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Ambipolar electrical spin injection and spin transport in organic semiconductors

机译:双极性电自旋注入和有机半导体中的自旋输运

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摘要

We present a model to describe electrical injection of spin polarized electrons and holes from ferromagnetic contacts into a conjugated organic semiconductor. Transport in the semiconductor is treated by the spin dependent continuity equations coupled with Poisson's equation. The recombination of injected electrons and holes is modeled as a Langevin process. The boundary conditions used to solve the continuity equations are formulated in terms of spin polarized particle currents at the boundaries. Injected spin currents are related to the charge currents via the transport parameters of the ferromagnetic contacts. Spin injection strongly depends on the contact polarization and the conductivity of the contact material. No approximations that limit the model to small current polarizations are made. In the case of conventional ferromagnetic metal contacts, the relatively weak polarization and high conductivity hinder spin polarized injection. Spin injection can be greatly enhanced if (spin dependent) tunneling is the limiting process, which may be described by spin dependent contact resistances. The dependence of the current polarization on these contact resistances is explored. On the other hand, if the injecting contacts are made from half-metallic materials with low conductivity, spin injection is strong even for thermionic injection and the spin current approaches the charge current.
机译:我们提出一个模型来描述自旋极化电子和空穴从铁磁触点注入共轭有机半导体的电注入。半导体中的传输通过自旋相关的连续性方程式与Poisson方程式相结合来处理。注入的电子和空穴的复合被建模为兰格文过程。用于求解连续性方程的边界条件是根据边界处的自旋极化粒子电流来制定的。注入的自旋电流通过铁磁触点的传输参数与充电电流相关。自旋注入在很大程度上取决于接触极化和接触材料的电导率。没有进行将模型限制为小电流极化的近似计算。在常规铁磁金属触点的情况下,相对较弱的极化和较高的导电性阻碍了自旋极化注入。如果(自旋相关的)隧穿是限制过程,则可以极大地增强自旋注入,这可以用自旋相关的接触电阻来描述。探索了电流极化对这些接触电阻的依赖性。另一方面,如果注入触点由具有低电导率的半金属材料制成,则即使对于热电子注入,自旋注入也很牢固,并且自旋电流接近充电电流。

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  • 来源
    《Journal of Applied Physics》 |2008年第10期|499-506|共8页
  • 作者单位
  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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