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Feature Papers in Refractories and Ceramics: Microstructure, Properties and Applications, Volume II

A special issue of Materials (ISSN 1996-1944). This special issue belongs to the section "Advanced and Functional Ceramics and Glasses".

Deadline for manuscript submissions: closed (10 June 2024) | Viewed by 8977

Special Issue Editors


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Guest Editor
The State Key Laboratory of Refractories and Metallurgy, Wuhan University of Science & Technology, Wuhan, China
Interests: functional refractory; refractory castable; powder technology; porous ceramic; nanomaterials
Special Issues, Collections and Topics in MDPI journals
School of Materials Science and Engineering, University of Science and Technology Beijing, Beijing, China
Interests: refractory; structure ceramics; nanomaterials; high-temperature ceramic; powder technology
Special Issues, Collections and Topics in MDPI journals

Special Issue Information

Dear Colleagues,

Refractories, as a class of ceramics with high fusion points, are basic materials in high-temperature industries such as metallurgy, cement/glass production and thermal power. Today, “new refractory” is being developed to not only meet the high-temperature support of fine structure precise regulation but also to be designed or tailored to special functional requirements, such as the purification of liquid steel, energy conservation, low carbon emissions and pollution reduction. In terms of eco-friendliness, long life and safety, the overall performance (e.g., mechanical strength, thermal/chemical stability, corrosion/oxidation/thermal shock resistances, workability) of “new refractory” can be greatly improved with the development of new material systems, precise control of microstructures and use of intelligent manufacturing technology.

The “new refractory” is extending the frontiers of design and preparation of traditional high-temperature ceramics and allows significant improvements in high-temperature industries on economic and environmental impacts. In addition, the “structure–function” relationship of these ceramics as related to their high-temperature service performance should be known for every application.

This Special Issue focuses on the development of new refractories and novel ceramics. The potential topics concerning their microstructure, properties and applications include but are not limited to:

  • Functional refractory;
  • Novel ceramics;
  • Non-oxide ceramics;
  • High-temperature heat-insulating materials;
  • Green ecological refractory;
  • Refractory castable;
  • Refractory raw materials;
  • High-temperature behavior;
  • Refractory and inclusions.

Dr. Zhong Huang
Dr. Bin Li
Guest Editors

Manuscript Submission Information

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Submitted manuscripts should not have been published previously, nor be under consideration for publication elsewhere (except conference proceedings papers). All manuscripts are thoroughly refereed through a single-blind peer-review process. A guide for authors and other relevant information for submission of manuscripts is available on the Instructions for Authors page. Materials is an international peer-reviewed open access semimonthly journal published by MDPI.

Please visit the Instructions for Authors page before submitting a manuscript. The Article Processing Charge (APC) for publication in this open access journal is 2600 CHF (Swiss Francs). Submitted papers should be well formatted and use good English. Authors may use MDPI's English editing service prior to publication or during author revisions.

Keywords

  • refractory
  • ceramic
  • non-oxide
  • castable
  • green refractory
  • raw material
  • microstucture
  • high-temperature process and behavior.

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Published Papers (10 papers)

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12 pages, 2073 KiB  
Article
Preparation and Properties of Lightweight Aggregates from Discarded Al2O3-ZrO2-C Refractories
by Shuli Sun, Junfeng Qu, Mengyong Sun, Xinming Ren, Cheng Gong, Xin Mu, Wenyu Zan, Zhangyan Zhou, Chengji Deng and Beiyue Ma
Materials 2024, 17(16), 3968; https://doi.org/10.3390/ma17163968 - 9 Aug 2024
Viewed by 575
Abstract
Refractory materials are an important pillar for the stable development of the high-temperature industry. A large amount of waste refractories needs to be further disposed of every year, so it is of great significance to carry out research on the recycling of used [...] Read more.
Refractory materials are an important pillar for the stable development of the high-temperature industry. A large amount of waste refractories needs to be further disposed of every year, so it is of great significance to carry out research on the recycling of used refractories. In this work, lightweight composite aggregate was prepared by using discarded Al2O3-ZrO2-C refractories as the main raw material, and the performance of the prepared lightweight aggregate was improved by adjusting the calcination temperature and introducing light calcined magnesia additives. The results showed that the cold compressive strength and thermal shock resistance of the lightweight aggregates were significantly improved with increasing calcination temperature. Moreover, the introduction of light calcined magnesia can effectively improve the apparent porosity, cold compressive strength, and thermal shock resistance of the prepared lightweight aggregates at the calcination temperature of 1400 °C. Consequently, this work provides a useful reference for the resource utilization of used refractories, while the prepared lightweight aggregates are expected to be applied in the field of high-temperature insulation. Full article
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<p>XRD patterns of the sample with 40% of magnesia additive after calcining at 1200, 1300, and 1400 °C for 1 h.</p>
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<p>SEM images of the sample with 40% of magnesia additive after calcining at 1200 °C (<b>a</b>), 1300 °C (<b>b</b>), and 1400 °C (<b>c</b>) for 1 h.</p>
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<p>(<b>a</b>) Linear shrinkage, (<b>b</b>) apparent porosity, and (<b>c</b>) bulk density of the samples with 40% of magnesia additive after calcining at 1200 °C, 1300 °C, and 1400 °C for 1 h.</p>
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<p>Cold compressive strength and thermal shock resistance of the samples with 40% of magnesia additive after calcining at 1200 °C, 1300 °C, and 1400 °C for 1 h.</p>
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<p>XRD patterns of the samples with different amounts of light calcined magnesia after calcining at 1400 °C for 1 h.</p>
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<p>SEM images of the samples with different amounts of light calcined magnesia after cal-cining at 1400 °C for 1 h. (<b>a</b>) 0%; (<b>b</b>) 30%; (<b>c</b>) 40%; (<b>d</b>) 50%.</p>
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<p>(<b>a</b>) Linear shrinkage, (<b>b</b>) apparent porosity, and (<b>c</b>) bulk density of the samples of the samples with different amounts of light calcined magnesia after calcining at 1400 °C for 1 h.</p>
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<p>Cold compressive strength and thermal shock resistance of the samples with different amounts of light calcined magnesia after calcining at 1400 °C for 1 h.</p>
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<p>Relationship between Δ<span class="html-italic">G</span><sup>θ</sup> and temperature for related reactions.</p>
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<p>Different crystal forms of ZrO<sub>2</sub>.</p>
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11 pages, 3882 KiB  
Article
Mullite-Fibers-Reinforced Bagasse Cellulose Aerogels with Excellent Mechanical, Flame Retardant, and Thermal Insulation Properties
by Shuang Wang, Miao Sun, Junyi Lv, Jianming Gu, Qing Xu, Yage Li, Xin Zhang, Hongjuan Duan and Shaoping Li
Materials 2024, 17(15), 3737; https://doi.org/10.3390/ma17153737 - 28 Jul 2024
Viewed by 545
Abstract
Cellulose aerogels are considered as ideal thermal insulation materials owing to their excellent properties such as a low density, high porosity, and low thermal conductivity. However, they still suffer from poor mechanical properties and low flame retardancy. In this study, mullite-fibers-reinforced bagasse cellulose [...] Read more.
Cellulose aerogels are considered as ideal thermal insulation materials owing to their excellent properties such as a low density, high porosity, and low thermal conductivity. However, they still suffer from poor mechanical properties and low flame retardancy. In this study, mullite-fibers-reinforced bagasse cellulose (Mubce) aerogels are designed using bagasse cellulose as the raw material, mullite fibers as the reinforcing agent, glutaraldehyde as the cross-linking agent, and chitosan as the additive. The resulted Mubce aerogels exhibit a low density of 0.085 g/cm3, a high porosity of 93.2%, a low thermal conductivity of 0.0276 W/(m∙K), superior mechanical performances, and an enhanced flame retardancy. The present work offers a novel and straightforward strategy for creating high-performance aerogels, aiming to broaden the application of cellulose aerogels in thermal insulation. Full article
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Graphical abstract

Graphical abstract
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<p>(<b>a</b>) SEM image of raw MF. (<b>b</b>) Schematic illustration of the fabrication process of Mubce aerogels. (<b>c</b>) SEM image of as-prepared Mubce-150 aerogels (MF are encapsulated within the BCE, as marked by the yellow arrow, while others are nestled between layers of BCE, as pointed out by the blue arrow). The optical image of (<b>d</b>) Mubce-150 aerogels with different shapes and (<b>e</b>) the photo of the aerogel standing on a petal. And (<b>f</b>) pore size distribution curve of Mubce aerogels obtained by mercury intrusion porosimetry.</p>
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<p>(<b>a</b>) FTIR spectra of MF, BCE aerogels, and Mubce-150 aerogels; C 1s survey spectra of (<b>b</b>) BCE and (<b>c</b>) Mubce-150 aerogels. N 1s survey spectra of (<b>d</b>) BCE and (<b>e</b>) Mubce-150 aerogels; (<b>f</b>) XRD pattern of BCE and Mubce-150 aerogels; SEM images of (<b>g</b>) BCE aerogels, (<b>h</b>) Mubce-50 aerogels, (<b>i</b>) Mubce-100 aerogels, (<b>j</b>) Mubce-150 aerogels, and (<b>k</b>) Mubce-200 aerogels. And (<b>l</b>) schematic diagram of enhanced mechanical properties of BCE aerogels.</p>
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<p>(<b>a</b>) Stress–strain curves of BCE and Mubce aerogels. (<b>b</b>) The corresponding compressive strength and density. (<b>c</b>) Photographs of Mubce-150 aerogel withstanding 1561 times its own weight. (<b>d</b>) Stress–strain curves of Mubce-150 aerogels at different compressive strains. Fatigue test of (<b>e</b>) Mubce-150 aerogels and (<b>f</b>) BCE aerogels under 40% compressive strain.</p>
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<p>(<b>a</b>) Thermal conductivity of Mubce-150 aerogels at different temperatures. (<b>b</b>) Comparison of the volume density and thermal conductivity of Mubce aerogels with other reported aerogels [<a href="#B24-materials-17-03737" class="html-bibr">24</a>,<a href="#B31-materials-17-03737" class="html-bibr">31</a>,<a href="#B32-materials-17-03737" class="html-bibr">32</a>,<a href="#B33-materials-17-03737" class="html-bibr">33</a>,<a href="#B34-materials-17-03737" class="html-bibr">34</a>,<a href="#B35-materials-17-03737" class="html-bibr">35</a>]. (<b>c</b>) Temperature variation curve of the upper surface of the samples heated at 160 °C for 60 min and infrared images of the samples at different heating times on a heating stage. Optical photographs of (<b>d</b>) BCE and (<b>e</b>) Mubce-150 aerogels heated by butane torch flame (aerogel specimen sizes are 90 × 90 × 15 mm<sup>3</sup>). (<b>f</b>) Optical image of Mubce-150 aerogels under butane flame for 45s. SEM iages of Mubce-150 aerogels: (<b>g</b>) area far away from the butane torch flame, (<b>h</b>) carbonized region not directly in contact with the butane torch flame, and (<b>i</b>) ablation region in direct contact with the butane torch flame. And (<b>j</b>) Heat Release Rate (HRR), (<b>k</b>) Total Heat Release (THR), and (<b>l</b>) Mass Loss Rate (MLR) curves of BCE and Mubce-150 aerogels.</p>
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10 pages, 4552 KiB  
Article
Effects of Alumina Bubble Addition on the Properties of Corundum–Spinel Castables Containing Cr2O3
by Haonan Chen, Xingfu Shi, Jing Chen, Mengyang Sang, Haoxuan Ma, Xinhong Liu and Quanli Jia
Materials 2024, 17(13), 3139; https://doi.org/10.3390/ma17133139 - 27 Jun 2024
Viewed by 553
Abstract
Purging plugs made of corundum–spinel castables containing Cr2O3 have been widely utilized in secondary refining process. However, their poor thermal shock resistance has greatly limited the improvement of their service life. Aiming to enhance their properties, we introduced alumina bubbles [...] Read more.
Purging plugs made of corundum–spinel castables containing Cr2O3 have been widely utilized in secondary refining process. However, their poor thermal shock resistance has greatly limited the improvement of their service life. Aiming to enhance their properties, we introduced alumina bubbles (ABs) to corundum–spinel castables, and the effects of the AB addition on the properties of the castables are studied in this manuscript. The results indicate that the apparent porosity, permanent linear change, cold strength, and hot strength all increased with an increasing AB amount. The thermal shock resistance of the samples with the AB addition was improved; the residual strength and residual strength ratio of the sample with 4 wt% ABs was the best. The effects of ABs on the tabular alumina aggregate distribution and relationship between the cold strength of the samples and the AB content was evaluated via the box dimension method. With the increments of AB content, the box dimension value of the tabular alumina within the samples significantly decreased, indicating that the tabular alumina aggregate distribution was related to the amount of ABs. In addition, the relationship between the box dimension and the strength was also established. Full article
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<p>(<b>a</b>,<b>d</b>) surficial morphology of ABs, (<b>b</b>,<b>e</b>) internal morphology of ABs, (<b>c</b>) XRD pattern of ABs, and (<b>f</b>) floating state of ABs in water.</p>
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<p>Physical properties of the samples. (<b>a</b>) AP, (<b>b</b>) BD, (<b>c</b>) PLC, (<b>d</b>) CMOR, and (<b>e</b>) CCS.</p>
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<p>(<b>a</b>) HMOR and (<b>b</b>) TSR of the samples with different amounts of ABs.</p>
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<p>Digital photos of the cross-sections and binarized pictures of the samples: (<b>a</b>,<b>b</b>) AB0, (<b>c</b>,<b>d</b>) AB2, (<b>e</b>,<b>f</b>) AB4, and (<b>g</b>,<b>h</b>) AB6. (Here, yellow circles refer to ABs).</p>
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<p>The equations of linear regression of the samples: (<b>a</b>)AB0, (<b>b</b>) AB2, (<b>c</b>) AB4, and (<b>d</b>) AB6.</p>
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<p>Schematic diagram of the volume content of ABs in castables.</p>
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<p>The fracture morphologies of AB2 fired at (<b>a</b>) 1100 °C, (<b>b</b>) 1400 °C, and (<b>c</b>) 1600 °C.</p>
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<p>SEM photos and schematic diagrams of crack propagation in the samples: (<b>a</b>,<b>b</b>) AB0 and (<b>c</b>,<b>d</b>) AB4.</p>
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14 pages, 6961 KiB  
Article
Oxide Scale Microstructure and Scale Growth Kinetics of the Hot-Pressed SiBCN-Ti Ceramics Oxidized at 1500 °C
by Hao Peng, Haobo Jiang, Daxin Li, Zhihua Yang, Wenjiu Duan, Dechang Jia and Yu Zhou
Materials 2024, 17(13), 3118; https://doi.org/10.3390/ma17133118 - 25 Jun 2024
Viewed by 846
Abstract
In this study, the SiBCN-Ti series ceramics with different Ti contents were fabricated, and the oxidation resistance and microstructural evolution of the ceramics at 1500 °C for different times were explored. The results show that with the increase in oxidation time, pores and [...] Read more.
In this study, the SiBCN-Ti series ceramics with different Ti contents were fabricated, and the oxidation resistance and microstructural evolution of the ceramics at 1500 °C for different times were explored. The results show that with the increase in oxidation time, pores and bubbles are gradually formed in the oxide layer. When the oxidation time is less than or more than 4 h, the Ti(C, N) in the ceramics will maintain its initial structure or mostly transform to TiN. The introduction of Ti content can promote the formation of rutile silicate glass, thus healing the cracks and improving the oxidation resistance of the ceramics effectively. Full article
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<p>XRD patterns of the Ti-5 ceramics oxidized at 1500 °C at different times.</p>
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<p>XRD patterns of the hot-pressed various SiBCN-Ti ceramics oxidized at 1500 °C for 2 h.</p>
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<p>XRD patterns of the hot-pressed various SiBCN ceramics oxidized at 1500 °C for 4 h.</p>
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<p>Raman spectra of the hot-pressed Ti-5 ceramics oxidized at 1500 °C for 1~12 h.</p>
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<p>XPS spectra of the hot-pressed Ti-5 ceramics oxidized at 1500 °C for 1 h: (<b>a</b>) Survey; (<b>b</b>) Si 2p; (<b>c</b>) C 1s; (<b>d</b>) Ti 2p; (<b>e</b>) O 1s.</p>
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<p>TG-DSC curves of the hot-pressed Ti-5 ceramics heated to 1500 °C in air.</p>
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<p>The surface morphologies of hot-pressed Ti-5 ceramics after oxidation at 1500 °C: (<b>a</b>–<b>d</b>) 1 h; (<b>e</b>,<b>f</b>) 2 h; (<b>g</b>–<b>j</b>) 8 h; (<b>k</b>,<b>l</b>) 12 h.</p>
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<p>SEM image and element distribution of hot-pressed Ti-5 ceramics after oxidation at 1500 °C for 12 h: (<b>a</b>) Si mapping; (<b>b</b>) Ti mapping; (<b>c</b>) C mapping; (<b>d</b>) O mapping; (<b>e</b>) N mapping; (<b>f</b>) B mapping.</p>
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<p>Element distribution of the hot-pressed Ti-5 ceramics after oxidation at 1500 °C for 2 h: (<b>a</b>) Si mapping; (<b>b</b>) O mapping; (<b>c</b>) C mapping; (<b>d</b>) Ti mapping; (<b>e</b>) N mapping; (<b>f</b>) B mapping.</p>
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<p>Cross-sectional morphologies and element distribution of the hot-pressed Ti-5 ceramics oxidized at 1500 °C: (<b>a</b>) 1 h; (<b>b</b>) 2 h; (<b>c</b>) 8 h; (<b>d</b>) 12 h; (<b>e</b>) EDS line scanning of the cross-section area from the lower ceramics to the upper oxide layer in <a href="#materials-17-03118-f010" class="html-fig">Figure 10</a>d; (<b>f</b>) EDS spot analysis of the oxide layer in <a href="#materials-17-03118-f010" class="html-fig">Figure 10</a>d.</p>
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<p>Oxide layer thickness as a function of oxidation time for the hot-pressed Ti-5 ceramics oxidized at 1500 °C.</p>
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<p>Oxide layer microstructure of the hot-pressed Ti-5 ceramics after oxidation at 1500 °C for 4 h: (<b>a</b>) A FIB slice; (<b>b</b>) HAADF-STEM image; (<b>c</b>) TEM bright-field image; (<b>d</b>–<b>i</b>) corresponding EDS maps.</p>
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<p>Calculated Gibbs free energy changes for the possible oxidation reactions (1)–(12) during oxidation tests.</p>
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9 pages, 2626 KiB  
Article
Preparation and Electromagnetic Wave Absorption Properties of N-Doped SiC Nanowires
by Ranran Shi, Zheng Liu, Wenxiu Liu and Jianlei Kuang
Materials 2023, 16(17), 5765; https://doi.org/10.3390/ma16175765 - 23 Aug 2023
Cited by 3 | Viewed by 980
Abstract
Enhancing the conductivity loss of SiC nanowires through doping is beneficial for improving their electromagnetic wave absorption performance. In this work, N-doped SiC nanowires were synthesized using three different methods. The results indicate that a large amount of Si2ON will be [...] Read more.
Enhancing the conductivity loss of SiC nanowires through doping is beneficial for improving their electromagnetic wave absorption performance. In this work, N-doped SiC nanowires were synthesized using three different methods. The results indicate that a large amount of Si2ON will be generated during the microwave synthesis of SiC nanowires in a nitrogen atmosphere. In addition, the secondary heat-treatment of the as-synthesized SiC nanowires under nitrogen atmosphere will significantly reduce their stacking fault density. When ammonium chloride is introduced as a doped nitrogen source in the reaction raw material, the N-doped SiC nanowires with high-density stacking faults can be synthesized by microwave heating. Therefore, the polarization loss induced by faults and the conductivity loss caused by doping will synergistically enhance the dielectric and EMW absorption properties of SiC nanowires in the range of 2–18 GHz. When the filling ratio of N-doped SiC nanowires is 20 wt.%, the composite shows a minimum reflection loss of –22.2 [email protected] GHz, and an effective absorption (RL ≤ –10 dB) bandwidth of 4.24 GHz at the absorber layer thickness of 2.2 mm. Further, the N-doped SiC nanowires also exhibit enhanced high-temperature EMW absorption properties with increasing temperature. Full article
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<p>XRD patterns of the N-doped SiC nanowires prepared by different doping methods.</p>
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<p>SEM and TEM images of (<b>a</b>,<b>c</b>) SN-B and (<b>b</b>,<b>d</b>) SN-C samples.</p>
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<p>Permittivity properties of N-doped SiC nanowires as a function of frequency: (<b>a</b>) dielectric constant, (<b>b</b>) dielectric loss, and (<b>c</b>) loss angle tangent.</p>
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<p>Cole–Cole curves of samples (<b>a</b>) SN-B and (<b>b</b>) SN-C.</p>
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<p>Three-dimensional patterns of reflection loss of N-doped SiC nanowires versus the absorber thickness and frequency: (<b>a</b>) SN-B and (<b>b</b>) SN-C.</p>
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<p>Reflection loss of SN-C SiC nanowires/resin composite coating (2.2 mm thickness) versus the frequency and temperature.</p>
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14 pages, 3533 KiB  
Article
Synthesis and Structural and Strength Properties of xLi2ZrO3-(1-x)MgO Ceramics—Materials for Blankets
by Dmitriy I. Shlimas, Daryn B. Borgekov, Artem L. Kozlovskiy and Maxim V. Zdorovets
Materials 2023, 16(14), 5176; https://doi.org/10.3390/ma16145176 - 23 Jul 2023
Cited by 1 | Viewed by 760
Abstract
The article considers the effect of doping with magnesium oxide (MgO) on changes in the properties of lithium-containing ceramics based on lithium metazirconate (Li2ZrO3). There is interest in this type of ceramics on account of their prospects for application [...] Read more.
The article considers the effect of doping with magnesium oxide (MgO) on changes in the properties of lithium-containing ceramics based on lithium metazirconate (Li2ZrO3). There is interest in this type of ceramics on account of their prospects for application in tritium production in thermonuclear power engineering, as well as several other applications related to alternative energy sources. During the investigations undertaken, it was found that variation in the MgO dopant concentration above 0.10–0.15 mol resulted in the formation of impurity inclusions in the ceramic structure in the form of a MgLi2ZrO4 phase, the presence of which resulted in a rise in the density of the ceramics, along with elevation in resistance to external influences. Moreover, during experimental work on the study of the thermal stability of the ceramics to external influences, it was found that the formation of two-phase ceramics resulted in growth in the preservation of stable strength properties during high-temperature cyclic tests. The decrease in strength characteristics was observed to be less than 1%. Full article
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<p>SEM images of synthesized xLi<sub>2</sub>ZrO<sub>3</sub>-(1-x)MgO ceramics versus MgO dopant concentration: (<b>a</b>) Pristine; (<b>b</b>) 0.05 mol; (<b>c</b>) 0.10 mol; (<b>d</b>) 0.15 mol; (<b>e</b>) 0.20 mol; (<b>f</b>) 0.25 mol. (red circles highlight the presence of fine grains characteristic of impurity inclusions of various phases).</p>
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<p>SEM images of synthesized xLi<sub>2</sub>ZrO<sub>3</sub>-(1-x)MgO ceramics versus MgO dopant concentration: (<b>a</b>) Pristine; (<b>b</b>) 0.05 mol; (<b>c</b>) 0.10 mol; (<b>d</b>) 0.15 mol; (<b>e</b>) 0.20 mol; (<b>f</b>) 0.25 mol. (red circles highlight the presence of fine grains characteristic of impurity inclusions of various phases).</p>
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<p>Results of X-ray diffraction of the studied xLi<sub>2</sub>ZrO<sub>3</sub>-(1-x)MgO ceramics versus MgO dopant concentration.</p>
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<p>Variations in the phase composition of xLi<sub>2</sub>ZrO<sub>3</sub>-(1-x)MgO ceramics versus MgO dopant concentration.</p>
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<p>The assessment results of the xLi<sub>2</sub>ZrO<sub>3</sub>-(1-x)MgO ceramic density versus MgO dopant concentration.</p>
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<p>Results of changes in the porosity of xLi<sub>2</sub>ZrO<sub>3</sub>-(1-x)MgO ceramics versus MgO dopant concentration.</p>
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<p>Frequency dependencies of the permittivity (<b>a</b>) and the dielectric loss tangent (<b>b</b>) of the acquired samples.</p>
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<p>Variation in the hardness values of the studied ceramics versus MgO dopant concentration.</p>
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<p>Variations in porosity and hardening versus MgO dopant concentration.</p>
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<p>Evaluation results of changes in the hardness of ceramic specimens versus number of serial test cycles.</p>
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<p>Results of maintaining the stability of strength properties after heat resistance tests.</p>
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12 pages, 4289 KiB  
Article
Study of the Aid Effect of CuO-TiO2-Nb2O5 on the Dielectric and Structural Properties of Alumina Ceramics
by Rafael I. Shakirzyanov, Natalia O. Volodina, Kayrat K. Kadyrzhanov, Artem L. Kozlovskiy, Dmitriy I. Shlimas, Gulzada A. Baimbetova, Daryn B. Borgekov and Maxim V. Zdorovets
Materials 2023, 16(14), 5018; https://doi.org/10.3390/ma16145018 - 15 Jul 2023
Cited by 2 | Viewed by 854
Abstract
The aim of this work is to study the structural, dielectric, and mechanical properties of aluminum oxide ceramics with the triple sintering additive 4CuO-TiO2-2Nb2O5. With an increase in sintering temperature from 1050 to 1500 °C, the average [...] Read more.
The aim of this work is to study the structural, dielectric, and mechanical properties of aluminum oxide ceramics with the triple sintering additive 4CuO-TiO2-2Nb2O5. With an increase in sintering temperature from 1050 to 1500 °C, the average grain size and the microhardness value at a load of 100 N (HV0.1) increased with increasing density. It has been shown that at a sintering temperature of 1300 °C, the addition of a 4CuO-TiO2-2Nb2O5 additive increases the low-frequency permittivity (2–500 Hz) in alumina ceramic by more than an order of magnitude due to the presence of a quadruple perovskite phase. At the same time, the density of such ceramics reached 89% of the theoretical density of α-Al2O3, and the microhardness value HV0.1 was 1344. It was observed that the introduction of 5 wt.% 4CuO-TiO2-2Nb2O5 in the raw mixture remarkably increases values of shrinkage and density of sintered ceramics. Overall, the results of this work confirmed that introducing the 4CuO-TiO2-2Nb2O5 sintering additive in the standard solid-phase ceramics route can significantly reduce the processing temperature of alumina ceramics, even when micron-sized powders are used as a starting material. The obtained samples demonstrated the potential of α-Al2O3 with the triple additive in such applications as electronics, microwave technology, and nuclear power engineering. Full article
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<p>The dependence of volumetric shrinkage (<b>a</b>) and apparent density (<b>b</b>) of samples on the weight percentage of PVA. 1—sample without addition of CTN and T<sub>s</sub> = 1500 °C (black squares), 2—sample with addition of CTN and T<sub>s</sub> = 1050 °C (red circles), 3—sample with addition of CTN, and T<sub>s</sub> = 1300 °C (green triangle), 4—sample with addition of CTN and T<sub>s</sub> = 1500 °C (blue rhombs).</p>
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<p>The results of XRD phase analysis of obtained samples. 1—sample without addition of CTN, T<sub>s</sub> = 1500 °C; 2—sample with additive T<sub>s</sub> = 1050 °C; 3—sample with additive T<sub>s</sub> = 1300 °C; 4—sample with additive T<sub>s</sub> = 1500 °C.</p>
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<p>Williamson–Hall plots for α-Al<sub>2</sub>O<sub>3</sub> phase.</p>
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<p>Micrographs of cross-sections of synthesized samples. Points 1 and 2 are spots where EDX spectra were collected. (<b>a</b>)—sample without additive, T<sub>s</sub> = 1500 °C; (<b>b</b>)—sample with CTN additive T<sub>s</sub> = 1050 °C; (<b>c</b>)—sample with CTN additive T<sub>s</sub> = 1300 °C; (<b>d</b>)—sample with CTN additive T<sub>s</sub> = 1500 °C.</p>
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<p>EDX spectra inside the grain (<b>a</b>), in the grain boundary (<b>b</b>), and the average elemental composition of the grain (<b>c</b>), grain boundary (<b>d</b>). 1—sample without addition of CTN and T<sub>s</sub> = 1500 °C, 2—sample with addition of CTN and T<sub>s</sub> = 1050 °C, 3—sample with addition of CTN and T<sub>s</sub> = 1300 °C, 4—sample with addition of CTN and T<sub>s</sub> = 1500 °C.</p>
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<p>Frequency dependences of permittivity (<b>a</b>) and dielectric loss tangent (<b>b</b>). 1—sample without addition of CTN and T<sub>s</sub> = 1500 °C, 2—sample with addition of CTN and T<sub>s</sub> = 1050 °C, 3—sample with addition of CTN and T<sub>s</sub> = 1300 °C, 4—sample with addition of CTN and T<sub>s</sub> = 1500 °C.</p>
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<p>Frequency dependence of AC conductivity (<b>a</b>) and Nyquist diagram (<b>b</b>) for a sample with T<sub>s</sub> = 1300 °C.</p>
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<p>Microphotographs of sample’s surfaces after Vickers indentation test. (<b>a</b>) T<sub>s</sub> = 1050 °C, (<b>b</b>) T<sub>s</sub> = 1300 °C, (<b>c</b>) T<sub>s</sub> = 1500 °C.</p>
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15 pages, 12203 KiB  
Article
Effect of Zr2Al4C5 Content on the Mechanical Properties and Oxidation Behavior of ZrB2-SiC-Zr2Al4C5 Ceramics
by Qilong Guo, Liang Hua, Hao Ying, Ronghao Liu, Mei Lin, Leilei Li and Jing Wang
Materials 2023, 16(12), 4495; https://doi.org/10.3390/ma16124495 - 20 Jun 2023
Viewed by 1245
Abstract
ZrB2-SiC-Zr2Al4C5 multi-phase ceramics with uniform structure and high density were successfully prepared through the introduction of in situ synthesized Zr2Al4C5 into ZrB2-SiC ceramic via SPS at 1800 °C. A [...] Read more.
ZrB2-SiC-Zr2Al4C5 multi-phase ceramics with uniform structure and high density were successfully prepared through the introduction of in situ synthesized Zr2Al4C5 into ZrB2-SiC ceramic via SPS at 1800 °C. A systematic analysis and discussion of the experimental results and proposed mechanisms were carried out to demonstrate the composition-dependent sintering properties, mechanical properties and oxidation behavior. The results showed that the in situ synthesized Zr2Al4C5 could be evenly distributed in the ZrB2-SiC ceramic matrix and inhibited the growth of ZrB2 grains, which played a positive role in the sintering densification of the composite ceramics. With increasing Zr2Al4C5 content, the Vickers hardness and Young’s modulus of composite ceramics gradually decreased. The fracture toughness showed a trend that first increased and then decreased, and was increased by about 30% compared with ZrB2-SiC ceramics. The major phases resulting from the oxidation of samples were ZrO2, ZrSiO4, aluminosilicate and SiO2 glass. With increasing Zr2Al4C5 content, the oxidative weight showed a trend that first increased then decreased; the composite ceramic with 30 vol.% Zr2Al4C5 showed the smallest oxidative weight gain. We believe that the presence of Zr2Al4C5 results in the formation of Al2O3 during the oxidation process, subsequently resulting in a lowering of the viscosity of the glassy silica scale, which in turn intensifies the oxidation of the composite ceramics. This would also increase oxygen permeation through the scale, adversely affecting the oxidation resistance of the composites with high Zr2Al4C5 content. Full article
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<p>Displacement curve of pressure punch at different temperatures.</p>
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<p>XRD patterns of composite ceramics at different Zr<sub>2</sub>Al<sub>4</sub>C<sub>5</sub> contents: (<b>a</b>) ZAC0, (<b>b</b>) ZAC10, (<b>c</b>) ZAC20, (<b>d</b>) ZAC30, (<b>e</b>) ZAC40.</p>
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<p>Backscattered electron phase pictures of polished surfaces of multi-phase ceramics at different Zr<sub>2</sub>Al<sub>4</sub>C<sub>5</sub> contents: (<b>a</b>) ZAC0, (<b>b</b>) ZAC10, (<b>c</b>) ZAC20, (<b>d</b>) ZAC30, (<b>e</b>) ZAC40.</p>
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<p>SEM fracture surface morphologies of samples with different Zr<sub>2</sub>Al<sub>4</sub>C<sub>5</sub> content: (<b>a</b>) ZAC0, (<b>b</b>) ZAC10, (<b>c</b>) ZAC20, (<b>d</b>) ZAC30, (<b>e</b>) ZAC40.</p>
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<p>Expansion path diagram of the crack tip of multi-phase ceramics: (<b>a</b>) ZAC0, (<b>b</b>) ZAC20, (<b>c</b>) ZAC30, (<b>d</b>) ZAC30.</p>
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<p>(<b>a</b>) Changes of oxidative weight gain and (<b>b</b>) oxidation layer thickness of samples at different contents of Zr<sub>2</sub>Al<sub>4</sub>C<sub>5</sub>.</p>
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<p>TG–DSC curve of multi-phase ceramics: (<b>a</b>) ZAC30, (<b>b</b>) ZAC40. Red line is differential scanning calorimetry, blue line is thermogravimetry.</p>
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<p>XRD patterns of composite ceramics oxidized for 30min at different oxidation temperatures: (<b>a</b>) ZAC10, (<b>b</b>) ZAC20, (<b>c</b>) ZAC30, (<b>d</b>) ZAC40.</p>
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<p>SEM pictures of the cross section and surface of the samples after oxidation at 1200 °C for 30 min: (<b>a</b>,<b>b</b>) ZAC10, (<b>c</b>,<b>d</b>) ZAC20, (<b>e</b>,<b>f</b>) ZAC30, (<b>g</b>,<b>h</b>) ZAC40.</p>
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<p>SEM and EDS pictures of the cross section and surface of the samples after oxidation at 1200 °C for 30 min: (<b>a</b>,<b>b</b>) ZAC10, (<b>c</b>,<b>d</b>) ZAC20, (<b>e</b>,<b>f</b>) ZAC30, (<b>g</b>,<b>h</b>) ZAC40.</p>
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<p>EDS pattern of the ZAC30 sample at different oxidation temperatures: (<b>a</b>) 1200 °C, (<b>b</b>) 1400 °C, (<b>c</b>) 1500 °C.</p>
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<p>BESEM and EDS micrographs of the oxide layer section of the ZAC30 specimen after oxidation at 1500 °C for 30 min (<b>a</b>–<b>c</b>). (<b>a</b>,<b>c</b>) magnified SEM images of the areas enclosed in yellow dotted rectangles in (<b>b</b>).</p>
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11 pages, 7177 KiB  
Article
Low-Temperature Fabrication of Plate-like α-Al2O3 with Less NH4F Additive
by Haiyang Chen, Bin Li, Meng Liu, Xue Yang, Jie Liu, Tingwei Qin, Zejian Xue, Yun Xing and Junhong Chen
Materials 2023, 16(12), 4415; https://doi.org/10.3390/ma16124415 - 15 Jun 2023
Cited by 1 | Viewed by 1220
Abstract
Fluorinated compounds are effective mineralization agents for the fabrication of plate-like α-Al2O3. However, in the preparation of plate-like α-Al2O3, it is still an extremely challenging task to reduce the content of fluoride while ensuring a [...] Read more.
Fluorinated compounds are effective mineralization agents for the fabrication of plate-like α-Al2O3. However, in the preparation of plate-like α-Al2O3, it is still an extremely challenging task to reduce the content of fluoride while ensuring a low synthesis temperature. Herein, oxalic acid and NH4F are proposed for the first time as additives in the preparation of plate-like α-Al2O3. The results showed that plate-like α-Al2O3 can be synthesized at a low temperature of 850 °C with the synergistic effect of oxalic acid and 1 wt.% NH4F. Additionally, the synergistic effect of oxalic acid and NH4F not only can reduce the conversion temperature of α-Al2O3 but also can change the phase transition sequence. Full article
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<p>FTIR spectra of: (<b>a</b>) the specimens A2–A5; (<b>b</b>) local amplification at 1200–400 cm<sup>−1</sup>.</p>
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<p>SEM pictures of A2–A5: (<b>a</b>) A2; (<b>b</b>) A3; (<b>c</b>) A4; (<b>d</b>) A5.</p>
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<p>XRD patterns of the alumina phases received from A2–A5 at different calcination temperatures: (<b>a</b>) A2; (<b>b</b>) A3; (<b>c</b>) A4; (<b>d</b>) A5.</p>
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<p>XRD patterns of: (<b>a</b>) the transition Al<sub>2</sub>O<sub>3</sub> as obtained from A5 at 800 °C for distinct times; (<b>b</b>) local amplification at 2θ = 30°–50°.</p>
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<p>XPS spectrum of transition Al<sub>2</sub>O<sub>3</sub> as-obtained from A5 at 500 °C (<b>a</b>); the overall XPS spectrum and the individual lines of: (<b>b</b>) O 1s; and (<b>c</b>) Al 2p (<b>d</b>) F 1s.</p>
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<p>TG-DSC curves of: (<b>a</b>) Al(OH)<sub>3</sub>; (<b>b</b>) A1; (<b>c</b>) A5.</p>
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<p>SEM images of α-Al<sub>2</sub>O<sub>3</sub> obtained from A2–A5 at different temperatures: (<b>a</b>) A2-950; (<b>b</b>) A3-950; (<b>c</b>) A4-950; (<b>d</b>) A5-950; (<b>e</b>) A4-850; (<b>f</b>) A5-800.</p>
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Review

Jump to: Research

25 pages, 5472 KiB  
Review
Principles and Methods for Improving the Thermoelectric Performance of SiC: A Potential High-Temperature Thermoelectric Material
by Yun Xing, Bo Ren, Bin Li, Junhong Chen, Shu Yin, Huan Lin, Jie Liu and Haiyang Chen
Materials 2024, 17(15), 3636; https://doi.org/10.3390/ma17153636 - 23 Jul 2024
Viewed by 802
Abstract
Thermoelectric materials that can convert thermal energy to electrical energy are stable and long-lasting and do not emit greenhouse gases; these properties render them useful in novel power generation devices that can conserve and utilize lost heat. SiC exhibits good mechanical properties, excellent [...] Read more.
Thermoelectric materials that can convert thermal energy to electrical energy are stable and long-lasting and do not emit greenhouse gases; these properties render them useful in novel power generation devices that can conserve and utilize lost heat. SiC exhibits good mechanical properties, excellent corrosion resistance, high-temperature stability, non-toxicity, and environmental friendliness. It can withstand elevated temperatures and thermal shock and is well suited for thermoelectric conversions in high-temperature and harsh environments, such as supersonic vehicles and rockets. This paper reviews the potential of SiC as a high-temperature thermoelectric and third-generation wide-bandgap semiconductor material. Recent research on SiC thermoelectric materials is reviewed, and the principles and methods for optimizing the thermoelectric properties of SiC are discussed. Thus, this paper may contribute to increasing the application potential of SiC for thermoelectric energy conversion at high temperatures. Full article
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<p>Typical operating temperature of various thermoelectric materials [<a href="#B14-materials-17-03636" class="html-bibr">14</a>,<a href="#B15-materials-17-03636" class="html-bibr">15</a>].</p>
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<p>Stacking order of different SiC polytypes [<a href="#B26-materials-17-03636" class="html-bibr">26</a>].</p>
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<p>Dependence of <span class="html-italic">S</span>, <span class="html-italic">σ</span>, and <span class="html-italic">κ</span> on carrier concentration [<a href="#B14-materials-17-03636" class="html-bibr">14</a>,<a href="#B15-materials-17-03636" class="html-bibr">15</a>].</p>
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<p>Strategies for optimizing the thermoelectric properties of SiC.</p>
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<p>Diagrammatic representation of the N-doping process in SiC ceramics in a N<sub>2</sub> environment [<a href="#B40-materials-17-03636" class="html-bibr">40</a>].</p>
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<p>Thermoelectric characteristics of variously structured SiC ceramics in relation to temperature: (<b>a</b>) <span class="html-italic">S</span>, (<b>b</b>) <span class="html-italic">ρ</span>, (<b>c</b>) <span class="html-italic">κ</span>, and (<b>d</b>) <span class="html-italic">Z</span> [<a href="#B69-materials-17-03636" class="html-bibr">69</a>].</p>
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<p>Thermoelectric parameters of each nanowire as a function of temperature: (<b>a</b>) <span class="html-italic">S</span>, (<b>b</b>) <span class="html-italic">σ</span>, (<b>c</b>) <span class="html-italic">κ</span>, and (<b>d</b>) <span class="html-italic">ZT</span> [<a href="#B79-materials-17-03636" class="html-bibr">79</a>].</p>
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<p>Electronic density of states for a (<b>a</b>) 3D bulk semiconductor, (<b>b</b>) 2D quantum well, (<b>c</b>) 1D nanowire, and (<b>d</b>) 0D quantum dot [<a href="#B93-materials-17-03636" class="html-bibr">93</a>].</p>
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<p>Energy-band diagram of ZnO/SiC. The middle number represents the band arrangement of the ZnO/SiC interfaces with interface-induced band bending [<a href="#B105-materials-17-03636" class="html-bibr">105</a>]. All numbers are in eV.</p>
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<p>(<b>a</b>) Charge carrier concentration in the electrode, (<b>b</b>) energy-band diagram of the 3C-SiC/Si heterojunction <span class="html-italic">E<sub>h</sub></span> electrode under heating conditions, and (<b>c</b>) energy-band diagram of the 3C-SiC/Si heterojunction <span class="html-italic">E<sub>c</sub></span> under heating conditions [<a href="#B106-materials-17-03636" class="html-bibr">106</a>].</p>
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