Publication | Closed Access
Dynamic defect reactions induced by multiphonon nonradiative recombination of injected carriers at deep levels in semiconductors
83
Citations
25
References
1984
Year
Violent lattice vibrations, induced by nonradiative capture of a free carrier by a deep-level defect in semiconductors, enhance greatly defect reactions such as movement of the defect itself or production of a new one, through reduction of the thermal activation energy (TAE). A theory of this phenomenon is presented. When capture takes place at a critical value ${\ensuremath{\Delta}}_{P}$ of a configuration coordinate ${Q}_{P}$, the total energy of the induced vibrations is larger than ${E}_{P}$ of the minimum lattice energy obtained under ${Q}_{P}={\ensuremath{\Delta}}_{P}$. A defect reaction with TAE of ${E}_{A}$ in thermal equilibrium takes place when another configuration coordinate ${Q}_{R}$ exceeds a critical value ${\ensuremath{\Delta}}_{R}$. Both ${Q}_{P}$ and ${Q}_{R}$ are a linear combination of many normal-mode coordinates in general. Energy flow from ${Q}_{P}$ to ${Q}_{R}$ occurs through the direction cosine $g$ between them in the phonon space, and $g$ is nonvanishing when there exist normal-mode components common between them. Under the condition that ${Q}_{P}$ started from ${\ensuremath{\Delta}}_{P}$ at time zero while ${Q}_{R}$ reaches ${\ensuremath{\Delta}}_{R}$ thereafter, we determine the minimum lattice energy written as ${E}_{P}+{E}_{H}$. Energy ${E}_{H}$ is smaller than ${E}_{A}$ when $g\ensuremath{\ne}0$ and gives the TAE of the quantum yield of the defect reaction occurring subsequently after carrier capture. We find that ${E}_{H}={E}_{A}\ensuremath{-}{E}_{P}$ for ${E}_{P}<{g}^{2}{E}_{A}$, ${E}_{H}=\frac{{[{({E}_{A})}^{\frac{1}{2}}\ensuremath{-}|g|{({E}_{P})}^{\frac{1}{2}}]}^{2}}{(1\ensuremath{-}{g}^{2})}$ for ${g}^{2}{E}_{A}<{E}_{P}<\frac{{E}_{A}}{{g}^{2}}$, and ${E}_{H}=0$ for ${E}_{P}>\frac{{E}_{A}}{{g}^{2}}$. The TAE of the defect reaction observed is given by ${E}_{H}$ plus the TAE of carrier capture, which is shown to explain experimental data quite well.
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