919 research outputs found

    Dopants adsorbed as single atoms prevent degradation of catalysts

    Full text link
    The design of catalysts with desired chemical and thermal properties is viewed as a grand challenge for scientists and engineers. For operation at high temperatures, stability against structural transformations is a key requirement. Although doping has been found to impede degradation, the lack of atomistic understanding of the pertinent mechanism has hindered optimization. For example, porous gamma-Al2O3, a widely used catalyst and catalytic support, transforms to non-porous alpha-Al2O3 at ~1,100C. Doping with La raises the transformation temperature to ~1,250C, but it has not been possible to establish if La atoms enter the bulk, adsorb on surfaces as single atoms or clusters, or form surface compounds. Here, we use direct imaging by aberration-corrected Z-contrast scanning transmission electron microscopy coupled with extended X-ray absorption fine structure and first-principles calculations to demonstrate that, contrary to expectations, stabilization is achieved by isolated La atoms adsorbed on the surface. Strong binding and mutual repulsion of La atoms effectively pin the surface and inhibit both sintering and the transformation to alpha-Al2O3. The results provide the first guidelines for the choice of dopants to prevent thermal degradation of catalysts and other porous materials.Comment: RevTex4, 4 pages, 4 JPEG figures, published in Nature Material

    Effect of lanthanide doping on structural, microstructural and functional properties of K0.5Na0.5NbO3 lead-free piezoceramics

    Get PDF
    Lanthanides-doped K0.5Na0.5NbO3(KNN) lead-free piezoelectric ceramics are prepared by conventional solid-state reaction. The effects of lanthanum concentration and the lanthanide type on the structure, microstructure and ferro-piezoelectric properties are evaluated. Ln3+ doping has a slight effect on the structure, but greatly inhibits the grain growth. Moreover, a decrease in the Curie temperature and an increase in the dielectric constant values are observed when doping. Large amounts of lanthanum induce a diffuse phase transition and an increase of the dielectric losses. The piezoelectric properties are greatly improved when doping with small amounts of dopants. As the ionic radii of the lanthanide is reduced, the piezoelectric properties of the ceramics are increased, the Eu3+-doped ceramics show an increase of 29% of the piezoelectric coefficient d33 with respect to pure KNN. The results show that low concentrations of lanthanides improve significantly the functional properties of KNN lead-free piezoceramics. Doping with lanthanides should be taken into consideration in some other compositions based on KNN.Postprint (author's final draft

    Characterization of nanoporous lanthanide-doped gadolinium gallium garnet powders obtained by propellant synthesis

    Get PDF
    In the present work we study the nanocrystalline powders of lanthanide-doped Gd3Ga5O12 (GGG, gadolinium gallium garnet) prepared using propellant synthesis. A series of GGG samples containing a number of different trivalent lanthanide ions (Tm, Er, Ho, Eu, Sm, Nd, and Pr) in different quantities (1%, 5%, 10%) were produced. Samples were characterized by X-ray diffraction (pre- and post calcination) for phase identification and line-broadening analysis, and by electron microscopy (SEM and TEM) for morphological and nanostructural investigation. Thermal behavior of the powder was investigated by thermal gravimetric analysis (TGA) and differential thermal analysis (DTA). The samples have a polycrystalline porous structure. Elemental microanalysis made by energy dispersive X-ray spectroscopy (EDX) detector attached to TEM and XRD unit-cell determinations confirmed that the lanthanides ions entered the structure of GGG. Crystallites have a high degree of disorder

    Spectral Engineering of Optical Fiber Through Active Nanoparticle Doping

    Get PDF
    The spectral engineering of optical fiber is a method of intentional doping of the core region in order to absorb/emit specific wavelengths of light therby providing enhanced performance over current fibers. Efforts here focused on developing an understanding of optically active nanoparticles based on alkaline earth fluorides that could be easily and homogeneously incorporated into the core of a silica based optical fiber preform and result in efficient and tailorable spectral emissions. Doped and undoped calcium, strontium and barium fluoride nanoparticles were successfully synthesized and characterized for their physical, chemical, and optical behavior. Distinct spectroscopic differences as a result of different host materials, varying rare earth doping levels and processing conditions, indicated the ability to influence the spectral behavior of the doped nanoparticle. By using photoluminescence to predict diffusion behavior, the application of a simple one dimensional model for diffusion provided a method for predicting the diffusion coefficient of europium ions in alkaline earth fluorides with order of magnitude accuracy. Modified chemical vapor deposition derived silica preforms were individually solution doped with europium doped alkaline earth fluoride nanoparticles. By using the rare earth doped alkaline earth fluoride nanoparticles as the dopant materials in the core of optical fiber preforms, the resultant optical properties of the glass were significantly influenced by their presence in the core. The incorporation of these rare earth doped alkaline earth fluoride nanoparticles was found to significantly influence the local chemical and structural environment about the rare earth ion, demonstrated homogeneity and uniform distribution of the rare earth dopant and resulted in specifically unique spectral behavior when compared to conventional doping methods. A more detailed structural model of the doped core glass region has been developed based on the spectral behavior of these active fiber preforms. It has been shown that rare earth doping of alkaline earth fluoride nanoparticles provides a material which can be `tuned\u27 to specific applications through the use of different host materials, processing conditions and doping levels of the rare earth and when used as dopant materials for active optical fibers, provides a means to tailor the optical behavior

    In Situ Raman Characterization of SOFC Materials in Operational Conditions: A Doped Ceria Study

    Get PDF
    [EN] The particular operational conditions of electrochemical cells make the simultaneous characterization of both structural and transport properties challenging. The rapidity and flexibility of the acquisition of Raman spectra places this technique as a good candidate to measure operating properties and changes. Raman spectroscopy has been applied to well-known lanthanide ceria materials and the structural dependence on the dopant has been extracted. The evolution of Pr-doped ceria with temperature has been recorded by means of a commercial cell showing a clear increment in oxygen vacancies concentration. To elucidate the changes undergone by the electrolyte or membrane material in cell operation, the detailed construction of a homemade Raman cell is reported. The cell can be electrified, sealed and different gases can be fed into the cell chambers, so that the material behavior in the reaction surface and species evolved can be tracked. The results show that the Raman technique is a feasible and rather simple experimental option for operating characterization of solid-state electrochemical cell materials, although the treatment of the extracted data is not straightforward.This research was funded by the Spanish Government (IJCI-2017-34110, RTI2018-102161 and SEV-2016-0683 grants).SolĂ­s, C.; Balaguer Ramirez, M.; Serra Alfaro, JM. (2020). In Situ Raman Characterization of SOFC Materials in Operational Conditions: A Doped Ceria Study. Membranes. 10(7):1-16. https://doi.org/10.3390/membranes10070148S116107Maher, R. C., Duboviks, V., Offer, G. J., Kishimoto, M., Brandon, N. P., & Cohen, L. F. (2013). Raman Spectroscopy of Solid Oxide Fuel Cells: Technique Overview and Application to Carbon Deposition Analysis. Fuel Cells, 13(4), 455-469. doi:10.1002/fuce.201200173Cheng, Z., Wang, J.-H., Choi, Y., Yang, L., Lin, M. C., & Liu, M. (2011). From Ni-YSZ to sulfur-tolerant anode materials for SOFCs: electrochemical behavior, in situ characterization, modeling, and future perspectives. Energy & Environmental Science, 4(11), 4380. doi:10.1039/c1ee01758fLiu, M., Lynch, M. E., Blinn, K., Alamgir, F. M., & Choi, Y. (2011). Rational SOFC material design: new advances and tools. Materials Today, 14(11), 534-546. doi:10.1016/s1369-7021(11)70279-6Maher, R. C., Shearing, P. R., Brightman, E., Brett, D. J. L., Brandon, N. P., & Cohen, L. F. (2015). Reduction Dynamics of Doped Ceria, Nickel Oxide, and Cermet Composites Probed Using In Situ Raman Spectroscopy. Advanced Science, 3(1), 1500146. doi:10.1002/advs.201500146Laguna-Bercero, M. A., & Orera, V. M. (2011). Micro-spectroscopic study of the degradation of scandia and ceria stabilized zirconia electrolytes in solid oxide electrolysis cells. International Journal of Hydrogen Energy, 36(20), 13051-13058. doi:10.1016/j.ijhydene.2011.07.082Brett, D. J. L., Kucernak, A. R., Aguiar, P., Atkins, S. C., Brandon, N. P., Clague, R., 
 Vesovic, V. (2010). What Happens Inside a Fuel Cell? Developing an Experimental Functional Map of Fuel Cell Performance. ChemPhysChem, 11(13), 2714-2731. doi:10.1002/cphc.201000487Sheppard, N. (1982). Recent developments in the vibrational spectroscopies (infrared, Raman, electron energy loss etc.) as applied to the structural analysis of species chemisorbed on metal surfaces. Journal of Molecular Structure, 80, 163-174. doi:10.1016/0022-2860(82)87225-6Balaguer, M., SolĂ­s, C., & Serra, J. M. (2012). Structural–Transport Properties Relationships on Ce1–xLnxO2−ή System (Ln = Gd, La, Tb, Pr, Eu, Er, Yb, Nd) and Effect of Cobalt Addition. The Journal of Physical Chemistry C, 116(14), 7975-7982. doi:10.1021/jp211594dMogensen, M. (2000). Physical, chemical and electrochemical properties of pure and doped ceria. Solid State Ionics, 129(1-4), 63-94. doi:10.1016/s0167-2738(99)00318-5Balaguer, M., GarcĂ­a-Fayos, J., SolĂ­s, C., & Serra, J. M. (2013). Fast Oxygen Separation Through SO2- and CO2-Stable Dual-Phase Membrane Based on NiFe2O4–Ce0.8Tb0.2O2-ÎŽ. Chemistry of Materials, 25(24), 4986-4993. doi:10.1021/cm4034963Degen, T., Sadki, M., Bron, E., König, U., & NĂ©nert, G. (2014). The HighScore suite. Powder Diffraction, 29(S2), S13-S18. doi:10.1017/s0885715614000840Rietveld, H. M. (1969). A profile refinement method for nuclear and magnetic structures. Journal of Applied Crystallography, 2(2), 65-71. doi:10.1107/s0021889869006558RodrĂ­guez-Carvajal, J. (1993). Recent advances in magnetic structure determination by neutron powder diffraction. Physica B: Condensed Matter, 192(1-2), 55-69. doi:10.1016/0921-4526(93)90108-iShannon, R. D. (1976). Revised effective ionic radii and systematic studies of interatomic distances in halides and chalcogenides. Acta Crystallographica Section A, 32(5), 751-767. doi:10.1107/s0567739476001551Taniguchi, T., Watanabe, T., Sugiyama, N., Subramani, A. K., Wagata, H., Matsushita, N., & Yoshimura, M. (2009). Identifying Defects in Ceria-Based Nanocrystals by UV Resonance Raman Spectroscopy. The Journal of Physical Chemistry C, 113(46), 19789-19793. doi:10.1021/jp9049457Weber, W. H., Hass, K. C., & McBride, J. R. (1993). Raman study ofCeO2: Second-order scattering, lattice dynamics, and particle-size effects. Physical Review B, 48(1), 178-185. doi:10.1103/physrevb.48.178Parayanthal, P., & Pollak, F. H. (1984). Raman Scattering in Alloy Semiconductors: «Spatial Correlation» Model. Physical Review Letters, 52(20), 1822-1825. doi:10.1103/physrevlett.52.1822Kosacki, I., Suzuki, T., Anderson, H. U., & Colomban, P. (2002). Raman scattering and lattice defects in nanocrystalline CeO2 thin films. Solid State Ionics, 149(1-2), 99-105. doi:10.1016/s0167-2738(02)00104-2McBride, J. R., Hass, K. C., Poindexter, B. D., & Weber, W. H. (1994). Raman and x‐ray studies of Ce1−xRExO2−y, where RE=La, Pr, Nd, Eu, Gd, and Tb. Journal of Applied Physics, 76(4), 2435-2441. doi:10.1063/1.357593Esther Jeyanthi, C., Siddheswaran, R., Kumar, P., Siva Shankar, V., & Rajarajan, K. (2014). Structural and spectroscopic studies of rare earths doped ceria (RELa,Sc,Yb:CeO2) nanopowders. Ceramics International, 40(6), 8599-8605. doi:10.1016/j.ceramint.2014.01.076Shirbhate, S., Nayyar, R. N., Ojha, P. K., Yadav, A. K., & Acharya, S. (2019). Exploration of Atomic Scale Changes during Oxygen Vacancy Dissociation Mechanism in Nanostructure Co-Doped Ceria: As Electrolytes for IT-SOFC. Journal of The Electrochemical Society, 166(8), F544-F554. doi:10.1149/2.1191908jesArtini, C. (2018). Rare-Earth-Doped Ceria Systems and Their Performance as Solid Electrolytes: A Puzzling Tangle of Structural Issues at the Average and Local Scale. Inorganic Chemistry, 57(21), 13047-13062. doi:10.1021/acs.inorgchem.8b02131Spanier, J. E., Robinson, R. D., Zhang, F., Chan, S.-W., & Herman, I. P. (2001). Size-dependent properties ofCeO2−ynanoparticles as studied by Raman scattering. Physical Review B, 64(24). doi:10.1103/physrevb.64.245407Zhang, F., Chan, S.-W., Spanier, J. E., Apak, E., Jin, Q., Robinson, R. D., & Herman, I. P. (2002). Cerium oxide nanoparticles: Size-selective formation and structure analysis. Applied Physics Letters, 80(1), 127-129. doi:10.1063/1.1430502Suzuki, T., Kosacki, I., Anderson, H. U., & Colomban, P. (2004). Electrical Conductivity and Lattice Defects in Nanocrystalline Cerium Oxide Thin Films. Journal of the American Ceramic Society, 84(9), 2007-2014. doi:10.1111/j.1151-2916.2001.tb00950.xDohčević-Mitrović, Z. D., Ơćepanović, M. J., Grujić-Brojčin, M. U., Popović, Z. V., BoĆĄković, S. B., Matović, B. M., 
 Aldinger, F. (2006). The size and strain effects on the Raman spectra of Ce1−xNdxO2−ή (0≀x≀0.25) nanopowders. Solid State Communications, 137(7), 387-390. doi:10.1016/j.ssc.2005.12.006Balaguer, M., SolĂ­s, C., & Serra, J. M. (2011). Study of the Transport Properties of the Mixed Ionic Electronic Conductor Ce1−xTbxO2−ή + Co (x = 0.1, 0.2) and Evaluation As Oxygen-Transport Membrane. Chemistry of Materials, 23(9), 2333-2343. doi:10.1021/cm103581wBalaguer, M., SolĂ­s, C., Roitsch, S., & Serra, J. M. (2014). Engineering microstructure and redox properties in the mixed conductor Ce0.9Pr0.1O2−ή+ Co 2 mol%. Dalton Trans., 43(11), 4305-4312. doi:10.1039/c3dt52167bAcharya, S. A., Gaikwad, V. M., Sathe, V., & Kulkarni, S. K. (2014). Influence of gadolinium doping on the structure and defects of ceria under fuel cell operating temperature. Applied Physics Letters, 104(11), 113508. doi:10.1063/1.4869116Zallen, R., & Conwell, E. M. (1979). The effect of temperature on libron frequencies in molecular crystals: Implications for TTF-TCNQ. Solid State Communications, 31(8), 557-561. doi:10.1016/0038-1098(79)90252-7Hart, T. R., Aggarwal, R. L., & Lax, B. (1970). Temperature Dependence of Raman Scattering in Silicon. Physical Review B, 1(2), 638-642. doi:10.1103/physrevb.1.638Lughi, V., & Clarke, D. R. (2007). Temperature dependence of the yttria-stabilized zirconia Raman spectrum. Journal of Applied Physics, 101(5), 053524. doi:10.1063/1.2697347Long, R. Q., Huang, Y. P., & Wan, H. L. (1997). Surface Oxygen Species Over Cerium Oxide and Their Reactivities with Methane and Ethane by Means ofin situConfocal Microprobe Raman Spectroscopy. Journal of Raman Spectroscopy, 28(1), 29-32. doi:10.1002/(sici)1097-4555(199701)28:13.0.co;2-gPushkarev, V. V., Kovalchuk, V. I., & d’ Itri, J. L. (2004). Probing Defect Sites on the CeO2 Surface with Dioxygen. The Journal of Physical Chemistry B, 108(17), 5341-5348. doi:10.1021/jp0311254Weber, A., & McGinnis, E. A. (1960). The Raman spectrum of gaseous oxygen. Journal of Molecular Spectroscopy, 4(1-6), 195-200. doi:10.1016/0022-2852(60)90081-3HornĂ©s, A., Bera, P., FernĂĄndez-GarcĂ­a, M., Guerrero-Ruiz, A., & MartĂ­nez-Arias, A. (2012). Catalytic and redox properties of bimetallic Cu–Ni systems combined with CeO2 or Gd-doped CeO2 for methane oxidation and decomposition. Applied Catalysis B: Environmental, 111-112, 96-105. doi:10.1016/j.apcatb.2011.09.022Duboviks, V., Maher, R. C., Offer, G., Cohen, L. F., & Brandon, N. P. (2013). In-Operando Raman Spectroscopy Study of Passivation Effects on Ni-CGO Electrodes in CO2 Electrolysis Conditions. ECS Transactions, 57(1), 3111-3117. doi:10.1149/05701.3111ecstDuboviks, V., Maher, R. C., Kishimoto, M., Cohen, L. F., Brandon, N. P., & Offer, G. J. (2014). A Raman spectroscopic study of the carbon deposition mechanism on Ni/CGO electrodes during CO/CO2 electrolysis. Phys. Chem. Chem. Phys., 16(26), 13063-13068. doi:10.1039/c4cp01503

    Spectral engineering of optical fiber preforms through active nanoparticle doping

    Get PDF
    Europium doped alkaline earth fluoride [Eu:AEF(2) (AE = Ca, Sr, Ba)] nanoparticles were synthesized and systematically incorporated into the core of modified chemical vapor deposition (MCVD)-derived silica-based preforms by solution doping. The resulting preforms were examined to determine the impact of the nanoparticles chemistry on the spectroscopic behavior of the glass. The dominant existence of Eu3+ was demonstrated in all preforms, which is in contrast to conventional solution doped preforms employing dissolved europium salts where Eu2+ is primarily observed. Raman spectroscopy and fluorescence lifetime measurements indicated that the nanoparticles composition is effective in controlling, at a local chemical and structural level, the spectroscopic properties of active dopants in optical fiber glasses. Further, there is a systematic and marked increase in radiative lifetime, tau, of the Eu3+ emission that follows the cationic mass; tau(Ca) \u3c tau(Sr) \u3c tau(Ba) with the BaF2-derived sample yielding a 37% lengthening of the lifetime over the CaF2-derived one. Such nanoscale control of what otherwise is silica glass could be useful for realizing property-enhanced and tailored spectroscopic performance from otherwise standard materials, e.g., vapor-derived silica, in next generation optical fibers

    Spectral Engineering of Optical Fiber Preforms Through Active Nanoparticle Doping

    Get PDF
    Europium doped alkaline earth fluoride [Eu:AEF2 (AE = Ca, Sr, Ba)] nanoparticles were synthesized and systematically incorporated into the core of modified chemical vapor deposition (MCVD)-derived silica-based preforms by solution doping. The resulting preforms were examined to determine the impact of the nanoparticles chemistry on the spectroscopic behavior of the glass. The dominant existence of Eu3+ was demonstrated in all preforms, which is in contrast to conventional solution doped preforms employing dissolved europium salts where Eu2+ is primarily observed. Raman spectroscopy and fluorescence lifetime measurements indicated that the nanoparticles composition is effective in controlling, at a local chemical and structural level, the spectroscopic properties of active dopants in optical fiber glasses. Further, there is a systematic and marked increase in radiative lifetime, τ, of the Eu3+ emission that follows the cationic mass; τCa \u3c τSr \u3c τBa with the BaF2-derived sample yielding a 37% lengthening of the lifetime over the CaF2-derived one. Such nanoscale control of what otherwise is silica glass could be useful for realizing property-enhanced and tailored spectroscopic performance from otherwise “standard” materials, e.g., vapor-derived silica, in next generation optical fibers

    Lanthanide-doped lanthanum hafnate nanoparticles as multicolor phosphors for warm white lighting and scintillators

    Get PDF
    Designing luminescent materials especially nanomaterials with multifunctional applications is highly challenging and demanding. In this work, we explored pyrochlore La2Hf2O7 nanoparticles (NPs) singly and triply codoped with Eu3+, Tb3+ and Dy3+. Under both ultraviolet and X-ray irradiations, the La2Hf2O7 NPs singly doped with Eu3+, Tb3+ and Dy3+ displayed red, green and yellowish-blue emission, respectively. The concentration quenching study revealed a non-radiative energy transfer in Eu3+ doped La2Hf2O7 NPs, which takes place via dipole-quadrupole mechanism. On the other hand, a dipole-dipole interaction prevails in Tb3+ and Dy3+ doped La2Hf2O7 NPs. Lifetime spectroscopy reveals the stabilization of Eu3+ and Dy3+ ions at La3+ site at low doping concentration whereas a fraction of them migrates to Hf4+ site at high doping concentration. For the La2Hf2O7:Tb3+ NPs, Tb3+ ions are localized at Hf4+ site at all doping concentrations. Furthermore, when triply codoped with Eu3+, Tb3+ and Dy3+ ions, the La2Hf2O7 NPs display beautiful warm white light as a new strategy for color tunability through doping percentage. To sum, our complete spectrum of studies on the structure, UV excited photoluminescence, concentration quenching, and local site spectroscopy of the La2Hf2O7:Ln3+ NPs suggests that they are potential candidates as single-component multicolor-emitting phosphors for lighting and scintillating applications
    • 

    corecore