https://w3id.org/np/RA1hIh4Y6gBucGVC8L-NSMuxiK1M4w1Zsi-4DrVO9Z94Q/Head https://w3id.org/np/RA1hIh4Y6gBucGVC8L-NSMuxiK1M4w1Zsi-4DrVO9Z94Q http://www.nanopub.org/nschema#hasAssertion https://w3id.org/np/RA1hIh4Y6gBucGVC8L-NSMuxiK1M4w1Zsi-4DrVO9Z94Q/assertion https://w3id.org/np/RA1hIh4Y6gBucGVC8L-NSMuxiK1M4w1Zsi-4DrVO9Z94Q http://www.nanopub.org/nschema#hasProvenance https://w3id.org/np/RA1hIh4Y6gBucGVC8L-NSMuxiK1M4w1Zsi-4DrVO9Z94Q/provenance https://w3id.org/np/RA1hIh4Y6gBucGVC8L-NSMuxiK1M4w1Zsi-4DrVO9Z94Q http://www.nanopub.org/nschema#hasPublicationInfo https://w3id.org/np/RA1hIh4Y6gBucGVC8L-NSMuxiK1M4w1Zsi-4DrVO9Z94Q/pubinfo https://w3id.org/np/RA1hIh4Y6gBucGVC8L-NSMuxiK1M4w1Zsi-4DrVO9Z94Q http://www.w3.org/1999/02/22-rdf-syntax-ns#type http://www.nanopub.org/nschema#Nanopublication https://w3id.org/np/RA1hIh4Y6gBucGVC8L-NSMuxiK1M4w1Zsi-4DrVO9Z94Q/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/curie1895-04--gemini http://purl.org/dc/terms/description This claim specifies the exact substance (O2 gas), temperature range (20–450 °C, i.e., 293–723 K), variables (log K vs log T), and quantitative criterion (straight line of slope -1). Because O2 has a 3Σ_g^- triplet ground state with negligible excited-state population below 750 K, its molar paramagnetic susceptibility strictly follows χ_m = C/T, which can be verified immediately from Curie's own published table (p. 316) and modern reference compilations. https://w3id.org/delphi/resource/assessment/curie1895-04--gemini http://purl.org/dc/terms/subject https://w3id.org/delphi/resource/concept/dataset-resolvability-0.2.0 https://w3id.org/delphi/resource/assessment/curie1895-04--gemini http://www.w3.org/1999/02/22-rdf-syntax-ns#type https://w3id.org/delphi/ontology/LLMClaimAssessment https://w3id.org/delphi/resource/assessment/curie1895-04--gemini http://www.w3.org/2000/01/rdf-schema#comment Proposed test with existing data: Take measured mass magnetic susceptibility K of gaseous O2 across temperatures T between 293 K (20 °C) and 723 K (450 °C) and fit an ordinary least-squares regression of log(K) against log(T). 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