6 research outputs found

    Highly Conductive Porous Transition Metal Dichalcogenides via Water Steam Etching for High-Performance Lithium–Sulfur Batteries

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    Lithium–sulfur (Li–S) batteries show significant advantages for next-generation energy storage systems owing to their high energy density and cost effectiveness. The main challenge in the development of long-life and high-performance Li–S batteries is to simultaneously facilitate the redox kinetics of sulfur species and suppress the shuttle effect of polysulfides. In this contribution, we present a general and green water-steam-etched approach for the fabrication of H- and O-incorporated porous TiS<sub>2</sub> (HOPT). The conductivity, porosity, chemisorptive capability, and electrocatalytic activity of HOPT are enhanced significantly when compared with those of raw TiS<sub>2</sub>. The synthetic method can be expanded to the fabrication of other highly conductive transition metal dichalcogenides such as porous NbS<sub>2</sub> and CoS<sub>2</sub>. The as-obtained HOPT can serve as both a substitute of conductive agents and an additive of interlayer materials. The optimal electrode delivers discharge capacities of 950 mA h g<sup>–1</sup> after 300 cycles at 0.5 C and 374 mA h g<sup>–1</sup> after 1000 cycles at 10 C. Impressively, an unprecedented reversible capacity of 172 mA h g<sup>–1</sup> is achieved after 2500 cycles at 30 C, and the average capacity fading rate per cycle is as low as 0.015%. Importantly, four half-cells based on this electrode in series could drive 60 light-emitting diode indicator modules (the nominal power 3 W) after 20 s of charging. The instantaneous current and power of this device on reaching 275 A g<sup>–1</sup> and 2611 W g<sup>–1</sup>, respectively, indicate outstanding high-power discharge performance and potential applications in electric vehicles and other large-scale energy storage systems

    [ZnBi<sub>4</sub>]<sup>3–</sup> Pentagon in K<sub>6</sub>ZnBi<sub>5</sub>: Aromatic All-Metal Heterocycle

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    The first aromatic all-metal heterocycle, [ZnBi<sub>4</sub>]<sup>3–</sup>, found in the metallic salt, K<sub>6</sub>ZnBi<sub>5</sub>, has been synthesized and structurally characterized. The exactly planar [ZnBi<sub>4</sub>]<sup>3–</sup> pentagon with six π electrons coupled with multiply bonded Zn–Bi and Bi–Bi bonds, multicentered π-conjugated bonding, and negative nucleus-independent chemical shift values reveals its aromatic character. The metallic nature of K<sub>6</sub>ZnBi<sub>5</sub> has been established by Pauli-type temperature-independent paramagnetism and theoretical analysis of the band structure and total/partial density of states

    Predicting Single-Layer Technetium Dichalcogenides (TcX<sub>2</sub>, X = S, Se) with Promising Applications in Photovoltaics and Photocatalysis

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    One of the least known compounds among transition metal dichalcogenides (TMDCs) is the layered triclinic technetium dichalcogenides (TcX<sub>2</sub>, X = S, Se). In this work, we systematically study the structural, mechanical, electronic, and optical properties of TcS<sub>2</sub> and TcSe<sub>2</sub> monolayers based on density functional theory (DFT). We find that TcS<sub>2</sub> and TcSe<sub>2</sub> can be easily exfoliated in a monolayer form because their formation and cleavage energy are analogous to those of other experimentally realized TMDCs monolayer. By using a hybrid DFT functional, the TcS<sub>2</sub> and TcSe<sub>2</sub> monolayers are calculated to be indirect semiconductors with band gaps of 1.91 and 1.69 eV, respectively. However, bilayer TcS<sub>2</sub> exhibits direct-bandgap character, and both TcS<sub>2</sub> and TcSe<sub>2</sub> monolayers can be tuned from semiconductor to metal under effective tensile/compressive strains. Calculations of visible light absorption indicate that 2D TcS<sub>2</sub> and TcSe<sub>2</sub> generally possess better capability of harvesting sunlight compared to single-layer MoS<sub>2</sub> and ReSe<sub>2</sub>, implying their potential as excellent light-absorbers. Most interestingly, we have discovered that the TcSe<sub>2</sub> monolayer is an excellent photocatalyst for splitting water into hydrogen due to the perfect fit of band edge positions with respect to the water reduction and oxidation potentials. Our predictions expand the two-dimensional (2D) family of TMDCs, and the remarkable electronic/optical properties of monolayer TcS<sub>2</sub> and TcSe<sub>2</sub> will place them among the most promising 2D TMDCs for renewable energy application in the future

    Ultralow Lattice Thermal Transport and Considerable Wave-like Phonon Tunneling in Chalcogenide Perovskite BaZrS<sub>3</sub>

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    Chalcogenide perovskites provide a promising avenue for nontoxic, stable thermoelectric materials. Here, the thermal transport and thermoelectric properties of BaZrS3 as a typical orthorhombic perovskite are investigated. An extremely low lattice thermal conductivity κL of 1.84 W/mK at 300 K is revealed for BaZrS3, due to the softening effect of Ba atoms on the lattice and the strong anharmonicity caused by the twisted structure. We demonstrate that coherence contributions to κL, arising from wave-like phonon tunneling, lead to an 18% thermal transport contribution at 300 K. The increasing temperature softens the phonons, thus reducing the group velocity of materials and increasing the scattering phase space. However, it simultaneously reduces the anharmonicity, which is dominant in BaZrS3 and ultimately improves the particle-like thermal transport. In addition, via replacement of the S atom with Se- and Ti-alloying strategy, the ZT value of BaZrS3 is significantly increased from 0.58 to 0.91 at 500 K, making it an important candidate for thermoelectric applications

    Ultralow Lattice Thermal Transport and Considerable Wave-like Phonon Tunneling in Chalcogenide Perovskite BaZrS<sub>3</sub>

    No full text
    Chalcogenide perovskites provide a promising avenue for nontoxic, stable thermoelectric materials. Here, the thermal transport and thermoelectric properties of BaZrS3 as a typical orthorhombic perovskite are investigated. An extremely low lattice thermal conductivity κL of 1.84 W/mK at 300 K is revealed for BaZrS3, due to the softening effect of Ba atoms on the lattice and the strong anharmonicity caused by the twisted structure. We demonstrate that coherence contributions to κL, arising from wave-like phonon tunneling, lead to an 18% thermal transport contribution at 300 K. The increasing temperature softens the phonons, thus reducing the group velocity of materials and increasing the scattering phase space. However, it simultaneously reduces the anharmonicity, which is dominant in BaZrS3 and ultimately improves the particle-like thermal transport. In addition, via replacement of the S atom with Se- and Ti-alloying strategy, the ZT value of BaZrS3 is significantly increased from 0.58 to 0.91 at 500 K, making it an important candidate for thermoelectric applications

    Novel Excitonic Solar Cells in Phosphorene–TiO<sub>2</sub> Heterostructures with Extraordinary Charge Separation Efficiency

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    Constructing van der Waals heterostructures is an efficient approach to modulate the electronic structure, to advance the charge separation efficiency, and thus to optimize the optoelectronic property. Here, we theoretically investigated the phosphorene interfaced with TiO<sub>2</sub>(110) surface (1L-BP/TiO<sub>2</sub>) with a type-II band alignment, showing enhanced photoactivity. The 1L-BP/TiO<sub>2</sub> excitonic solar cell (XSC) based on the 1L-BP/TiO<sub>2</sub> exhibits large built-in potential and high power conversion efficiency (PCE), dozens of times higher than conventional solar cells, comparable to MoS<sub>2</sub>/WS<sub>2</sub> XSC. The nonadiabatic molecular dynamics simulation shows the ultrafast electron transfer time of 6.1 fs, and slow electron–hole recombination of 0.58 ps, yielding >98% internal quantum efficiency for charge separation, further guaranteeing the practical PCE. Moreover, doping in phosphorene has a tunability on built-in potential, charge transfer, light absorbance, as well as electron dynamics, which greatly helps to optimize the optoelectronic efficiency of a XSC
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