3 research outputs found

    Directional Negative Thermal Expansion and Large Poisson Ratio in CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> Perovskite Revealed by Strong Coherent Shear Phonon Generation

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    Despite the enormous amount of attention CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> has received, we are still lacking an in-depth understanding of its basic properties. In particular, the directional mechanical and structural characteristics of this material have remained elusive. Here, we investigate these properties by monitoring the propagation of longitudinal and shear phonons following the absorption of a femtosecond pulse along various crystalline directions of a CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> single crystal. We first extract the sound velocities of longitudinal and transverse phonons along these directions of the crystal. Our study then reveals the negative directional thermal expansion of CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>, which is responsible for strong coherent shear phonon generation. Finally, from these observations, we perform elastic characterization of this material, revealing a large directional Poisson’s ratio, which reaches 0.7 and that we associate with the weak mechanical stability of this material. Our results also provide guidelines to fabricate a transducer of high-frequency transverse phonons

    Carrier Recombination Processes in Gallium Indium Phosphide Nanowires

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    Understanding of recombination and photoconductivity dynamics of photogenerated charge carriers in Ga<sub><i>x</i></sub>In<sub>1–x</sub>P NWs is essential for their optoelectronic applications. In this letter, we have studied a series of Ga<sub><i>x</i></sub>In<sub>1–x</sub>P NWs with varied Ga composition. Time-resolved photoinduced luminescence, femtosecond transient absorption, and time-resolved THz transmission measurements were performed to assess radiative and nonradiative recombination and photoconductivity dynamics of photogenerated charges in the NWs. We conclude that radiative recombination dynamics is limited by hole trapping, whereas electrons are highly mobile until they recombine nonradiatively. We also resolve gradual decrease of mobility of photogenerated electrons assigned to electron trapping and detrapping in a distribution of trap states. We identify that the nonradiative recombination of charges is much slower than the decay of the photoluminescence signal. Further, we conclude that trapping of both electrons and holes as well as nonradiative recombination become faster with increasing Ga composition in Ga<sub><i>x</i></sub>In<sub>1–x</sub>P NWs. We have estimated early time electron mobility in Ga<sub><i>x</i></sub>In<sub>1–x</sub>P NWs and found it to be strongly dependent on Ga composition due to the contribution of electrons in the X-valley

    Graphene-to-Substrate Energy Transfer through Out-of-Plane Longitudinal Acoustic Phonons

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    Practically, graphene is often deposited on substrates. Given the major substrate-induced modification of properties and considerable energy transfer at the interface, the graphene–substrate interaction has been widely discussed. However, the proposed mechanisms were restricted to the two-dimensional (2D) plane and interface, while the energy conduction in the third dimension is hardly considered. Herein, we disclose the transfer of energy perpendicular to the interface of the combined system of the 2D graphene and the 3D base. More precisely, our observation of the energy dissipation of optically excited graphene via emitting out-of-plane longitudinal acoustic phonon into the substrate is presented. By applying nanoultrasonic spectroscopy with a piezoelectric nanolayer embedded in the substrate, we found that under photoexcitation by a femtosecond laser pulse graphene can emit longitudinal coherent acoustic phonons (CAPs) with frequencies over 1 THz into the substrate. In addition, the waveform of the CAP pulse infers that the photocarriers and sudden lattice heating in graphene caused modification of graphene–substrate bond and consequently generated longitudinal acoustic phonons in the substrate. The direct observation of this unexplored graphene-to-substrate vertical energy transfer channel can bring new insights into the understanding of the energy dissipation and limited transport properties of supported graphene
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