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Transition between direct and indirect band gap in silicon nanocrystals

机译:硅纳米晶体中直接带隙和间接带隙之间的过渡

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Using ground-state density functional theory we study the transition from indirect to direct band gap in hydrogen-terminated silicon nanocrystals (NCs) as a function of decreasing diameter. The studied range, from 1.0 to 4.6 nm diameter of nanocrystals, with spherical and Wulff-shape NCs, covers the transition from nano- to bulk regime. A change in the symmetry of the lowest unoccupied state as a function of decreasing NC diameter is observed, gradually increasing the oscillator strength of transitions from the highest occupied to the lowest unoccupied state. Real space and Fourier space characteristics of highest occupied and lowest unoccupied states are explored in detail and linked to a smooth transition from nano- to bulk regime.
机译:使用基态密度泛函理论,我们研究了氢终止的硅纳米晶体(NCs)从间接带隙到直接带隙的转变随直径减小的变化。研究范围为直径从1.0到4.6 nm的纳米晶体,具有球形和Wulff形状的NC,涵盖了从纳米到本体的转变。观察到最低空位状态的对称性随NC直径的减小而变化,逐渐增加了从最高空位到最低空位状态的振荡器强度。详细探讨了最高占用状态和最低未占用状态的实际空间和傅立叶空间特征,并将其与从纳米态到体态的平稳过渡联系起来。

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