2016
DOI: 10.21474/ijar01/1954
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THE ELECTRONIC PROPERTIES SIMULATION OF INDIUM NITRIDE (InN) WURTZITE NANOCRYSTAL USING DENSITY FUNCTIONAL THEORY WITH GENERALIZED GRADIENT APPROXIMATION

Abstract: Density functional theory, Large unit cell, InN wurtzite nanocrystal. We have stimulated the electronic properties of wurtzite Indium Nitride by using density functional theory (DFT). The energy gap is size dependent at which E g increase with decreasing the size of InN nanocrystals. Also the lattice constant behaves in the same way as energy gap do. The cohesive energy is also calculated for the InN nanocrystals for 4, 8, 32 and 64 core atoms. Results shows that the cohesive energy values become larger as the… Show more

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Cited by 3 publications
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“…Note that n b used is that of C d x Z n 1−x Te calculated from Table 1 and Equation ( 5). The conduction band discontinuity ΔE c is calculated from the electron affinity EA as [23] Δ E c = EA (active) − EA (barrier ) (6) The valence band discontinuity ΔE v is then obtained from it. The adequate dopant for this structure is the Mn dopant [24,25].…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Note that n b used is that of C d x Z n 1−x Te calculated from Table 1 and Equation ( 5). The conduction band discontinuity ΔE c is calculated from the electron affinity EA as [23] Δ E c = EA (active) − EA (barrier ) (6) The valence band discontinuity ΔE v is then obtained from it. The adequate dopant for this structure is the Mn dopant [24,25].…”
Section: Resultsmentioning
confidence: 99%
“…Note that nb${n_b}$ used is that of CdxZn1xTe$C{d_x}Z{n_{1 - x}}Te$ calculated from Table 1 and Equation (5). The conduction band discontinuity normalΔEc$\Delta {E_c}$ is calculated from the electron affinity EA$EA$ as [23] normalΔ0.28emEcbadbreak=0.28emEA()activegoodbreak−EA()barrier$$\begin{equation}\Delta \;{E_c} = \;EA\left( {active} \right) - EA\left( {barrier} \right)\end{equation}$$…”
Section: Resultsmentioning
confidence: 99%