dc.contributorUniversidade de São Paulo (USP)
dc.contributorUniversidade Estadual Paulista (UNESP)
dc.contributorC.N.R. Bologna
dc.contributorIstituto FRAE del CNR
dc.contributorTech. University of Gdańsk
dc.date.accessioned2022-04-28T18:54:09Z
dc.date.accessioned2022-12-20T00:44:40Z
dc.date.available2022-04-28T18:54:09Z
dc.date.available2022-12-20T00:44:40Z
dc.date.created2022-04-28T18:54:09Z
dc.date.issued1996-01-01
dc.identifierJournal of Polymer Science, Part B: Polymer Physics, v. 34, n. 4, p. 623-629, 1996.
dc.identifier0887-6266
dc.identifierhttp://hdl.handle.net/11449/219191
dc.identifier10.1002/(SICI)1099-0488(199603)34:4<623
dc.identifier2-s2.0-0030105555
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/5399320
dc.description.abstractThe conductivity of poly(p-phenylene sulfide) (PPS) amorphous samples sandwiched between metallic electrodes has been studied as a function of applied voltage, temperature, and electrode material. The voltage (U) dependence of the currents for electric fields within the range 103-106 V/cm exhibits exp βU1/2 behavior with β = βSchottky below the glass transition temperature (Tg ≅ 90°C), and β = βPoole-Frenkel above Tg. Coordinated temperature measurements of dc currents with different metallic contacts and thermally stimulated currents (TSC) indicate, however, that the conductivity at T < Tg is consistent with the so-called anomalous Poole-Frenkel effect rather than the Schottky effect. Consequently, the p-type conductivity in amorphous PPS is proposed to be a bulk-limited process due to ionization of two different types of acceptor centers in the presence of neutral hole traps. © 1996 John Wiley & Sons, Inc.
dc.languageeng
dc.relationJournal of Polymer Science, Part B: Polymer Physics
dc.sourceScopus
dc.subjectElectrical conductivity of poly(p-phenylene sulfide)
dc.subjectPoly(p-phenylene sulfide)
dc.subjectPoole-Frenkel effect
dc.titlePoole-Frenkel effect in amorphous poly(p-phenylene sulfide)
dc.typeArtículos de revistas


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