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However, a unified description of metallic resistivity is still missing. An empirical analysis of a large variety of metals shows that the parallel resistor formalism used in the cuprates, which includes T-linear and T-quadratic dependence of the electron scattering rates, can be used to provide a phenomenological description of the electrical resistivity in all metals. Here, we show that the different metallic classes are then determined by the relative magnitude of these two components and the magnitude of the extrapolated residual resistivity. These two parameters allow us to categorize a few systems that are notoriously hard to ascribe to one of the currently accepted metallic classes."},"dsDescriptionDate":{"typeName":"dsDescriptionDate","multiple":false,"typeClass":"primitive","value":"2022"}}]},{"typeName":"subject","multiple":true,"typeClass":"controlledVocabulary","value":["Chemistry","Physics"]},{"typeName":"keyword","multiple":true,"typeClass":"compound","value":[{"keywordValue":{"typeName":"keywordValue","multiple":false,"typeClass":"primitive","value":"Metals"}},{"keywordValue":{"typeName":"keywordValue","multiple":false,"typeClass":"primitive","value":"Resistivity"}},{"keywordValue":{"typeName":"keywordValue","multiple":false,"typeClass":"primitive","value":"Parallel Resistor"}},{"keywordValue":{"typeName":"keywordValue","multiple":false,"typeClass":"primitive","value":"Taylor Expansion"}},{"keywordValue":{"typeName":"keywordValue","multiple":false,"typeClass":"primitive","value":"Planckian dissipation"}}]},{"typeName":"publication","multiple":true,"typeClass":"compound","value":[{"publicationCitation":{"typeName":"publicationCitation","multiple":false,"typeClass":"primitive","value":"Qikai Guo, César Magén, Marcelo J. Rozenberg, and Beatriz Noheda.Phenomenological classification of metals based on resistivity. Physical Review B, 2022, 106(8): 085141."},"publicationIDType":{"typeName":"publicationIDType","multiple":false,"typeClass":"controlledVocabulary","value":"doi"},"publicationIDNumber":{"typeName":"publicationIDNumber","multiple":false,"typeClass":"primitive","value":"10.1103/PhysRevB.106.085141"},"publicationURL":{"typeName":"publicationURL","multiple":false,"typeClass":"primitive","value":"https://doi.org/10.1103/PhysRevB.106.085141"}}]},{"typeName":"depositor","multiple":false,"typeClass":"primitive","value":"Elsenga, Christina"},{"typeName":"dateOfDeposit","multiple":false,"typeClass":"primitive","value":"2022-06-20"}]},"dansDataVaultMetadata":{"displayName":"Data Vault Metadata","name":"dansDataVaultMetadata","fields":[{"typeName":"dansDataversePid","multiple":false,"typeClass":"primitive","value":"doi:10.34894/A1AHZR"},{"typeName":"dansDataversePidVersion","multiple":false,"typeClass":"primitive","value":"1.0"},{"typeName":"dansBagId","multiple":false,"typeClass":"primitive","value":"urn:uuid:b43ad1b3-6618-433a-81c4-4ec466f91cb9"},{"typeName":"dansNbn","multiple":false,"typeClass":"primitive","value":"urn:nbn:nl:ui:13-acb0ccc4-bdf7-4a25-9c7c-a8b8c896a4e6"}]}},"files":[{"label":"Experimental and simulated data of resistivtiy for different metals-1.xlsx","restricted":false,"version":1,"datasetVersionId":21481,"dataFile":{"id":309062,"persistentId":"","filename":"Experimental and simulated data of resistivtiy for different metals-1.xlsx","contentType":"application/vnd.openxmlformats-officedocument.spreadsheetml.sheet","friendlyType":"MS Excel Spreadsheet","filesize":346447,"storageIdentifier":"surf://store:182c35d6c31-48e6a27a9aee","rootDataFileId":-1,"checksum":{"type":"SHA-1","value":"839af10d251e3974f42c485240b26001d23a2353"},"tabularData":false,"creationDate":"2022-08-22","publicationDate":"2022-09-29","lastUpdateTime":"2022-09-29T14:30:38Z","fileAccessRequest":false}},{"label":"Raw data of Figure 1.xlsx","restricted":false,"version":1,"datasetVersionId":21481,"dataFile":{"id":309059,"persistentId":"","filename":"Raw data of Figure 1.xlsx","contentType":"application/vnd.openxmlformats-officedocument.spreadsheetml.sheet","friendlyType":"MS Excel Spreadsheet","filesize":47138,"storageIdentifier":"surf://store:182bad0e749-7bd06d5b3291","rootDataFileId":-1,"checksum":{"type":"SHA-1","value":"c250c11f8125e50bb7718de4396eaf3dfea3283c"},"tabularData":false,"creationDate":"2022-08-20","publicationDate":"2022-09-29","lastUpdateTime":"2022-09-29T14:30:38Z","fileAccessRequest":false}},{"label":"Raw data of Figure S10.xlsx","restricted":false,"version":1,"datasetVersionId":21481,"dataFile":{"id":309063,"persistentId":"","filename":"Raw data of Figure S10.xlsx","contentType":"application/vnd.openxmlformats-officedocument.spreadsheetml.sheet","friendlyType":"MS Excel Spreadsheet","filesize":9715,"storageIdentifier":"surf://store:182c36b2758-0a2050a01479","rootDataFileId":-1,"checksum":{"type":"SHA-1","value":"46abcb367cf28c892e280b3e0e0c6cdab49f6ace"},"tabularData":false,"creationDate":"2022-08-22","publicationDate":"2022-09-29","lastUpdateTime":"2022-09-29T14:30:38Z","fileAccessRequest":false}},{"label":"Raw data of Figure S35-Figure S37.xlsx","restricted":false,"version":1,"datasetVersionId":21481,"dataFile":{"id":309064,"persistentId":"","filename":"Raw data of Figure S35-Figure S37.xlsx","contentType":"application/vnd.openxmlformats-officedocument.spreadsheetml.sheet","friendlyType":"MS Excel Spreadsheet","filesize":42801,"storageIdentifier":"surf://store:182c373a826-b2eb2b74b8a2","rootDataFileId":-1,"checksum":{"type":"SHA-1","value":"0903427de36dfa200120e10497ba675779d12b68"},"tabularData":false,"creationDate":"2022-08-22","publicationDate":"2022-09-29","lastUpdateTime":"2022-09-29T14:30:38Z","fileAccessRequest":false}},{"label":"Read me first.txt","restricted":false,"version":1,"datasetVersionId":21481,"dataFile":{"id":309065,"persistentId":"","filename":"Read me first.txt","contentType":"text/plain","friendlyType":"Plain Text","filesize":1624,"storageIdentifier":"surf://store:182c375c82f-244ded426e62","rootDataFileId":-1,"checksum":{"type":"SHA-1","value":"4680b44792ca08ccc96489c595f2f0530f50726f"},"tabularData":false,"creationDate":"2022-08-22","publicationDate":"2022-09-29","lastUpdateTime":"2022-09-29T14:30:38Z","fileAccessRequest":false}},{"label":"Summary of parameters.xlsx","restricted":false,"version":1,"datasetVersionId":21481,"dataFile":{"id":309061,"persistentId":"","filename":"Summary of parameters.xlsx","contentType":"application/vnd.openxmlformats-officedocument.spreadsheetml.sheet","friendlyType":"MS Excel Spreadsheet","filesize":14002,"storageIdentifier":"surf://store:182c35d6da6-07ea5a06d191","rootDataFileId":-1,"checksum":{"type":"SHA-1","value":"065d78eaa5734dbb9cf2e7fe2385fa7b58fd657d"},"tabularData":false,"creationDate":"2022-08-22","publicationDate":"2022-09-29","lastUpdateTime":"2022-09-29T14:30:38Z","fileAccessRequest":false}}]}}}