@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 "The linear reversal of electric polarization polarity between contraction and dilatation is the defining odd-parity response of the direct piezoelectric effect (P_i = e_{ijk} ε_{jk}) and secondary pyroelectricity. Signed piezoelectric tensors in the Materials Project and experimental reference tables in SpringerMaterials/NIST immediately verify that compressive and tensile strains along a polar axis generate opposite electric poles."; dc:subject ; "Proposed test with existing data: For piezoelectric and pyroelectric crystals (e.g., tourmaline, quartz, ZnO, BaTiO3), evaluate the sign of induced electric polarization P_i = d_{ijk} σ_{jk} (or e_{ijk} ε_{jk}) under compressive (ε < 0) versus tensile/dilatational (ε > 0) strain along a polar axis, whether driven by mechanical stress or thermal expansion/contraction. Confirm if reversing the sign of strain reverses the polarity of the induced surface charge."; "Gemini 4 Argon on curie1880-02: resolvable-now, resolvability 0.91"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0"; "In pyroelectricity, total measured charge change with temperature includes both a primary (clamped-lattice) contribution and a secondary (thermal-expansion piezoelectric) contribution, which in rare cases can differ in sign"; "0.9"^^xsd:double; , ; "0.91"^^xsd:double; "resolvable-now" . a ; dc:isPartOf ; dc:subject ; "Analysis feasibility of curie1880-02 by Gemini 4 Argon: 0.9"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/analysis-feasibility"; "0.9"^^xsd:double . a ; dc:isPartOf ; dc:subject ; "Data adequacy of curie1880-02 by Gemini 4 Argon: 0.85"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/data-adequacy"; "0.85"^^xsd:double . a ; dc:isPartOf ; dc:subject ; "Data existence of curie1880-02 by Gemini 4 Argon: 0.9"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/data-existence"; "0.9"^^xsd:double . a ; dc:isPartOf ; dc:subject ; "Discriminating power of curie1880-02 by Gemini 4 Argon: 0.95"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/discriminating-power"; "0.95"^^xsd:double . a ; dc:isPartOf ; dc:subject ; "Operationalizability of curie1880-02 by Gemini 4 Argon: 0.95"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/operationalizability"; "0.95"^^xsd:double . , , , , , . a ; dc:description "Supplies signed third-rank piezoelectric stress (e_{ij}) and strain (d_{ij}) tensors for thousands of polar and non-centrosymmetric crystals."; "Candidate dataset: Materials Project"; prov:wasDerivedFrom . a ; dc:description "Provides reference piezoelectric and pyroelectric property data for standard crystalline materials."; "Candidate dataset: NIST Standard Reference Data"; 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 curie1880-02: resolvable-now, resolvability 0.91"; . sub:sig npx:hasAlgorithm "RSA"; npx:hasPublicKey "MIIBIjANBgkqhkiG9w0BAQEFAAOCAQ8AMIIBCgKCAQEAyFHtPB6p0mCjDozxlOY9CmO3nBm7Te3jFbXyLmM+G1tGe47Da0jYIbhkl9Oo1ZjxmCa3LCwlEqK8gj6hEIcL4ahW30JXh9HycfKVk1bugkzMEV15tJdTzAU3sGMFnbNsn43xY2LFLy45tApkRm5byEiM7oRRrooIdwoQKnP4Wzq/bfAoJ9qvW+MGkelyOTd1jbSt+KfmT7xKmDfWzAHddUlWwMX2QJOLxDaffOteTop6ZRgPiNmPJKA/S62Gac9XtSYT3oDkZ6/nr5cxxNLpOyxTf5FPISiCe11xYO/unYjY+mwnOfA8yhJIyx1l0O9I0vpOpn+E5TvyHJV+oSTrvwIDAQAB"; npx:hasSignature "tVJCGdNwJxo13c8cmnFDc6ku9bO1IHsX/IfsntI2KvXoUG2SDYjL/LwBFvNJpyM8Uwb+T8VbGtRgCpw6Py3s49c0CnkqE+Iftdbse6Y2T/M81MpgKwINLxPMU1t/lHa79IOq4DRODS07jTJIzQNPQNjU8tr+6OYdgk1D4+V72/8YJw+RjVpxHfe23UjkAlsNY216TaN/DmN1mR/uPWDJhoFYPSWW/QLr8TU+yeqrxurBFLOzlGV7E3MxVh+PfGZYCJd+sFJeLPPp+iSyAGsWfHEwlfS5Qnq0LsMHqA0mAnJVsYe6d1AsjsXnmVr53ACPQlbwoP6TUFztR+JSAlKRbA=="; npx:hasSignatureTarget this:; npx:signedBy . }