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在自旋半导体石墨烯纳米带中分离的自旋载流子。

Spatially separated spin carriers in spin-semiconducting graphene nanoribbons.

机构信息

Department of Materials Science and Engineering, University of Utah, Salt Lake City, Utah 84112, USA.

出版信息

Phys Rev Lett. 2013 Aug 30;111(9):096803. doi: 10.1103/PhysRevLett.111.096803. Epub 2013 Aug 29.

Abstract

A graphene nanoribbon with sawtooth edges has a ferromagnetic ground state. Using first-principles and tight-binding model calculations, we show that, under a transverse electrical field, the sawtooth graphene nanoribbons become a spin semiconductor whose charge carriers are not only spin polarized in energy space but also spatially separated at different edges. Low-energy excitation produces spin-up electrons localized at one edge and spin-down holes at the opposite edge, and the excitation energy of spin carries can be tuned by the electric field to reach a new state of spin gapless semiconductor. Also, the spin semiconducting states are shown to be robust against at least 10% edge disorder. These features demonstrate a good tunability of spin carriers for spintronics applications.

摘要

锯齿状边缘的石墨烯纳米带具有铁磁基态。通过第一性原理和紧束缚模型计算,我们表明,在横向电场作用下,锯齿状石墨烯纳米带成为一种自旋半导体,其载流子不仅在能量空间中具有自旋极化,而且在不同边缘处空间分离。低能激发产生局域在一个边缘的自旋向上电子和相反边缘的自旋向下空穴,并且自旋载流子的激发能量可以通过电场进行调节,从而达到无能隙自旋半导体的新状态。此外,自旋半导体态被证明对至少 10%的边缘无序具有鲁棒性。这些特性表明,对于自旋电子学应用来说,自旋载流子具有很好的可调谐性。

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