https://w3id.org/np/RACfKTebm5R8iu3Eu42gCzBOuJzlbPS_kG08qihiA6-xs/Head https://w3id.org/np/RACfKTebm5R8iu3Eu42gCzBOuJzlbPS_kG08qihiA6-xs http://www.nanopub.org/nschema#hasAssertion https://w3id.org/np/RACfKTebm5R8iu3Eu42gCzBOuJzlbPS_kG08qihiA6-xs/assertion https://w3id.org/np/RACfKTebm5R8iu3Eu42gCzBOuJzlbPS_kG08qihiA6-xs http://www.nanopub.org/nschema#hasProvenance https://w3id.org/np/RACfKTebm5R8iu3Eu42gCzBOuJzlbPS_kG08qihiA6-xs/provenance https://w3id.org/np/RACfKTebm5R8iu3Eu42gCzBOuJzlbPS_kG08qihiA6-xs http://www.nanopub.org/nschema#hasPublicationInfo https://w3id.org/np/RACfKTebm5R8iu3Eu42gCzBOuJzlbPS_kG08qihiA6-xs/pubinfo https://w3id.org/np/RACfKTebm5R8iu3Eu42gCzBOuJzlbPS_kG08qihiA6-xs http://www.w3.org/1999/02/22-rdf-syntax-ns#type http://www.nanopub.org/nschema#Nanopublication https://w3id.org/np/RACfKTebm5R8iu3Eu42gCzBOuJzlbPS_kG08qihiA6-xs/assertion https://w3id.org/delphi/resource/agent/delphisci-resolvability-assessor-gemini-4-argon-medium http://www.w3.org/1999/02/22-rdf-syntax-ns#type http://www.w3.org/ns/prov#SoftwareAgent https://w3id.org/delphi/resource/agent/delphisci-resolvability-assessor-gemini-4-argon-medium http://www.w3.org/2000/01/rdf-schema#label delphisci dataset-resolvability assessor (Gemini 4 Argon) https://w3id.org/delphi/resource/agent/delphisci-resolvability-assessor-gemini-4-argon-medium http://www.w3.org/ns/prov#actedOnBehalfOf https://orcid.org/0009-0007-4948-9192 https://w3id.org/delphi/resource/agent/delphisci-resolvability-assessor-gemini-4-argon-medium https://w3id.org/delphi/ontology/usesModel https://w3id.org/delphi/resource/model/gemini-4-argon-medium https://w3id.org/delphi/resource/assessment/curie1895-05--gemini http://purl.org/dc/terms/description The transition of a ferromagnet upon heating through its Curie point into a linear paramagnet (M ∝ H passing through the origin) is a foundational, sharply defined physical phenomenon. Isothermal M(H, T) curves in Curie's 1895 memoir and modern magnetic reference tables in Landolt-Börnstein/SpringerMaterials confirm that above ~770 °C pure iron loses spontaneous magnetization and exhibits linear paramagnetic response curves through the origin. https://w3id.org/delphi/resource/assessment/curie1895-05--gemini http://purl.org/dc/terms/subject https://w3id.org/delphi/resource/concept/dataset-resolvability-0.2.0 https://w3id.org/delphi/resource/assessment/curie1895-05--gemini http://www.w3.org/1999/02/22-rdf-syntax-ns#type https://w3id.org/delphi/ontology/LLMClaimAssessment https://w3id.org/delphi/resource/assessment/curie1895-05--gemini http://www.w3.org/2000/01/rdf-schema#comment Proposed test with existing data: Measure isothermal magnetization curves M(H) of ferromagnetic iron (Fe), nickel (Ni), and magnetite (Fe3O4) across temperatures spanning below and above their Curie temperatures T_C (~770 °C for Fe). Confirm if below T_C, M(H) exhibits spontaneous magnetization, hysteresis, and saturation curvature, whereas above ~760–770 °C for iron, M(H) becomes linear through the origin (M = χH with M(0) = 0) with a small paramagnetic susceptibility χ. https://w3id.org/delphi/resource/assessment/curie1895-05--gemini http://www.w3.org/2000/01/rdf-schema#label Gemini 4 Argon on curie1895-05: resolvable-now, resolvability 0.90 https://w3id.org/delphi/resource/assessment/curie1895-05--gemini http://www.w3.org/ns/prov#wasAttributedTo https://w3id.org/delphi/resource/agent/delphisci-resolvability-assessor-gemini-4-argon-medium https://w3id.org/delphi/resource/assessment/curie1895-05--gemini https://w3id.org/delphi/ontology/assessmentType dataset-resolvability/0.2.0 https://w3id.org/delphi/resource/assessment/curie1895-05--gemini https://w3id.org/delphi/ontology/evidenceAgainst Critical fluctuations very close to T_C (~770 °C in pure Fe) produce slight non-linear Arrott-plot curvature (M ∝ H^(1/δ)) 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