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Keywords = lanthanides

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14 pages, 925 KiB  
Article
Evaluation of Metal Accumulation in Escherichia coli Expressing SPL2 by Single-Cell Inductively Coupled Plasma Mass Spectrometry
by Yasunori Fukumoto, Enhui Li, Yu-ki Tanaka, Noriyuki Suzuki and Yasumitsu Ogra
Int. J. Mol. Sci. 2025, 26(5), 1905; https://doi.org/10.3390/ijms26051905 (registering DOI) - 22 Feb 2025
Abstract
Rare earth elements, comprising 17 elements including 15 lanthanides, are essential components in numerous high-tech applications. While physicochemical methods are commonly employed to remove toxic heavy metals (e.g., cadmium and mercury) from industrial wastewater, biological approaches offer increasingly attractive alternatives. Biomining, which utilizes [...] Read more.
Rare earth elements, comprising 17 elements including 15 lanthanides, are essential components in numerous high-tech applications. While physicochemical methods are commonly employed to remove toxic heavy metals (e.g., cadmium and mercury) from industrial wastewater, biological approaches offer increasingly attractive alternatives. Biomining, which utilizes microorganisms to extract valuable metals from ores and industrial wastes, and bioremediation, which leverages microorganisms to adsorb and transport metal ions into cells via active transport, provide eco-friendly solutions for resource recovery and environmental remediation. In this study, we investigated the potential of three recently identified lanthanide-binding proteins—SPL2, lanpepsy, and lanmodulin—for applications in these areas using single-cell inductively coupled plasma mass spectrometry (scICP-MS). Our results demonstrate that SPL2 exhibits superior characteristics for lanthanide and cadmium bioremediation. Heterologous expression of a cytosolic fragment of SPL2 in bacteria resulted in high expression levels and solubility. Single-cell ICP-MS analysis revealed that these recombinant bacteria accumulated lanthanum, cobalt, nickel, and cadmium, effectively sequestering lanthanum and cadmium from the culture media. Furthermore, SPL2 expression conferred enhanced bacterial tolerance to cadmium exposure. These findings establish SPL2 as a promising candidate for developing recombinant bacterial systems for heavy metal bioremediation and rare earth element biomining. Full article
(This article belongs to the Special Issue Mechanisms of Heavy Metal Toxicity: 3rd Edition)
14 pages, 5032 KiB  
Article
Er(III) and Yb(III) Complexes with a Tripodal Nitroxyl Radical: Magnetochemical Study and Ab Initio Calculations
by Mauro Perfetti, Alexey A. Dmitriev and Kira E. Vostrikova
Magnetochemistry 2025, 11(2), 16; https://doi.org/10.3390/magnetochemistry11020016 - 14 Feb 2025
Viewed by 253
Abstract
In this paper, we investigate the magnetic exchange interaction and magnetization dynamics of two new members of the [LnRad(NO3)3] family, where Rad is a tripodal nitroxide, and Ln is Er(III) or Yb(III), having the prolate type electron density. Single [...] Read more.
In this paper, we investigate the magnetic exchange interaction and magnetization dynamics of two new members of the [LnRad(NO3)3] family, where Rad is a tripodal nitroxide, and Ln is Er(III) or Yb(III), having the prolate type electron density. Single OK crystal and powder X-ray diffraction studies showed that these complexes are isostructural with their previously investigated Y, Gd, Dy, Tm, Tb, Eu, and Lu congeners. A magnetometric investigation, supported by ab initio calculations, showed the presence of antiferromagnetic coupling between the lanthanide ion and the radical in both compounds with estimated J values of ≈7 and ≈20 cm−1 for Er and Yb, respectively (+J SeffS formalism). Full article
(This article belongs to the Special Issue Latest Research on the Magnetic Properties of Coordination Compounds)
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Figure 1

Figure 1
<p>(<b>a</b>) Tridentate oxazolidine radical, (Rad): 4,4-dimethyl-2,2-bis(pyridin-2-yl)-1,3-oxazolidine-3-oxyl.; (<b>b</b>) molecular structure of [LnRad(NO<sub>3</sub>)<sub>3</sub>], hydrogen atoms are omitted for clarity.</p>
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<p>Simulated (blue) and experimental powder patterns of the compounds [LnRad(NO<sub>3</sub>)<sub>3</sub>].</p>
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<p>Experimental (circles) and theoretical (red solid lines) magnetic data: (<b>a</b>) dependence of <span class="html-italic">χT</span> vs. <span class="html-italic">T</span> and magnetization plots <span class="html-italic">M</span> vs. <span class="html-italic">B</span> for <b>1</b> at three different temperatures (insert); (<b>b</b>) dependence of <span class="html-italic">χT</span> vs. <span class="html-italic">T</span> and magnetization plots <span class="html-italic">M</span> vs. <span class="html-italic">B</span> at three different temperatures (insert) for <b>2</b>; (<b>c</b>) magnetization plot <span class="html-italic">M</span> vs. <span class="html-italic">B</span> for <b>1</b> at 2 K; (<b>d</b>) magnetization plot <span class="html-italic">M</span> vs. <span class="html-italic">B</span> for <b>2</b> at 2 K. See text for details.</p>
Full article ">Figure 4
<p>MOs involved in the active space of the CASSCF (n<sub>el</sub>,8) (n<sub>el</sub> = 12 for Er, 14 for Yb) calculations for complexes <b>1</b> and <b>2</b>.</p>
Full article ">Figure 5
<p>(<b>a</b>) The 35 quintets and triplets for <b>1</b> found at SA–CASSCF(12,8) (CASSCF) and SA–CASSCF(12,8)/NEVPT2 (NEVPT2) levels and SO multiplets after the accounting of SOC at QDPT level (CASSCF–SOC and NEVPT2–SOC). (<b>b</b>) The 7 triplets and singlets for <b>2</b> obtained at SA–CASSCF(12,8) (CASSCF) and SA–CASSCF(12,8)/NEVPT2 (NEVPT2) levels and SO–multiplets after the accounting of SOC at QDPT level (CASSCF–SOC and NEVPT2–SOC). The energy structure under 3000 cm<sup>−1</sup> for (<b>c</b>) <b>1</b> and (<b>d</b>) <b>2</b>. See, also, <a href="#app1-magnetochemistry-11-00016" class="html-app">Tables S2 and S3</a> in <a href="#app1-magnetochemistry-11-00016" class="html-app">Supplementary Materials</a>.</p>
Full article ">Figure 6
<p><span class="html-italic">M</span> vs. <span class="html-italic">B</span> plot of <b>1</b> (<b>a</b>) and <b>2</b> (<b>b</b>). The symbols are the experimental points, while the blue and red solid lines represent the best simulation using the <span class="html-italic">g</span> and <span class="html-italic">J</span> parameters reported in <a href="#magnetochemistry-11-00016-t003" class="html-table">Table 3</a>.</p>
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15 pages, 5216 KiB  
Article
Anomalous Diffusion and Decay of Clusters of Dopants in Lanthanide-Doped Nanocrystals
by Grzegorz Pawlik and Antoni C. Mitus
Materials 2025, 18(4), 815; https://doi.org/10.3390/ma18040815 - 13 Feb 2025
Viewed by 326
Abstract
Upconversion (UC) luminescence in doped lanthanide nanocrystals is associated with the energy migration (EM) process within clusters of dopant ions. The process of the synthesis of core–shell nanocrystals occurs at elevated temperatures, promoting the diffusion of the dopants into the shell accompanied by [...] Read more.
Upconversion (UC) luminescence in doped lanthanide nanocrystals is associated with the energy migration (EM) process within clusters of dopant ions. The process of the synthesis of core–shell nanocrystals occurs at elevated temperatures, promoting the diffusion of the dopants into the shell accompanied by the decay of dopant clusters. The details of this unwanted effect are poorly understood. In this paper, we theoretically study a model of the diffusion of dopant ions in a nanocrystal using Monte Carlo (MC) simulations. We characterize the diffusion, spatial neighboring relations and clustering of dopant ions regarding the function of reduced temperature and MC time of the heating process. The dopants undergo a weak subdiffusion caused by trapping effects. The main results of this study are as follows: (i) the phase diagram of the variables reduced the temperature and MC time, which separates the enhanced and limited cluster-driven EM regimes, and (ii) a dependence of the average nearest distance between Yb ions as a function of reduced temperature, the concentration of Yb ions and MC time was found. In both cases, the requirements for an effective EM are formulated. Full article
(This article belongs to the Special Issue Development and Research on Theoretical Chemistry in Materials)
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Figure 1

Figure 1
<p>(<b>a</b>) Visualization of the geometry of the core–shell nanocrystal. <math display="inline"><semantics> <mrow> <mi>D</mi> </mrow> </semantics></math> denotes the thickness of the shell. Red atoms represent ions Yb/Er in the initial state. (<b>b</b>) Potential energy diagram for the direct atom–atom exchange.</p>
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<p>The cell for Y atoms and possible directions of movements of a dopant atom for <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>R</mi> </mrow> <mrow> <mi>c</mi> </mrow> </msub> <mo>=</mo> <mn>0.4</mn> </mrow> </semantics></math> nm (<b>a</b>). Non-normalized histogram of nearest neighbors (Y atoms) of a dopant calculated for <math display="inline"><semantics> <mrow> <mi>R</mi> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math> nm (<b>b</b>). Cross-section of the nanocrystal with positions of Y atoms and 5% of dopant Yb atoms (red spheres) for the core with radius <math display="inline"><semantics> <mrow> <mi>R</mi> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math> nm and the shell with thickness <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math> nm (<b>c</b>).</p>
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<p>Trajectory of a chosen dopant atom in core–shell system for 1000 MCS (<math display="inline"><semantics> <mrow> <msup> <mrow> <mi>T</mi> </mrow> <mrow> <mo>*</mo> </mrow> </msup> <mo>=</mo> <mn>0.4</mn> <mo>)</mo> </mrow> </semantics></math>.</p>
Full article ">Figure 4
<p>Exemplary trajectory of a dopant ion (red) in time interval of 1000 MCS and positions of 27,985 Y atoms (gray) (<b>a</b>). Unnormalized histogram of the first passage time for dopant atom to cross the surface of the nanocrystal (with the mean value <math display="inline"><semantics> <mrow> <mn>4.8</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mn>3</mn> </mrow> </msup> </mrow> </semantics></math> MCS) for <math display="inline"><semantics> <mrow> <mi>R</mi> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math> nm, <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>T</mi> </mrow> <mrow> <mo>*</mo> </mrow> </msup> <mo> </mo> </mrow> </semantics></math>= 0.4 (<b>b</b>).</p>
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<p>Temperature dependence of the exponent γ (red full circles) and linear fit (red line). The log–log plot of displacement <math display="inline"><semantics> <mrow> <msup> <mrow> <mfenced separators="|"> <mrow> <mo>∆</mo> <mi>r</mi> </mrow> </mfenced> </mrow> <mrow> <mn>2</mn> </mrow> </msup> <mfenced separators="|"> <mrow> <mi>t</mi> </mrow> </mfenced> </mrow> </semantics></math> and linear fits for the time interval <math display="inline"><semantics> <mrow> <mn>1.5</mn> <mo>&lt;</mo> <mi>l</mi> <mi>o</mi> <mi>g</mi> <mo>⁡</mo> <mfenced separators="|"> <mrow> <mi>t</mi> </mrow> </mfenced> <mo>&lt;</mo> <mn>3</mn> </mrow> </semantics></math> for <span class="html-italic">T</span>* = 0.15 (inset).</p>
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<p>The average number of nearest neighbors in a simple cubic lattice as a function of obstacle concentration (<b>a</b>) and the crossover from normal to anomalous diffusion (<b>b</b>,<b>c</b>).</p>
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<p>Plots of the upper boundary for the diffusion constant <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi>D</mi> <mo> </mo> </mrow> <mo>~</mo> </mover> </mrow> </semantics></math> against temperature. Inset: time dependence of <math display="inline"><semantics> <mrow> <msup> <mrow> <mfenced separators="|"> <mrow> <mo>∆</mo> <mover accent="true"> <mrow> <mi>r</mi> </mrow> <mo stretchy="false">→</mo> </mover> </mrow> </mfenced> </mrow> <mrow> <mn>2</mn> </mrow> </msup> <mo>/</mo> <mo stretchy="false">(</mo> <mn>6</mn> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>.</p>
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<p>Plot of average distance <math display="inline"><semantics> <mrow> <mfenced open="&#x27E8;" close="&#x27E9;" separators="|"> <mrow> <msub> <mrow> <mi>d</mi> </mrow> <mrow> <mi>m</mi> <mi>i</mi> <mi>n</mi> </mrow> </msub> </mrow> </mfenced> </mrow> </semantics></math> as a function of reduced temperature <span class="html-italic">T</span>* (<b>a</b>). Temporal dependence of <math display="inline"><semantics> <mrow> <mfenced open="&#x27E8;" close="&#x27E9;" separators="|"> <mrow> <msub> <mrow> <mi>d</mi> </mrow> <mrow> <mi>m</mi> <mi>i</mi> <mi>n</mi> </mrow> </msub> </mrow> </mfenced> </mrow> </semantics></math> for a few dopant concentrations at <span class="html-italic">T</span>* = 0.4 (<b>b</b>).</p>
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<p>The dependence of <math display="inline"><semantics> <mrow> <mfenced open="&#x27E8;" close="&#x27E9;" separators="|"> <mrow> <msub> <mrow> <mi>d</mi> </mrow> <mrow> <mi>m</mi> <mi>i</mi> <mi>n</mi> </mrow> </msub> </mrow> </mfenced> </mrow> </semantics></math> on time and temperature <span class="html-italic">T</span>* for the dopant concentration 20% (<b>a</b>) and 5% (<b>b</b>).</p>
Full article ">Figure 10
<p>The dependence of <math display="inline"><semantics> <mrow> <mfenced open="&#x27E8;" close="&#x27E9;" separators="|"> <mrow> <msub> <mrow> <mi>d</mi> </mrow> <mrow> <mi>m</mi> <mi>i</mi> <mi>n</mi> </mrow> </msub> </mrow> </mfenced> </mrow> </semantics></math> on time and dopant concentration <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>c</mi> </mrow> <mrow> <mi>Y</mi> <mi>b</mi> </mrow> </msub> </mrow> </semantics></math> for <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>T</mi> </mrow> <mrow> <mi mathvariant="normal">*</mi> </mrow> </msup> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math> (<b>a</b>), <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>T</mi> </mrow> <mrow> <mi mathvariant="normal">*</mi> </mrow> </msup> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math> (<b>b</b>), <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>T</mi> </mrow> <mrow> <mi mathvariant="normal">*</mi> </mrow> </msup> <mo>=</mo> <mn>0.4</mn> </mrow> </semantics></math> (<b>c</b>).</p>
Full article ">Figure 11
<p>The distribution of sizes of Yb clusters for <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>c</mi> </mrow> <mrow> <mi>Y</mi> <mi>b</mi> </mrow> </msub> <mo>=</mo> <mn>10</mn> <mo>%</mo> </mrow> </semantics></math> (<b>a</b>) and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>c</mi> </mrow> <mrow> <mi>Y</mi> <mi>b</mi> </mrow> </msub> <mo>=</mo> <mn>40</mn> <mo>%</mo> </mrow> </semantics></math> (<b>b</b>). Connection/transfer probability between Yb ions. Vertical lines denote nearest distances between Yb ions (<b>c</b>). Temporal dependence of spatial distribution of Yb ions (<b>d</b>–<b>f</b>). Calculations were performed for <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>T</mi> </mrow> <mrow> <mo>*</mo> </mrow> </msup> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 12
<p>The dependence of the threshold time <math display="inline"><semantics> <mrow> <mi mathvariant="normal">τ</mi> </mrow> </semantics></math> on reduced temperature; see text for more details.</p>
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<p>Total number <span class="html-italic">N</span>(<span class="html-italic">k</span>) of Er ions which have <span class="html-italic">k</span> (<span class="html-italic">k</span> = 0, …, 8) Yb ions as nearest neighbors, calculated for a few concentrations of Yb ions, and at chosen stages of dopant ion diffusion from the core into the shell. Calculations performed for <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>c</mi> </mrow> <mrow> <mi>E</mi> <mi>r</mi> </mrow> </msub> <mo>=</mo> <mn>5</mn> <mo>%</mo> </mrow> </semantics></math>.</p>
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14 pages, 2930 KiB  
Article
High-Level Lanthanide-Doped Upconversion Nanoparticles-Based Aptasensor to Increase Carcinoembryonic Antigen Detection Sensitivity
by Lujun Niu, Qiren Sun, Shijia Wei, Dixiang Gong, Enhui Wang, Yan Chen, Lu Xia, Xingyu Liu, Langping Tu, Long Shao, Hongfei Li and Jing Zuo
Materials 2025, 18(4), 796; https://doi.org/10.3390/ma18040796 - 11 Feb 2025
Viewed by 409
Abstract
Boosting the accuracy and speed of cancer detection is highly desirous in tumor detection, and sensors capable of detecting carcinoembryonic antigen (CEA) have great application prospects in this field. A highly sensitive sensor is constructed based on the fluorescence resonance energy transfer (FRET) [...] Read more.
Boosting the accuracy and speed of cancer detection is highly desirous in tumor detection, and sensors capable of detecting carcinoembryonic antigen (CEA) have great application prospects in this field. A highly sensitive sensor is constructed based on the fluorescence resonance energy transfer (FRET) with heavily rare-earth-doped upconversion nanoparticles (UCNPs) as energy donors and polydopamine nanoparticles (PDA NPs) as energy acceptors. This sensor detects the fluctuations in CEA molecules via luminescence quenching and recovery resulting from a competitive binding assay between CEA and PDA NPs. The high-level-doped design of UCNPs (i.e., NaYF4@NaYbF4:1%Tm@NaYF4) is beneficial, providing upconversion luminescence intensity that is more than 10 times higher than that of the conventional low-level-doped UCNPs (i.e., NaYF4@NaYF4:20%Yb, 0.2%Tm@NaYF4). The sensor exhibits impressive sensitivity. Specifically, in diluted fetal bovine serum, the detection limit reaches 0.013 ng/mL in the range of 0–1.5 ng/mL (S/N = 3), while the detection limit is 1.38 ng/mL in the range of 1.5–250 ng/mL (S/N = 3). This method has great potential for future applications in the rapid and early diagnosis and treatment of cancer. Full article
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Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>A schematic illustration of the formation of a biosensor for detecting carcinoembryonic antigen (CEA) based on upconversion nanoparticles (UCNPs)-polydopamine nanoparticles (PDA NPs): (<b>a</b>) the synthesis process of NaYF<sub>4</sub>@NaYF<sub>4</sub>:Yb,Tm@NaYF<sub>4</sub> core–shell–shell UCNPs; (<b>b</b>) the construction of the UCNP and CEA aptamer combination; (<b>c</b>) polydopamine synthesis; (<b>d</b>) the fluorescence quenching and fluorescence recovery processes of the detecting system.</p>
Full article ">Figure 2
<p>Characterization of synthesized nanoparticles: (<b>a</b>) HAADF-STEM image of NaYF<sub>4</sub>@NaYbF<sub>4</sub>:1%Tm@NaYF<sub>4</sub> core–shell–shell nanoparticles; (<b>b</b>) scanning TEM image and element mappings of Tm, Yb, Y, and Na, with an overlap of Y, Tm, and Yb for the sample in panel a; (<b>c</b>) the particle size distribution of the sample in panel a; (<b>d</b>) high-resolution TEM image of one NaYF<sub>4</sub>@NaYbF<sub>4</sub>:1%Tm@NaYF<sub>4</sub> core–shell–shell nanoparticle; (<b>e</b>) XRD image of NaYF<sub>4</sub>@NaYbF<sub>4</sub>:1%Tm@NaYF<sub>4</sub> and the standard card (JCDSP No. 16-0334).</p>
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<p>(<b>a</b>) FTIR spectra of NaYF<sub>4</sub>@NaYbF<sub>4</sub>:1%Tm@NaYF<sub>4</sub> (without an organic layer, bule line), and NaYF<sub>4</sub>@NaYbF<sub>4</sub>:1%Tm@NaYF<sub>4</sub>-CEA aptamer (green line); (<b>b</b>) UV–vis absorption spectra of NaYF<sub>4</sub>@NaYbF<sub>4</sub>:1%Tm@NaYF<sub>4</sub> and NaYF<sub>4</sub>@NaYbF<sub>4</sub>:1%Tm@NaYF<sub>4</sub>-CEA aptamer; (<b>c</b>) FTIR spectra of dopamine and PDA NPs; (<b>d</b>) absorption spectra of PDA NPs, and emission spectra of NaYF<sub>4</sub>@NaYbF<sub>4</sub>:1%Tm@NaYF<sub>4</sub> UCNPs.</p>
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<p>(<b>a</b>) Fluorescence quenching of NaYF<sub>4</sub>@NaYbF<sub>4</sub>:1%Tm@NaYF<sub>4</sub>-CEA aptamer system with different concentrations of PDA NPs (the reaction time was fixed at 20 min); (<b>b</b>) reaction-time-dependent fluorescence quenching of NaYF<sub>4</sub>@NaYbF<sub>4</sub>:1%Tm@NaYF<sub>4</sub>-CEA aptamer-PDA system (the concentration of PDA NPs was fixed at 0.35 μg/μL).</p>
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<p>(<b>a</b>) Fluorescence recovery of Y@99Yb1Tm@Y-CEA aptamer-PDA NP system with different CEA concentrations; (<b>b</b>) fluorescence recovery of Y@20Yb0.2Tm@Y-CEA aptamer-PDA NP system with different CEA concentrations; (<b>c</b>) steady-state emission spectra of two types of UCNP under 980 nm laser irradiation (0.80 W cm<sup>−2</sup>); (<b>d</b>) relative fluorescence intensity of sensor (0.01 mg/mL) in presence of Gly (1.0 μg/mL), L-AscH2 (1.0 μg/mL), L-Cys (1.0 μg/mL), Glu (1.0 μg/mL), BSA (1.0 μg/mL), NaCl (1.0 μg/mL), and CEA (50 ng/mL). Experiments were performed in HEPES buffer (10 mM, pH 7.4).</p>
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<p>Fluorescence recovery of Y@99Yb1Tm@Y-CEA aptamer-PDA NPs system with different CEA concentrations in diluted fetal bovine serum.</p>
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27 pages, 2585 KiB  
Review
Lanthanide-Doped Upconversion Luminescence: A New Frontier in Pathogenic Bacteria and Metabolite Detection from Design to Point-of-Care Application
by Huanhuan Li, Yu Wu, Muhammad Shoaib, Wei Sheng, Qiyi Bei and Arul Murugesan
Chemosensors 2025, 13(2), 60; https://doi.org/10.3390/chemosensors13020060 - 8 Feb 2025
Viewed by 425
Abstract
Pathogens and their metabolites in food present significant risks to both human health and economic development. Rising living standards and increasing awareness of food safety have driven the demand for sensitive and rapid detection methods. Lanthanide-doped upconversion nanoparticles (UCNPs), with their exceptional optical [...] Read more.
Pathogens and their metabolites in food present significant risks to both human health and economic development. Rising living standards and increasing awareness of food safety have driven the demand for sensitive and rapid detection methods. Lanthanide-doped upconversion nanoparticles (UCNPs), with their exceptional optical properties, have emerged as a promising platform for developing biosensors to detect pathogenic bacteria and their metabolites. The integration of UCNPs with point-of-care testing (POCT) has garnered considerable attention for its portability and immediacy, highlighting a promising future for biosensing, particularly in applications requiring quick and accurate diagnostics. This review explores the recognition elements and design principles commonly used in UCNP-based biosensors and examines various applications, including lateral flow assays, microfluidic systems, photoelectrochemical devices, and smartphone-integrated platforms. Despite significant advancements, challenges remain in the applicability and commercialization of UCNP-based biosensing technology. Future research should focus on enhancing sensitivity and specificity, developing scalable and cost-effective production methods, and integrating with advanced digital technologies to enable broader adoption. Addressing these challenges, establishing regulatory frameworks, and considering sustainability will be crucial to fully realizing the potential of UCNP-based biosensors. Full article
(This article belongs to the Special Issue Advanced Materials Based Fluorescent Sensors)
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Figure 1

Figure 1
<p>Schematic illustration on the timeline of the development of the UCNPs, especially its application in detecting foodborne bacteria and their metabolites.</p>
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<p>The recent challenges and future prospects of UCNP-based sensing systems for food safety applications.</p>
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<p>Schematic illustration of recognition elements utilized for constructing UCNP-based biosensors, including Abs, Apts, MIPs, and enzymes.</p>
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<p>The design principles for constructing UCNP-based biosensors, including FRET, IFE, MNPs, PET, centrifugation, and test strips.</p>
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<p>Schematic illustration of (<b>A</b>) an aptamer-based LFA based on UCNPs for the quantitative detection of ZEN [<a href="#B34-chemosensors-13-00060" class="html-bibr">34</a>]; (<b>B</b>) an aptamer-based test strip based on the UCNPs for quantitatively detecting ZEN [<a href="#B129-chemosensors-13-00060" class="html-bibr">129</a>]; (<b>C</b>) a cNIR-PECIA based on UCNPs for the portable detection of OA [<a href="#B133-chemosensors-13-00060" class="html-bibr">133</a>]; (<b>D</b>) a handheld UCNP-LFA biosensor with the assistance of a smartphone [<a href="#B135-chemosensors-13-00060" class="html-bibr">135</a>].</p>
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11 pages, 2898 KiB  
Article
Environmentally Friendly Photoluminescent Coatings for Corrosion Sensing
by Carmen R. Tubio, Laura Garea, Bárbara D. D. Cruz, Daniela M. Correia, Verónica de Zea Bermudez and Senentxu Lanceros-Mendez
Polymers 2025, 17(3), 389; https://doi.org/10.3390/polym17030389 - 31 Jan 2025
Viewed by 642
Abstract
Although an increasing number of studies are being devoted to the field of corrosion, with topics from protection to sensing strategies, there is still a lack of research based on environmentally eco-friendly materials, which is essential in the transition to sustainable technologies. Herein, [...] Read more.
Although an increasing number of studies are being devoted to the field of corrosion, with topics from protection to sensing strategies, there is still a lack of research based on environmentally eco-friendly materials, which is essential in the transition to sustainable technologies. Herein, environmentally friendly composites, based on photoluminescent salts dispersed in vegetable oil-based resins, are prepared and investigated as corrosion sensing coatings. Two salts NaA, where A- is a lanthanide complex anion (with Ln = Nd3+, and Yb3+), are incorporated into the resins as active functional fillers and different coatings are prepared on carbon steel substrates to assess their functional properties. The influence exerted by a corrosive saline solution on the morphology, structural, and photoluminescent properties of the coatings is evaluated, and their suitability for the practical detection of the early corrosion of coated carbon steel is demonstrated. The photoluminescence of the composite coatings depends on the corrosion time, with the effect being more important for the coatings doped with Nd3+. The present work shows that the composites obtained are suitable candidates for corrosion sensing coating applications, offering improved sustainability. Full article
(This article belongs to the Special Issue Polymers/Their Hybrid Materials for Optoelectronic Applications)
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<p>Chemical structure of Na[Ln(tta)<sub>4</sub>].</p>
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<p>FTIR spectra of the neat resin and resin-10Ln samples.</p>
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<p>Cross-sectional SEM image and corresponding EDS elemental mapping of the resin-xLn as-prepared samples: (<b>a</b>) neat resin; (<b>b</b>) resin-10Nd; (<b>c</b>) resin-10Yb. Scale bar: 10 µm.</p>
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<p>SEM images of the resin-xLn samples before and after immersion in 5 wt. % NaCl for 1 and 4 days. The scale is 10 µm.</p>
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<p>SEM images and corresponding EDS elemental mapping for the distribution of Fe elements in the resin-xLn after immersion in 5 wt. % NaCl for 4 days: (<b>a</b>) resin-5Nd (up) and resin-10Nd (down), and (<b>b</b>) resin-5Yb (up) and resin-10Yb (down). Scale bar: 10 µm.</p>
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<p>(<b>a</b>) A comparison of the Fe content values of the resin-xLn samples after 1 and 4 immersion days in 5 wt. % NaCl solution, as determined by XRF testing. (<b>b</b>) A schematic illustration of the system in the initial stage and after immersion in 5 wt. % NaCl solution.</p>
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<p>Emission spectra of the resin-10Ln samples, excited at 300 nm, before and after 1 and 4 immersion days in 5 wt. % NaCl solution: (<b>a</b>) Ln = Nd and (<b>b</b>) Ln = Yb.</p>
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37 pages, 5182 KiB  
Article
Hybrid Lanthanide Metal–Organic Compounds with Flavonoids: Magneto-Optical Properties and Biological Activity Profiles
by Sevasti Matsia, Anastasios Papadopoulos, Antonios Hatzidimitriou, Lars Schumacher, Aylin Koldemir, Rainer Pöttgen, Angeliki Panagiotopoulou, Christos T. Chasapis and Athanasios Salifoglou
Int. J. Mol. Sci. 2025, 26(3), 1198; https://doi.org/10.3390/ijms26031198 - 30 Jan 2025
Viewed by 727
Abstract
Lanthanides have seen rapid growth in the pharmaceutical and biomedical field, thus necessitating the development of hybrid metal–organic materials capable of exerting defined biological activities. Ternary hybrid lanthanide compounds were synthesized through reaction systems of Ln(III) (Ln = La, Nd, Eu) involving the [...] Read more.
Lanthanides have seen rapid growth in the pharmaceutical and biomedical field, thus necessitating the development of hybrid metal–organic materials capable of exerting defined biological activities. Ternary hybrid lanthanide compounds were synthesized through reaction systems of Ln(III) (Ln = La, Nd, Eu) involving the antioxidant flavonoid chrysin (Chr) and 1,10-phenanhtroline (phen) under solvothermal conditions, thus leading to pure crystalline materials. The so-derived compounds were characterized physicochemically in the solid state through analytical (elemental analysis), spectroscopic (FT-IR, UV-visible, luminescence, ESI-MS, circular dichroism, 151Eu Mössbauer), magnetic susceptibility, and X-ray crystallographic techniques. The analytical and spectroscopic data corroborate the 3D structure of the mononuclear complex assemblies and are in line with theoretical calculations (Bond Valence Sum and Hirshfeld analysis), with their luminescence suggesting quenching on the flavonoid-phen electronic signature. Magnetic susceptibility data suggest potential correlations, which could be envisioned, supporting future functional sensors. At the biological level, the title compounds were investigated for their (a) ability to interact with bovine serum albumin and (b) antibacterial efficacy against Gram(−) (E. coli) and Gram(+) (S. aureus) bacteria, collectively revealing distinctly configured biological profiles and suggesting analogous applications in cellular (patho)physiologies. Full article
(This article belongs to the Section Physical Chemistry and Chemical Physics)
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<p>(<b>A</b>) Molecular structure of <b>1</b>; aromatic hydrogen atoms as well as solvate methanol molecules are omitted for clarity; atom colors: lanthanum, yellow; nitrogen, blue; oxygen, red; hydrogen, green. (<b>B</b>) Coordination polyhedron (real positions of the coordinated atoms together with the normal polyhedron) of <b>1</b>; atom colors: lanthanum, yellow; nitrogen, blue; oxygen, red.</p>
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<p>(<b>A</b>) Molecular structure of <b>2</b>; Aromatic hydrogen atoms as well as solvate methanol molecules are omitted for clarity; atom colors: neodymium, yellow; nitrogen, blue; oxygen, red; hydrogen, green. (<b>B</b>) Coordination polyhedron (real positions of the coordinated atoms together with the normal polyhedron) of <b>2</b>; atom colors: neodymium, yellow; nitrogen, blue; oxygen, red. (<b>C</b>) Hydrogen bonding interactions (blue dotted lines) in <b>2</b>.</p>
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<p>(<b>A</b>) Molecular structure of <b>3</b>; aromatic hydrogen atoms are omitted for clarity; atom colors: europium, yellow; nitrogen, blue; oxygen, red; hydrogen, green. (<b>B</b>) Coordination polyhedron (real positions of the coordinated atoms together with the normal polyhedron) of <b>3</b>; atom colors: europium, yellow; nitrogen, blue; oxygen, red.</p>
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<p>(<b>A</b>) Crystal Explorer plot of <b>1</b>. (<b>B</b>) d<sub>norm</sub> mapping of <b>1</b> through Hirshfeld surface analysis. (<b>C</b>) Shape index mapping of <b>1</b> through Hirshfeld surface analysis. (<b>D</b>) Curvedness mapping of <b>1</b> through Hirshfeld surface analysis. The different colors shown in the figure are identified and explained in detail in the text.</p>
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<p>(<b>A</b>) Full fingerprint plot of <b>1</b> and d<sub>norm</sub> mapping. (<b>B</b>) Internal vs. external 2D fingerprint plot distances of H···H contacts of <b>1</b> with the relevant percentage contribution mapped over d<sub>norm</sub>. (<b>C</b>) 2D fingerprint plot of H···O/O···H contacts and their appropriate percentage contribution reflected onto the Hirshfeld surface area mapper over d<sub>norm</sub> of <b>1</b>. (<b>D</b>) 2D Fingerprint plot of H···C/C···H contacts, with the relevant percentage contribution reflected onto the Hirshfeld surface area mapper over d<sub>norm</sub> of <b>1</b>.</p>
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<p>(<b>A</b>) Comparative UV-visible spectra of <b>1</b> with phen and Chr in methanol at 10<sup>−5</sup> M. (<b>B</b>) Electronic spectrum (red line) and spectral fitting (scatter) of compound <b>1</b> in methanol (10<sup>−5</sup> M).</p>
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<p>ESI-MS spectra of <b>3</b> and the appropriate species in methanol solution through the positive mode of ionization.</p>
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<p>Comparative and normalized solid-state luminescence spectra between <b>2</b> and (<b>A</b>) Chr at λ<sub>ex</sub> 445 nm. (<b>B</b>) Phen at λ<sub>ex</sub> 373 nm.</p>
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<p>(<b>A</b>) Temperature dependence of the magnetic susceptibility of <b>1</b> measured at 10 kOe. (<b>B</b>) Magnetic properties of <b>2</b>: (<b>top</b>) temperature dependence of the magnetic susceptibility (<span class="html-italic">χ</span> and <span class="html-italic">χ</span><sup>−1</sup> data) measured at 10 kOe; (<b>bottom</b>) magnetization isotherms at 3, 10, and 50 K. (<b>C</b>) Magnetic properties of <b>3</b>: (<b>top</b>) temperature dependence of the magnetic susceptibility measured at 10 kOe. The calculated susceptibilities (red line) were obtained using the Van Vleck expression for the paramagnetic susceptibilities of free Eu(III) ions with λ = 734(1) K; (<b>bottom</b>) magnetization isotherms at 3, 10 and 50 K.</p>
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<p>Experimental (data points) and simulated (red line) <sup>151</sup>Eu Mössbauer spectrum of <b>3</b> measured at 78 K.</p>
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<p>UV-visible absorption spectra of solutions containing BSA (3 μΜ, PBS) and increasing molar ratios of <b>2</b> (DMSO).</p>
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<p>Fluorescence spectra of solutions containing BSA (1.5 μM, PBS) and molar ratios of <b>2</b> (DMSO). <b>Inset</b>: Stern–Volmer plot acquired from steady-state fluorescence at (<b>A</b>) 20 °C, (<b>B</b>) 30 °C, and (<b>C</b>) 37 °C.</p>
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<p>Van’t Hoff plot of <b>2</b> from measurements at 20 °C, 30 °C, and 37 °C.</p>
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<p>Circular dichroism spectra of solutions containing BSA (1 μM, PBS) and increasing molar ratios of (<b>A</b>) <b>1</b> (MeOH) and (<b>B</b>) <b>3</b> (MeOH).</p>
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<p>(<b>A</b>) Compound <b>1</b> was docked against the 3D structure of BSA. (<b>B</b>) 2D interaction diagrams illustrate the interactions between compound <b>1</b> and the BSA binding motif (hydrophobic contacts are indicated in red).</p>
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14 pages, 2568 KiB  
Article
Charge-Ordering and Magnetic Transitions in Nanocrystalline Half-Doped Rare Earth Manganite Ho0.5Ca0.5MnO3
by Giuseppe Muscas, Francesco Congiu, Alessandra Geddo Lehmann and Giorgio Concas
Nanomaterials 2025, 15(3), 203; https://doi.org/10.3390/nano15030203 - 27 Jan 2025
Viewed by 556
Abstract
This work investigates nanostructured Ho0.5Ca0.5MnO3, considered a model system of the Ln0.5Ca0.5MnO3 series of manganites with perovskite structures featuring small lanthanide (Ln) ions half-substituted by Ca ions. Here, we propose a modified [...] Read more.
This work investigates nanostructured Ho0.5Ca0.5MnO3, considered a model system of the Ln0.5Ca0.5MnO3 series of manganites with perovskite structures featuring small lanthanide (Ln) ions half-substituted by Ca ions. Here, we propose a modified hybrid sol–gel–solid-state approach to produce multiple samples with a single batch, obtaining very high crystalline quality and ensuring the same chemical composition, with an average particle size in the range 39–135 nm modulated on-demand by a controlled calcination process. Our findings evidence that, provided the crystalline structure is preserved, the charge-ordering transition can be observed even at the nanoscale. Additionally, this research explores the presence of glassy phenomena, which are commonly seen in this class of materials, to enhance our understanding beyond simplistic qualitative observations. Comprehensive characterization using DC and AC magnetometry, along with relaxation and aging measurements, reveals that the complex dynamics typical of glassy phenomena emerge only at the nanoscale and are not visible in the bulk counterpart. Nevertheless, the analysis confirms that even the sample with the smallest nanoparticles cannot be intrinsically classified as canonical spin glass. Full article
(This article belongs to the Section Nanoelectronics, Nanosensors and Devices)
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<p>Rietveld refined X-ray powder diffraction patterns: (<b>a</b>) sample T650, (<b>b</b>) sample T750, (<b>c</b>) sample T900, (<b>d</b>) sample T1000, and (<b>e</b>) sample T1100. The experimental data (empty black dots) and the fit curve (red) are shown together with the residuals (gray bottom curve). The Bragg reflection positions of the orthorhombic Pnma main phase are represented as blue lines below the pattern. The green arrows indicate the two peaks of the secondary phase visible in the samples T900 and T1000.</p>
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<p>(<b>a</b>) TEM image of sample T650 with (<b>b</b>) the particle size distribution of the same sample. (<b>c</b>) Images of samples T750 and (<b>d</b>) T900.</p>
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<p>Sample T650 (<b>a</b>) ZFC susceptibility (black curve), FC susceptibility (red), and difference between them (blue). (<b>b</b>) Inverse of the ZFC susceptibility: experimental curve (black) and fit curves (red and blue). (<b>c</b>) Sample T1100 ZFC susceptibility (black curve), FC susceptibility (red), and difference between them (blue). (<b>d</b>) Inverse of the ZFC susceptibility: experimental curve (black) and fit curves (red and blue). In panels (<b>b</b>,<b>d</b>), the arrows delimit the two linear temperature ranges used in the fitting procedure.</p>
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<p>(<b>a</b>) ZFC hysteresis loop of sample T650 at 5 K (black solid curve) and of sample T1100 at 5 K (red), 20 K (green), 60 K (blue), and 120 K (cyan). As a reference, a straight line (magenta) was drawn for comparison with the 60 K curve. (<b>b</b>) ZFC hysteresis loop at 5 K of the samples T650 (black curve) and T1100 (red) in the field range from –50 to 50 mT.</p>
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<p>Susceptibility vs. time at 5 K and 2 mT of sample T650 (red empty dots) and sample T1100 (black empty dots). The field was applied immediately after a zero-field cooling down to 5 K.</p>
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11 pages, 1773 KiB  
Article
Stretching the Limits of Refractometric Sensing in Water Using Whispering-Gallery-Mode Resonators
by Kevin Soler-Carracedo, Antonia Ruiz, Susana Ríos, Sergio de Armas-Rillo, Leopoldo L. Martín, Martin Hohmann, Inocencio R. Martín and Fernando Lahoz
Chemosensors 2025, 13(2), 33; https://doi.org/10.3390/chemosensors13020033 - 24 Jan 2025
Viewed by 516
Abstract
A novel application of microresonators for refractometric sensing in aqueous media is presented. To carry out this approach, microspheres of different materials and sizes were fabricated and doped with Nd3+ ions. Under 532 nm excitation, the microspheres presented typical NIR Nd3+ [...] Read more.
A novel application of microresonators for refractometric sensing in aqueous media is presented. To carry out this approach, microspheres of different materials and sizes were fabricated and doped with Nd3+ ions. Under 532 nm excitation, the microspheres presented typical NIR Nd3+ emission bands with superimposed sharp peaks, related to the Whispering Gallery Modes (WGMs), due to the geometry of the microspheres. When the microspheres were submerged in water with increasing concentrations of glycerol, spectral shifts for the WGMs were observed as a function of the glycerol concentration. These spectral shifts were studied and calibrated for three different microspheres and validated with the theoretical shifts, obtained by solving the Helmholtz equations for the electromagnetic field, considering the geometry of the system, and also by calculating the extinction cross-section. WGM shifts strongly depend on the diameter of the microspheres and their refractive index (RI) difference compared with the external medium, and are greater for decreasing values of the diameter and lower values of RI difference. Experimental sensitivities ranging from 2.18 to 113.36 nm/RIU (refractive index unit) were obtained for different microspheres. Furthermore, reproducibility measurements were carried out, leading to a repeatability of 2.3 pm and a limit of detection of 5 × 10−4 RIU. The proposed sensors, taking advantage of confocal microscopy for excitation and detection, offer a robust, reliable, and contactless alternative for environmental water analysis. Full article
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<p>Scheme of (<b>a</b>) the fabrication process used to obtain Nd<sup>3+</sup>-doped microspheres and (<b>b</b>) WGM detection using a confocal microscope.</p>
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<p>(<b>a</b>) Bulk sample NIR emission spectrum of SBN:Nd<sup>3+</sup>, (<b>b</b>) emission spectrum from the highlighted zone obtained from a ~23 µm diameter microsphere fabricated from the same bulk material, and (<b>c</b>) optical image of the microsphere.</p>
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<p>(<b>a</b>) Fittings of a single WGM peak when changing the RI in the outside medium. (<b>b</b>) Experimentally (scatter) and theoretically (line) determined WGM shift as a function of the RI of the outside medium, for SBN:Nd<sup>3+</sup> microspheres of RI 2 and with diameters 6, 23, and 45 µm (black, blue, and red, respectively). (<b>c</b>) Histogram of the distribution of WGM uncertainty.</p>
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<p>Experimentally (scatter) and theoretically (line) determined WGM shift for microspheres with different diameters and inner RI (black: d~33 µm, <span class="html-italic">n</span>~1.46; blue: d~32 µm, <span class="html-italic">n</span>~1.6; red: d~23 µm, <span class="html-italic">n</span>~2) as a function of changes in the outside medium RI.</p>
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35 pages, 1042 KiB  
Review
Potential Applications of Rare Earth Metal Nanoparticles in Biomedicine
by Svetlana A. Titova, Maria P. Kruglova, Victor A. Stupin, Natalia E. Manturova and Ekaterina V. Silina
Pharmaceuticals 2025, 18(2), 154; https://doi.org/10.3390/ph18020154 - 24 Jan 2025
Viewed by 891
Abstract
In recent years, the world scientific community has shown increasing interest in rare earth metals in general and their nanoparticles in particular. Medicine and pharmaceuticals are no exception in this matter. In this review, we have considered the main opportunities and potential applications [...] Read more.
In recent years, the world scientific community has shown increasing interest in rare earth metals in general and their nanoparticles in particular. Medicine and pharmaceuticals are no exception in this matter. In this review, we have considered the main opportunities and potential applications of rare earth metal (gadolinium, europium, ytterbium, holmium, lutetium, dysprosium, erbium, terbium, thulium, scandium, yttrium, lanthanum, europium, neodymium, promethium, samarium, praseodymium, cerium) nanoparticles in biomedicine, with data ranging from single reports of effects found in vitro to numerous independent in vivo studies, as well as a number of challenges to their potential for wider application. The main areas of application of rare earth metals, including in the future, are diagnosis and treatment of malignant neoplasms, therapy of infections, as well as the use of antioxidant and regenerative properties of a number of nanoparticles. These applications are determined both by the properties of rare earth metal nanoparticles themselves and the need to search for new approaches to solve a number of urgent biomedical and public health problems. Oxide forms of lanthanides are most often used in biomedicine due to their greatest biocompatibility and nanoscale size, providing penetration through biological membranes. However, the existing contradictory or insufficient data on acute and chronic toxicity of lanthanides still make their widespread use difficult. There are various modification methods (addition of excipients, creation of nanocomposites, and changing the morphology of particles) that can reduce these effects. At the same time, despite the use of some representatives of lanthanides in clinical practice, further studies to establish the full range of pharmacological and toxic effects, as well as the search for approaches to modify nanoparticles remain relevant. Full article
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<p>Rare earth metal nanoparticles as agents for biomedical applications.</p>
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15 pages, 6281 KiB  
Article
Structure and Mixed Proton–Electronic Conductivity in Pr and Nb-Substituted La5.4MoO12−δ Ceramics
by Abraham Sánchez-Caballero, José M. Porras-Vázquez, Lucía dos Santos-Gómez, Javier Zamudio-García, Antonia Infantes-Molina, Jesús Canales-Vázquez, Enrique R. Losilla and David Marrero-López
Materials 2025, 18(3), 529; https://doi.org/10.3390/ma18030529 - 24 Jan 2025
Viewed by 650
Abstract
Lanthanide molybdates are materials known for their mixed proton–ionic conductivity. This study investigates the effects of Pr content and Nb-doping on the crystal structure and electrical properties of the La5.4−xPrxMo1−yNbyO12−δ (x = 0, 1.35, [...] Read more.
Lanthanide molybdates are materials known for their mixed proton–ionic conductivity. This study investigates the effects of Pr content and Nb-doping on the crystal structure and electrical properties of the La5.4−xPrxMo1−yNbyO12−δ (x = 0, 1.35, 2.7, 4.05, 5.4; y = 0, 0.1) series. The research focuses on two primary objectives: (i) enhancing the electronic conductivity through the use of Pr4+/Pr3+ redox pairs and (ii) increasing the ionic conductivity through Nb5+ aliovalent doping. The materials were thoroughly characterized by X-ray powder diffraction (XRD), X-ray photoelectron spectroscopy (XPS), transmission and scanning electron microscopy (TEM and SEM), and complex impedance spectroscopy. The average crystal structure of the materials depended significantly on the Pr content. In general, compositions with a higher Pr content crystallize in a cubic fluorite-type structure, whereas those with a lower Pr content stabilize a rhombohedral polymorph. However, detailed TEM studies reveal a more complex local crystal structure characterized by nanodomains and incommensurate modulations. The highest conductivity values were observed in a N2 atmosphere for compositions with an elevated Pr content, with values of 0.17 and 204.4 mS cm−1 for x = 0 and x = 5.4, respectively, at 700 °C, which is attributed to electronic conduction mediated by the Pr4+/Pr3+ redox pair, as confirmed by XPS. These findings highlight the potential of tailored doping strategies to optimize the conducting properties of lanthanide molybdates for specific high-temperature electrochemical applications. Full article
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<p>XRD patterns for La<sub>5.4−x</sub>Pr<sub>x</sub>Mo<sub>1−y</sub>Nb<sub>y</sub>O<sub>12−δ</sub> (La<sub>5.4−x</sub>Pr<sub>x</sub>) samples (x = 1.35, 2.7, 4.05, 5.4; y = 0, 0.1) heated at 1500 °C and cooled down at (<b>a</b>,<b>c</b>) 5 °C min<sup>−1</sup> and (<b>b</b>,<b>d</b>) 0.5 °C min<sup>−1</sup>. The symmetry of the samples is indicated within the figure: cubic (<math display="inline"><semantics> <mrow> <mi mathvariant="normal">F</mi> <mi mathvariant="normal">m</mi> <mover accent="true"> <mrow> <mn>3</mn> </mrow> <mo>¯</mo> </mover> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>) and rhombohedral (<math display="inline"><semantics> <mrow> <mi mathvariant="normal">R</mi> <mover accent="true"> <mrow> <mn>3</mn> </mrow> <mo>¯</mo> </mover> </mrow> </semantics></math>) for both R1 and R2 polymorphs. Several samples (*) exhibit broad diffraction peaks, suggesting a deviation from cubic symmetry. The peak splitting observed in some cubic polymorphs at high angles is due to CuKα<sub>2</sub> contribution.</p>
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<p>XRD Rietveld plots for (<b>a</b>) La<sub>2.7</sub>Pr<sub>2.7</sub>_5, (<b>b</b>) La<sub>2.7</sub>Pr<sub>2.7</sub>Nb<sub>0.1</sub>_5, (<b>c</b>) La<sub>4.05</sub>Pr<sub>1.35</sub>_0.5, and (<b>d</b>) Pr<sub>5.4</sub>_Q. Crystal system and agreement factors are displayed within the figure. [Observed data (crosses), calculated pattern (red continuous line), difference curve (cyan line) and reflection marks (blue short lines)]. The inset figures highlight the details of several diffraction peaks for both cubic and R1 polymorphs.</p>
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<p>SAED patterns of (<b>a</b>) Pr<sub>5.4</sub>_5, (<b>b</b>) La<sub>2.7</sub>Pr<sub>2.7</sub>_0.5, and (<b>c</b>) La<sub>2.7</sub>Pr<sub>2.7</sub>Nb<sub>0.1</sub>_0.5 in the <math display="inline"><semantics> <mrow> <mo>[</mo> <mn>01</mn> <mover accent="true"> <mrow> <mn>1</mn> </mrow> <mo>¯</mo> </mover> <mo>]</mo> </mrow> </semantics></math> zone axis. HRTEM images of (<b>d</b>) Pr<sub>5.4</sub>_0.5, (<b>e</b>) La<sub>2.7</sub>Pr<sub>2.7</sub>_0.5, (<b>f</b>) La<sub>2.7</sub>Pr<sub>2.7</sub>Nb<sub>0.1</sub>_0.5, and (<b>g</b>) La<sub>4.05</sub>Pr<sub>1.35</sub>_5 in the <math display="inline"><semantics> <mrow> <mo>[</mo> <mn>01</mn> <mover accent="true"> <mrow> <mn>1</mn> </mrow> <mo>¯</mo> </mover> <mo>]</mo> </mrow> </semantics></math> zone axis.</p>
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<p>XPS spectra of (<b>a</b>,<b>b</b>) Mo 3<span class="html-italic">d</span> and (<b>c</b>,<b>d</b>) Pr 3<span class="html-italic">d</span> core levels for the La<sub>5.4−x</sub>Pr<sub>x</sub>Mo<sub>1−y</sub>Nb<sub>y</sub>O<sub>12−δ</sub> (x = 1.35, 2.7. 4.05, 5.4; y = 0, 0.1) series.</p>
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<p>SEM micrographs of the La<sub>5.4−x</sub>Pr<sub>x</sub>Mo<sub>1−y</sub>Nb<sub>y</sub>O<sub>12−<span class="html-italic">δ</span></sub> samples (La<sub>5.4−x</sub>Pr<sub>x</sub>Mo<sub>1−y</sub>_C) (x = 1.35, 2.7. 4.05, 5.4; y = 0, 0.1) sintered at 1500 °C for 1 h and cooled down at different rates. Average grain size is denoted at the top right of the images.</p>
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<p>Representative impedance spectra of La<sub>2.7</sub>Pr<sub>2.7</sub>_0.5 and Pr<sub>5.4</sub>_Q under (<b>left</b> dry/wet N<sub>2</sub> at 300 °C and (<b>right</b>) 5% H<sub>2</sub>-Ar gasses at 500 °C. The equivalent circuit used to fit the spectra is shown in the insets.</p>
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<p>Arrhenius plots of La<sub>5.4</sub>Q, La<sub>2.7</sub>Pr<sub>2.7</sub>_Q, and Pr<sub>5.4</sub>_Q sintered at 1500 °C for 1 h and cooled down by quenching under dry N<sub>2</sub> and wet 5% H<sub>2</sub>-Ar atmospheres.</p>
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40 pages, 9873 KiB  
Review
Luminescent Lanthanide Infinite Coordination Polymers for Ratiometric Sensing Applications
by Ziqin Song, Yuanqiang Hao, Yunfei Long, Peisheng Zhang, Rongjin Zeng, Shu Chen and Wansong Chen
Molecules 2025, 30(2), 396; https://doi.org/10.3390/molecules30020396 - 18 Jan 2025
Viewed by 553
Abstract
Ratiometric lanthanide coordination polymers (Ln-CPs) are advanced materials that combine the unique optical properties of lanthanide ions (e.g., Eu3+, Tb3+, Ce3+) with the structural flexibility and tunability of coordination polymers. These materials are widely used in biological [...] Read more.
Ratiometric lanthanide coordination polymers (Ln-CPs) are advanced materials that combine the unique optical properties of lanthanide ions (e.g., Eu3+, Tb3+, Ce3+) with the structural flexibility and tunability of coordination polymers. These materials are widely used in biological and chemical sensing, environmental monitoring, and medical diagnostics due to their narrow-band emission, long fluorescence lifetimes, and excellent resistance to photobleaching. This review focuses on the composition, sensing mechanisms, and applications of ratiometric Ln-CPs. The ratiometric fluorescence mechanism relies on two distinct emission bands, which provides a self-calibrating, reliable, and precise method for detection. The relative intensity ratio between these bands varies with the concentration of the target analyte, enabling real-time monitoring and minimizing environmental interference. This ratiometric approach is particularly suitable for detecting trace analytes and for use in complex environments where factors like background noise, temperature fluctuations, and light intensity variations may affect the results. Finally, we outline future research directions for improving the design and synthesis of ratiometric Ln-CPs, such as incorporating long-lifetime reference luminescent molecules, exploring near-infrared emission systems, and developing up-conversion or two-photon luminescent materials. Progress in these areas could significantly broaden the scope of ratiometric Ln-CP applications, especially in biosensing, environmental monitoring, and other advanced fields. Full article
(This article belongs to the Special Issue Nano-Functional Materials for Sensor Applications—2nd Edition)
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<p>Schematic diagram of the structure of ratiometric Ln-CPs.</p>
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<p>Schematic diagram of the sensing mechanism of ratiometric Ln-CPs sensors. (<b>A</b>) Sensitization effect of the target analyte on the lanthanide ion; (<b>B</b>) Reaction between the analyte and the ligand or guest molecules in the Ln-CPs; (<b>C</b>) Reaction between the analyte and the guest molecule (second luminescent center).</p>
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<p>Schematic illustration of the preparation of dual-emission GOx&amp;CDs@AMP/Tb-CPBA coordination polymers and their working principle for ratiometric glucose detection. Reproduced with permission [<a href="#B65-molecules-30-00396" class="html-bibr">65</a>]. Copyright 2018 American Chemical Society.</p>
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<p>Schematic diagram of the preparation of COU@Eu-ICPs and its mechanism for phosphate ion detection. Reproduced with permission [<a href="#B82-molecules-30-00396" class="html-bibr">82</a>]. Copyright 2022 Elsevier.</p>
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<p>Schematic illustration of the preparation of dual-emission GOx&amp;CDs@AMP/Tb-CPBA coordination polymers and their working principle for ratiometric glucose detection. Reproduced with permission [<a href="#B93-molecules-30-00396" class="html-bibr">93</a>]. Copyright 2017 Royal Society of Chemistry.</p>
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<p>Schematic diagram of the preparation of COU@Eu-ICPs and its mechanism for phosphate ion detection. Reproduced with permission [<a href="#B103-molecules-30-00396" class="html-bibr">103</a>]. Copyright 2021 Elsevier.</p>
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<p>(<b>A</b>) Schematic diagram of the preparation of TPE-TS@Eu/GMP ICP nanoparticles and their response mechanism to DPA. (<b>B</b>) Schematic diagram of the point-of-use application. Reproduced with permission [<a href="#B121-molecules-30-00396" class="html-bibr">121</a>]. Copyright 2020 American Chemical Society.</p>
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<p>(<b>A</b>) Schematic representation of the composition of the H<sub>4</sub>TCPE@Eu/AMP ICP sensor array and its process for antibiotic analysis. (<b>B</b>) Schematic illustration of paper-based analysis for on-site applications, assisted by a smartphone. Reproduced with permission [<a href="#B135-molecules-30-00396" class="html-bibr">135</a>]. Copyright 2021 American Chemical Society.</p>
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<p>Schematic diagram of the preparation of Ln/AMP/CIP and its mechanism for ALP detection based on the aggregation-enhanced antenna effect. Reproduced with permission [<a href="#B146-molecules-30-00396" class="html-bibr">146</a>]. Copyright 2023 Elsevier.</p>
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<p>Schematic diagram of the sensing mechanism of luminol-Tb-GMPCu for amyloid β-peptide. Reproduced with permission [<a href="#B158-molecules-30-00396" class="html-bibr">158</a>]. Copyright 2022 Elsevier.</p>
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<p>(<b>A</b>) Schematic structure of pNIPAM nanoparticles grafted with lanthanide complexes. (<b>B</b>) Schematic diagram illustrating the temperature-responsive mechanism of the pNIPAM nanoprobe. Reproduced with permission [<a href="#B170-molecules-30-00396" class="html-bibr">170</a>]. Copyright 2020 Royal Society of Chemistry.</p>
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15 pages, 4059 KiB  
Article
Magnetically Diluted Dy3+ and Yb3+ Squarates Showing Relaxation Tuning and Matrix Dependence
by Rina Takano and Takayuki Ishida
Molecules 2025, 30(2), 356; https://doi.org/10.3390/molecules30020356 - 16 Jan 2025
Viewed by 468
Abstract
A new compound [Y2(sq)3(H2O)4] (Y-sq; sq = squarate (C4O42–)) was prepared and structurally characterized. Since the RE-sq family (RE = Y, Dy, Yb, Lu) gave isostructural crystals, the objective of [...] Read more.
A new compound [Y2(sq)3(H2O)4] (Y-sq; sq = squarate (C4O42–)) was prepared and structurally characterized. Since the RE-sq family (RE = Y, Dy, Yb, Lu) gave isostructural crystals, the objective of this study is to explore the effects of diamagnetic dilution on the SIM behavior through systematic investigation and comparison of diamagnetically diluted and undiluted forms. The 1%-Diluted Dy compounds, Dy@Y-sq and Dy@Lu-sq, showed AC magnetic susceptibility peaks without any DC bias field (HDC), whereas undiluted Dy-sq showed no AC out-of-phase response under the same conditions. The Orbach and Raman mechanisms are assumed in the Arrhenius plots, giving Ueff/kB = 139(5) and 135(8) K for Dy@Y-sq and Dy@Lu-sq, respectively, at HDC = 0 Oe. In contrast, Yb@Y-sq and Yb@Lu-sq behaved different; Yb@Y-sq can be regarded as a field-induced SIM because AC out-of-phase response was recorded only when HDC was present. On the other hand, Yb@Lu-sq showed a relaxation independent from temperature around 2 K at HDC = 0 Oe, possibly ascribed to a quantum-tunneling-magnetization mechanism. Applying HDC = 400 Oe afforded Ueff = 61.2(14) and 62.5(16) K for Yb@Y-sq and Yb@Lu-sq, respectively. The Y/Lu matrix dependence may be related to spin–phonon coupling. The dilution technique is a facile and versatile tool for modification of SIM characteristics. Full article
(This article belongs to the Special Issue Inorganic Chemistry in Asia)
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<p>(<b>a</b>) Experimental and calculated powder XRD profiles for RE-sq. (<b>b</b>) X-ray crystal structure of [Y<sub>2</sub>(sq)<sub>3</sub>(H<sub>2</sub>O)<sub>8</sub>]<span class="html-italic"><sub>n</sub></span>. Thermal ellipsoids are drawn at the 50% probability level. Symmetry operation code: i: <span class="html-italic">x</span>, <span class="html-italic">y</span> + 1, <span class="html-italic">z</span>; ii: <span class="html-italic">x</span>, –<span class="html-italic">y</span> + 1, <span class="html-italic">z</span> + 1/2; iii: <span class="html-italic">x</span>, –<span class="html-italic">y</span> + 1, <span class="html-italic">z</span>–1/2; iv: <span class="html-italic">x</span>, <span class="html-italic">y</span>–1, <span class="html-italic">z</span>. Color code: C: gray; H: turquoise; O: red; Y: green. (<b>c</b>) Molecular arrangement viewed along the <span class="html-italic">b</span> axis. Yellow thick lines stand for the direction between two basal plane centroids in a YO<sub>8</sub> square antiprism. (<b>d</b>) Coordination polyhedra for the Y<sup>3+</sup> ions in [Y<sub>2</sub>(sq)<sub>3</sub>(H<sub>2</sub>O)<sub>8</sub>]<span class="html-italic"><sub>n</sub></span>.</p>
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<p>(<b>a</b>) AC magnetic susceptibilities, in-phase <span class="html-italic">χ</span><sub>AC</sub>′ and out-of-phase <span class="html-italic">χ</span><sub>AC</sub>″, for 1% Dy-sq diluted in a Y-sq matrix (Dy@Y-sq), measured without any DC bias field. The susceptibilities are converted per the undiluted composition formula [RE<sub>2</sub>(sq)<sub>3</sub>(H<sub>2</sub>O)<sub>8</sub>]. Lines are drawn only for a guide to the eye. (<b>b</b>) For 1%-diluted Dy@Y-sq, measured at a DC field of 1000 Oe. (<b>c</b>) AC magnetic susceptibilities for 1%-diluted Dy@Lu-sq, measured without any DC field. (<b>d</b>) For 1%-diluted Dy@Lu-sq, measured at a DC field of 1000 Oe. (<b>e</b>) AC magnetic susceptibilities for undiluted Dy-sq [<a href="#B12-molecules-30-00356" class="html-bibr">12</a>], measured at the DC fields of 0 Oe and (<b>f</b>) at 1000 Oe.</p>
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<p>(<b>a</b>) AC magnetic susceptibilities, in-phase <span class="html-italic">χ</span><sub>AC</sub>′ and out-of-phase <span class="html-italic">χ</span><sub>AC</sub>″, for 1% Yb-sq diluted in a Y-sq matrix (Yb@Y-sq), measured without any DC bias field. The susceptibilities are converted per the undiluted composition formula [RE<sub>2</sub>(sq)<sub>3</sub>(H<sub>2</sub>O)<sub>8</sub>]. Lines are drawn only for a guide to the eye. (<b>b</b>) For 1%-diluted Yb@Y-sq, measured at a DC field of 400 Oe. (<b>c</b>) AC magnetic susceptibilities for 1%-diluted Yb@Lu-sq, measured without any DC field. (<b>d</b>) For 1%-diluted Yb@Lu-sq, measured at a DC field of 400 Oe. (<b>e</b>) AC magnetic susceptibilities for undiluted Yb-sq [<a href="#B12-molecules-30-00356" class="html-bibr">12</a>], measured at the DC fields of 0 Oe and (<b>f</b>) at 400 Oe.</p>
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<p>The Arrhenius plot for Dy@Y-sq at <span class="html-italic">H</span><sub>DC</sub> = 0 Oe (<b>a</b>) and at <span class="html-italic">H</span><sub>DC</sub> = 1000 Oe (<b>b</b>), and Dy@Lu-sq at <span class="html-italic">H</span><sub>DC</sub> = 0 Oe (<b>c</b>) and at <span class="html-italic">H</span><sub>DC</sub> = 1000 Oe (<b>d</b>). The data of (<b>a</b>–<b>d</b>) were given from <a href="#molecules-30-00356-f002" class="html-fig">Figure 2</a>a, b, c, and d, respectively. Solid lines are drawn from the parameter optimization. For details, see the text.</p>
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<p>The Arrhenius plot for Yb@Y-sq at <span class="html-italic">H</span><sub>DC</sub> = 0 Oe (<b>a</b>) and at <span class="html-italic">H</span><sub>DC</sub> = 400 Oe (<b>b</b>), and Yb@Lu-sq at <span class="html-italic">H</span><sub>DC</sub> = 0 Oe (<b>c</b>) and at <span class="html-italic">H</span><sub>DC</sub> = 400 Oe (<b>d</b>). The data of (<b>a</b>–<b>d</b>) were given from <a href="#molecules-30-00356-f003" class="html-fig">Figure 3</a>a, b, c, and d, respectively. Solid lines are drawn from the parameter optimization. For details, see the text.</p>
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<p>Canonical structures of squarate (sq).</p>
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18 pages, 5651 KiB  
Article
Methane Decomposition over a Titanium-Alumina and Iron Catalyst Assisted by Lanthanides to Produce High-Performance COx-Free H2 and Carbon Nanotubes
by Hamid Ahmed, Anis H. Fakeeha, Fayez M. Al-Alweet, Ahmed E. Abasaeed, Ahmed A. Ibrahim, Rawesh Kumar, Alaaddin M. M. Saeed and Ahmed S. Al-Fatesh
Catalysts 2025, 15(1), 77; https://doi.org/10.3390/catal15010077 - 15 Jan 2025
Viewed by 724
Abstract
COx-free H2, along with uniform carbon nanotubes, can be achieved together in high yield by CH4 decomposition. It only needs a proper catalyst and reaction condition. Herein, Fe-based catalyst dispersed over titania-incorporated-alumina (Fe/Ti-Al), with the promotional addition of lanthanides, like [...] Read more.
COx-free H2, along with uniform carbon nanotubes, can be achieved together in high yield by CH4 decomposition. It only needs a proper catalyst and reaction condition. Herein, Fe-based catalyst dispersed over titania-incorporated-alumina (Fe/Ti-Al), with the promotional addition of lanthanides, like CeO2 and La2O3, over it, is investigated for a methane decomposition reaction at 800 °C with GHSV 6 L/(g·h) in a fixed-bed reactor. The catalysts are characterized by temperature-programmed reduction (TPR), powder X-ray diffraction (XRD), Raman spectroscopy, and transmission electron microscopy (TEM). The promoted catalysts are facilitated with higher surface area and enhanced dispersion and concentration of active sites, resulting in higher H2 and carbon yields than unpromoted catalysts. Ceria-promoted 20Fe/Ti-Al catalyst had the highest concentration of active sites and always attained the highest activity in the initial hours. The 20Fe-2.5Ce/Ti-Al catalyst attains >90% CH4 conversion, >80% H2-yield, and 92% carbon yield up to 480 min time on stream. The carbon nanotube over this catalyst is highly uniform, consistent, and has the highest degree of crystallinity. The supremacy of ceria-promoted catalyst attained >90% CH4 conversion even after the second cycle of regeneration studies (against 87% in lanthanum-promoted catalyst), up to 240 min time on stream. This study plots the path of achieving catalytic and carbon excellence over Fe-based catalysts through CH4 decomposition. Full article
(This article belongs to the Section Industrial Catalysis)
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<p>N<sub>2</sub> adsorption–desorption isotherms (<b>A</b>) and pore size distribution (<b>B</b>) of a fresh prompted iron catalyst loading on Ti-Al support calcined at 500 °C.</p>
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<p>H<sub>2</sub>-TPR spectra for fresh Ti-Al support and fresh promoted iron catalysts loaded on Ti-Al support calcined at 500 °C.</p>
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<p>XRD patterns for fresh prompted iron catalysts loaded on Ti-Al support calcined at 500 °C.</p>
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<p>SEM images (<b>A</b>) &amp; particle distribution (<b>a</b>) of the 20Fe-2.5Ce/Ti-Al and SEM images (<b>B</b>) &amp; particle distribution of (<b>b</b>) 20Fe-2.5La/Ti-Al catalysts at different magnifications.</p>
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<p>TEM images (<b>A</b>) &amp; particle distribution (<b>B</b>) of the fresh 20Fe-2.5Ce/Ti-Al catalyst at different magnifications.</p>
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<p>Time on Stream (TOS) of methane conversion (<b>A</b>) and hydrogen yield (<b>B</b>) versus time on stream for promoted iron-based catalysts loaded on Ti-Al support calcined at 500 °C, CH<sub>4</sub>/N<sub>2</sub> = 1:2, T = 800 °C, P = 1 atm, GHSV = 6 L gcat<sup>−1</sup> h<sup>−1</sup>.</p>
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<p>CH<sub>4</sub> conversion for various regeneration cycles (<b>A</b>) prior to recycling; (<b>B</b>) following the initial recycling; and (<b>C</b>) following the subsequent recycling GHSV = 6 L gcat<sup>−1</sup> h<sup>−1</sup>, T = 800 °C, P = 1 atm, and CH<sub>4</sub>/N<sub>2</sub> = 1:2.</p>
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<p>Methane conversion (<b>A</b>) and hydrogen Yield (<b>B</b>) for long-term experiment of 20Fe-2.5Ce/Ti-Al catalyst with GHSV = 6 L gcat<sup>−1</sup> h<sup>−1</sup> at 800 °C on stream CH<sub>4</sub>/N<sub>2</sub> = 1:2, P = 1 atm.</p>
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<p>TGA curves (<b>A</b>) and Carbon yield (<b>B</b>) of the catalysts for used promoted iron-based catalysts loaded on Ti-Al support for a reaction time of 240 min at 800 °C.</p>
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<p>Raman spectra of used promoted iron-based catalysts loaded on Ti-Al support after a reaction time of 240 min at 800 °C.</p>
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<p>TPO profiles (<b>A</b>) and XRD patterns (<b>B</b>) used promoted iron-based catalysts loaded on Ti-Al support after a reaction time of 240 min at 800 °C.</p>
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<p>Used 20Fe-2.5Ce/Ti-Al catalysts before and after the regeneration cycle are shown in TEM pictures (<b>A</b>,<b>C</b>) and particle distribution (<b>B</b>,<b>D</b>).</p>
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<p>TGA (<b>A</b>), carbon yield (<b>B</b>), Raman (<b>C</b>), and XRD (<b>D</b>) curves for the spent promoted Fe-based catalysts loaded on Ti-Al support after a regeneration and long stability test at 800 °C.</p>
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<p>The reaction scheme for (<b>a</b>) CH<sub>4</sub> decomposition at Fe sites, (<b>b</b>) iron carburization, (<b>c</b>) CH<sub>4</sub> decomposition at Fe end of Fe<sub>3</sub>C, (<b>d</b>) and carbon nucleation at carbon end of Fe<sub>3</sub>C.</p>
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<p>The schematic diagram of the preparation process of synthesis catalysts.</p>
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12 pages, 649 KiB  
Article
High-Coercivity Ferrimagnet Co₂FeO₂BO₃: XMCD Insights into Charge-Ordering and Cation Distribution
by Mikhail S. Platunov
Inorganics 2025, 13(1), 24; https://doi.org/10.3390/inorganics13010024 - 15 Jan 2025
Viewed by 687
Abstract
The multi-sublattice ferrimagnet Co2FeO2BO3, a prominent example of lanthanide-free magnets, was the subject of element-selective studies using X-ray magnetic circular dichroism (XMCD) observations at the L- and K- X-ray absorption edges. Research findings indicate that [...] Read more.
The multi-sublattice ferrimagnet Co2FeO2BO3, a prominent example of lanthanide-free magnets, was the subject of element-selective studies using X-ray magnetic circular dichroism (XMCD) observations at the L- and K- X-ray absorption edges. Research findings indicate that the distinct magnetic characteristics of Co2FeO2BO3, namely its remarkable high coercivity (which surpasses 7 Tesla at low temperatures), originate from an atypical arrangement of magnetic ions in the crystal structure (sp.gr. Pbam). The antiferromagnetic nature of the Co2+-O-Fe3+ exchange interaction was confirmed by identifying the spin and orbital contributions to the total magnetization from Co (mL = 0.27 ± 0.1 μB/ion and meffS = 0.53 ± 0.1 μB/ion) and Fe (mL = 0.05 ± 0.1 μB/ion and meffS = 0.80 ± 0.1 μB/ion) ions through element-selective XMCD analysis. Additionally, the research explicitly revealed that the strong magnetic anisotropy is a result of the significant unquenched orbital magnetic moment of Co, a feature that is also present in the related compound Co3O2BO3. A complex magnetic structure in Co2FeO2BO3, with infinite Co²⁺O6 layers in the bc-plane and strong antiferromagnetic coupling through Fe3⁺ ions, is suggested by element-selective hysteresis data, which revealed that Co²⁺ ions contribute both antiferromagnetic and ferromagnetic components to the total magnetization. The findings underline the suitability of Co2FeO2BO3 for applications in extreme environments, such as low temperatures and high magnetic fields, where its unique magnetic topology and anisotropy can be harnessed for advanced technologies, including materials for space exploration and quantum devices. This XMCD study opens the door to the production of novel high-coercivity, lanthanide-free magnetic materials by showing that targeted substitution at specific crystallographic sites can significantly enhance the magnetic properties of such materials. Full article
(This article belongs to the Special Issue Inorganic Materials for Applications in Extreme Environments)
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<p>Crystal structure of Co<sub>2</sub>FeO<sub>2</sub>BO<sub>3</sub> in the <b>ab</b>-plane. The structure comprises octahedra that correspond to divalent and trivalent metal ions positioned at non-equivalent crystallographic sites (1, 2, 3, and 4). Planar BO<sub>3</sub> triangles are also illustrated. Black octahedra indicate (Co/Fe)<sup>3+</sup>O<sub>6</sub>, with a specific emphasis on FeO<sub>6</sub>, while gray octahedra represent continuous Co<sup>2+</sup>O<sub>6</sub> layers that interact through BO<sub>3</sub> groups and Fe<sup>3+</sup>O<sub>6</sub> octahedra.</p>
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<p>Comparison of macroscopic magnetic hysteresis curve (measured with H = ±9 T) with element-selective magnetization curves for Co<sub>2</sub>FeO<sub>2</sub>BO<sub>3</sub>, measured at 779.3 eV of the Co <span class="html-italic">L</span><sub>3</sub>-edge, at 710.3 eV of the Fe <span class="html-italic">L</span><sub>3</sub>-edge, at 7711.0 eV of the Co <span class="html-italic">K</span>-edge, at 7119.5 eV of the Fe <span class="html-italic">K</span>-edge along the <b>b</b>-axis.</p>
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<p>Orbital magnetic moments, effective spin magnetic moments, and total magnetic moment Co<sub>2</sub>FeO<sub>2</sub>BO<sub>3</sub>, obtained via sum rules [<a href="#B37-inorganics-13-00024" class="html-bibr">37</a>,<a href="#B38-inorganics-13-00024" class="html-bibr">38</a>], as a function of temperature along the <b>b</b>-axis.</p>
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<p>Temperature-dependent Co<span class="html-italic">K</span>- and Fe<span class="html-italic">K</span>-edge XMCD H<sub>C</sub> areas for Co<sub>2</sub>FeO<sub>2</sub>BO<sub>3</sub>, measured across a temperature range of 5 to 130 K.</p>
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