{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2025,10,18]],"date-time":"2025-10-18T15:02:22Z","timestamp":1760799742610},"reference-count":0,"publisher":"Wiley","issue":"9-10","license":[{"start":{"date-parts":[[2014,5,2]],"date-time":"2014-05-02T00:00:00Z","timestamp":1398988800000},"content-version":"vor","delay-in-days":0,"URL":"http:\/\/onlinelibrary.wiley.com\/termsAndConditions#vor"}],"content-domain":{"domain":[],"crossmark-restriction":false},"short-container-title":["Phys. Status Solidi C"],"published-print":{"date-parts":[[2014,9]]},"abstract":"<jats:title>Abstract<\/jats:title><jats:p>Organic electronic materials, or amorphous electronic materials in general, have relatively low conductivity and this limits their application to the low\u2010frequency electronics market. To describe electronic conduction in these materials it is common to use percolation [1] or (variable range) hopping theory [2] (the two being equivalent). This is an inheritance from the earlier research in organic materials that were invariably insulators, where conduction was a perturbation \u2013 movement of charge was a rare event.<\/jats:p><jats:p>Summarizing in this paper our work on organic electronic materials, it is shown that for electronic materials, instead, it is better to revert to classical semiconductor theories, like band theory [3]. If we include a large density of traps in the energy system, all observed phenomena are easily explained. This includes 1. strong temperature dependent charge\u2010carrier mobility, 2. field\u2010dependent mobility, 3. anomalous transient behavior. Moreover, it is consistent with observations in many types of devices, ranging from two\u2010terminal devices such as diodes to three\u2010terminal devices such as thin\u2010film transistors [4].<\/jats:p><jats:p>(\u00a9 2014 WILEY\u2010VCH Verlag GmbH &amp; Co. KGaA, Weinheim)<\/jats:p>","DOI":"10.1002\/pssc.201300508","type":"journal-article","created":{"date-parts":[[2014,5,2]],"date-time":"2014-05-02T11:27:05Z","timestamp":1399030025000},"page":"1389-1392","source":"Crossref","is-referenced-by-count":2,"title":["Electrical characterization of organic (amorphous) electronic materials"],"prefix":"10.1002","volume":"11","author":[{"given":"Peter","family":"Stallinga","sequence":"first","affiliation":[]}],"member":"311","published-online":{"date-parts":[[2014,5,2]]},"container-title":["physica status solidi c"],"original-title":[],"language":"en","link":[{"URL":"https:\/\/api.wiley.com\/onlinelibrary\/tdm\/v1\/articles\/10.1002%2Fpssc.201300508","content-type":"unspecified","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/api.wiley.com\/onlinelibrary\/tdm\/v1\/articles\/10.1002%2Fpssc.201300508","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/onlinelibrary.wiley.com\/doi\/pdf\/10.1002\/pssc.201300508","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/onlinelibrary.wiley.com\/doi\/pdf\/10.1002\/pssc.201300508","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2023,8,30]],"date-time":"2023-08-30T08:10:43Z","timestamp":1693383043000},"score":1,"resource":{"primary":{"URL":"https:\/\/onlinelibrary.wiley.com\/doi\/10.1002\/pssc.201300508"}},"subtitle":[],"short-title":[],"issued":{"date-parts":[[2014,5,2]]},"references-count":0,"journal-issue":{"issue":"9-10","published-print":{"date-parts":[[2014,9]]}},"alternative-id":["10.1002\/pssc.201300508"],"URL":"https:\/\/doi.org\/10.1002\/pssc.201300508","archive":["Portico"],"relation":{},"ISSN":["1862-6351","1610-1642"],"issn-type":[{"value":"1862-6351","type":"print"},{"value":"1610-1642","type":"electronic"}],"subject":[],"published":{"date-parts":[[2014,5,2]]}}}