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Excitonic fine structure and recombination dynamics in single-crystalline<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi mathvariant="normal">ZnO</mml:mi></mml:mrow></mml:math>

Ali TekeDepartment of Electrical Engineering, Virginia Commonwealth University, Richmond, Virginia 23284, USAÜ. ÖzgürDepartment of Electrical Engineering, Virginia Commonwealth University, Richmond, Virginia 23284, USAS. DoğanDepartment of Electrical Engineering, Virginia Commonwealth University, Richmond, Virginia 23284, USAXing GuDepartment of Electrical Engineering, Virginia Commonwealth University, Richmond, Virginia 23284, USAH. MorkoçDepartment of Electrical Engineering, Virginia Commonwealth University, Richmond, Virginia 23284, USABill NemethDepartment of Electrical Engineering, Virginia Commonwealth University, Richmond, Virginia 23284, USAJeff NauseDepartment of Electrical Engineering, Virginia Commonwealth University, Richmond, Virginia 23284, USAHenry O. EverittDepartment of Electrical Engineering, Virginia Commonwealth University, Richmond, Virginia 23284, USA
2004lv
ABI

Abstract

The optical properties of a high quality bulk $\mathrm{ZnO}$, thermally post treated in a forming gas environment are investigated by temperature dependent continuous wave and time-resolved photoluminescence (PL) measurements. Several bound and free exciton transitions along with their first excited states have been observed at low temperatures, with the main neutral-donor-bound exciton peak at $3.3605\phantom{\rule{0.3em}{0ex}}\mathrm{eV}$ having a linewidth of $0.7\phantom{\rule{0.3em}{0ex}}\mathrm{meV}$ and dominating the PL spectrum at $10\phantom{\rule{0.3em}{0ex}}\mathrm{K}$. This bound exciton transition was visible only below $150\phantom{\rule{0.3em}{0ex}}\mathrm{K}$, whereas the A-free exciton transition at $3.3771\phantom{\rule{0.3em}{0ex}}\mathrm{eV}$ persisted up to room temperature. A-free exciton binding energy of $60\phantom{\rule{0.3em}{0ex}}\mathrm{meV}$ is obtained from the position of the excited states of the free excitons. Additional intrinsic and extrinsic fine structures such as polariton, two-electron satellites, donor-acceptor pair transitions, and longitudinal optical-phonon replicas have also been observed and investigated in detail. Time-resolved PL measurements at room temperature reveal a biexponential decay behavior with typical decay constants of $\ensuremath{\sim}170$ and $\ensuremath{\sim}864\phantom{\rule{0.3em}{0ex}}\mathrm{ps}$ for the as-grown sample. Thermal treatment is observed to increase the carrier lifetimes when performed in a forming gas environment.

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