https://w3id.org/np/RAaxbCLR3IGRKsixYvjynG2kKbjAwr0ZE-YYhqztgIBuo/Head https://w3id.org/np/RAaxbCLR3IGRKsixYvjynG2kKbjAwr0ZE-YYhqztgIBuo http://www.nanopub.org/nschema#hasAssertion https://w3id.org/np/RAaxbCLR3IGRKsixYvjynG2kKbjAwr0ZE-YYhqztgIBuo/assertion https://w3id.org/np/RAaxbCLR3IGRKsixYvjynG2kKbjAwr0ZE-YYhqztgIBuo http://www.nanopub.org/nschema#hasProvenance https://w3id.org/np/RAaxbCLR3IGRKsixYvjynG2kKbjAwr0ZE-YYhqztgIBuo/provenance https://w3id.org/np/RAaxbCLR3IGRKsixYvjynG2kKbjAwr0ZE-YYhqztgIBuo http://www.nanopub.org/nschema#hasPublicationInfo https://w3id.org/np/RAaxbCLR3IGRKsixYvjynG2kKbjAwr0ZE-YYhqztgIBuo/pubinfo https://w3id.org/np/RAaxbCLR3IGRKsixYvjynG2kKbjAwr0ZE-YYhqztgIBuo http://www.w3.org/1999/02/22-rdf-syntax-ns#type http://www.nanopub.org/nschema#Nanopublication https://w3id.org/np/RAaxbCLR3IGRKsixYvjynG2kKbjAwr0ZE-YYhqztgIBuo/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/curie1894-03--gemini http://purl.org/dc/terms/description That effects can be more symmetric than their causes is directly demonstrable both mathematically and empirically in crystal physics: any second-rank symmetric tensor (optical indicatrix, electrical conductivity, thermal expansion) in a cubic crystal has full spherical symmetry ∞∞m, which is strictly higher than the cubic point group of the crystal lattice. Furthermore, acentric crystals with accidental or vanishingly small piezoelectric coefficients show zero response despite lacking inversion symmetry. Public tensor databases such as the Materials Project verify this across thousands of compounds immediately. https://w3id.org/delphi/resource/assessment/curie1894-03--gemini http://purl.org/dc/terms/subject https://w3id.org/delphi/resource/concept/dataset-resolvability-0.2.0 https://w3id.org/delphi/resource/assessment/curie1894-03--gemini http://www.w3.org/1999/02/22-rdf-syntax-ns#type https://w3id.org/delphi/ontology/LLMClaimAssessment https://w3id.org/delphi/resource/assessment/curie1894-03--gemini http://www.w3.org/2000/01/rdf-schema#comment Proposed test with existing data: Compare the symmetry group G_effect of second-rank and fourth-rank physical property tensors (such as dielectric permittivity, magnetic susceptibility, thermal expansion, or optical refractivity) against the crystallographic point group G_crystal of the host crystal. 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