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                    Open all abstracts<span class="offscreen-hidden">,&nbsp;in this tab</span></button></p><!--    articleEntryList start--><div class="art-list"><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><div class="eyebrow"><span class="offscreen-hidden">The following article is </span><span class="red">Open access</span></div><a href="/article/10.1149/2.0011508ssl" class="art-list-item-title event_main-link">Room Temperature Photoluminescence Characterization of Low Dose As<sup>+</sup> Implanted Si after Rapid Thermal Annealing</a><p class="small art-list-item-meta">Woo Sik Yoo <em>et al</em> 2015 <em>ECS Solid State Lett.</em> <b>4</b> P51 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.0011508ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Room Temperature Photoluminescence Characterization of Low Dose As+ Implanted Si after Rapid Thermal Annealing</span></a><a href="/article/10.1149/2.0011508ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Room Temperature Photoluminescence Characterization of Low Dose As+ Implanted Si after Rapid Thermal Annealing</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Room Temperature Photoluminescence Characterization of Low Dose As+ Implanted Si after Rapid Thermal Annealing" data-link-purpose-append-open="Room Temperature Photoluminescence Characterization of Low Dose As+ Implanted Si after Rapid Thermal Annealing">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>Arsenic (As<sup>+</sup> 150 keV, 1.0 × 10<sup>13</sup> cm<sup>−2</sup>) implanted p<sup>−</sup>-Si(100) wafers were spike annealed at 1100°C for 1s in a commercially available rapid thermal annealing (RTA) system. Significant variations in sheet resistance were observed while As dopant profiles, measured by secondary ion mass spectroscopy (SIMS), were almost identical. Photoluminescence (PL) spectra were measured from all wafers under three different excitation wavelengths (532, 650 and 827 nm) at room temperature. PL spectra showed large intensity variation, corresponding to the sheet resistance. PL excitation wavelength dependence suggests the variation in density of residual damage as the possible cause of sheet resistance variation.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.0011508ssl">https://doi.org/10.1149/2.0011508ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><a href="/article/10.1149/2.005405ssl" class="art-list-item-title event_main-link">Carbonized Wood for Supercapacitor Electrodes</a><p class="small art-list-item-meta">Shiang Teng <em>et al</em> 2014 <em>ECS Solid State Lett.</em> <b>3</b> M25 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.005405ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Carbonized Wood for Supercapacitor Electrodes</span></a><a href="/article/10.1149/2.005405ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Carbonized Wood for Supercapacitor Electrodes</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Carbonized Wood for Supercapacitor Electrodes" data-link-purpose-append-open="Carbonized Wood for Supercapacitor Electrodes">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>Three-dimensional network structures with interconnected micro-channels were formed through the carbonization of three different varieties of wood. Performance of these carbonized woods was tested for their application as supercapacitor electrodes. From charge-discharge cycling in a KOH electrolyte solution, a maximum energy density of ∼45.6 Wh/kg (discharge current of 200 mA/g) and a maximum power density of ∼2000 W/kg (discharge current of 4000 mA/g) were obtained. The carbonized wood electrodes exhibited excellent cyclability, with 99.7% of the specific capacitance being retained after 2000 cycles. These remarkable results demonstrate the exciting potential for carbonized wood materials as inexpensive, high performance supercapacitor electrodes.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.005405ssl">https://doi.org/10.1149/2.005405ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><div class="eyebrow"><span class="offscreen-hidden">The following article is </span><span class="red">Open access</span></div><a href="/article/10.1149/2.0041504ssl" class="art-list-item-title event_main-link">Hysteresis of Transistor Characteristics of Amorphous IGZO TFTs Studied by Controlling Measurement Speed</a><p class="small art-list-item-meta">Yi-Jung Chen and Ya-Hsiang Tai 2015 <em>ECS Solid State Lett.</em> <b>4</b> Q10 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.0041504ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Hysteresis of Transistor Characteristics of Amorphous IGZO TFTs Studied by Controlling Measurement Speed</span></a><a href="/article/10.1149/2.0041504ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Hysteresis of Transistor Characteristics of Amorphous IGZO TFTs Studied by Controlling Measurement Speed</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Hysteresis of Transistor Characteristics of Amorphous IGZO TFTs Studied by Controlling Measurement Speed" data-link-purpose-append-open="Hysteresis of Transistor Characteristics of Amorphous IGZO TFTs Studied by Controlling Measurement Speed">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>We investigate the hysteresis in the transfer characteristic of amorphous indium-gallium-zinc-oxide thin-film transistor by controlling the sweep waveform of the gate voltage (Vg) provided by parameter measure unit. It is conventionally studied by double sweeping Vg with the default setup of the source measure units, which speed may vary with the current level. By manipulating the step time of sweeping Vg, we found that the response time of charge traps or donor-like states is in the range that overlaps with the conventional time step in the measurement and must be considered.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.0041504ssl">https://doi.org/10.1149/2.0041504ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><div class="eyebrow"><span class="offscreen-hidden">The following article is </span><span class="red">Open access</span></div><a href="/article/10.1149/2.0011512ssl" class="art-list-item-title event_main-link">Effects of Anisotropy and Supporting Configuration on Silicon Wafer Profile Measurements for Pattern Overlay Estimation</a><p class="small art-list-item-meta">Woo Sik Yoo <em>et al</em> 2015 <em>ECS Solid State Lett.</em> <b>4</b> P91 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.0011512ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Effects of Anisotropy and Supporting Configuration on Silicon Wafer Profile Measurements for Pattern Overlay Estimation</span></a><a href="/article/10.1149/2.0011512ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Effects of Anisotropy and Supporting Configuration on Silicon Wafer Profile Measurements for Pattern Overlay Estimation</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Effects of Anisotropy and Supporting Configuration on Silicon Wafer Profile Measurements for Pattern Overlay Estimation" data-link-purpose-append-open="Effects of Anisotropy and Supporting Configuration on Silicon Wafer Profile Measurements for Pattern Overlay Estimation">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>Wafer geometry and residual stress go through significant changes at different points in the semiconductor manufacturing process flow. Precise wafer geometry measurement is very important to assess process induced wafer geometry change (PIWGC) and minimize pattern overlay in lithography steps of advanced node devices and 3-D (3-dimensional) packaged devices. However, the precise wafer geometry measurement is very difficult due to gravitational wafer sag and interaction between the anisotropy of mechanical properties of Si and wafer supporting configurations. Effects of anisotropy and supporting configuration on 300 mm Si (001) wafer profile measurements were investigated for pattern overlay estimation and process optimization.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.0011512ssl">https://doi.org/10.1149/2.0011512ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><a href="/article/10.1149/2.006306ssl" class="art-list-item-title event_main-link">Mechanism of Edge Bonding Void Formation in Hydrophilic Direct Wafer Bonding</a><p class="small art-list-item-meta">A. Castex <em>et al</em> 2013 <em>ECS Solid State Lett.</em> <b>2</b> P47 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.006306ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Mechanism of Edge Bonding Void Formation in Hydrophilic Direct Wafer Bonding</span></a><a href="/article/10.1149/2.006306ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Mechanism of Edge Bonding Void Formation in Hydrophilic Direct Wafer Bonding</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Mechanism of Edge Bonding Void Formation in Hydrophilic Direct Wafer Bonding" data-link-purpose-append-open="Mechanism of Edge Bonding Void Formation in Hydrophilic Direct Wafer Bonding">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>The formation of edge bonding voids during hydrophilic direct wafer bonding is investigated. These defects are linked to the bonding wave propagation and to fluid dynamics between the wafers. Fluid mechanics modeling shows that a gas pressure drop occurs at the wafer edge described by a Joule-Thomson expansion. This adiabatic process results in a gas temperature change which can lead to the condensation of small water droplets close to the wafer edge. Therefore, controlling the gas atmosphere during the bonding process is needed to avoid such bonding defects. Several solutions are proposed to avoid the formation of edge bonding voids.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.006306ssl">https://doi.org/10.1149/2.006306ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><div class="eyebrow"><span class="offscreen-hidden">The following article is </span><span class="red">Open access</span></div><a href="/article/10.1149/2.0031509ssl" class="art-list-item-title event_main-link">Carbon Nanotube Synthesis via the Calciothermic Reduction of Carbon Dioxide with Iron Additives</a><p class="small art-list-item-meta">Tatsuya Kikuchi <em>et al</em> 2015 <em>ECS Solid State Lett.</em> <b>4</b> M19 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.0031509ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Carbon Nanotube Synthesis via the Calciothermic Reduction of Carbon Dioxide with Iron Additives</span></a><a href="/article/10.1149/2.0031509ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Carbon Nanotube Synthesis via the Calciothermic Reduction of Carbon Dioxide with Iron Additives</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Carbon Nanotube Synthesis via the Calciothermic Reduction of Carbon Dioxide with Iron Additives" data-link-purpose-append-open="Carbon Nanotube Synthesis via the Calciothermic Reduction of Carbon Dioxide with Iron Additives">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>The novel fabrication of multi-walled carbon nanotube (MWCNT)/cementite (Fe<sub>3</sub>C) nanocomposites was demonstrated via the calciothermic reduction of carbon dioxide (CO<sub>2</sub>) through electrolysis in molten CaCl<sub>2</sub>/CaO with iron additives at 1173 K. In this technique, CO<sub>2</sub> generated from a graphite anode is reduced to carbon with a metallic calcium reductant formed on a graphite cathode via electrolysis in molten salt. Calciothermic reduction without iron additives resulted in the formation of onion-like carbons (OLCs) with spherical graphite layers and thin graphite sheets. In contrast, MWCNT/Fe<sub>3</sub>C nanocomposites and OLCs were successfully fabricated via calciothermic reduction with iron additives through their catalytic activities.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.0031509ssl">https://doi.org/10.1149/2.0031509ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><div class="eyebrow"><span class="offscreen-hidden">The following article is </span><span class="red">Open access</span></div><a href="/article/10.1149/2.0011504ssl" class="art-list-item-title event_main-link">Effect of Nitrogen Doping on Variability of TaO<sub>x</sub> -RRAM for Low-Power 3-Bit MLC Applications</a><p class="small art-list-item-meta">Saiful Haque Misha <em>et al</em> 2015 <em>ECS Solid State Lett.</em> <b>4</b> P25 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.0011504ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Effect of Nitrogen Doping on Variability of TaOx -RRAM for Low-Power 3-Bit MLC Applications</span></a><a href="/article/10.1149/2.0011504ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Effect of Nitrogen Doping on Variability of TaOx -RRAM for Low-Power 3-Bit MLC Applications</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Effect of Nitrogen Doping on Variability of TaOx -RRAM for Low-Power 3-Bit MLC Applications" data-link-purpose-append-open="Effect of Nitrogen Doping on Variability of TaOx -RRAM for Low-Power 3-Bit MLC Applications">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>The switching uniformity and reliability of the TaO<sub>x</sub> based resistive random access memory (RRAM) device were investigated with varying nitrogen doping concentration. The nitrogen doped samples shows excellent electrical and reliability characteristics such as small switching variability for 3-bit multilevel per cell (MLC), low power operation and good retention properties. Compared with control sample, improved device characteristics of nitrogen doped device can be explained by nitrogen induced filament confinement.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.0011504ssl">https://doi.org/10.1149/2.0011504ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><a href="/article/10.1149/2.004311ssl" class="art-list-item-title event_main-link">Electrochemically Induced p-Type Conductivity in Carbon Nanotubes</a><p class="small art-list-item-meta">Vidhya Chakrapani <em>et al</em> 2013 <em>ECS Solid State Lett.</em> <b>2</b> M57 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.004311ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Electrochemically Induced p-Type Conductivity in Carbon Nanotubes</span></a><a href="/article/10.1149/2.004311ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Electrochemically Induced p-Type Conductivity in Carbon Nanotubes</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Electrochemically Induced p-Type Conductivity in Carbon Nanotubes" data-link-purpose-append-open="Electrochemically Induced p-Type Conductivity in Carbon Nanotubes">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>Vacuum-annealed semiconducting single walled nanotubes are n-type, but become p-type when exposed to ambient air. Here we present evidence that this effect arises from pinning of the Fermi energy by the four-electron oxygen redox couple in an adsorbed water film, a type of surface transfer doping. The pronounced electrical sensitivity to O<sub>2</sub>, O<sub>3</sub>, NO<sub>2</sub>, SO<sub>2</sub>, NH<sub>3</sub> and HNO<sub>3</sub> vapors results from electron exchange between the redox couple and the nanotube. This effect must be considered when using nanotubes for any application in humid air. We also suggest that changes in the electrical properties of graphene and multi-walled nanotubes can be explained by this phenomenon.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.004311ssl">https://doi.org/10.1149/2.004311ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><div class="eyebrow"><span class="offscreen-hidden">The following article is </span><span class="red">Open access</span></div><a href="/article/10.1149/2.0031511ssl" class="art-list-item-title event_main-link">Ferroelectricity in Rare-Earth Modified Hafnia Thin Films Deposited by Sequential Pulsed Laser Deposition</a><p class="small art-list-item-meta">Yogesh Sharma <em>et al</em> 2015 <em>ECS Solid State Lett.</em> <b>4</b> N13 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.0031511ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Ferroelectricity in Rare-Earth Modified Hafnia Thin Films Deposited by Sequential Pulsed Laser Deposition</span></a><a href="/article/10.1149/2.0031511ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Ferroelectricity in Rare-Earth Modified Hafnia Thin Films Deposited by Sequential Pulsed Laser Deposition</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Ferroelectricity in Rare-Earth Modified Hafnia Thin Films Deposited by Sequential Pulsed Laser Deposition" data-link-purpose-append-open="Ferroelectricity in Rare-Earth Modified Hafnia Thin Films Deposited by Sequential Pulsed Laser Deposition">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>Room temperature ferroelectricity in pulsed laser deposited rare-earth doped hafnium oxide (HfO<sub>2</sub>) thin films is discussed. Maximum values of remnant polarizations (P<sub>r</sub>) ∼13.5 and 12 μC/cm<sup>2</sup> along with coercive fields (E<sub>C</sub>) ∼334 and 384 kV/cm are observed in 6 mol. % of rare-earth (Sm or Gd) doped-HfO<sub>2</sub> thin films (Sm:HfO<sub>2</sub> and Gd:HfO<sub>2</sub>), respectively. Piezoresponse force microscopy measurements confirmed ferroelectric nature of films by showing phase hysteresis and butterfly amplitude loops. It is noticed that wake-up cycles improved the remnant polarization and found to be necessary for the forming of well saturated hysteresis loops. Our results showed potential toward realization of future highly scaled non-volatile ferroelectric memories.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.0031511ssl">https://doi.org/10.1149/2.0031511ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><div class="eyebrow"><span class="offscreen-hidden">The following article is </span><span class="red">Open access</span></div><a href="/article/10.1149/2.0021506ssl" class="art-list-item-title event_main-link">Preparation of Ultrathin Germanium on Insulator Films Using a Wet Etching Process</a><p class="small art-list-item-meta">Chuanchuan Sun <em>et al</em> 2015 <em>ECS Solid State Lett.</em> <b>4</b> P43 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.0021506ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Preparation of Ultrathin Germanium on Insulator Films Using a Wet Etching Process</span></a><a href="/article/10.1149/2.0021506ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Preparation of Ultrathin Germanium on Insulator Films Using a Wet Etching Process</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Preparation of Ultrathin Germanium on Insulator Films Using a Wet Etching Process" data-link-purpose-append-open="Preparation of Ultrathin Germanium on Insulator Films Using a Wet Etching Process">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>We demonstrate a wet etching method to reduce the thickness of thin germanium-on-insulator (GOI) films using a dilute solution (a NH<sub>4</sub>OH:H<sub>2</sub>O<sub>2</sub>:H<sub>2</sub>O 2:1:4000 mixture) at a low temperature (5°C). The etch rate and thickness uniformity were well controlled. The root mean square roughness after wet etching was less than 0.5 nm and did not degrade compared with the original sample. Finally, back gate junctionless transistors were fabricated using the GOI wafers with 15-nm-thick Ge films, thinned by the developed method. The transistors had good I<sub>on</sub>/I<sub>off</sub> ratio and mobility qualities, indicating that the wet etching process effectively thinned the Ge films.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.0021506ssl">https://doi.org/10.1149/2.0021506ssl</a></div></div></div></div></div><!--    articleEntryList end--></div></div></div><!-- End Most read tabpanel --><!-- Start Latest tabpanel --><!-- End Latest tabpanel --><!-- Express Letters tabpanel --><!-- Express Letters tabpanel --><!-- Start Review tabpanel --><!-- End Review tabpanel --><!-- Start Featured tabpanel --><!-- End Featured tabpanel --><!-- Start Editor's chocie tabpanel --><!-- End Editor's chocie tabpanel --><!-- Start AM tabpanel --><!-- End AM tabpanel --><!-- Start Trending tabpanel --><div tabindex="0"
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                    Open all abstracts<span class="offscreen-hidden">,&nbsp;in this tab</span></button></p><!--    articleEntryList start--><div class="art-list"><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><a href="/article/10.1149/2.008201ssl" class="art-list-item-title event_main-link">Metal-Semiconductor Field-Effect Transistor Made Using Amorphous In-Ga-Zn-O Channel and Bottom Pt Schottky Contact Structure at 200°C</a><p class="small art-list-item-meta">Dong Hee Lee <em>et al</em> 2012 <em>ECS Solid State Lett.</em> <b>1</b> Q8 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.008201ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Metal-Semiconductor Field-Effect Transistor Made Using Amorphous In-Ga-Zn-O Channel and Bottom Pt Schottky Contact Structure at 200°C</span></a><a href="/article/10.1149/2.008201ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Metal-Semiconductor Field-Effect Transistor Made Using Amorphous In-Ga-Zn-O Channel and Bottom Pt Schottky Contact Structure at 200°C</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Metal-Semiconductor Field-Effect Transistor Made Using Amorphous In-Ga-Zn-O Channel and Bottom Pt Schottky Contact Structure at 200°C" data-link-purpose-append-open="Metal-Semiconductor Field-Effect Transistor Made Using Amorphous In-Ga-Zn-O Channel and Bottom Pt Schottky Contact Structure at 200°C">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>Amorphous In-Ga-Zn-O (a-IGZO) based metal-semiconductor field-effect transistors (MESFETs) were fabricated at 200°C. A bottom Pt structure was employed to form a good Schottky gate, and channel thickness was optimized to 230 nm to obtain high on-currents <i>I<sub>on</sub></i> &gt; 10<sup>−6</sup> A, on-to-off current ratios &gt; 10<sup>6</sup> and low subthreshold voltage swing of 129 mV/decade. The field-effect mobility (<i>μ<sub>FE</sub></i>) was as small as 0.5 cm<sup>2</sup>(Vs)<sup>−1</sup>, which is explained quantitatively by the subgap trap density in the 200°C-annealed a-IGZO. The present result suggests that a double-layered channel with different donor densities will be effective to improve <i>I<sub>on</sub></i> and <i>μ<sub>FE</sub></i> of a-IGZO MESFETs.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.008201ssl">https://doi.org/10.1149/2.008201ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><a href="/article/10.1149/2.013206ssl" class="art-list-item-title event_main-link">Fabrication and Characterization of Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> Thin Films for Lithium Ion Battery</a><p class="small art-list-item-meta">Jiajia Tan and Ashutosh Tiwari 2012 <em>ECS Solid State Lett.</em> <b>1</b> Q57 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.013206ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Fabrication and Characterization of Li7La3Zr2O12 Thin Films for Lithium Ion Battery</span></a><a href="/article/10.1149/2.013206ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Fabrication and Characterization of Li7La3Zr2O12 Thin Films for Lithium Ion Battery</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Fabrication and Characterization of Li7La3Zr2O12 Thin Films for Lithium Ion Battery" data-link-purpose-append-open="Fabrication and Characterization of Li7La3Zr2O12 Thin Films for Lithium Ion Battery">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>Thin films of Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> were deposited on SrTiO<sub>3</sub> (100) and Sapphire (0001) substrates at room-temperature using a pulsed-laser-deposition technique. Detailed structural, compositional, optical, and electrochemical characterizations of the films were performed. The films deposited at room-temperature had amorphous structure, and exhibited a lithium-ion conductivity of 3.35 × 10<sup>−7</sup> S/cm. The effects of thermal annealing and pulsed laser annealing on the properties of the films were investigated. Pulsed laser annealed films were found to have a superior lithium-ion conductivity value of 7.36 × 10<sup>−7</sup> S/cm. Moreover, the Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> films were found to be electrochemically stable against lithium metal.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.013206ssl">https://doi.org/10.1149/2.013206ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><a href="/article/10.1149/2.011404ssl" class="art-list-item-title event_main-link">Effect of Electron Mobility of the Electron Transport Layer on Fluorescent Organic Light-Emitting Diodes</a><p class="small art-list-item-meta">Sang Ho Rhee <em>et al</em> 2014 <em>ECS Solid State Lett.</em> <b>3</b> R19 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.011404ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Effect of Electron Mobility of the Electron Transport Layer on Fluorescent Organic Light-Emitting Diodes</span></a><a href="/article/10.1149/2.011404ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Effect of Electron Mobility of the Electron Transport Layer on Fluorescent Organic Light-Emitting Diodes</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Effect of Electron Mobility of the Electron Transport Layer on Fluorescent Organic Light-Emitting Diodes" data-link-purpose-append-open="Effect of Electron Mobility of the Electron Transport Layer on Fluorescent Organic Light-Emitting Diodes">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>The charge balance mechanism in green fluorescent organic light-emitting diodes is investigated for different electron transport layers (ETLs) and electron mobilities. Carrier accumulation and an increase in the exciton recombination probability are shown to be critical for improving the current and power efficiencies by aligning the bands at the interface between the emitting layer (EML) and ETL. The peak in the electroluminescence (EL) spectra was found to shift slightly in response to changes in the width of the emission zone and reflected the electron mobility of the ETL. Higher electron mobility resulted in a wider recombination zone in the EML that was manifested by a blue-shift of the EL peak.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.011404ssl">https://doi.org/10.1149/2.011404ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><a href="/article/10.1149/2.0081512ssl" class="art-list-item-title event_main-link">Advantage of Ti-Doped Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> Material for Phase Change Memory Applications</a><p class="small art-list-item-meta">Liangliang Cao <em>et al</em> 2015 <em>ECS Solid State Lett.</em> <b>4</b> P102 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.0081512ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Advantage of Ti-Doped Ge2Sb2Te5 Material for Phase Change Memory Applications</span></a><a href="/article/10.1149/2.0081512ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Advantage of Ti-Doped Ge2Sb2Te5 Material for Phase Change Memory Applications</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Advantage of Ti-Doped Ge2Sb2Te5 Material for Phase Change Memory Applications" data-link-purpose-append-open="Advantage of Ti-Doped Ge2Sb2Te5 Material for Phase Change Memory Applications">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>Ti-doped Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> (GSTT) materials have been investigated for phase change memory (PCM) applications. Compared with GST, GSTT5.67% phase change material has a higher crystallization temperature (∼230°C), a higher crystallization activation energy (2.79 eV) and a better data retention ability (∼134°C for 10-year). The PCM cell based on GSTT5.67% exhibits lower power consumption than GST based one. Endurance up to 1 × 10<sup>4</sup> cycles with high/low resistance ratio of over one order of magnitude has been achieved.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.0081512ssl">https://doi.org/10.1149/2.0081512ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><a href="/article/10.1149/2.0051408ssl" class="art-list-item-title event_main-link">Homo-Junction pn Diode Using p-Type SnO and n-Type SnO<sub>2</sub> Thin Films</a><p class="small art-list-item-meta">Joseph Um and Sarah Eunkyung Kim 2014 <em>ECS Solid State Lett.</em> <b>3</b> P94 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.0051408ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Homo-Junction pn Diode Using p-Type SnO and n-Type SnO2 Thin Films</span></a><a href="/article/10.1149/2.0051408ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Homo-Junction pn Diode Using p-Type SnO and n-Type SnO2 Thin Films</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Homo-Junction pn Diode Using p-Type SnO and n-Type SnO2 Thin Films" data-link-purpose-append-open="Homo-Junction pn Diode Using p-Type SnO and n-Type SnO2 Thin Films">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>Tin oxide thin films are of great interest for device applications, but in spite of their good optical transparency and outstanding semiconductor properties, stable p-type tin oxide needs to be developed. In this study both p-type SnO and n-type SnO<sub>2</sub> thin films were deposited by reactive rf magnetron sputtering using Sn target in Ar and O<sub>2</sub> gas mixture. The structural, electrical, and optical properties of both p-type SnO and n-type SnO<sub>2</sub> thin films were analysed. The transparent homo-junction pn diode was also fabricated and it showed a fairly good rectification behavior with a turn-on voltage of 2.3 V.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.0051408ssl">https://doi.org/10.1149/2.0051408ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><a href="/article/10.1149/2.003205ssl" class="art-list-item-title event_main-link">Improvement of Mobility in ZnO Thin Film Transistor with an Oxygen Enriched MgO Gate Dielectric</a><p class="small art-list-item-meta">Wei-Yu Chen <em>et al</em> 2012 <em>ECS Solid State Lett.</em> <b>1</b> N17 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.003205ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Improvement of Mobility in ZnO Thin Film Transistor with an Oxygen Enriched MgO Gate Dielectric</span></a><a href="/article/10.1149/2.003205ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Improvement of Mobility in ZnO Thin Film Transistor with an Oxygen Enriched MgO Gate Dielectric</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Improvement of Mobility in ZnO Thin Film Transistor with an Oxygen Enriched MgO Gate Dielectric" data-link-purpose-append-open="Improvement of Mobility in ZnO Thin Film Transistor with an Oxygen Enriched MgO Gate Dielectric">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>The performance of bottom-gate ZnO thin film transistors (TFTs) using MgO gate dielectrics evaporated with and without introducing oxygen have been investigated. The oxygen introduced during MgO deposition improves the field-effect mobility significantly as compared to the device without introducing oxygen during MgO deposition. The oxygen-introduced MgO exhibits a dielectric constant of 10.9 and the field-effect mobility of the TFT device is enhanced to 78.3 cm<sup>2</sup>/V s. The threshold voltages can also be related to whether the oxygen is introduced into MgO or not. The interface between oxygen-introduced MgO and ZnO is examined and its connection with mobility enhancement is discussed.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.003205ssl">https://doi.org/10.1149/2.003205ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><a href="/article/10.1149/2.001310ssl" class="art-list-item-title event_main-link">Effect of Ge Concentration in Ge<i><sub>x</sub></i>Se<sub>1−<i>x</i></sub> Chalcogenide Glass on the Electronic Structures and the Characteristics of Ovonic Threshold Switching (OTS) Devices</a><p class="small art-list-item-meta">Su-Dong Kim <em>et al</em> 2013 <em>ECS Solid State Lett.</em> <b>2</b> Q75 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.001310ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Effect of Ge Concentration in GexSe1−x Chalcogenide Glass on the Electronic Structures and the Characteristics of Ovonic Threshold Switching (OTS) Devices</span></a><a href="/article/10.1149/2.001310ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Effect of Ge Concentration in GexSe1−x Chalcogenide Glass on the Electronic Structures and the Characteristics of Ovonic Threshold Switching (OTS) Devices</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Effect of Ge Concentration in GexSe1−x Chalcogenide Glass on the Electronic Structures and the Characteristics of Ovonic Threshold Switching (OTS) Devices" data-link-purpose-append-open="Effect of Ge Concentration in GexSe1−x Chalcogenide Glass on the Electronic Structures and the Characteristics of Ovonic Threshold Switching (OTS) Devices">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>We studied Ge<i><sub>x</sub></i>Se<sub>1−<i>x</i></sub> for the potential application in the Ovonic Threshold Switching (OTS) device. We found that, as Ge concentration increased, the thermal stability was deteriorated while the device performances were improved. In addition, using Spectroscopic Ellipsometry (SE) technique, the energy gap (<i>E</i><sub>g</sub>) and the Urbach energy (<i>E</i><sub>U</sub>) were found to show non-monotonic dependences, with their minimum of about 1.0 eV of <i>E</i><sub>g</sub> for Ge<sub>0.6</sub>Se<sub>0.4</sub> and 40 meV of <i>E</i><sub>U</sub> for Ge<sub>0.5</sub>Se<sub>0.5</sub>. These changes are consistent with the changes in device characteristics, which might be explained in terms of the change in the number of Se-Se bondings.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.001310ssl">https://doi.org/10.1149/2.001310ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><a href="/article/10.1149/2.007306ssl" class="art-list-item-title event_main-link">Facile Hydrothermal Synthesis of Sb<sub>2</sub>S<sub>3</sub> Nanorods and Their Magnetic and Electrochemical Properties</a><p class="small art-list-item-meta">Kang Xiao <em>et al</em> 2013 <em>ECS Solid State Lett.</em> <b>2</b> P51 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.007306ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Facile Hydrothermal Synthesis of Sb2S3 Nanorods and Their Magnetic and Electrochemical Properties</span></a><a href="/article/10.1149/2.007306ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Facile Hydrothermal Synthesis of Sb2S3 Nanorods and Their Magnetic and Electrochemical Properties</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Facile Hydrothermal Synthesis of Sb2S3 Nanorods and Their Magnetic and Electrochemical Properties" data-link-purpose-append-open="Facile Hydrothermal Synthesis of Sb2S3 Nanorods and Their Magnetic and Electrochemical Properties">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>Single crystalline Sb<sub>2</sub>S<sub>3</sub> nanorods were fabricated through a soft chemical route without the assistance of any templates or surfactants. The as-prepared samples were characterized by powder X-ray diffraction (XRD), scanning electron microscopy (SEM), energy dispersive X-ray spectrometry (EDS), transmission electron microscopy (TEM), and X-ray photoelectron spectroscopy (XPS). TEM results indicate the Sb<sub>2</sub>S<sub>3</sub> nanorods grow along with [001] direction and were composed of orthorhombic structure. The magnetic properties of Sb<sub>2</sub>S<sub>3</sub> nanorods were studied. In addition, Sb<sub>2</sub>S<sub>3</sub> nanorods were evaluated as electrode materials in lithium secondary batteries, and the first discharge capacity reached about 850 mA h g<sup>−1</sup>.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.007306ssl">https://doi.org/10.1149/2.007306ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><a href="/article/10.1149/2.006306ssl" class="art-list-item-title event_main-link">Mechanism of Edge Bonding Void Formation in Hydrophilic Direct Wafer Bonding</a><p class="small art-list-item-meta">A. Castex <em>et al</em> 2013 <em>ECS Solid State Lett.</em> <b>2</b> P47 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.006306ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Mechanism of Edge Bonding Void Formation in Hydrophilic Direct Wafer Bonding</span></a><a href="/article/10.1149/2.006306ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Mechanism of Edge Bonding Void Formation in Hydrophilic Direct Wafer Bonding</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Mechanism of Edge Bonding Void Formation in Hydrophilic Direct Wafer Bonding" data-link-purpose-append-open="Mechanism of Edge Bonding Void Formation in Hydrophilic Direct Wafer Bonding">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>The formation of edge bonding voids during hydrophilic direct wafer bonding is investigated. These defects are linked to the bonding wave propagation and to fluid dynamics between the wafers. Fluid mechanics modeling shows that a gas pressure drop occurs at the wafer edge described by a Joule-Thomson expansion. This adiabatic process results in a gas temperature change which can lead to the condensation of small water droplets close to the wafer edge. Therefore, controlling the gas atmosphere during the bonding process is needed to avoid such bonding defects. Several solutions are proposed to avoid the formation of edge bonding voids.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.006306ssl">https://doi.org/10.1149/2.006306ssl</a></div></div></div></div><div class="art-list-item reveal-container reveal-closed"><div class="art-list-item-body"><a href="/article/10.1149/2.004311ssl" class="art-list-item-title event_main-link">Electrochemically Induced p-Type Conductivity in Carbon Nanotubes</a><p class="small art-list-item-meta">Vidhya Chakrapani <em>et al</em> 2013 <em>ECS Solid State Lett.</em> <b>2</b> M57 </p><div class="art-list-item-tools small wd-abstr-upper"><a href="/article/10.1149/2.004311ssl/meta" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="View article"><span class="icon-article"></span>View article<span class="offscreen-hidden">,&nbsp;Electrochemically Induced p-Type Conductivity in Carbon Nanotubes</span></a><a href="/article/10.1149/2.004311ssl/pdf" class="mr-2 mb-0 nowrap event_mini-link" data-event-action="PDF"><span class="icon-file-pdf"></span>PDF<span class="offscreen-hidden">,&nbsp;Electrochemically Induced p-Type Conductivity in Carbon Nanotubes</span></a><button type="button" class="reveal-trigger mr-2 nowrap"><svg aria-hidden="true" class="fa-icon fa-icon--left fa-icon--flip" role="img" focusable="false" xmlns="http://www.w3.org/2000/svg" viewBox="0 0 320 512"><!--caret-down--><!--!Font Awesome Free 6.5.1 by @fontawesome - https://fontawesome.com License - https://fontawesome.com/license/free Copyright 2024 Fonticons, Inc.--><path d="M137.4 374.6c12.5 12.5 32.8 12.5 45.3 0l128-128c9.2-9.2 11.9-22.9 6.9-34.9s-16.6-19.8-29.6-19.8L32 192c-12.9 0-24.6 7.8-29.6 19.8s-2.2 25.7 6.9 34.9l128 128z"/></svg><span class="reveal-trigger-label" data-reveal-text="Open abstract" data-reveal-label-alt="Close abstract" data-link-purpose-append="Electrochemically Induced p-Type Conductivity in Carbon Nanotubes" data-link-purpose-append-open="Electrochemically Induced p-Type Conductivity in Carbon Nanotubes">Open abstract</span></button></div><div class="reveal-content"><div class="article-text view-text-small"><p>Vacuum-annealed semiconducting single walled nanotubes are n-type, but become p-type when exposed to ambient air. Here we present evidence that this effect arises from pinning of the Fermi energy by the four-electron oxygen redox couple in an adsorbed water film, a type of surface transfer doping. The pronounced electrical sensitivity to O<sub>2</sub>, O<sub>3</sub>, NO<sub>2</sub>, SO<sub>2</sub>, NH<sub>3</sub> and HNO<sub>3</sub> vapors results from electron exchange between the redox couple and the nanotube. This effect must be considered when using nanotubes for any application in humid air. We also suggest that changes in the electrical properties of graphene and multi-walled nanotubes can be explained by this phenomenon.</p></div><div class="art-list-item-tools small wd-abstr-lower"><a class="mr-2" href="https://doi.org/10.1149/2.004311ssl">https://doi.org/10.1149/2.004311ssl</a></div></div></div></div></div><!--    articleEntryList end--></div></div></div><!-- End Featured tabpanel --></div><!-- End Article listing tabs --><!--  Start of google banners in the middle.  --><section aria-label="Main column advert"><div class="ad-iframe-wrap"><div id='div-gpt-ad-1562594774007-0' style='width: 728px; height: 90px; display: block;'><script>
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                ECS Transactions
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                The Electrochemical Society Interface
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                ECS Electrochemistry Letters
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            <a class="partners-list__link" href="/journal/2162-8750">
                ECS Solid State Letters
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            <a class="partners-list__link" href="/journal/1944-8775">
                Electrochemical and Solid State Letters
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                ECS Proceedings Volumes
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                    ECS Solid State Letters
                    <br/>doi: 10.1149/issn.2162-8750<br/>Online ISSN: 2162-8750<br/></li></ul><br/></div><!-- End Journal history --><!-- End Journal Sidebar --></div></div></main></div><!-- End two column layout --></div><div data-scroll-header="" class="data-header-anchor" id="exp"></div><footer class="footer content-grid__full-width" data-footer-content role="contentinfo"><nav aria-label="Further resources" class="footer__grid"><div><h2 class="footer__heading">IOPscience</h2><ul class="footer__list"><li class="footer__item"><a class="link--colour--white" href="/journalList">Journals</a></li><li class="footer__item"><a class="link--colour--white" href="/booklistinfo/home">Books</a></li><li class="footer__item"><a class="link--colour--white" href="/conference-series">IOP Conference Series</a></li><li class="footer__item"><a class="link--colour--white" href="/page/aboutiopscience">About IOPscience</a></li><li class="footer__item"><a class="link--colour--white" href="https://ioppublishing.org/about-us/contact-us/">Contact Us</a></li><li class="footer__item"><a class="link--colour--white" href="/info/page/developing-countries-access">Developing countries access</a></li><li class="footer__item"><a class="link--colour--white" href="https://publishingsupport.iopscience.iop.org/open_access/">IOP Publishing open access policy</a></li><li class="footer__item"><a class="link--colour--white" href="/page/accessibility">Accessibility</a></li></ul></div><div><h2 class="footer__heading">IOP Publishing</h2><ul class="footer__list"><li class="footer__item"><a class="link--colour--white" href="https://ioppublishing.org/legal/copyright/">Copyright 2024 IOP Publishing</a></li><li class="footer__item"><a class="link--colour--white" href="/page/terms">Terms and Conditions</a></li><li class="footer__item"><a class="link--colour--white" href="/page/disclaimer">Disclaimer</a></li><li class="footer__item"><a class="link--colour--white" href="https://ioppublishing.org/legal/privacy-cookies-policy/">Privacy and Cookie Policy</a></li><li class="footer__item"><a class="link--colour--white" href="https://ioppublishing.org/legal/textanddataminingpolicy/">Text and Data mining policy</a></li></ul><h2 class="footer__heading">Publishing Support</h2><ul class="footer__list"><li class="footer__item"><a class="link--colour--white" href="https://publishingsupport.iopscience.iop.org/" data-ga-event="footer-pub-support-link">Authors</a></li><li class="footer__item"><a class="link--colour--white" href="https://publishingsupport.iopscience.iop.org/publishing-support/reviewers/" data-ga-event="footer-pub-support-link">Reviewers</a></li><li class="footer__item"><a class="link--colour--white" href="https://publishingsupport.iopscience.iop.org/publishing-support/organisers/" data-ga-event="footer-pub-support-link">Conference Organisers</a></li></ul></div><div><h2 class="footer__heading">About IOP Publishing</h2><span>
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