4 research outputs found

    Transparent Long-Pass Filter with Short-Wavelength Scattering Based on <i>Morpho</i> Butterfly Nanostructures

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    We combine the principles of moth-eye antireflection, Bragg scattering, and thin-film interference to design and fabricate a short-wavelength scattering/long-pass filter with sharp cutoff, high transmission of infrared light, and strong reflection of visible light into high angles. Based on the lamellae-edge features on <i>Morpho didius</i> butterfly wings, nanostructures are self-assembled via sequential one-chamber chemical vapor deposition, metal nanoparticle formation, and wet-chemical etching. Finite-element modeling demonstrates strong (>45%) reflection into the first diffracted order for short wavelengths, while retaining >80% transmission for longer wavelengths. Fabricated nanostructures couple more than 50% of reflected light into angles of >10° while enabling broadband long-pass transmission. Such structures have potential applications in light trapping for tandem solar cells, stealth, and signals processing

    Ultralow Absorption Coefficient and Temperature Dependence of Radiative Recombination of CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> Perovskite from Photoluminescence

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    Spectrally resolved photoluminescence is used to measure the band-to-band absorption coefficient α<sub>BB</sub>(ℏω) of organic–inorganic hybrid perovskite methylammonium lead iodide (CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>) films from 675 to 1400 nm. Unlike other methods used to extract the absorption coefficient, photoluminescence is only affected by band-to-band absorption and is capable of detecting absorption events at very low energy levels. Absorption coefficients as low as 10<sup>–14</sup> cm<sup>–1</sup> are detected at room temperature for long wavelengths, which is 14 orders of magnitude lower than reported values at shorter wavelengths. The temperature dependence of α<sub>BB</sub>(ℏω) is calculated from the photoluminescence spectra of CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> in the temperature range 80–360 K. Based on the temperature-dependent α<sub>BB</sub>(ℏω), the product of the radiative recombination coefficient and square of the intrinsic carrier density, <i>B</i>(<i>T</i>) × <i>n</i><sub><i>i</i></sub><sup>2</sup>, is also obtained

    Inverted Hysteresis in CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> Solar Cells: Role of Stoichiometry and Band Alignment

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    J–V hysteresis in perovskite solar cells is known to be strongly dependent on many factors ranging from the cell structure to the preparation methods. Here we uncover one likely reason for such sensitivity by linking the stoichiometry in pure CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> (MAPbI<sub>3</sub>) perovskite cells with the character of their hysteresis behavior through the influence of internal band offsets. We present evidence indicating that in some cells the ion accumulation occurring at large forward biases causes a temporary and localized increase in recombination at the MAPbI<sub>3</sub>/TiO<sub>2</sub> interface, leading to inverted hysteresis at fast scan rates. Numerical semiconductor models including ion accumulation are used to propose and analyze two possible origins for these localized recombination losses: one based on band bending and the other on an accumulation of ionic charge in the perovskite bulk
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