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  1. Photoluminescence fatigue and inhomogeneous line broadening in semi-insulating Tl6 SeI4 single crystals

    Photoluminescence (PL) properties of semi-insulating Tl6SeI4 have been investigated. A broad emission band centered at 1.63 ± 0.02 eV was observed in all samples. The PL emission band is excitonic in nature and is tentatively attributed to a bound exciton emission. PL fatigue (a reduction in PL intensity under prolonged laser excitation) was always observed. The amount of PL fatigue depended on excitation power and temperature. PL fatigue kinetics are described by a stretched exponential with nominal lifetimes in the 10–265 s range. The recovery of the PL occurred within a few seconds of light cessation. The magnitude of PLmore » fatigue in different samples correlated with inhomogeneous line broadening of the 1.63 eV emission band, such that broader bands exhibited more fatigue. An additional luminescence band centered at 1.78 eV was observed which increased in intensity under prolonged laser irradiation. The fatigue phenomenon is tentatively attributed to two mechanisms—the formation of photo-induced defects and the formation of quasi-stable particles. Both of these mechanisms introduce additional radiative and non-radiative recombination channels that lead to a decrease in the PL intensity under prolonged laser irradiation. Finally, since inhomogeneous line broadening and PL fatigue are related to the concentration of defects or impurities, the measurement of these two parameters is an effective method to screen sample quality.« less
  2. Excitonic emissions and above-band-gap luminescence in the single-crystal perovskite semiconductors CsPbB r 3 and CsPbC l 3

    The ternary compounds CsPbX3 (X = Br or Cl) have perovskite structures that are being considered for optical and electronic applications such as lasing and gamma-ray detection. An above-band-gap excitonic photoluminescence (PL) band is seen in both CsPbX3 compounds. An excitonic emission peak centered at 2.98 eV, ~0.1 eV above the room-temperature band gap, is observed for CsPbCl3. The thermal quenching of the excitonic luminescence is well described by a two-step quenching model, yielding activation energies of 0.057 and 0.0076 eV for high- and low-temperature regimes, respectively. CsPbBr3 exhibits bound excitonic luminescence peaks located at 2.29 and 2.33 eV thatmore » are attributed to recombination involving Br vacancy centers. Activation energies for thermal quenching of the excitonic luminescence of 0.017 and 0.0007 eV were calculated for CsPbBr3. Temperature-dependent PL experiments reveal unexpected blueshifts for all excitonic emission peaks in CsPbX3 compounds. A phonon-assisted step-up process leads to the blueshift in CsPbBr3 emission, while there is a contribution from band-gap widening in CsPbCl3. Finally, the absence of significant deep level defect luminescence in these compounds makes them attractive candidates for high-resolution, room-temperature radiation detection.« less

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"Peters, J A"

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