Current density equations representing the transition between the injection- and bulk-limited currents for organic semiconductors

Sang Gun Lee, Reiji Hattori

    Research output: Contribution to journalArticle

    4 Citations (Scopus)

    Abstract

    The theoretical current density equations for organic semiconductors was derived according to the internal carrier emission equation based on the diffusion model at the Schottky barrier contact and the mobility equation based on the field dependence model, the so-called “Poole-Frenkel mobility model.” The electric field becomes constant because of the absence of a space charge effect in the case of a higher injection barrier height and a lower sample thickness, but there is distribution in the electric field because of the space charge effect in the case of a lower injection barrier height and a higher sample thickness. The transition between the injection- and bulk-limited currents was presented according to the Schottky barrier height and the sample thickness change.

    Original languageEnglish
    Pages (from-to)143-148
    Number of pages6
    JournalJournal of Information Display
    Volume10
    Issue number4
    DOIs
    Publication statusPublished - Jan 1 2009

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    Semiconducting organic compounds
    Current density
    Electric space charge
    Electric fields

    All Science Journal Classification (ASJC) codes

    • Materials Science(all)
    • Electrical and Electronic Engineering

    Cite this

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    abstract = "The theoretical current density equations for organic semiconductors was derived according to the internal carrier emission equation based on the diffusion model at the Schottky barrier contact and the mobility equation based on the field dependence model, the so-called “Poole-Frenkel mobility model.” The electric field becomes constant because of the absence of a space charge effect in the case of a higher injection barrier height and a lower sample thickness, but there is distribution in the electric field because of the space charge effect in the case of a lower injection barrier height and a higher sample thickness. The transition between the injection- and bulk-limited currents was presented according to the Schottky barrier height and the sample thickness change.",
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    AU - Hattori, Reiji

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    N2 - The theoretical current density equations for organic semiconductors was derived according to the internal carrier emission equation based on the diffusion model at the Schottky barrier contact and the mobility equation based on the field dependence model, the so-called “Poole-Frenkel mobility model.” The electric field becomes constant because of the absence of a space charge effect in the case of a higher injection barrier height and a lower sample thickness, but there is distribution in the electric field because of the space charge effect in the case of a lower injection barrier height and a higher sample thickness. The transition between the injection- and bulk-limited currents was presented according to the Schottky barrier height and the sample thickness change.

    AB - The theoretical current density equations for organic semiconductors was derived according to the internal carrier emission equation based on the diffusion model at the Schottky barrier contact and the mobility equation based on the field dependence model, the so-called “Poole-Frenkel mobility model.” The electric field becomes constant because of the absence of a space charge effect in the case of a higher injection barrier height and a lower sample thickness, but there is distribution in the electric field because of the space charge effect in the case of a lower injection barrier height and a higher sample thickness. The transition between the injection- and bulk-limited currents was presented according to the Schottky barrier height and the sample thickness change.

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