7 research outputs found

    Localized Laser-Based Photohydrothermal Synthesis of Functionalized Metal-Oxides

    Get PDF
    We discuss the rapid in situ hydrothermal synthesis of metal oxide materials based on the photothermal superheating of light-absorbing metal layers for simple and facile on-demand placement of semiconductor materials with micrometer-scale lateral resolution. Localized heating from pulsed and focused laser illumination enables ultrafast growth of metal oxide materials with high spatiotemporal precision in aqueous precursor solution. Among many possible electronic and optoelectronic applications, the proposed method can be used for laser-based in situ real-time soldering of separated metal structures and electrodes with functionalized semiconductor materials. Resistive electrical interconnections of metal strip lines as well as sensitive UV detection using photohydrothermally grown metal oxide bumps are experimentally demonstrated

    Glass Substrate Dust Removal Using 233 fs Laser-Generated Shockwave

    No full text
    Eliminating dust is gaining importance as a critical requirement in the display panel manufacturing process. The pixel resolution of display panels is increasing rapidly, which means that even small dust particles on the order of a few micrometers can affect them. Conventional surface cleaning methods such as ultrasonic cleaning (USC), CO2 cleaning, and wet cleaning may not be sufficiently efficient, economical, or environment friendly. In this study, a laser shockwave cleaning (LSC) method with a 233 fs pulsed laser was developed, which is different from the laser ablation cleaning method. To minimize thermal damage to the glass substrate, the effect of the number of pulses and the gap distance between the focused laser beam and the glass substrate were studied. The optimum number of pulses and gap distance to prevent damage to the glass substrate was inferred as 500 and 20 μm, respectively. With the optimal pulse number and gap distance, cleaning efficiency was tested at a 95% removal ratio regardless of the density of the particles. The effective cleaning area was measured using the removal ratio map and compared with the theoretical value

    Influence of Thermally Activated Solid-State Crystal-to-Crystal Structural Transformation on the Thermoelectric Properties of the Ca<sub>5–<i>x</i></sub>Yb<sub><i>x</i></sub>Al<sub>2</sub>Sb<sub>6</sub> (1.0 ≤ <i>x</i> ≤ 5.0) System

    No full text
    The solid-solution Zintl compounds with the mixed cations of Ca<sup>2+</sup>and Yb<sup>2+</sup> in the Ca<sub>5–<i>x</i></sub>Yb<sub><i>x</i></sub>Al<sub>2</sub>Sb<sub>6</sub> (1.0 ≤ <i>x</i> ≤ 5.0) system have been synthesized by high-temperature solid-state reactions. Two slightly different crystal structures of the Ba<sub>5</sub>Al<sub>2</sub>Bi<sub>6</sub>-type and Ca<sub>5</sub>Ga<sub>2</sub>Sb<sub>6</sub>-type phases have been characterized for seven compounds with 2.5 ≤ <i>x</i> ≤ 5.0 and three compounds with 1.0 ≤ <i>x</i> ≤ 2.0, respectively, by both powder and single-crystal X-ray diffraction analyses. The two title phases adopt the orthorhombic space group <i>Pbam</i> (<i>Z</i> = 2, <i>oP</i>26) with seven independent asymmetric atomic sites and share certain structural similarities, including infinite one-dimensional [Al<sub>2</sub>Sb<sub>8</sub>] double chains and isolated space-filling Ca<sup>2+</sup>/Yb<sup>2+</sup> cations. Interestingly, we reveal the crystal-to-crystal solid-state structural transformation of the Yb-rich compound Ca<sub>1.5</sub>Yb<sub>3.5</sub>Al<sub>2</sub>Sb<sub>6</sub> from the Ba<sub>5</sub>Al<sub>2</sub>Bi<sub>6</sub>-type to the Ca<sub>5</sub>Ga<sub>2</sub>Sb<sub>6</sub>-type phase through the postannealing process, which can be rationalized as the phase transition from the kinetically more stable structure to the thermodynamically more stable crystal structure on the basis of theoretical calculations. Discrepancies of the local coordination geometries of the anionic [Al<sub>2</sub>Sb<sub>8</sub>] units and the geometrical arrangements of structural building moieties in the two distinct phases provoke the different electrical properties of metallic and semiconducting conduction, respectively, for the Ba<sub>5</sub>Al<sub>2</sub>Bi<sub>6</sub>-type and Ca<sub>5</sub>Ga<sub>2</sub>Sb<sub>6</sub>-type phases. Density of states and crystal orbital Hamilton population analyses based on tight-binding linear muffin-tin orbital calculations prove that the band-gap opening in the Ca<sub>5</sub>Ga<sub>2</sub>Sb<sub>6</sub>-type phase should mainly be attributed to an extended bond distance of the bridging Sb–Sb in the [Al<sub>2</sub>Sb<sub>8</sub>] unit. A series of thermoelectric (TE) property measurements indicates that the phase transition via the postannealing process eventually results in an enhancement of the TE performance of Yb-rich Ca<sub>1.5</sub>Yb<sub>3.5</sub>Al<sub>2</sub>Sb<sub>6</sub>

    Enhancing p‑Type Thermoelectric Performances of Polycrystalline SnSe via Tuning Phase Transition Temperature

    No full text
    SnSe emerges as a new class of thermoelectric materials since the recent discovery of an ultrahigh thermoelectric figure of merit in its single crystals. Achieving such performance in the polycrystalline counterpart is still challenging and requires fundamental understandings of its electrical and thermal transport properties as well as structural chemistry. Here we demonstrate a new strategy of improving conversion efficiency of bulk polycrystalline SnSe thermoelectrics. We show that PbSe alloying decreases the transition temperature between <i>Pnma</i> and <i>Cmcm</i> phases and thereby can serve as a means of controlling its onset temperature. Along with 1% Na doping, delicate control of the alloying fraction markedly enhances electrical conductivity by earlier initiation of bipolar conduction while reducing lattice thermal conductivity by alloy and point defect scattering simultaneously. As a result, a remarkably high peak <i>ZT</i> of ∼1.2 at 773 K as well as average <i>ZT</i> of ∼0.5 from RT to 773 K is achieved for Na<sub>0.01</sub>(Sn<sub>1–<i>x</i></sub>Pb<sub><i>x</i></sub>)<sub>0.99</sub>Se. Surprisingly, spherical-aberration corrected scanning transmission electron microscopic studies reveal that Na<sub><i>y</i></sub>Sn<sub>1–<i>x</i></sub>Pb<sub><i>x</i></sub>Se (0 < <i>x</i> ≤ 0.2; <i>y</i> = 0, 0.01) alloys spontaneously form nanoscale particles with a typical size of ∼5–10 nm embedded inside the bulk matrix, rather than solid solutions as previously believed. This unexpected feature results in further reduction in their lattice thermal conductivity
    corecore