:wasAttributedTo ; prov:wasDerivedFrom , ; prov:wasGeneratedBy sub:assessment . sub:assessment a prov:Activity; prov:qualifiedAssociation sub:assessmentPlan; prov:wasAssociatedWith . sub:assessmentPlan prov:hadPlan . } sub:pubinfo { "crystals-and-form" . this: dc:created "2026-11-07T03:18:24.087Z"^^xsd:dateTime; dc:creator ; dc:license ; npx:hasNanopubType ; npx:introduces ; "Gemini 4 Argon on curie1895-07: resolvable-now, resolvability 0.83"; . sub:sig npx:hasAlgorithm "RSA"; npx:hasPublicKey "MIIBIjANBgkqhkiG9w0BAQEFAAOCAQ8AMIIBCgKCAQEAyFHtPB6p0mCjDozxlOY9CmO3nBm7Te3jFbXyLmM+G1tGe47Da0jYIbhkl9Oo1ZjxmCa3LCwlEqK8gj6hEIcL4ahW30JXh9HycfKVk1bugkzMEV15tJdTzAU3sGMFnbNsn43xY2LFLy45tApkRm5byEiM7oRRrooIdwoQKnP4Wzq/bfAoJ9qvW+MGkelyOTd1jbSt+KfmT7xKmDfWzAHddUlWwMX2QJOLxDaffOteTop6ZRgPiNmPJKA/S62Gac9XtSYT3oDkZ6/nr5cxxNLpOyxTf5FPISiCe11xYO/unYjY+mwnOfA8yhJIyx1l0O9I0vpOpn+E5TvyHJV+oSTrvwIDAQAB"; npx:hasSignature "KRfVKF+bShkN8nG9CvmnX1M/WLrCiYeDJxnwieX5xXHJIaZFOvyDmUySE9XHvlX9/vYjgJvU8M/neJ3xnQN4LN+uZGyXlFw9/X3Bq/tVzJO0RWKu8hbe3LECNbQhUmFVMpbnyUeDmK4WnOO/V3jwXDQreddOkuuQFm6KVGDO7UhKqWtdhutIFMGvSvSjHUDoXVPKqnLbOIc+hExZ7mU7vUTOIrlZ/2MolfY+gCAf04+spA17N8aOTrBy0skBU2nMxrb79o3yOtWgBSJ9slENXZ9hEj+61W/8ZnHdQzQKjH+j1sTNE3Aul2UcGCQbuS5Kg95XVWDq4xiLr3hXgJhN1w=="; npx:hasSignatureTarget this:; npx:signedBy . }