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2010, Journal of Physics: Conference Series
A samarium doped polycrystalline ZrO 2 bulk sample was investigated for its phase composition as well as optical properties within the temperature range 6-300 K. From micro-Raman measurements the existence of tetragonal as well as monoclinic phase was confirmed. The emission spectrum of Sm 3+ reveals drastic changes under excitation near the region of fundamental absorption. Combined excitation-emission spectroscopy (CEES) measurements reveal three different sites for the dopant ions to be present in the sample. Nature and excitation scheme of the three sites are discussed.
Journal of Non-Crystalline Solids, 2008
We obtained samarium-doped zirconia using two different routes. In one, atomic layer deposited thin crystalline films were doped by using ion implantation; this sample was mainly monoclinic. The other method, the skull-melting technique, yielded polycrystalline bulk zirconia containing both monoclinic and tetragonal phases of ZrO 2 . Thorough photoluminescence (PL) measurements of Sm emission in these materials were performed using pulsed laser excitation at 405, 320 and 230 nm, respectively corresponding to direct, defect-related and host-sensitized excitation. Both samples exhibited well-resolved emission series of Sm 3+ . In general, the recorded spectra may be considered as superpositions of two different sets of lines attributable to Sm 3+ centers in different crystalline phases of ZrO 2 . These results have been confirmed by time-resolved measurements, which also suggest that all emission lines originate from a common initial state ( 4 G 5/2 ) with a lifetime of about 1 ms. As expected, the host-mediated excitation leads to a prolonged decay profile attributed to the retarded energy transfer from host to guest.
2020
15 at% Mg-doped ZrO2 ceramic material was synthesized by solid-state reaction at 1600 oC. Particle size analysis of raw materials mixture depicts the formation of a narrow particle size distribution (PSD) with a mean particle size of about 56 nm. The structural analysis confirms that the assynthesized Mg-doped ZrO2 product is of pure tetragonal phase (t-ZrO2) with a crystallite size of 55.76 nm. The UV–VIS diffuse reflectance spectrum (DRS) showed a maximum %R at 550 nm and the estimated optical bandgap was about 3.83 eV. The morphology of the sample examined by scanning electron microscopy (SEM) shows interconnected grains in the sintered ceramics. Moreover, EDX analyses confirm the presence of Mg, Zr, and O, with a homogenous distribution throughout the sample.
Journal of The American Ceramic Society, 2010
Pure and Sm3+ (0.33, 0.46, 1.48, and 2.19 at.%)-doped ZrO2 thin films have been prepared using radio-frequency (RF) sputtering technique. The phase composition and photoluminescence (PL) properties have been studied on these pure and doped thin films as a function of annealing temperature and doping concentration. Phase composition analysis indicates the increment in the monoclinic content and crystallite size of the pure sample with the increase in annealing temperature. Higher doping promotes the tetragonal phase of the material. From PL studies, Sm3+ (0.33 at.%)-doped zirconia thin film shows a stronger emission spectra than other higher doping. All doped samples exhibit a well-resolved emission series of Sm3+ at higher annealing temperatures. The effect of structural modifications on the PL spectra of the zirconia system has been investigated. Monoclinic phase promotes the luminescence efficiency of this system. PL study shows one to one correspondence with that of structural modification of zirconia system.
Journal of the American …, 2010
Pure and Sm 31 (0.33, 0.46, 1.48, and 2.19 at.%)-doped ZrO 2 thin films have been prepared using radio-frequency (RF) sputtering technique. The phase composition and photoluminescence (PL) properties have been studied on these pure and doped thin films as a function of annealing temperature and doping concentration. Phase composition analysis indicates the increment in the monoclinic content and crystallite size of the pure sample with the increase in annealing temperature. Higher doping promotes the tetragonal phase of the material. From PL studies, Sm 31 (0.33 at.%)-doped zirconia thin film shows a stronger emission spectra than other higher doping. All doped samples exhibit a well-resolved emission series of Sm 31 at higher annealing temperatures. The effect of structural modifications on the PL spectra of the zirconia system has been investigated. Monoclinic phase promotes the luminescence efficiency of this system. PL study shows one to one correspondence with that of structural modification of zirconia system.
Physical Chemistry Chemical Physics, 2012
Pure and europium (Eu 3+ ) doped ZrO 2 synthesized by an oil-in-water microemulsion reaction method were investigated by in situ and ex situ X-ray diffraction (XRD), ex situ Raman spectroscopy, high-resolution transmission electron microscopy (HRTEM), steady state and time-resolved photoluminescence (PL) spectroscopies. Based on the Raman spectra excited at three different wavelengths i.e. 488, 514 and 633 nm and measured in the spectral range of 150-4000 cm À1 the correlation between the phonon spectra of ZrO 2 and luminescence of europium is clearly evidenced. The PL investigations span a variety of steady-state and time resolved measurements recorded either after direct excitation of the Eu 3+ f-f transitions or indirect excitation into UV charge-transfer bands. After annealing at 500 1C, the overall Eu 3+ emission is dominated by Eu 3+ located in tetragonal symmetry lattice sites with a crystal-field splitting of the 5 D 0 -7 F 1 emission of 20 cm À1 . Annealing of ZrO 2 at 1000 1C leads to a superposition of Eu 3+ emissions from tetragonal and monoclinic lattice sites with monoclinic crystal-field splitting of 200 cm À1 for the 5 D 0 -7 F 1 transition. At all temperatures, a non-negligible amorphous/disordered content is also measured and determined to be of monoclinic nature. It was found that the evolutions with calcination temperature of the average PL lifetimes corresponding to europium emission in the tetragonal and monoclinic sites and the monoclinic phase content of the Eu 3+ doped ZrO 2 samples follow a similar trend. By use of specific excitation conditions, the distribution of europium on the amorphous/disordered surface or ordered/crystalline sites can be identified and related to the phase content of zirconia. The role of zirconia host as a sensitizer for the europium PL is also discussed in both tetragonal and monoclinic phases.
physica status solidi (c), 2014
Glasses with chemical compositional {[(TeO 2 ) 0.7 (B 2 O 3 ) 0.3 }] 0.7 [ZnO] 0.3 } 1_x {Sm 2 O 3 } x , (where x=0, 0.005, 0.01, 0.02, 0.03, 0.04, 0.05 mol %); were prepared by conventional melt-quenching technique. The structural properties of the prepared glasses were determined by X-ray diffraction (XRD) analysis and FTIR analysis. It was confirmed that the prepared glasses are amorphous. The bonding parameters of the glasses were analyzed by using FTIR analysis and were confirmed to be ionic in nature. The density, molar volume, and optical energy band gap of these glasses have been measured.The refractive index, molar refraction and polarizability of oxide ion have been estimated by using Lorentz-Lorentz relations. The optical absorption spectra of these glasses were revealed that fundamental absorption edge shifts to higher wavelengths as the content of Sm 2 O 3 increases.The refractive index, optical energy band gap and Urbach energy had been calculated and explained.
Materials Proceedings, 2020
Nanosized coatings of ZrO2 were deposited on silicon substrates using sol-gel and spin coating techniques. The precursor solutions were prepared from ZrOCl2.8H2O with the addition of different percentage (0.5–5%) of rare earth Gd3+ ions as dopant. The thin films were homogeneous, with average thickness of 115 nm and refractive index (n) of 1.83. The X-ray diffraction analysis (XRD) revealed the presence of a varying mixture of monoclinic and tetragonal ZrO2 polycrystalline phases, depending on the dopant, all of which with nanosized crystallites. Scanning electron microscopy (SEM) as well as atomic force microscopy (AFM) methods were deployed to investigate the surface morphology and roughness of the thin films, respectively. They revealed a smooth, well uniform and crack-free surface with average roughness of 0.8 nm. It was established that the dopant concentration affects the photoluminescence (PL) properties of the samples. The undoped films exhibited broad violet-blue PL emissio...
Journal of Physics and Chemistry of Solids, 1999
The properties of dynamically compacted monoclinic zirconia have been studied by X-ray powder diffraction, IR, Raman, EPR and luminescence spectroscopy. Compaction introduces a large number of defects into the sample, which leads to a broadening of the X-ray lines, and IR and Raman bands. Besides, Raman spectra of compacted samples recorded with both 1064 and 488 nm excitation show additional bands in comparison with original monoclinic zirconia. The bands in the region 540-730 nm with 488 nm excitation are ascribed to electronic transitions of Sm 3ϩ ions. The nature of the extra bands in the 3000-1830 cm Ϫ1 region observed with 1064 nm excitation is unknown. Their intensity depends on the concentration of defects, but these bands are still observed for a sample containing no paramagnetic defects. In contrast to uncompacted zirconia, the EPR spectrum of the dynamically compacted material shows defects, most likely related to V H O (oxygen vacancies), which might be an indication for ionic conduction. As monoclinic zirconia is not an ionic conductor, it could be that shock-compaction introduces sample conductivity, e.g. ionic conduction, which can be important for the development of new applications such as batteries.
RSC Advances, 2014
A combined experimental and theoretical study on the photoluminescence (PL) properties of strontium zirconate (SZ) and Sm3+ doped SZ nanostructures is presented in this work.
Journal of Applied Physics, 2012
ZrO 2 samples with 11% Nd and La doping and with 7, 9, 11, and 13% Gd doping have been prepared by co-precipitation route followed by sintering at 700 C and 1100 C, for potential application as high conductivity electrolytes in solid oxide fuel cells. The samples have been characterized by x-ray diffraction with laboratory x-ray source of Cu K a radiation and extended x-ray absorption fine structure (EXAFS) spectroscopy measurement at Zr K edge with synchrotron radiation. The XRD spectra have been analyzed to determine the structure of the samples and the EXAFS data have been analyzed to find out relevant local structure parameters of the Zr-O and Zr-Zr shells, viz., bond distances, co-ordinations, and disorder parameters. The effect of change in ionic radius as well as concentration of the dopants on the above parameters has been thoroughly studied. The experimental results, in some cases, have also been corroborated by first principle calculations of the energetics of the systems. V C 2012 American Institute of Physics.
2001
Photoluminescence (PL) of pure and 0.2 mol percent Sm3+ doped zirconium oxide prepared by the Sol-Gel process and annealed at 1000 degrees C to stabilize the monoclinic phase were performed. The experimental spectra suggest the presence of energy transfer pro9cesses between the host and the dopant when the host was excited with a signal centered at 320 nm. The Sm3+ doped monoclinic zirconium oxide shows strong emission at the green and red bands, corresponding to the 4G5/2 yields 6H5/2 and 4G5/2 yields 6H7/2 samarium transition, respectively; whereas the undoped sample only shows a broad band emission centered at 495 nm. The main mechanism that allows the samarium emission under UV-excitation appears to be non-radiative energy transfer from the ZoO2 host to the Sm3+ ions.
The Journal of Physical Chemistry C, 2012
The local structure of europium doped and impregnated ZrO 2 in the amorphous state and during crystallization is investigated by in situ X-ray diffraction and in situ Raman, high-resolution transmission electron microscopy (HRTEM) and time-resolved photoluminescence spectroscopy. From Raman spectra excited at three different wavelengths (λ ex = 488, 514, and 633 nm), both phonon modes of ZrO 2 and photoluminescence (PL) corresponding to europium electronic transitions were investigated. In the assynthetized state, samples were X-ray and Raman amorphous with few tetragonal (also monoclinic) crystallites being observed under HRTEM microscopy. In situ XRD patterns show that all samples crystallize in the tetragonal phase around 450°C. The time-resolved PL spectra of europium doped and impregnated ZrO 2 show spectral dynamics with time delay after lamp/laser pulse which is assigned to the coexistence of the different amorphous and crystalline components or unreacted europium precursor. From in situ Raman spectra, crystallization was detected at 300−350°C, monitoring for the characteristic tetragonal-like 5 D 0 − 7 F 2 emission of europium at 606 nm. The ratio of tetragonal to amorphous emission increased abruptly from ca. 2−4% at 300−400°C to almost 25% at 400−450°C, whereas at 500°C the emission is mostly tetragonal. A similar trend was found with the ex situ calcined samples, but relative strong tetragonal emission was observed at lower temperature in the range of 350 to 400°C.
Journal of Applied Physics, 2003
Embedding luminescent rare earth ions into transparent oxides such as ZnO is a well-known approach to functionalize the material by adding photon-management properties. In this paper we present a detailed study of the luminescence properties and energy level structure of Pr 3+ and Yb 3+ ions embedded in ZnO thin films deposited by magnetron reactive sputtering. Careful study of the photoluminescence and excitation spectra allowed identifying and locating almost all excited levels of Pr 3+ and Yb 3+ ions. Thus, an almost complete electronic energy level diagram of these ions in the ZnO crystal lattice can be drawn for the first time. In particular, we show that the crystal field of ZnO strongly modifies the energy level structure of the Pr 3+ and Yb 3+ ions creating energy mismatches between the transitions useful for cooperative down conversion. Finally, we demonstrate that light emission from Pr 3+ ions can be induced both by direct excitation of the ions and indirectly by energy transfer from the ZnO matrix.
Optical Materials, Volume 31, Issue 8, Pages 1134–1143, 2009
(Sr0.995Tm0.005)ZrO3 (STZO) powders were prepared by the polymeric precursor method and heat treated at different temperatures for 2 h under oxygen flow. These powders were analyzed by X-ray diffraction (XRD), Ultraviolet–visible (UV–vis) absorption spectroscopy, photoluminescence (PL) measurements, field-emission gun-scanning electron microscopy (FEG-SEM) and energy dispersive X-ray spectrometry (EDXS). XRD patterns revealed that the powders crystallize in an orthorhombic structure without the presence of secondary phases. UV–vis absorption spectra suggest that the STZO powders heat treated at low temperatures present intermediary energy levels within the band gap as consequence of structural defects in the lattice. PL measurements indicated the presence of broad, broad/narrow and narrow bands in STZO powders. The broad bands were associated to the asymmetric STZO structure and/or p–d transitions while, the narrow bands were ascribed to f–f transitions arising from thulium ions. A simple model was proposed in order to explain the PL behavior of these powders. FEG-SEM micrographs showed that these powders are composed by several microparticles with irregular morphologies and agglomerated nature. EDXS data were used for analyses of chemical compositional of powders.
Journal of Physics D: Applied Physics, 2009
The structural, magnetic and luminescence properties of praseodymium-doped zirconia powders of compositions Pr 0.03 Zr 0.97 O 2 and Pr 0.05 Zr 0.95 O 2 synthesized by a sol-gel process have been investigated. X-ray diffraction patterns indicate that these materials crystallize in a tetragonal fluorite-type structure. Scanning electron microscopy shows that the powders exhibit an agglomerated microcrystalline structure and the grain size may be in the order of 5-20 µm. The study of the magnetic properties of these doped metal oxides indicates a Curie-Weiss behaviour in the temperature range (100-300) K that allow us to estimate an effective magnetic moment of 3.51 µ B , which indicates the presence of Pr 3+ in the grown samples. Cathodoluminescence spectra recorded at temperatures between 85 and 295 K show emission peaks that can be attributed to transitions between different states within the 4f 2 configuration of Pr 3+ ions incorporated in the zirconia crystal lattice. Thermoluminescence measured at temperatures ranging from 373 to 773 K and at 550 nm wavelength show an intense and broad peak around 653 K for the Pr-doped zirconia which is not observed in the undoped material.
Optical Materials, 2005
Strong visible emission under UV (320 nm) and IR (967 nm) excitation on ZrO 2 :Sm 3+ and ZrO 2 :Er 3+ nanophosphors were obtained and the concentration effect on the luminescence and crystalline structure is reported. Experimental results shows that phase composition depend on the ion concentration. The visible emission obtained under UV excitation is produced by the transitions 4 G 5/2 ! 6 H 5/2,7/2,9/2 of Sm 3+ through a non-radiative energy transfer process from the host to the active ion. Energy transfer and quenching effect due to ion concentration was confirmed by measuring the fluorescence decay time. Green (545 nm) and red (680 nm) emissions bands were observed under IR excitation troughs an upconversion process. It was proved that visible emission for both nanophosphor could be tuned by controlling the ion concentration. The nature of this behavior is discussed taking into account the phase composition for ZrO 2 :Sm 3+ and two photon absorption and cross-relaxation process was considered for ZrO 2 :Er 3+ nanophosphor.
PHYSICAL REVIEW B 85(15), 155202 (2012)
deA combination of experiments and ab initio quantum-mechanical calculations has been applied to examine electronic, structural, and hyperfine interactions in pure and Ta-doped zirconium dioxide in its monoclinic phase (m-ZrO2). From the theoretical point of view, the full-potential linear augmented plane wave plus local orbital (APW + lo) method was applied to treat the electronic structure of the doped system including the atomic relaxations introduced by the impurities in the host in a fully self-consistent way using a supercell approach. Different charge states of the Ta impurity were considered in the study and its effects on the electronic, structural, and hyperfine properties are discussed. Our results suggest that two different charge states coexist in Ta-doped m-ZrO2. Further, ab initio calculations predict that depending on the impurity charge state, a sizeable magnetic moment can be induced at the Ta-probe site. This prediction is confirmed by a new analysis of experimental data.
Proceedings of …, 2001
Photoluminescence (PL) of pure and 0.2 mol% Sm3 doped zirconium oxide prepared by the Sot-Gel process and annealed at 1 000°C to stabilize the monoclinic phase were performed. The experimental spectra suggest the presence of energy transfer processes between the host (Zr02) and the dopant (Sm3+), when the host was excited with a. 3+. .. .. . signal centered at 320 nm. The Sm doped monochnic zirconium oxide shows strong emission at the green (569 nm) and red (607, 613 and 61 8 nm) bands, corresponding to the 4G512-6H512 and 4G512-> 6H712 samarium transition, respectively; whereas the undoped sample only shows a broad band emission centered at 495 nm. The main mechanism that allows the samarium emission under UV-excitation appears to be non-radiative energy transfer from the Zr02 host to the Sm3 ions.
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