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Search Results (3,278)

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12 pages, 1354 KiB  
Review
The Case for Bisphosphonate Use in Astronauts Flying Long-Duration Missions
by Reece Rosenthal, Victor S. Schneider, Jeffrey A. Jones and Jean D. Sibonga
Cells 2024, 13(16), 1337; https://doi.org/10.3390/cells13161337 (registering DOI) - 13 Aug 2024
Viewed by 135
Abstract
Changes in the structure of bone can occur in space as an adaptive response to microgravity and on Earth due to the adaptive effects to exercise, to the aging of bone cells, or to prolonged disuse. Knowledge of cell-mediated bone remodeling on Earth [...] Read more.
Changes in the structure of bone can occur in space as an adaptive response to microgravity and on Earth due to the adaptive effects to exercise, to the aging of bone cells, or to prolonged disuse. Knowledge of cell-mediated bone remodeling on Earth informs our understanding of bone tissue changes in space and whether these skeletal changes might increase the risk for fractures or premature osteoporosis in astronauts. Comparisons of skeletal health between astronauts and aging humans, however, may be both informative and misleading. Astronauts are screened for a high level of physical fitness and health, are launched with high bone mineral densities, and perform exercise daily in space to combat skeletal atrophy as an adaptive response to reduced weight-bearing function, while the elderly display cellular and tissue pathology as a response to senescence and disuse. Current clinical testing for age-related bone change, applied to astronauts, may not be sufficient for fully understanding risks associated with rare and uniquely induced bone changes. This review aims to (i) highlight cellular analogies between spaceflight-induced and age-related bone loss, which could aid in predicting fractures, (ii) discuss why overreliance on terrestrial clinical approaches may miss potentially irreversible disruptions in trabecular bone microarchitecture induced by spaceflight, and (iii) detail how the cellular effects of the bisphosphonate class of drugs offer a prophylactic countermeasure for suppressing the elevated bone resorption characteristically observed during long-duration spaceflights. Thus the use of the bisphosphonate will help protect the bone from structural changes while in microgravity either along with exercise or alone when exercise is not performed, e.g. after an injury or illness. Full article
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Figure 1
<p>Differential Effects of Spaceflight and of ARED Exercise as Influenced by Bisphosphonate Supplementation. Changes in DXA, QCT-cortical, and QCT-trabecular bone mineral density of the left total hip (from preflight to postflighttesting) were compiled from previously published reports of astronauts from whom informed consents were acquired [<a href="#B24-cells-13-01337" class="html-bibr">24</a>,<a href="#B32-cells-13-01337" class="html-bibr">32</a>,<a href="#B33-cells-13-01337" class="html-bibr">33</a>]. Pre-ARED represented data acquired from astronauts before ARED was flown on-board the ISS. The access and use of ARED alone (red) were protective against spaceflight losses in QCT-cortical bone but not for changes detected by DXA aBMD and by QCT-measured trabecular bone. Bisphosphonate use combined with ARED (green) was associated with no significant change between pre- and post-flight measurements using DXA and QCT-cortical bone and QCT-trabecular bone.</p>
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<p>Percent change of level of N-Telopeptide Cross-links (NTX), a marker of bone resorption, from pre-flight levels at increasing flight days (FD). An increase in bone resorptive biomarker NTX is observed when resistive exercise is utilized in isolation (hollow square). When bisphosphonates are used to supplement resistive exercise (solid square), the level of NTX remains stable at pre-flight levels Bis: bisphosphonate; iRED: Interim Resistive. Exercise Device; ARED: Advanced Resistive Exercise Device [<a href="#B35-cells-13-01337" class="html-bibr">35</a>]. Superscript 1 denotes a significant Within-Group delta change in assay results when compared to pre-flight specimens; superscript 2 denotes a significant Between Group delta change between the ARED vs. Bis+ ARED treatments at the specified time point. (Reprinted/adapted with permission from [<a href="#B35-cells-13-01337" class="html-bibr">35</a>]. 2019, Sibonga).</p>
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<p>Percent change of level of bone-specific alkaline phosphatase (BSAP), a bone formation biomarker, from pre-flight levels at increasing flight days (FD). ARED alone leads to an increase in BSAP with increasing mission durations (solid circle), while bisphosphonate addition (solid square) tempers this effect perhaps due to a decrease in overall bone turnover. Bis: bisphosphonate; iRED: Interim Resistive Exercise Device; ARED: Advanced Resistive Exercise Device [<a href="#B35-cells-13-01337" class="html-bibr">35</a>]. Superscript 1 denotes a significant Within-Group delta change in assay results when compared to pre-flight specimens; superscript 2 denotes a significant Between-Group delta change between the ARED vs. Bis+ ARED treatments at the specified time point (Reprinted/adapted with permission from [<a href="#B35-cells-13-01337" class="html-bibr">35</a>]. 2019, Sibonga).</p>
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12 pages, 15092 KiB  
Article
Utilisation of Biosilica as Active Silica Source for Metakaolin-Based Geopolymers
by Haozhe Guo, Zhihao Huang, Thammaros Pantongsuk, Ting Yu, Baifa Zhang, Jinghan Luo and Peng Yuan
Minerals 2024, 14(8), 816; https://doi.org/10.3390/min14080816 (registering DOI) - 12 Aug 2024
Viewed by 230
Abstract
This study explores the potential of biosilica including diatom and diatomaceous earth as alternative silica sources for metakaolin-based geopolymers. Diatomaceous earth, composed of fossilised diatom frustules rich in amorphous silica, and diatoms, a sustainable source of renewable biosilica, are investigated for their effectiveness [...] Read more.
This study explores the potential of biosilica including diatom and diatomaceous earth as alternative silica sources for metakaolin-based geopolymers. Diatomaceous earth, composed of fossilised diatom frustules rich in amorphous silica, and diatoms, a sustainable source of renewable biosilica, are investigated for their effectiveness in enhancing geopolymer properties. Through detailed analyses including FTIR, XRD, and SEM, the study evaluates the impact of these biosilica sources on geopolymer compressive strength and microstructure, comparing them with conventional sodium silicate. Results show that diatoms exhibit significant promise, achieving 28-day strength up to 17.9 MPa at a 30% mass fraction, while diatomaceous earth reaches 26.2 MPa at a 50% addition rate, demonstrating their potential as active silica sources. Furthermore, the study elucidates the role of organic matter in biosilica on geopolymerisation, highlighting its influence on active silica release and the strength performance of products. This study proposes a novel pathway to enhance the sustainability of geopolymers through the utilisation of biosilica from diatoms, contributing to advancements in eco-efficient construction materials. Full article
(This article belongs to the Section Clays and Engineered Mineral Materials)
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Figure 1
<p>(<b>a</b>) The compressive strength of geopolymers at 7 and 28 days with the error bar representing the upper and lower 95% confidence interval; (<b>b</b>) The growth rate of compressive strengths between 7 to 28 days.</p>
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<p>(<b>a</b>) XRD patterns of DB, CDB, G<sub>B30</sub>, and G<sub>CB30</sub>; (<b>b</b>) XRD patterns of DE, CDE, G<sub>E50</sub>, and G<sub>CE50</sub>. The XRD patterns of all the geopolymers were obtained at 28 days. (A: albite; C: chlorite; M: muscovite; P: paragonite; Q: quartz).</p>
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<p>(<b>a</b>) FTIR spectra of DB, CDB, G<sub>B30</sub>, and G<sub>CB30</sub>; (<b>b</b>) FTIR spectra of DE, CDE, G<sub>E50</sub>, and G<sub>CE50</sub>. The FTIR spectra of all the geopolymers were obtained at 28 days.</p>
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<p>SEM images of (<b>a</b>) DB, (<b>b</b>) G<sub>B30</sub>, (<b>c</b>) CDB, (<b>d</b>) G<sub>CB30</sub>, (<b>e</b>) DE, (<b>f</b>) G<sub>E50</sub>, (<b>g</b>) DE, and (<b>h</b>) G<sub>CB50</sub>. The SEM images of the geopolymers and the corresponding EDS analysis results, listed below, were measured at 28 d.</p>
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14 pages, 3694 KiB  
Article
Crystal Lattice Recovery and Optical Activation of Yb Implanted into β-Ga2O3
by Mahwish Sarwar, Renata Ratajczak, Vitalii Yu. Ivanov, Sylwia Gieraltowska, Aleksandra Wierzbicka, Wojciech Wozniak, René Heller, Stefan Eisenwinder and Elżbieta Guziewicz
Materials 2024, 17(16), 3979; https://doi.org/10.3390/ma17163979 - 10 Aug 2024
Viewed by 277
Abstract
β-Ga2O3 is an ultra-wide bandgap semiconductor (Eg~4.8 eV) of interest for many applications, including optoelectronics. Undoped Ga2O3 emits light in the UV range that can be tuned to the visible region of the spectrum by [...] Read more.
β-Ga2O3 is an ultra-wide bandgap semiconductor (Eg~4.8 eV) of interest for many applications, including optoelectronics. Undoped Ga2O3 emits light in the UV range that can be tuned to the visible region of the spectrum by rare earth dopants. In this work, we investigate the crystal lattice recovery of (2¯01)-oriented β-Ga2O3 crystals implanted with Yb ions to the fluence of 1 ×1014 at/cm2. Post-implantation annealing at a range of temperature and different atmospheres was used to investigate the β-Ga2O3 crystal structure recovery and optical activation of Yb ions. Ion implantation is a renowned technique used for material doping, but in spite of its many advantages such as the controlled introduction of dopants in concentrations exceeding the solubility limits, it also causes damage to the crystal lattice, which strongly influences the optical response from the material. In this work, post-implantation defects in β-Ga2O3:Yb crystals, their transformation, and the recovery of the crystal lattice after thermal treatment have been investigated by channeling Rutherford backscattering spectrometry (RBS/c) supported by McChasy simulations, and the optical response was tested. It has been shown that post-implantation annealing at temperatures of 700–900 °C results in partial crystal lattice recovery, but it is accompanied by the out-diffusion of Yb ions toward the surface if the annealing temperature and time exceed 800 °C and 10 min, respectively. High-temperature implantation at 500–900 °C strongly limits post-implantation damage to the crystal lattice, but it does not cause the intense luminescence of Yb ions. This suggests that the recovery of the crystal lattice is not a sufficient condition for strong rare-earth photoluminescence at room temperature and that oxygen annealing is beneficial for intense infrared luminescence compared to other tested environments. Full article
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Graphical abstract

Graphical abstract
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<p>Schematic of β-Ga<sub>2</sub>O<sub>3</sub> crystal structure and damaged β-Ga<sub>2</sub>O<sub>3</sub> after Yb ion implantation with Yb on interstitial sites.</p>
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<p>Random (ran, solid symbols) and aligned (ali, open symbols) RBS spectra for β-Ga<sub>2</sub>O<sub>3</sub> implanted with Yb ions at the fluence of 1 × 10<sup>14</sup> at/cm<sup>2</sup> and post-implantation annealed at 800 °C, in O<sub>2</sub> for different time durations.</p>
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<p>Random (ran, solid symbols) and aligned (ali, open symbols) RBS spectra for β-Ga<sub>2</sub>O<sub>3</sub> implanted with Yb ions at the fluence of 1 × 10<sup>14</sup> at/cm<sup>2</sup> and post-implantation annealed in O<sub>2</sub> at different temperatures for 10 min.</p>
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<p>Random (ran, solid symbols) and aligned (ali, open symbols) RBS spectra for β-Ga<sub>2</sub>O<sub>3</sub> implanted with Yb ions at the fluence of 1 × 10<sup>14</sup> at/cm<sup>2</sup> at high temperatures.</p>
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<p>Comparison of various annealing processes. Random (ran, solid symbols) and aligned (ali, open symbols) RBS spectra for β-Ga<sub>2</sub>O<sub>3</sub> implanted with Yb ions at with the fluence of 1 × 10<sup>14</sup> at/cm<sup>2</sup> at HT and RT, and subsequently post-RT implantation annealed at different conditions. The solid line represents the results of the McChasy simulations.</p>
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<p>Depth distributions of RDA-type defects and DIS-type defects obtained via McChasy simulations for β-Ga<sub>2</sub>O<sub>3</sub> implanted with Yb ions with a fluence of 1 × 10<sup>14</sup> at/cm<sup>2</sup> at HT and RT, and subsequently post-RT implantation annealed under different conditions.</p>
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<p>Aligned (ali, solid symbols) RBS spectra for Yb signal of β-Ga<sub>2</sub>O<sub>3</sub> implanted with Yb ions at the fluence of 1 × 10<sup>14</sup> at/cm<sup>2</sup> at HT and RT, and subsequently post-RT implantation annealed at different conditions.</p>
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<p>The 2θ-ω scan of the symmetrical −402 reflection of a virgin β-Ga<sub>2</sub>O<sub>3</sub> crystal (black). This crystal was implanted at RT with Yb ions with a fluence of 1 × 10<sup>14</sup> at/cm<sup>2</sup> (red) and subsequently post-RT-implantation annealed for 10 min. at 800 °C in the O<sub>2</sub> (blue), N<sub>2</sub> (yellow), and Ar (green) atmosphere.</p>
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<p>AFM imaging of the surface morphology for virgin β-Ga<sub>2</sub>O<sub>3</sub>, implanted with 150 keV Yb ions to the fluence of 1 × 10<sup>14</sup> at/cm<sup>2</sup>, RTA-annealed in different conditions, and HT-implanted.</p>
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<p>RT PL spectra in IR region obtained for β-Ga<sub>2</sub>O<sub>3</sub> crystal implanted with Yb ions to a fluence of 1 × 10<sup>14</sup> at/cm<sup>2</sup> for as-implanted sample at RT and HT temperatures and for RT-implanted and subsequently RTA-annealed samples for 10 min. at different conditions.</p>
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20 pages, 31392 KiB  
Article
Involvement of the Northeastern Margin of South China Block in Rodinia Supercontinent Evolution: A Case Study of Neoproterozoic Granitic Gneiss in Rizhao Area, Shandong Province
by Xiaolong He, Zeyu Yang, Kai Liu, Wei Zhu, Honglei Zhan, Peng Yang, Tongzheng Wei, Shuxun Wang and Yaoyao Zhang
Minerals 2024, 14(8), 807; https://doi.org/10.3390/min14080807 (registering DOI) - 9 Aug 2024
Viewed by 290
Abstract
The South China Plate is an important part of the Rodinia supercontinent in the Neoproterozoic. The Rizhao area, located on the northeastern margin of the South China Plate, records multiple periods of magmatism, among which Neoproterozoic granitic gneiss is of great significance to [...] Read more.
The South China Plate is an important part of the Rodinia supercontinent in the Neoproterozoic. The Rizhao area, located on the northeastern margin of the South China Plate, records multiple periods of magmatism, among which Neoproterozoic granitic gneiss is of great significance to the tectonic evolution of the South China Block. In this study, systematic petrology, geochemistry, isotopic chronology, and zircon Hf isotopic analyses were carried out on gneisses samples of biotite alkali feldspar granitic and biotite monzogranitic compositions in the Rizhao area. Geochemical analyses suggest that these granitic rocks belong to the sub-alkaline series and have high potassium contents. They are enriched in large-ion lithophile elements K, Rb, and Ba; depleted in high field strength elements P, Nb, and Ti; enriched in light rare earth elements and moderately depleted in heavy rare earth elements; and have weak to moderate negative Eu anomalies and weak negative Ce anomalies. These rocks are post-orogenic A-type granites. LA-MC-ICP-MS U-Pb dating of zircons from two biotite alkali-feldspar granitic gneiss samples yielded weighted mean ages of 785 ± 8 Ma (MSWD = 3.0) and 784 ± 6Ma (MSWD = 1.5), respectively, and a biotite monzogranitic gneiss sample yielded a weighted mean age of 789 ± 6 Ma (MSWD = 2.3). Lu-Hf isotopic analyses on zircon grains from the two types of Neoproterozoic-aged gneisses yielded negative εHf(t) values ranging from −19.3 to −8.8 and from −18.3 to −10.4, respectively, and the corresponding two-stage Hf model age ranges are 2848–3776 Ma and 2983–3682 Ma, respectively. These granites are the product of Neoproterozoic magmatic activity and are mainly derived from the partial melting of Archean continental crust. Combining the geochemical characteristics and zircon U-Pb-Lu-Hf isotopic analyses, these A-type granitic gneisses appear to have formed in an intracontinental rift extension environment during the initial break-up of the Rodinia supercontinent, as part of the supercontinent break-up process at the northeastern margin of the South China Block. Full article
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Figure 1
<p>Geological map of the Rizhao area of the South China Block. (<b>a</b>) The inset modified from [<a href="#B15-minerals-14-00807" class="html-bibr">15</a>] shows the location of the South China Block. (<b>b</b>) Tectonic sketch map of the Rizhao and adjacent areas, modified from [<a href="#B16-minerals-14-00807" class="html-bibr">16</a>]. Abbreviations: UHP = ultra-high-pressure; HP = high-pressure.</p>
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<p>Simplified geological map of the Rizhao area.</p>
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<p>Field photographs and photomicrographs of the Rizhao granitic gneisses: (<b>a</b>–<b>c</b>) porphyritic biotite alkali feldspar granitic gneiss; (<b>d</b>–<b>f</b>) porphyritic biotite alkali feldspar granitic gneiss; (<b>g</b>–<b>i</b>) porphyritic biotite monzogranitic gneiss; (<b>j</b>–<b>l</b>) medium-fine-grained biotite monzogranitic gneiss. Abbreviations: Qtz = quartz; Bt = biotite; Pl = plagioclase; Kfs = K-feldspar; Amp = amphibolite.</p>
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<p>(<b>a</b>) Total-alkali-silica (TAS) diagram [<a href="#B22-minerals-14-00807" class="html-bibr">22</a>]; (<b>b</b>) K<sub>2</sub>O–SiO<sub>2</sub> diagram ([<a href="#B23-minerals-14-00807" class="html-bibr">23</a>] for the Rizhao granitic gneisses).</p>
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<p>(<b>a</b>) Chondrite-normalized REE and (<b>b</b>) N-MORB-normalized trace element patterns of the Rizhao granitic gneisses (normalizing factors are from [<a href="#B24-minerals-14-00807" class="html-bibr">24</a>]; N-MORB compositions are from [<a href="#B24-minerals-14-00807" class="html-bibr">24</a>]).</p>
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<p>Zircon cathodoluminescence (CL) images and U–Pb concordia diagrams of the Rizhao granitic gneisses: (<b>a</b>,<b>b</b>) RZ07, (<b>c</b>,<b>d</b>) RZ30, and (<b>e</b>,<b>f</b>) RZ47.</p>
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<p>Plots of zircon <span class="html-italic">ε</span>Hf<sub>(<span class="html-italic">t</span>)</sub> values versus U-Pb ages of the Rizhao granitic gneisses (<b>a</b>,<b>b</b>), and (<b>a</b>) is modified after [<a href="#B29-minerals-14-00807" class="html-bibr">29</a>].</p>
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<p>Discrimination plots for magmatic, metamorphic, and hydrothermal zircon according to [<a href="#B30-minerals-14-00807" class="html-bibr">30</a>,<a href="#B51-minerals-14-00807" class="html-bibr">51</a>]. (<b>a</b>) zircon Th–U plot; (<b>b</b>) zircon LREE–REE plot; (<b>c</b>) zircon (Sm/La)<sub>N</sub>–La plot; (<b>d</b>) zircon (Ce/Ce*)<sub>N</sub>–(Sm/La)<sub>N</sub> plot.</p>
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<p>Genetic discrimination diagrams for the Rizhao granitic gneisses according to [<a href="#B48-minerals-14-00807" class="html-bibr">48</a>,<a href="#B50-minerals-14-00807" class="html-bibr">50</a>,<a href="#B52-minerals-14-00807" class="html-bibr">52</a>]. (<b>a</b>) Na<sub>2</sub>O + K<sub>2</sub>O–10,000 Ga/Al discrimination diagram; (<b>b</b>) TiO<sub>2</sub>–SiO<sub>2</sub> discrimination diagram; (<b>c</b>) Nb–Y–3Ga triangular discrimination diagram; (<b>d</b>) Nb–Y–Ce triangular discrimination diagram. Abbreviation: RRG = rift-related granites; CEUG = continental uplift-related granites; A1 = A1-type granites; A2 = A2-type granites.</p>
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<p>Tectonic discrimination diagrams [<a href="#B52-minerals-14-00807" class="html-bibr">52</a>] for the Rizhao granitic gneisses. (<b>a</b>) Rb–Y+Nb diagram; (<b>b</b>) Nb–Y discrimination diagram. Abbreviation: Syn-COLG = syn-collision granite; VAG = volcanic arc granite; WPG = within plate granite; ORG = ocean ridge granite; Post-COLG = post-collision granite.</p>
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<p>Simplified genetic model showing the Neoproterozoic tectonic–magmatic evolution in the northeastern margin of Yangtze Plate.</p>
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15 pages, 29396 KiB  
Article
Geochemistry, Mineralogy, and Geochronology of the NYF Pegmatites, Jiaolesayi, Northern Qaidam Basin, China
by Long Zhang, Xianzhi Pei, Yongbao Gao, Zuochen Li, Ming Liu, Yongkang Jing, Yuanwei Wang, Kang Chen, Nan Deng, Yi Zhang and Junwei Wu
Minerals 2024, 14(8), 805; https://doi.org/10.3390/min14080805 - 9 Aug 2024
Viewed by 233
Abstract
A significant amount of pegmatite has been discovered on the northwest margin of the Qaidam basin. Among this, the Jiaolesayi pegmatite, located in the northwestern margin of the Quanji Massif (Oulongbuluke micro-continent), shows rare element mineralization potential. Detailed field investigations, along with mineralogical, [...] Read more.
A significant amount of pegmatite has been discovered on the northwest margin of the Qaidam basin. Among this, the Jiaolesayi pegmatite, located in the northwestern margin of the Quanji Massif (Oulongbuluke micro-continent), shows rare element mineralization potential. Detailed field investigations, along with mineralogical, geochemical, and zircon U-Pb geochronological studies, were carried out on the pegmatite. The results show that the Jiaolesayi pegmatite is syenite, without obvious compositional zoning in the outcrop. It exhibits a peraluminous, high-K calc-alkaline nature with strong depletions in Eu, Sr, Ba, Ti, and P, and high contents of Nb, Ta, Y, Ti, U, Th, and heavy rare earth elements (HREEs), which are primarily concentrated in allanite-(Ce), euxenite-(Y), limonite, thorite, and zircon. The geochemical and mineralogical features of the syenite pegmatite indicate it belongs to the euxenite-type in the rare element class (REE) of the NYF family, with the characteristic accessory mineral being euxenite-(Y). Its 10,000 Ga/Al ratios (2.46 to 2.96), Zr + Nb + Ce + Y contents (998 to 6202 ppm), Y/Nb ratios (0.62 to 0.75), and Yb/Ta ratios (0.80 to 1.49) show an affinity with A1-type granite. Zircons from the syenite sample yielded a weighted mean 206Pb/238U age of 413.6 ± 1.4 Ma, while the elevated U and Th concentrations in the zircons and Th/U ratios (0.04 to 0.16) suggest the possible influence of hydrothermal processes in the late-stage fractional crystallization. In the context of the regional tectonic evolution, the syenite pegmatite may have formed from a basic alkaline magma derived from an OIB-like melt with minor crustal contamination, under the post-collisional extension setting. Full article
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Figure 1
<p>(<b>A</b>) Location of the study area (based on Google Earth image). (<b>B</b>) Geological map of the northwest margin of Quanji Massif. <a href="#minerals-14-00805-f002" class="html-fig">Figure 2</a> is shown as red rectangle. (<b>C</b>–<b>E</b>) Remote sensing images of pegmatites in Niubiziliang, Dachaigou, and Jiaolesayi (unpublished images from Xi’an Center of China Geological Survey, 2020).</p>
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<p>Simplified geological map of Jiaolesayi.</p>
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<p>Photographs and photomicrographs of pegmatite outcrops and rock samples from Jiaolesayi. (<b>A</b>) Previous reported Nb-Ta deposit, represented by the blue star in <a href="#minerals-14-00805-f002" class="html-fig">Figure 2</a>. (<b>B</b>) Newly discovered pegmatite, represented by the green star in <a href="#minerals-14-00805-f002" class="html-fig">Figure 2</a>, a person in the yellow circle as a scale. (<b>C</b>) Conjugated joints and brittle fractures developed in the flesh-red pegmatite. (<b>D</b>) Graphic structure and magnetite aggregates in the pegmatite. (<b>E</b>) Quartz veins intruded into the brecciated pegmatite. (<b>F</b>) Perthitic texture of perthite under a polarizing microscope. (<b>G</b>,<b>H</b>) Photomicrographs of graphic structure under a polarizing microscope. (<b>I</b>) Pegmatite with sericitization under a polarizing microscope. Abbreviations: Afs—alkali feldspar; Mc—mica; Or—orthoclase; Pl—plagioclase; Pth—perthite; Qz—quartz; Ser—sericite.</p>
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<p>Classification diagrams for the Jiaolesayi pegmatite. (<b>A</b>) Total alkalis (Na<sub>2</sub>O + K<sub>2</sub>O) vs. SiO<sub>2</sub> (TAS) diagram after Middlemost [<a href="#B47-minerals-14-00805" class="html-bibr">47</a>]; (<b>B</b>) (A/NK) vs. (A/CNK) diagram, solid lines are after Peccerillo [<a href="#B48-minerals-14-00805" class="html-bibr">48</a>]; (<b>C</b>) K<sub>2</sub>O vs. SiO<sub>2</sub> diagram after Rickwood [<a href="#B49-minerals-14-00805" class="html-bibr">49</a>], and (<b>D</b>) Chondrite-normalized REE patterns. (<b>E</b>) Primitive mantle-normalized trace element spider diagrams for the Jiaolesayi pegmatite samples. Normalizing data for the chondrite and primitive mantle are from Sun and McDonough [<a href="#B50-minerals-14-00805" class="html-bibr">50</a>]. Symbols: green diamond—syenite pegmatite samples.</p>
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<p>(<b>A</b>) Photomicrographs (cross-polarized light) and cathodoluminescence images of all tested zircons from Jiaolesayi pegmatite. (<b>B</b>) U-Pb Concordia diagram of sample D3301-1.</p>
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<p>Photomicrographs under a reflecting microscope. (<b>A</b>) Typical subhedral euxenite-(Y) grain. (<b>B</b>) Short columnar euxenite-(Y) aggregates. (<b>C</b>) Thorite and anhedral euxenite-(Y). (<b>D</b>) Zircon, euxenite-(Y), and later-formed limonite in between. (<b>E</b>) A partial enlargement of Figure (<b>D</b>). (<b>F</b>) Image (<b>E</b>) in plane-polarized light. (<b>G</b>) An allanite-(Ce) grain. (<b>H</b>,<b>I</b>) Euhedral euxenite-(Y) grains and the EPMA test locations. (<b>J</b>) Limonite pseudomorph with residual pyrite in the core. (<b>K</b>,<b>L</b>) BSE images of euhedral euxenite-(Y) grains. Abbreviations: Aln-(Ce)—allanite-(Ce); Eux—euxenite-(Y); Lm—limonite; Py—pyrite; Thr—thorite; Zr—zircon.</p>
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<p>(<b>A</b>) Canonical discrimination analysis of AGM and EGM and (<b>B</b>) triangular discriminant graph after Škoda [<a href="#B55-minerals-14-00805" class="html-bibr">55</a>]; (<b>C</b>) FeO*/MgO vs. Zr + Nb + Ce + Y; (<b>D</b>) ternary plot of Nb-Y-Ce after Eby [<a href="#B57-minerals-14-00805" class="html-bibr">57</a>] and (<b>E</b>) Zr vs. 10,000 Ga/Al, A-type granite discrimination diagrams after Whalen [<a href="#B58-minerals-14-00805" class="html-bibr">58</a>]. Symbols: pink squares—AGM, grey squares—EGM from Škoda [<a href="#B55-minerals-14-00805" class="html-bibr">55</a>], orange crosses—EPMA data in this study (<a href="#app1-minerals-14-00805" class="html-app">Supplementary Table S3</a>).</p>
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<p>(<b>A</b>) Plots of Nb/Yb vs. Th/Yb, after Wang [<a href="#B78-minerals-14-00805" class="html-bibr">78</a>], and (<b>B</b>) plots of Y/Nb vs. Yb/Ta, after Eby [<a href="#B56-minerals-14-00805" class="html-bibr">56</a>]. Black squares represent the three end-members in the MORB-OIB array. Abbreviations: OIB, oceanic island basalt; IAB, island arc basalt; N-MORB, normal middle oceanic ridge basalt; E-MORB, enriched middle oceanic ridge basalt; A1, A<sub>1</sub> type granite; A2, A<sub>2</sub> type granite.</p>
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18 pages, 3895 KiB  
Article
Core–Shell Interface Engineering Strategies for Modulating Energy Transfer in Rare Earth-Doped Nanoparticles
by Zhaoxi Zhou, Yuan Liu, Lichao Guo, Tian Wang, Xinrong Yan, Shijiong Wei, Dehui Qiu, Desheng Chen, Xiaobo Zhang and Huangxian Ju
Nanomaterials 2024, 14(16), 1326; https://doi.org/10.3390/nano14161326 - 7 Aug 2024
Viewed by 509
Abstract
Rare earth-doped nanoparticles (RENPs) are promising biomaterials with substantial potential in biomedical applications. Their multilayered core–shell structure design allows for more diverse uses, such as orthogonal excitation. However, the typical synthesis strategies—one-pot successive layer-by-layer (LBL) method and seed-assisted (SA) method—for creating multilayered RENPs [...] Read more.
Rare earth-doped nanoparticles (RENPs) are promising biomaterials with substantial potential in biomedical applications. Their multilayered core–shell structure design allows for more diverse uses, such as orthogonal excitation. However, the typical synthesis strategies—one-pot successive layer-by-layer (LBL) method and seed-assisted (SA) method—for creating multilayered RENPs show notable differences in spectral performance. To clarify this issue, a thorough comparative analysis of the elemental distribution and spectral characteristics of RENPs synthesized by these two strategies was conducted. The SA strategy, which avoids the partial mixing stage of shell and core precursors inherent in the LBL strategy, produces RENPs with a distinct interface in elemental distribution. This unique elemental distribution reduces unnecessary energy loss via energy transfer between heterogeneous elements in different shell layers. Consequently, the synthesis method choice can effectively modulate the spectral properties of RENPs. This discovery has been applied to the design of orthogonal RENP biomedical probes with appropriate dimensions, where the SA strategy introduces a refined inert interface to prevent unnecessary energy loss. Notably, this strategy has exhibited a 4.3-fold enhancement in NIR-II in vivo imaging and a 2.1-fold increase in reactive oxygen species (ROS)-related photodynamic therapy (PDT) orthogonal applications. Full article
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<p>(<b>a</b>,<b>b</b>) depict the synthesis of RENPs using the LBL strategy, while (<b>c</b>) illustrates simplified energy-level diagrams showing the energy transfer between Nd<sup>3+</sup>, Yb<sup>3+</sup>, and Er<sup>3+</sup> ions upon 808 nm excitation. (<b>d</b>,<b>e</b>) illustrate the energy transfer between rare earth ions in RENPs-LBL and RENPs-SA, respectively.</p>
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<p>Characterization of the as-synthesized core–shell Tm-RENPs. TEM image of as-synthesized Tm-RENPs-LBL: (<b>a</b>) core, (<b>b</b>) core@shell; Tm-RENPs-SA: (<b>e</b>) core, (<b>f</b>) core@shell; Er-RENPs-LBL: (<b>i</b>) core, (<b>j</b>) core@shell; Er-RENPs-SA: (<b>m</b>) core, (<b>n</b>) core@shell. HAADF-STEM images of (<b>c</b>) Tm-RENPs-LBL, (<b>g</b>) Tm-RENPs-SA, (<b>k</b>) Er-RENPs-LBL, and (<b>o</b>) Er-RENPs-SA. Chemical concentration profiles of (<b>d</b>) Tm-RENPs-LBL, (<b>h</b>) Tm-RENPs-SA, (<b>l</b>) Er-RENPs-LBL, and (<b>p</b>) Er-RENPs-SA. The concentration profiles were obtained from the EDXS line; white arrows indicate the EDXS scan direction.</p>
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<p>Characterization of the as-synthesized core–shell–shell Ce-RENPs. TEM image of as-synthesized Ce-RENPs-LBL (<b>a</b>) core; (<b>b</b>) core@shell 1; (<b>c</b>) core@shell 1@shell 2. TEM image of Ce-RENPs-SA: (<b>d</b>) core; (<b>e</b>) core@shell 1; (<b>f</b>) core@shell 1@shell 2. (<b>g</b>) XRD patterns of Ce-RENPs-LBL and Ce-RENPs-SA. Energy transfer diagram of (<b>h</b>) Ce-RENPs-LBL and (<b>k</b>) Ce-RENPs-SA. HAADF-STEM images of (<b>i</b>) Ce-RENPs-LBL and (<b>l</b>) Ce-RENPs-SA. Chemical concentration profiles of (<b>j</b>) Ce-RENPs-LBL and (<b>m</b>) Ce-RENPs-SA. The concentration profiles were obtained from the EDXS line; white arrows indicate the EDXS scan direction.</p>
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<p>Fluorescence spectra of Tm-RENPs synthesized by two strategies under (<b>a</b>) 980 nm laser excitation and (<b>b</b>) 808 nm laser excitation. Fluorescence spectra of Er-RENPs synthesized by two strategies under (<b>c</b>) 980 nm laser excitation and (<b>d</b>) 808 nm laser excitation. The red shaded part is the DSL spectrum detected by the NIR detector.</p>
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<p>Fluorescence spectra of Ce-RENPs synthesized by two strategies under (<b>a</b>) 808 nm and (<b>b</b>) 980 nm excitation in cyclohexane at a power density of 10.0 W cm<sup>−2</sup>. The red shaded part is the DSL spectrum detected by the NIR detector.</p>
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<p>DSL spectra of (<b>a</b>) Ce-RENPs-SA and (<b>b</b>) Ce-RENPs-LBL at 808 nm excitation. (<b>c</b>) The intensity ratio of 1060 nm emission to 980 nm emission of Ce-RENPs-SA and Ce-RENPs-LBL under 808 nm laser excitation varies with the thickness of shell 1. UCL spectra of (<b>d</b>) Ce-RENPs-SA and (<b>e</b>) Ce-RENPs-LBL at 980 nm excitation. (<b>f</b>) The intensity of 540 nm emission of Ce-RENPs-SA and Ce-RENPs-LBL under 980 nm laser excitation varies with the thickness of shell 1. The blue arrow shows that the fluorescence intensity increases with the increase of shell 1 thickness, and the green arrow vice versa.</p>
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<p>(<b>a</b>) Schematic diagram illustrating the modification process of Ce-RENPs@SiO<sub>2</sub>-RB/FA; (<b>b</b>) Ce-RENPs-RB/FA probes with dual-functional NIR-II in vivo imaging and ROS response and their corresponding UCL/DSL emissions; (<b>c</b>) UCL of the Ce-RENPs and the absorption of the RB; (<b>d</b>) hydrodynamic diameters and zeta potentials of Ce-RENPs-OA, Ce-RENPs@SiO<sub>2</sub>-NH<sub>2</sub>, Ce-RENPs@SiO<sub>2</sub>-RB, and Ce-RENPs@SiO<sub>2</sub>-RB/FA. Fluorogenic interactions between SOSG and <sup>1</sup>O<sub>2</sub>, generated by photoirradiation of Ce-RENPs@SiO<sub>2</sub>-RB; (<b>e</b>) fluorescence emission spectra of RB and SOSG before irradiation and a mixture of RB and SOSG before and at different time points after 980 nm irradiation; (<b>f</b>) dependence of the fluorescence intensity on 980 nm irradiation time.</p>
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<p>(<b>a</b>) Confocal fluorescence imaging of co-cultured HeLa cells with 50 μg/mL Ce-RENPs-RB/FA nanoprobes synthesized by the LBL/SA strategy and 50 μM SOSG under 980 nm excitation for 5 min and 10 min; (<b>b</b>) intensity ratio of confocal fluorescence between SOSG and RB; (<b>c</b>) NIR-II fluorescence imaging of subcutaneously injected mice treated with Ce-RENPs-SA (left circle) and Ce-RENPs-LBL (right circle) under 980 nm laser irradiation; (<b>d</b>) the NIR-II fluorescence imaging intensity values of Ce-RENPs-LBL/SA in mice.</p>
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13 pages, 2877 KiB  
Article
Modeling of High-Power Graded-Index Fiber Amplifiers
by Anuj P. Lara, Samudra Roy and Govind P. Agrawal
Photonics 2024, 11(8), 737; https://doi.org/10.3390/photonics11080737 - 7 Aug 2024
Viewed by 282
Abstract
Graded-index fibers have been used in recent years to make high-power fiber lasers and amplifiers. Such fibers exhibit self-imaging, a phenomenon in which any optical beam periodically reproduces its original shape in undoped fibers (no gain). In this work, we employed analytic and [...] Read more.
Graded-index fibers have been used in recent years to make high-power fiber lasers and amplifiers. Such fibers exhibit self-imaging, a phenomenon in which any optical beam periodically reproduces its original shape in undoped fibers (no gain). In this work, we employed analytic and numerical techniques to study how self-imaging affects the evolution of a signal beam inside a nonlinear graded-index fiber amplifier, doped with a rare-earth element and pumped optically to provide gain all along its length. We also exploited the variational technique to reduce the computing time and to provide physical insights into the amplification process. We compared the variational and fully numerical results for the two pumping schemes (clad pumping and edge pumping) commonly used for high-power fiber amplifiers and show that the variational results are reliable in most cases of practical interest. The stability of the signal beam undergoing amplification is examined numerically by launching a noisy Gaussian beam at the input end of the amplifier. Our results show that the quality of the amplified beam should improve in the case of edge pumping when a narrower pump beam provides an optical gain that varies considerably in the radial direction of the fiber. Such an improvement does not occur for the clad pumping scheme, for which the use of a relatively wide pump beam results in a nearly uniform gain all along the fiber. Full article
(This article belongs to the Special Issue High-Power Fiber Lasers)
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<p>Schematic of a GRIN fiber amplifier with (<b>a</b>) radially varying gain and (<b>b</b>) a parabolic index profile. (<b>c</b>) Schematic showing how the signal beam evolves in a periodic fashion inside such a GRIN fiber because of self-imaging provided by the parabolic index profile.</p>
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<p>Evolution of a noisy Gaussian beam inside a GRIN fiber amplifier over a distance of 6 periods (<math display="inline"><semantics> <mrow> <mi>ξ</mi> <mo>=</mo> <mn>6</mn> <mi>π</mi> </mrow> </semantics></math>): (<b>a</b>) side pumping and (<b>b</b>) edge pumping. We scaled the <span class="html-italic">x</span> and <span class="html-italic">y</span> coordinates using the beam’s input width <math display="inline"><semantics> <msub> <mi>w</mi> <mrow> <mi>s</mi> <mn>0</mn> </mrow> </msub> </semantics></math>. The beam’s spatial profile is shown in the upper panel at four distances.</p>
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<p>Schematic of two pumping schemes: (<b>a</b>) side pumping and (<b>b</b>) edge pumping.</p>
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<p>Comparison of the variational (lines) and numerical (dots) predictions for side pumping: (<b>a</b>) amplitude, (<b>b</b>) width, (<b>c</b>) phase-front curvature, and (<b>d</b>) phase of the signal beam for <math display="inline"><semantics> <mrow> <msub> <mi>α</mi> <mi>g</mi> </msub> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math> (see <a href="#photonics-11-00737-t001" class="html-table">Table 1</a> for other parameters). The top part in (<b>a</b>) shows periodic self-imaging of the signal beam in the <math display="inline"><semantics> <mrow> <mi>y</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math> plane. The beam’s 3D evolution is shown in the top part of (<b>b</b>).</p>
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<p>Same as <a href="#photonics-11-00737-f004" class="html-fig">Figure 4</a> except that the variational (lines) and numerical (dots) results are compared in the case of edge pumping using <math display="inline"><semantics> <mrow> <msub> <mi>α</mi> <mi>g</mi> </msub> <mo>=</mo> <mn>0.05</mn> </mrow> </semantics></math>. Other parameters are identical to those used in <a href="#photonics-11-00737-f004" class="html-fig">Figure 4</a> and given in <a href="#photonics-11-00737-t001" class="html-table">Table 1</a>.</p>
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<p>Changes with distance in the averaged (<b>a</b>,<b>c</b>) amplitude and (<b>b</b>,<b>d</b>) width of the signal beam in the case of clad pumping (<b>top row</b>) and edge pumping (<b>bottom row</b>). Variational results are shown by lines while solid dots corresponding to numerical simulations. Dashed lines in (<b>b</b>,<b>d</b>) show the solution of Equation (<a href="#FD15-photonics-11-00737" class="html-disp-formula">15</a>). Beam’s quality factor <math display="inline"><semantics> <msup> <mi>M</mi> <mn>2</mn> </msup> </semantics></math> (<b>e</b>) as a function of <math display="inline"><semantics> <msub> <mi>g</mi> <mi>a</mi> </msub> </semantics></math> for <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mrow> <mi>s</mi> <mn>0</mn> </mrow> </msub> <mo>=</mo> <mn>100</mn> </mrow> </semantics></math> W and (<b>f</b>) as a function of input signal power for <math display="inline"><semantics> <mrow> <msub> <mi>g</mi> <mi>a</mi> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>. The blue and red lines correspond to clad and edge pumping, respectively; solid dots are for numerical simulations.</p>
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<p>Comparison of the variational (lines) and numerical (solid dots) predictions for a 20-m-long GRIN fiber amplifier with realistic parameter values given in the text. (<b>a</b>) Evolution along the fiber’s length of the beam’s (<b>a</b>) amplitude <math display="inline"><semantics> <msub> <mi>ψ</mi> <mrow> <mi>s</mi> <mn>0</mn> </mrow> </msub> </semantics></math>, (<b>b</b>) its average value, (<b>c</b>) average width <math display="inline"><semantics> <mrow> <mo>〈</mo> <msub> <mi>r</mi> <mi>s</mi> </msub> <mo>〉</mo> </mrow> </semantics></math>, and (<b>d</b>) amplification factor. Inset in part (<b>a</b>) shows periodic self-imaging on a magnified scale.</p>
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<p>Variation of the relative signal power and beam quality (<math display="inline"><semantics> <msup> <mi>M</mi> <mn>2</mn> </msup> </semantics></math> factor) as a function of input signal width <math display="inline"><semantics> <msub> <mi>w</mi> <mrow> <mi>s</mi> <mn>0</mn> </mrow> </msub> </semantics></math> (<b>a</b>,<b>b</b>) and radial gain width <math display="inline"><semantics> <msub> <mi>ρ</mi> <mi>g</mi> </msub> </semantics></math> (<b>c</b>,<b>d</b>) for edge (<b>left column</b>) and clad (<b>right column</b>) pumping schemes.</p>
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20 pages, 6719 KiB  
Article
Source and U-Pb Chronology of Diagenetic Fluids in the Permian Maokou Formation Dolomite Reservoir, Eastern Sichuan Basin, China
by Shuangjian Li, Jian Gao, Tianbo Yang, Tianyi Li, Tianjia Liu, Yunqing Hao, Zhiliang He and Entao Liu
Minerals 2024, 14(8), 803; https://doi.org/10.3390/min14080803 - 7 Aug 2024
Viewed by 374
Abstract
The hydrothermal dolomitization, facilitated by basement fault activities, had an important impact on the Permian Maokou Formation dolomite in the Sichuan Basin, which experienced complex diagenesis and presented strong reservoir heterogeneity. The source and age of diagenetic fluids in this succession remain controversial. [...] Read more.
The hydrothermal dolomitization, facilitated by basement fault activities, had an important impact on the Permian Maokou Formation dolomite in the Sichuan Basin, which experienced complex diagenesis and presented strong reservoir heterogeneity. The source and age of diagenetic fluids in this succession remain controversial. In this study, various analyses were implemented on samples collected from outcrops and wells near the No. 15 fault in the eastern Sichuan Basin to reconstruct the multi-stage fluid activity and analyze the impact on reservoir development, including petrology, micro-domain isotopes, rare earth elements, homogenization temperature of fluid inclusions, and Laser Ablation Inductively Coupled Plasma Mass Spectrometry (LA-ICP-MS) U-Pb dating. The homogenization temperature of primary brine inclusions in fine-grained matrix dolomite and saddle dolomite is concentrated between 100 and 150 °C, which indicates that the impacts of abnormally high temperatures of other geological bodies. The δ13C and δ18O value and low 87Sr/86Sr value indicate that the diagenetic fluid of fine-grained matrix dolomite is mainly Permian seawater. The U-Pb ages of fine-grained matrix dolomite are ~260 Ma, which coincides with the age of the main magmatism of Emeishan Large Igneous Province (ELIP), and hydrothermal fluid provided a favorable high-temperature environment in the penecontemporaneous stage. While highly radiogenic 87Sr/86Sr compositions suggests those of saddle dolomite, the high-temperature Sr-rich formation fluid. The U-Pb ages of saddle dolomite are 245–250 Ma, which coincides with the age of the 255~251 Ma magmatism of ELIP. This indicates that those should be the diagenetic products of the ELIP hydrothermal fluid in the shallow burial stage. The U-Pb age of coarse-grained calcite is 190–220 Ma, and it should be the diagenetic product of the deep burial stage. Brine inclusions associated with primary methane inclusions were developed in coarse-grained calcite, with a homogenization temperature range of 140.8–199.8 °C, which indicates that the formation fluid activities were related to hydrocarbon charging. The Permian Maokou Formation dolomite was firstly formed in the penecontemporaneous shallow burial stage, and then it was subjected to further hydrothermal dolomitization due to the basement faulting and the abnormally high heat flow during the active period of ELIP. Hydrothermal dolomitization contributed to the formation and maintenance of intercrystalline and dissolution pores, whereas it also formed saddle dolomite to fill the pores, and reduce the pore space. The influence of deep fluid activities on reservoir evolution is further distinguished. Full article
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<p>(<b>a</b>) Tectonic sketch map of China and location of the Sichuan Basin. (<b>b</b>) Distributions and thickness of the Maokou Formation dolomite and basement faults. (<b>c</b>) Stratigraphy of the Maokou Formation in the Sichuan Basin. The yellow colour is dolomite reservoir, GR = natural gamma-ray logging.</p>
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<p>Correlation between wells drilled around the No. 15 basement fault in the eastern Sichuan Basin and outcropped Maokou Formation. The yellow colour is the reservoir, and the five-pointed star is the samples.</p>
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<p>Field photographs showing the Permian Maokou Formation dolomite reservoirs in the eastern Sichuan Basin. (<b>a</b>) Maokou Formation dolomite is macroscopically layered and patchy in Tuotuoba section ((<b>a<sub>1</sub></b>) zebra-like structures, caves, and chert nodule (Cht) in the dolomite; (<b>a<sub>2</sub></b>) Fissures are filled with dolomite content (CD); (<b>a<sub>3</sub></b>) Caves are filled with dolomite and calcite content (CC). (<b>b</b>) Maokou Formation dolomite is macroscopically either layered or patchy in Fangniuba section ((<b>b<sub>1</sub></b>) CD is parallel distributed in the dolomite; (<b>b<sub>2</sub></b>,<b>b<sub>3</sub></b>) CD is in the crumby and zebra-like structures).</p>
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<p>Core characteristics of Permian Maokou Formation dolomite reservoirs in the eastern Sichuan Basin. (<b>a</b>) Micro-cracks developed in dense limestone (Lime) and were filled with CD, TL7, 5106.6 m; (<b>b</b>) Karst caves associated with cracks were both developed in gray MD; the caves were filled with CD and CC in sequence, TL601, 5534.1 m; (<b>c</b>) Cracks were developed in gray MD and filled with CD, TL601, 5530.3 m; (<b>d</b>) Cht were developed in gray MD, and floating MD, chert breccia, and CD are seen in veins. TL601, 5528.4 m; (<b>e</b>) Cht were cut by network cracks, and the cracks were filled with CD. TL601, 5528.4 m; (<b>f</b>) Echelon fractures are developed in gray MD and partially filled with CD, with a small number of residual pores developed. TL6, 5490.3 m; (<b>g</b>) The cross-section of the rock core of d, floating matrix dolomite, and chert breccia can be seen in the network cracks; (<b>h</b>) The cross-section of the rock core of e, MD, was associated with flint nodules; (<b>i</b>) In the cross-section of the rock core of f, the pyrite crystals (Py) precipitate in the MD, and a small amount of sphalerite (Sph) and CD were developed in the fracture veins.</p>
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<p>Cathodoluminescence characteristics of the Permian Maokou Formation dolomite in the eastern Sichuan Basin. (<b>a</b>) fine-grained matrix dolomite (MD) exhibits dull red luminescence; (<b>b</b>) Cave is filled with calcite (CC) and saddle dolomite (SD), surrounding rock is limestone (Lime), and the CC is cut through by later SD, TL7; (<b>c</b>) Cathode luminescence of (<b>b</b>), the CC is dark red and dolomite content (CD) is shiny red; (<b>d</b>) Cave is filled with CD, barite (Brt), fluorite (Fl), and CC in sequence, TL601; (<b>e</b>) Cave is sequentially filled with sphalerite (Sph) SD, the surrounding rock is MD, TL6; (<b>f</b>) Cathode luminescence of (<b>e</b>).</p>
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<p>Pore space characteristics of the Permian Maokou Formation dolomite in the eastern Sichuan Basin. (<b>a</b>) Caves associated with fractures are developed in dolomite, filled with Qt, CD, and CC, with a small number of residual caves and pores which have not been fully filled (blue arrow), Tuotuoba section; (<b>b</b>) Zebra-like structures and residual caves and pores (blue arrow), Tuotuoba section; (<b>c</b>) Karst caves associated with fractures were developed in dolomite, with a cemented dolomite rim and coarse calcite visible. Most of the space in the caves is not filled; TL6, 5503.8 m [<a href="#B5-minerals-14-00803" class="html-bibr">5</a>]; (<b>d</b>) A small number of intergranular pores were developed in the MD; TL6, 5510.0 m [<a href="#B5-minerals-14-00803" class="html-bibr">5</a>]; (<b>e</b>) The karst caves in the MD were mainly filled with SD, with a small amount of residual karst pores developed. TL6, 5490.3 m; (<b>f</b>) Multiple sets of fractures are developed within the MD, which have not been fully filled by the SD, and a small number of residual pores are also developed.</p>
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<p>C and O isotopes of different diagenetic phases and limestone in the Permian Maokou Formation.</p>
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<p><sup>87</sup>Sr/<sup>86</sup>Sr values of different diagenetic phases and limestone in the Permian Maokou Formation (the <sup>87</sup>Sr/<sup>86</sup>Sr ratios of Permian seawater (0.70662–0.70774, [<a href="#B40-minerals-14-00803" class="html-bibr">40</a>]) were marked for comparison).</p>
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<p>REEs in different diagenetic phases and limestone of the Permian Maokou Formation. (<b>a</b>) LM (<b>b</b>) MD (<b>c</b>) SD (<b>d</b>) CC.</p>
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<p>In situ U-Pb ages of different diagenetic phases in the Permian Maokou Formation.</p>
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<p>Photographs of fluid inclusions within different diagenetic phases in the Permian Maokou Formation. (<b>a</b>) Matrix dolomite (<b>b</b>) Saddle dolomite (<b>c</b>) Calcite 1 (<b>d</b>) Calcite 2 (<b>e</b>) Quartz 1 (<b>f</b>) Quartz 2.</p>
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<p>Homogenization temperature (<b>a</b>) and salinity of fluid inclusions (<b>b</b>) in different diagenetic phases and limestone of the Permian Maokou Formation.</p>
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<p>Relationship between burial history and diagenetic events of Permian strata in Fangniuba area, eastern Sichuan Basin [<a href="#B44-minerals-14-00803" class="html-bibr">44</a>] and the U-Pb ages of the MD, SD, and CC.</p>
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<p>Schematic model illustrating hydrothermal dolomitization in the Permian Maokou Formation [<a href="#B32-minerals-14-00803" class="html-bibr">32</a>]. Dolomitization of the Permian Maokou Formation can be divided into three stages: micritic limestone and micritic bioclastic limestone were developed in an open platform during the sedimentary period; high heat flow facilitated the long-lasting dolomitization, which resulted to the formation of fine-grained dolomite in the penecontemporaneous stage. The magnesium-rich fluid from the deep source rose along the fault and entered the gractures and vugs, forming asddle dolomite.</p>
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16 pages, 2703 KiB  
Article
Contribution of Rare Earth Elements Is Key to the Economy of the Future
by Juan-Ramón Cuadros-Muñoz, Juan-Antonio Jimber-del-Río, Rafael Sorhegui-Ortega, Michelle Zea-De la Torre and Arnaldo Vergara-Romero
Land 2024, 13(8), 1220; https://doi.org/10.3390/land13081220 - 7 Aug 2024
Viewed by 290
Abstract
An econometric model was developed to analyze the contribution of various factors to the gross value added to the agricultural, manufacturing, and service sectors in the United States. The study found that variables such as rare earth element mining, the employment it generates, [...] Read more.
An econometric model was developed to analyze the contribution of various factors to the gross value added to the agricultural, manufacturing, and service sectors in the United States. The study found that variables such as rare earth element mining, the employment it generates, the domestic consumption, imports, and prices of certain elements significantly impact economic sectors. The models showed a good fit and met the necessary statistical assumptions. Rare earth elements are essential for a wide range of technological products, with China being the leading producer and consumer. This has raised concerns about the dependence on other countries. These elements significantly impact the economy’s primary, secondary, and tertiary sectors used in agriculture, manufacturing, and services. Rare earth elements’ mining and processing are complex and expensive processes, and demand is expected to continue to increase in the future. Full article
(This article belongs to the Special Issue The Socio-Economic Values in Land Resource Management)
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<p>GVA sector.</p>
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<p>Rare earth elements’ market behavior.</p>
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<p>Dysprosium, Europium, Neodymium, and Terbium prices.</p>
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<p>Q–Q plot of standardized residuals for Model 1.</p>
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<p>Q–Q plot of standardized residuals for Model 2.</p>
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<p>Q–Q Plot Standardized Residuals Model 3.</p>
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<p>Plot of residuals vs. predicted values. (<b>a</b>) Model 1, (<b>b</b>) Model 2, (<b>c</b>) Model 3.</p>
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17 pages, 4945 KiB  
Article
Metal–Organic Framework-Derived Rare Earth Metal (Ce-N-C)-Based Catalyst for Oxygen Reduction Reactions in Dual-Chamber Microbial Fuel Cells
by Shaik Ashmath, Hao Wu, Shaik Gouse Peera and Tae-Gwan Lee
Catalysts 2024, 14(8), 506; https://doi.org/10.3390/catal14080506 - 5 Aug 2024
Viewed by 410
Abstract
Pt supported on carbon (Pt/C) is deemed as the state-of-the-art catalyst towards oxygen reduction reactions (ORRs) in chemical and biological fuel cells. However, due to the high cost and scarcity of Pt, researchers have focused on the development of Earth-abundant non-precious metal catalysts, [...] Read more.
Pt supported on carbon (Pt/C) is deemed as the state-of-the-art catalyst towards oxygen reduction reactions (ORRs) in chemical and biological fuel cells. However, due to the high cost and scarcity of Pt, researchers have focused on the development of Earth-abundant non-precious metal catalysts, hoping to replace the traditional Pt/C catalyst and successfully commercialize the chemical and biological fuel cells. In this regard, electrocatalysts made of transition metals emerged as excellent candidates for ORRs, especially the electrocatalysts made of Fe and Co in combination with N-doped carbons, which produce potentially active M-N4-C (M=Co, Fe) ORR sites. At present, however, the transition metal-based catalysts are popular; recently, electrocatalysts made of rare earth metals are emerging as efficient catalysts, due to the fact that rare earth metals also have the potential to form rare earth metal-N4-C active sites, just like transition metal Fe-N4-C/Co-N4-C. In addition, mixed valance states and uniqueness of f-orbitals of the rare earth metals are believed to improve the redox properties of the catalyst that helps in enhancing ORR activity. Among the rare earth metals, Ce is the most interesting element that can be explored as an ORR electrocatalyst in combination with the N-doped carbon. Unique f-orbitals of Ce can induce distinctive electronic behavior to the catalyst that helps to form stable coordination structures with N-doped carbons, in addition to its excellent ability to scavenge the OH produced during ORRs, therefore helping in catalyst stability. In this study, we have synthesized Ce/N-C catalysts by a metal–organic framework and pyrolysis strategy. The ORR activity of Ce/N-C catalysts has been optimized by systematically increasing the Ce content and performing RDE studies in 0.1 M HClO4 electrolyte. The Ce/N-C catalyst has been characterized systematically by both physicochemical and electrochemical characterizations. The optimized Ce/N-C-3 catalyst exhibited a half-wave potential of 0.68 V vs. RHE. In addition, the Ce/N-C-3 catalyst also delivered acceptable stability with a loss of 70 mV in its half-wave potential when compared to 110 mV loss for Pt/C (10 wt.%) catalyst, after 5000 potential cycles. When Ce/N-C-3 is used as a cathode catalyst in dual-chamber microbial fuel cells, it delivered a volumetric power density of ~300 mW m−3, along with an organic matter degradation of 74% after continuous operation of DCMFCs for 30 days. Full article
(This article belongs to the Special Issue Recent Advances in Energy-Related Materials in Catalysts, 2nd Edition)
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<p>(<b>a</b>) X-ray diffraction images of the N/C and Ce/N-C-3 catalysts. (<b>b</b>–<b>d</b>) SEM images of the Ce/ZIF precursor.</p>
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<p>(<b>a</b>–<b>d</b>) TEM images of the Ce/N-C-3 catalysts. (<b>e</b>) HAADF image and corresponding elemental mapping of (<b>f</b>) carbon, (<b>g</b>) oxygen, (<b>h</b>) nitrogen, (<b>i</b>) cerium, (<b>j</b>) overall mapping of all the elements in the Ce/N-C-3 catalysts, and (<b>k</b>) line-mapping image and (<b>l</b>) corresponding line mapping of the elements in a particular region of the Ce/N-C-3 catalyst.</p>
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<p>Deconvoluted spectra of (<b>a</b>) C1s, (<b>b</b>) N 1s, and (<b>c</b>) Ce 3d elements in the CE/N-C-3 catalysts.</p>
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<p>(<b>a</b>) LSV curves of the Ce/N-C-1,2,3 and four catalysts along with N-C catalyst. (<b>b</b>) LSV comparison of Ce/N-C-3 and Pt/C (10 wt.%) catalyst. (<b>c</b>) Tafel slopes of the Ce/N-C-3 and Pt/C (10 wt.%) catalyst. Electrolyte: O<sub>2</sub>-saturated 0.1 M HClO<sub>4</sub>, scan rate 10 mV sec<sup>−1</sup>, 1600 rpm.</p>
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<p>LSV curves recorded at different rpms of the catalysts and their corresponding K-L plots for the N-C (<b>a</b>,<b>d</b>), Ce/N-C-3 (<b>b</b>,<b>e</b>), and Pt/C (<b>c</b>,<b>f</b>) catalysts.</p>
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<p>Stability analysis of the Pt/C and Ce/N-C-3 catalysts. Cyclic voltammograms of the (<b>a</b>) Pt/C and (<b>c</b>) Ce/N-C-3 catalysts. (<b>b</b>) Linear sweep voltammetry curves of the (<b>b</b>) Pt/C and (<b>d</b>) Ce/N-C-3 catalysts. The stability conditions are 0.1 M HClO<sub>4</sub> aqueous solution as the electrolyte. Scan rate for CV cycling test 50 mV sec<sup>−1</sup>; LSV: scan rate 10 mV sec<sup>−1</sup>; 1600 rpm in O<sub>2</sub>-saturated 0.1 M HClO<sub>4.</sub> All the tests were conducted at 25 °C.</p>
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<p>(<b>a</b>) Schematic operation of the dual-chamber microbial fuel cells set up and used in this study: (<b>b</b>) OCV values of Pt/C and Ce/N-C-3 catalysts; (<b>c</b>,<b>d</b>) i–v curves for Pt/C and Ce/N-C-3 catalysts; (<b>e</b>) TOC analysis of the anolyte of the microbial fuel cells with Pt/C and Ce/N-C-3 as the cathode catalysts.</p>
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<p>Schematic representation of the Ce/ZIF and Ce/N-C- catalyst synthesis and their ORR and MFC performance analysis.</p>
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15 pages, 5973 KiB  
Article
Systematic First-Principles Investigations of the Nucleation, Growth, and Surface Properties of Al11RE3 Second-Phase Particles in Al-Based Alloys
by Wei Yin, Yuming Liu, Lan Lin, Yiru Wang, Leyi Chen, Zhaoting Li, Honghu Peng, Touwen Fan, Yuanzhi Wu, Yuanxiang Deng, Xiong Liu and Dongchu Chen
Coatings 2024, 14(8), 983; https://doi.org/10.3390/coatings14080983 - 4 Aug 2024
Viewed by 328
Abstract
At room temperature, Al alloys have excellent mechanical properties and are widely used in automotive, electronics, aerospace and other fields, but it is difficult to maintain this advantage in the middle and high temperature ranges. To address this issue, second-phase Al11RE [...] Read more.
At room temperature, Al alloys have excellent mechanical properties and are widely used in automotive, electronics, aerospace and other fields, but it is difficult to maintain this advantage in the middle and high temperature ranges. To address this issue, second-phase Al11RE3 (RE represents rare earth element) was introduced into a Al-Mg-RE alloy as its primary constituent. By incorporating RE elements as additives, this material exhibits exceptional mechanical and thermal properties at elevated temperatures. Based on first principles and quasi-harmonic approximation (QHA), the nucleation growth mechanism and surface properties of second-phase Al11RE3 were studied in this paper. The interfacial energy γα/β, strain energy ΔECS and chemical driving force ΔGV of Al11RE3 were obtained. Models1, 4, and 6 have better properties of para-site connections than inter-site connections. It is found that the resistances of particle nucleation, interface energy γα/β and strain energy ΔECS, first increase and then decrease with increased atomic number REs, but they are much smaller than the chemical driving force ΔGV. A reduced chemical driving force and a diminished nucleation radius R* are more favorable for the process of nucleation. The addition of Sc is the most unfavorable for nucleation, and La has the strongest nucleating ability, which gradually decreases as the atomic number of the lanthanide element increases. The nucleation ability of the Al11RE3 phase decreases with increasing temperature, which is consistent with the experiments. The nucleation radius R* also increases with increasing temperature, indicating that the nucleation ability decreases as the atomic number of the lanthanide elements increases. Since the smaller the nucleation radius R* the easier the nucleation, compared with model4 and 6, model1 has a smaller nucleation radius R* and the smallest increment. Thus, model1 is more prominent in the nucleation mechanism. In the particle growth study, the smaller the diffusion activation energy Q, the faster the diffusion rate in the Al matrix, and hence the higher the coiling rate, which promotes the growth of second-phase particles. The diffusion activation energy Q decreases sequentially from La to Ce and then increases with atomic number. The coarsening rate KLSW of the Al11RE3 phase in models1, 4, and 6 increased with increasing temperature, which promoted the growth of particles. This paper is intended to provide a solid theoretical basis for the production and application of aluminum alloy at high temperatures. Full article
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<p>(<b>a</b>) The slab model; (<b>b</b>) Al<sub>11</sub>RE<sub>3</sub> (001) ||Al (001) interface model of model1–3, and Al<sub>11</sub>RE<sub>3</sub> (001) ||Al (010) interface model of model4–6.</p>
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<p>The calculated non-metered surface energy range values.</p>
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<p>(<b>a</b>) The interface energy <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>γ</mi> </mrow> <mrow> <mi mathvariant="sans-serif">α</mi> <mo>/</mo> <mi mathvariant="sans-serif">β</mi> </mrow> </msub> </mrow> </semantics></math>, (<b>b</b>) strain energy <math display="inline"><semantics> <mrow> <msub> <mrow> <mo>Δ</mo> <mi>E</mi> </mrow> <mrow> <mi mathvariant="normal">C</mi> <mi mathvariant="normal">S</mi> </mrow> </msub> </mrow> </semantics></math> and (<b>c</b>) variation in chemical potential <math display="inline"><semantics> <mrow> <msub> <mrow> <mo>Δ</mo> <mi>G</mi> </mrow> <mrow> <mi mathvariant="normal">V</mi> </mrow> </msub> </mrow> </semantics></math> with atomic number at different temperatures; (<b>d</b>) variation in chemical potential <math display="inline"><semantics> <mrow> <msub> <mrow> <mo>Δ</mo> <mi>G</mi> </mrow> <mrow> <mi mathvariant="normal">V</mi> </mrow> </msub> </mrow> </semantics></math> among different Al alloy particles with temperature.</p>
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<p>(<b>a</b>–<b>c</b>) The relationship between model1, model4 and model6’s nucleation radius <span class="html-italic">R</span>* as a function of atomic number; (<b>d</b>–<b>f</b>) the curve of nucleation radius <span class="html-italic">R</span>* of model1, model4 and model6 as a function of temperature.</p>
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<p>(<b>a</b>) The function of diffusion activation energy <span class="html-italic">Q</span> as a function of rare earth atomic number; (<b>b</b>,<b>c</b>) solute concentration <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>ε</mi> </mrow> <mrow> <mo>∞</mo> </mrow> </msub> </mrow> </semantics></math> as a function of temperature and the relationship between solute and rare earth atomic number at 600 K, respectively; (<b>d</b>) coarsening rate <span class="html-italic">K</span><sub>LSW</sub> as a function of rare earth atomic number for model1, model4 and model6; (<b>e</b>–<b>g</b>) coarsening rate <span class="html-italic">K</span><sub>LSW</sub> of model1, model4 and model6 as a function of temperature.</p>
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20 pages, 4575 KiB  
Article
Zircons from Eclogite-Associated Rocks of the Marun–Keu Complex, the Polar Urals: Trace Elements and U–Pb Dating
by Laysan Salimgaraeva, Aleksey Berezin, Sergey Sergeev, Nikolai Gubanov, Ekaterina Stetskaya and Sergey Skublov
Geosciences 2024, 14(8), 206; https://doi.org/10.3390/geosciences14080206 - 2 Aug 2024
Viewed by 288
Abstract
The Marun–Keu complex plays a significant role in our understanding of the geological evolution of the Ural orogen; however, it remains poorly understood. This study aims to provide insights into the complex’s age, protolith composition, rock formation conditions, and its position in the [...] Read more.
The Marun–Keu complex plays a significant role in our understanding of the geological evolution of the Ural orogen; however, it remains poorly understood. This study aims to provide insights into the complex’s age, protolith composition, rock formation conditions, and its position in the geological history. The zircons from the host granitic gneiss are characterized by magmatic cores with an age of 473 Ma and metamorphic rims with an age of approximately 370 Ma. We suggest that the metamorphic rims were formed during eclogite metamorphism and that the metagranitoids hosting the eclogites experienced eclogite metamorphism simultaneously with the basic and ultrabasic rocks that are common in this area. Heterogeneous zircons were also isolated from the selvage of a pegmatite vein, in which four domains are distinguished, two to three of which can be identified within single grains, as follows: (1) igneous cores with an age of approximately 470 Ma and the geochemical characteristics of zircon crystallized in basic rocks; (2) zircons recrystallized during eclogite metamorphism with geochemical characteristics intermediate between those of the magmatic cores and true eclogitic zircon; (3) pegmatitic zircon, exhibiting the most sharply differentiated REE spectra of all four domains, characterized by a prominent positive Ce anomaly and a weakly expressed negative Eu anomaly; and (4) eclogitic zircon, observed in the form of veins and rims, superimposed in relation to the other three domains. The age of the latter three domains is within the error range and is estimated to be approximately 370 Ma. This indicates that the processes of eclogite metamorphism and the formation of pegmatites occurred at approximately the same time in the studied area. Full article
(This article belongs to the Section Geochemistry)
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<p>(<b>a</b>) Simplified tectonic scheme of the Urals after [<a href="#B3-geosciences-14-00206" class="html-bibr">3</a>]. MUF—Main Uralian Fault. 1—the Cis-Ural foredeep; 2—the Central Ural megazone; 3—the East Ural megazone; 4—the West Ural megazone; 5—the Tagil–Magnitogorsk megazone; 6—the Trans-Ural megazone. (<b>b</b>) The inset shows the overall geographic location of the Marun–Keu complex. (<b>c</b>) Geological map of the Marun–Keu complex [<a href="#B5-geosciences-14-00206" class="html-bibr">5</a>]. Key: 1—Quaternary; 2—Ordovician (?); 3—greenschists of the Nyarovey formation; 4—Marun–Keu series: gneisses, eclogites; 5—gneisses, granite gneisses; 6—granites with fluorite; 7—meta-rhyolites; 8—diorites, 9—gabbroids; 10—ultramafic rocks (Syum–Keu complex); 11—predominately eclogites; 12—glaucophane-hosted rocks; 13—quartz–graphite schists; 14—faults.</p>
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<p>(<b>a</b>) Schematic sampling map. (<b>b</b>) General view of the peak 1040 area. (<b>c</b>) Selvage of a pegmatite vein at the contact with its host peridotites; white circle with sample number indicates the location from which sample 2209 was collected. (<b>d</b>) Contact between granitic gneisses and peridotites, cross-cut by a 1.5 m-wide pegmatite vein; white circle with sample number indicates the location from which sample 2218 was collected. The pegmatite vein was previously excavated for exploration purposes. (<b>e</b>) Migmatization zone in granitic gneisses indicated by a blue dashed line.</p>
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<p>Microphotographs of thin section of granitic gneiss (sample 2218): (<b>a</b>,<b>c</b>) transmitted polarized light; (<b>b</b>,<b>d</b>) birefringence.</p>
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<p>(<b>a</b>) CL images of zircons from granitic gneiss (sample 2218). Colored circles indicate the SIMS analytical spots, the numbers of which correspond to those in <a href="#app1-geosciences-14-00206" class="html-app">Table S2</a> and <a href="#geosciences-14-00206-f006" class="html-fig">Figure 6</a>. Blue circles indicate magmatic cores, while green circles indicate metamorphic rims. (<b>b</b>) BSE images of zircons from granitic gneiss (sample 2218) with labeled mineral inclusions. <span class="html-italic">Png</span>—<span class="html-italic">phengite</span>.</p>
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<p>(<b>a</b>) CL images of zircons from the selvage of a pegmatite vein (sample 2209). The colored circles indicate the SIMS analytical spots, the numbers of which correspond to those in <a href="#app1-geosciences-14-00206" class="html-app">Table S3</a> and <a href="#geosciences-14-00206-f007" class="html-fig">Figure 7</a>. Blue circles indicate magmatic cores (first domain), green circles indicate recrystallized cores (second domain), navy blue circles indicate pegmatite zircon (third domain), and yellow circles indicate eclogite rims and veinlets (fourth domain). (<b>b</b>,<b>c</b>) BSE images of zircons from the selvage of a pegmatite vein (sample 2209) with labeled mineral inclusions. <span class="html-italic">Png</span>—<span class="html-italic">phengite</span>.</p>
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<p>Trace element compositions of zircons from granitic gneiss (sample 2218). (<b>a</b>) REE distribution patterns normalized to CI chondrite [<a href="#B33-geosciences-14-00206" class="html-bibr">33</a>]. (<b>b</b>–<b>d</b>) Co-variation diagrams of element pairs. The position of the analytical spots in different zircon domains is shown in <a href="#geosciences-14-00206-f004" class="html-fig">Figure 4</a> by circles of the corresponding colors.</p>
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<p>Trace element compositions of zircons from the selvage of a pegmatite vein (sample 2209). (<b>a</b>) REE distribution patterns normalized to CI chondrite [<a href="#B33-geosciences-14-00206" class="html-bibr">33</a>]. (<b>b</b>–<b>d</b>) Co-variation diagrams of element pairs. The position of the analytical spots in different zircon domains is shown in <a href="#geosciences-14-00206-f005" class="html-fig">Figure 5</a> by circles of the corresponding colors.</p>
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<p>Geochemical discriminant diagrams for zircon after [<a href="#B35-geosciences-14-00206" class="html-bibr">35</a>]. Blue markers indicate the positions of zircon cores from the selvage of the pegmatite vein (sample 2209).</p>
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<p>Concordia plot for zircons (<b>a</b>) from granitic gneiss (sample 2218) and (<b>b</b>) from the selvage of a pegmatite vein (sample 2209). Error ellipses are at 2σ confidence. The blue ellipses represent the concordia age and error. Decay constant errors are included.</p>
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15 pages, 8000 KiB  
Article
Rapid and Precise Approaches for XRF Analysis of Rare Earth Niobates
by Alexandra Alexandrovna Arkhipenko, Galina Evgenievna Marina, Mikhail Alexandrovich Ryumin, Marina Sergeevna Doronina, Natalia Alexandrovna Korotkova, Tatiana Dmitrievna Ksenofontova and Vasilisa Borisovna Baranovskaya
Analytica 2024, 5(3), 343-357; https://doi.org/10.3390/analytica5030022 - 1 Aug 2024
Viewed by 299
Abstract
This work describes a two-stage technique of X-ray fluorescence (XRF) analysis of rare earth niobates. A comparison between the two approaches revealed that the Fundamental Parameters Method (FPM) can be employed for a rapid preliminary assessment of the composition of the resulting material [...] Read more.
This work describes a two-stage technique of X-ray fluorescence (XRF) analysis of rare earth niobates. A comparison between the two approaches revealed that the Fundamental Parameters Method (FPM) can be employed for a rapid preliminary assessment of the composition of the resulting material and the construction of calibration curves can be used to determine the contents of the major elements with precision. The results of the relative standard deviation (RSD) for FPM were no more than 7%, while the approach to construct calibration curves had an RSD of no more than 1%. Calibration samples were prepared using the same synthesis method as the study samples to construct the calibration curves. The possibility of constructing calibration dependencies using mixtures of oxides was assessed, but this approach could not provide the desired accuracy. The obtained results have been shown to have a good correlation with inductively coupled plasma optical emission spectrometry. The developed technique enables the determination of the major components in niobates containing two and three rare earth elements, which are used as optical materials and medium-entropy ceramics. Full article
(This article belongs to the Section Spectroscopy)
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<p>The main spectral overlays of Er, Y, Yb, and Nb on crystal analyzers LiF200 (1), LiF200 (2), PET (1), and C002 (2).</p>
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<p>The SEM micrographs of the surfaces of rare earth niobates.</p>
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<p>The SEM-EDX mapping.</p>
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<p>The calibration curves obtained using oxide mixtures.</p>
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<p>The calibration curves obtained using synthesized calibration samples for analysis of niobates with 3 REEs.</p>
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14 pages, 6481 KiB  
Article
Up-Conversion Luminescence and Optical Temperature Sensing Properties of NaLuF4:Yb3+/Ho3+ Micron-Sized Crystals at Low Temperature
by Tian Zhang, Zhaojin Wang, Jin Hou, Xinyi Xu, Xin Zhao, Zijie Li and Siyi Di
Nanomaterials 2024, 14(15), 1292; https://doi.org/10.3390/nano14151292 - 31 Jul 2024
Viewed by 407
Abstract
Non-contact temperature sensors utilising the fluorescence intensity ratio and the unique up-conversion (UC) luminescence of rare-earth ions have numerous benefits; however, their operational temperature range has remained limited. In this study, NaLuF4:Yb3+/Ho3+ samples were prepared by the hydrothermal [...] Read more.
Non-contact temperature sensors utilising the fluorescence intensity ratio and the unique up-conversion (UC) luminescence of rare-earth ions have numerous benefits; however, their operational temperature range has remained limited. In this study, NaLuF4:Yb3+/Ho3+ samples were prepared by the hydrothermal method. The samples exhibited exceptional UC luminescence properties at low temperatures. The intensity of the green emission (with peak wavelengths of 540 and 546 nm) gradually decreased with increasing temperature, and the green emissions showed a unique change at low temperatures. In addition, we studied the dependence of the UC luminescence intensity on the excitation power and the variation in the decay lifetime with temperature. The experiments revealed excellent luminous performance and significantly enhanced sensitivity at low temperatures; the maximum absolute sensitivity Sa and relative sensitivity Sr of the 540 and 546 nm thermally coupled energy levels were 1.02% and 0.55% K−1, respectively. The potential temperature sensing properties of Yb3+/Ho3+-co-doped NaLuF4 makes it suitable for temperature sensing applications at temperatures as low as 30 K. This study offers a novel approach for the advancement of temperature sensing technology at low temperatures. Full article
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<p>X-ray diffraction (XRD) pattern of prepared NaLuF<sub>4</sub>:20%Yb<sup>3+</sup>/2%Ho<sup>3+</sup> micron-sized crystal and β-NaLuF<sub>4</sub> standard pattern.</p>
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<p>(<b>a</b>,<b>b</b>) Scanning electron microscopy (SEM) images; (<b>c</b>) Element mapping (EM) of prepared NaLuF<sub>4</sub>:20%Yb<sup>3+</sup>/2%Ho<sup>3+</sup> micron-sized crystal sample. (<b>c<sub>1</sub></b>) The doping elements distribution of NaLuF<sub>4</sub>:20%Yb<sup>3+</sup>/2%Ho<sup>3+</sup>; (<b>c<sub>2</sub></b>–<b>c<sub>6</sub></b>) corresponding to elements F, Yb, Na, Ho, and Lu, respectively.</p>
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<p>(<b>a</b>) Fluorescence spectra of samples at high temperatures under 980 nm laser excitation; (<b>b</b>) variation in intensity with temperature for samples at 540, 546, and 642 nm.</p>
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<p>(<b>a</b>) Luminescence spectra at low temperatures; (<b>b</b>) integral area ratio for 540 nm (<sup>5</sup>F<sub>4</sub>) and 546 nm (<sup>5</sup>S<sub>2</sub>).</p>
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<p>Energy level diagram of Yb<sup>3+</sup> and Ho<sup>3+</sup> ions and up-conversion (UC) mechanism.</p>
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<p>Sample UC luminescence spectra for different excitation powers at (<b>a</b>) 303 K, (<b>b</b>) 483 K, and (<b>c</b>) 4 K.</p>
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<p>Double-log diagram at 540, 546, and 642 nm at (<b>a</b>) 303 K, (<b>b</b>) 483 K, and (<b>c</b>) 4 K.</p>
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<p>Decay lifetime at high temperatures at (<b>a</b>) 540 and (<b>b</b>) 642 nm; Decay lifetime at low temperatures at (<b>c</b>) 540 and (<b>d</b>) 642 nm.</p>
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<p>Fluorescence intensity ratio (FIR) changes and response to high temperature.</p>
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<p>(<b>a</b>) Luminescence intensity ratio (LIR) changes and response to temperature; (<b>b</b>) absolute sensitivity to temperature; (<b>c</b>) relative sensitivity to temperature.</p>
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<p>(<b>a</b>) FIR changes and response to low temperature; (<b>b</b>) the relationship between S<span class="html-italic"><sub>a</sub></span> and temperature; (<b>c</b>) the relationship between S<span class="html-italic"><sub>r</sub></span> and temperature.</p>
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<p>(<b>a</b>) Temperature cycling measurement of NaLuF<sub>4</sub>:Yb<sup>3+</sup>/Ho<sup>3+</sup> between 363 K and 483 K; (<b>b</b>) Temperature cycling measurement of NaLuF<sub>4</sub>:Yb<sup>3+</sup>/Ho<sup>3+</sup> between 30 and 150 K.</p>
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17 pages, 4948 KiB  
Article
Hydrocarbon Accumulation and Overpressure Evolution in Deep–Ultradeep Reservoirs in the Case of the Guole Area of the Tarim Basin
by Zhanfeng Qiao, Tianfu Zhang, Ruyue Wang, Yahao Huang, Yifan Xue, Jiajun Chen, Haonan Tian, Anjiang Shen and Chunsong Si
Minerals 2024, 14(8), 790; https://doi.org/10.3390/min14080790 - 31 Jul 2024
Viewed by 331
Abstract
Usually, deep oil and gas accumulation is often controlled by strike–slip faults. However, in the Tarim Basin, deep Ordovician oil and gas accumulations are also found in areas far from the fault zone. The process of oil and gas accumulation in deep reservoirs [...] Read more.
Usually, deep oil and gas accumulation is often controlled by strike–slip faults. However, in the Tarim Basin, deep Ordovician oil and gas accumulations are also found in areas far from the fault zone. The process of oil and gas accumulation in deep reservoirs far from strike–slip fault zones is still unclear at present. The source and evolution of Ordovician fluids were analyzed using inclusion geochemical methods and the U–Pb dating technique. The analysis of rare earth elements and carbon–oxygen–strontium isotopes in the reservoirs showed that the reservoirs were weakly modified by diagenetic fluid. The fluid was derived from the fluid formation during the same period as the seawater, and no oxidizing fluid invaded the reservoir. The late oil and gas reservoirs had good sealing properties. The U–Pb dating results combined with homogenization temperature data revealed that the first-stage oil was charged during the Late Caledonian Period, and the second-stage natural gas was charged during the Middle Yanshanian Period. The evolution of the paleo-pressure showed that the charging of natural gas in the Middle Yanshanian was the main reason for the formation of reservoir overpressure. The strike–slip fault zone was basically inactive in the Middle Yanshanian. During this period, the charged natural gas mainly migrated to the reservoir along the unconformity surface and the open strike–slip fault zone in the upper part of the Ordovician reservoir. The source of the fluid shows that the reservoir in the late stage had good sealing properties, and there was no intrusion of exogenous fluid. The overpressure in the reservoir is well preserved at present. Full article
(This article belongs to the Topic Petroleum Geology and Geochemistry of Sedimentary Basins)
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Figure 1

Figure 1
<p>Strike–slip fault structure distribution map of the Tarim Basin and Lower Paleozoic stratigraphic histogram of the Guole area.</p>
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<p>Transmitted-light and cathodoluminescence images of calcite veins in carbonate rock samples from the Guole area. (<b>a</b>,<b>b</b>,<b>d</b>): Transmission light photographs of calcite vein body in well GL1. (<b>c</b>,<b>e</b>): Cathode luminescence photographs of calcite vein body in well GL1. (<b>f</b>,<b>h</b>,<b>j</b>): Transmission light photographs of calcite vein body in well GL2. (<b>g</b>,<b>i</b>,<b>k</b>): Cathode luminescence photographs of calcite vein body in well GL2.</p>
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<p>Rare earth element partitioning model of calcite samples from Wells GL1 and GL2 in Guole area.</p>
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<p>(<b>a</b>) Fluorescence photograph of light-blue fluorescent crude oil inclusion in Well GL1; (<b>b</b>) fluorescence photograph of blue–green fluorescent crude oil inclusion in Well GL2; (<b>c</b>,<b>d</b>) transmitted-light photographs of secondary gas inclusion in Well GL2.</p>
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<p>Distribution of homogenization temperatures for oil inclusions coexisting with aqueous inclusions in calcite veins of Ordovician reservoirs in the Guole area.</p>
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<p>Burial–thermal–hydrocarbon generation history of the strike–slip fault zone in the Guole area.</p>
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<p>U–Pb isotope dating of isochrons in calcite veins with primary oil inclusions from Well GL2.</p>
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<p>Simulation curves of the minimum trapping pressure of oil inclusions in the calcite veins of the Ordovician Yijianfang Formation in the Guole area.</p>
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<p>Raman spectra of CH<sub>4</sub> inclusions in calcite veins of the Ordovician Yijianfang Formation in the Guole area.</p>
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<p>Pressure evolution restoration map of the Ordovician Yijianfang Formation in the Guole area.</p>
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<p>Strike–slip fault activity period and growth process diagram.</p>
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<p>Oil and gas accumulation model in Guole area. (<b>a</b>) Middle and Late Caledonian hydrocarbon accumulation model in Guole area. (<b>b</b>) Early and Middle Yanshanian hydrocarbon accumulation model in Guole area.</p>
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