2 research outputs found

    Mercury Telluride Colloidal Quantum Dots: Electronic Structure, Size-Dependent Spectra, and Photocurrent Detection up to 12 Ī¼m

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    HgTe colloidal quantum dots are synthesized with high monodispersivity with sizes up to āˆ¼15 nm corresponding to a room temperature absorption edge at āˆ¼5 Ī¼m. The shape is tetrahedral for larger sizes and up to five peaks are seen in the absorption spectra with a clear size dependence. The size range of the HgTe quantum dots is extended to āˆ¼20 nm using regrowth. The corresponding room temperature photoluminescence and absorption edge reach into the long-wave infrared, past 8 Ī¼m. Upon cooling to liquid nitrogen temperature, a photoconductive response is obtained in the long-wave infrared region up to 12 Ī¼m. Configuration-interaction tight-binding calculations successfully explain the spectra and the size dependence. The five optical features can be assigned to sets of single hole to single electron transitions whose strengths are strongly influenced by the multiband/multiorbital character of the quantum-dot electronic states

    Size Dependence of the Exciton Transitions in Colloidal CdTe Quantum Dots

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    In this paper, we present a detailed investigation of the size dependence of the optical transitions of colloidal CdTe QDs ranging in diameter from 2.9 to 14.8 nm. The energy integrated absorption cross section per CdTe unit is investigated in detail for the lowest two exciton transitions (1S<sub>3/2(h)</sub>ā€“1S<sub>(e)</sub> and 2S<sub>3/2(h)</sub>ā€“1S<sub>(e)</sub>) and shown to increase with decreasing size, although the size dependence of the 2S<sub>3/2(h)</sub>ā€“1S<sub>(e)</sub> is less pronounced. The experimental absorption spectra are compared to spectra calculated by using a tight-binding approach. The calculations were carried out with electronā€“hole configuration interaction (CI) and without (single-particle, SP). The optical absorption spectra calculated by using the CI approach are in excellent agreement with the experiment, as well as the evolution of the optical gap and the optical transitions with nanocrystal size
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