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1.
The effect of Zn2+ ion on the dopant occupancy and optical characteristic of Er3+ ion in Er/Zn-codoped LiNbO3 crystal is reported. The intense 1.54 μm and relatively weak green upconversion emissions are observed for Er (1 mol%)/Zn (6 mol%):LiNbO3 crystal. The OH? absorption and the time-resolved spectra show that the Zn2+ codoping decreases the threshold concentration of Er3+ ion in Er/Zn-codoped LiNbO3 crystal. The experimental results here imply that the potential application of Er3+-doped LiNbO3 crystal can be designed and optimized on the basis of the theoretical investigations.  相似文献   

2.
The Zn/Er/Yb:LiNbO3 and Er/Yb:LiNbO3 crystals were grown by the Czochralski technique. The laser characteristics of 1.54 μm emission were predicted based on the Judd–Ofelt theory, and the intensity parameters Ωt (Ω2=7.23×10?20 cm2, Ω4=3.15×10?20 cm2 and Ω6=1.43×10?20 cm2) were obtained. The stimulated emission cross sections (σem) at 1.54 μm emission in Zn/Er/Yb:LiNbO3 were calculated based on the McCumber theory and the Füchtbauer–Ladenburg theory. The gain cross section spectrum of Zn/Er/Yb:LiNbO3 crystal was also investigated. Under 980 nm excitation, a lenghthening lifetime of 1.54 μm emission and an enhancement of green upconversion emission were observed for Zn/Er/Yb:LiNbO3 crystal. The studies on the power pump dependence and the upconversion mechanism suggested that both green and red upconversion emissions were populated via the three-photon process, and Zn2+ ion tridoping increases the probability of cross relaxation process between the two neighboring Er3+ ions.  相似文献   

3.
We report a visible luminescence of Er3+ ions in an amorphous-nanocrystalline AlN:Er thin film prepared by co-deposition using AlN, Er, and SiO2 targets. A PL emission spectrum of Er3+ in the AlN:Er film annealed at 750 °C showed a strong bluish green emission of Er3+ in the amorphous-nanocrystalline AlN:Er thin film, which is attributed to the intra-4fEr3+ transitions of 2H11/2  4I15/2 and 4F7/2  4I15/2. It was found that crystallite diameters were between 3 and 5 nm by high-resolution transmission electron microscopy. The occurrence of the strong Er3+ emission in the annealed AlN:Er thin film with a mixture of amorphous and nanocrystalline phases may be contributed to an increase in the number of excitation Er3+ centers and a presence of oxygen related to Er3+ excitation and recombination process in the AlN:Er thin film.  相似文献   

4.
《Ultrasonics sonochemistry》2014,21(6):1964-1968
Through an ultrasound assisted method, TiO2/WO3 nanoparticles were synthesized at room temperature. The XRD pattern of as-prepared TiO2/WO3 nanoparticles matches well with that of pure monoclinic WO3 and rutile TiO2 nanoparticles. TEM images show that the prepared TiO2/WO3 nanoparticles consist of mixed square and hexagonal shape particles about 8–12 nm in diameter. The photocatalytic activity of TiO2/WO3 nanoparticles was tested for the degradation of a wastewater containing methylene blue (MB) under visible light illumination. The TiO2/WO3 nanoparticles exhibits a higher degradation rate constant (6.72 × 10−4 s−1) than bare TiO2 nanoparticles (1.72 × 10−4 s−1) under similar experimental conditions.  相似文献   

5.
The spectral characteristics of 1.54 μm emission in a series of Zn/Er:LiNbO3 crystals with heavy Er content and variable Zn content were reported. The inductively coupled plasma mass spectrometry (ICP-MS) was used to determine the concentration of Er3+ ion in the crystal. The absorption and emission spectra of Zn/Er:LiNbO3 crystals were measured. Based on Judd–Ofelt theory, the spectral parameters such as intensity parameters Ωt (t=2, 4 and 6), transition strengths, radiative transition probabilities, radiative lifetime and fluorescence branching ratio have been obtained in Zn/Er:LiNbO3 system. The emission cross section corresponding to 4I13/24I15/2 transition of Er3+ ion was obtained according to Füchtbauer–Ladenburg theory. The gain cross section of Er:LiNbO3 crystal codoped with 6 mol% Zn2+ ions were also discussed in this work.  相似文献   

6.
Spectroscopic characterization of Yb3+/Er3+ codoped TeO2–R2O–ZnO–Ln2O3 glasses as a function of network modifiers (R=Li, Na and K) has been investigated. The Judd–Ofelt parameters (Ωt), quantum efficiency in near infrared (1.55 μm) and visible up-conversion (546 and 660 nm) and quality factor spectroscopy (χ) were calculated. Three up-conversion emission bands centered at 525, 546 and 660 nm were observed as maxima for glasses containing potassium. The measured lifetime of 4I13/2, 4F9/2 and 4S3/2 from Er3+ and 4F5/2 from Yb3+ levels increased when potassium (K) replaced lithium (Li) and Na. The maximum emission cross-section (ECS) for 4I13/24I15/2 transition of Er3+ was calculated to be 1.02×10?20 cm2 for TeO2–Li2O–ZnO–Ln2O3 glasses. The energy transfer efficiency (ET) from Yb3+ to Er3+, (4F5/2)+(4I15/2)→(4F7/2)+(4I13/2), was calculated using the measured lifetimes of Yb3+ with and without the presence of acceptor (Er3+). The maximum calculated ET was 58% for 0.25 mol% of Er3+ and 3 mol% of Yb3+ for TeO2–K2O–ZnO–Ln2O3 glass composition.  相似文献   

7.
A detailed study of the fluorescence radiative dynamics and energy transfer processes between Er and Tm ions in the Er3+/Tm3+ doped fluoride glass is reported. The fluorescence properties of 2.7 μm emission, other infrared and visible emissions are investigated under different selective laser excitations. Three Judd–Ofelt intensity parameters, energy transfer microparameters and efficiency have been determined and discussed. It is found that present Er3+/Tm3+ doped fluoride glass possesses large calculated emission cross section (8.98×10–21 cm2) around 2.7 μm. The more suitable pumping scheme for laser applications at 2.7 μm laser is 980 nm excitation for Er3+/Tm3+ doped fluoride glass.  相似文献   

8.
Vibrational Raman spectra have been measured for strontium barium niobate (Sr0.5Ba0.5Nb2O6, SBN50) single crystals and nanopowders doped with 1 mol% of the luminescent ions Eu3+ and Er3+. The nanocrystalline materials show slightly broader spectra with respect to the single crystals with the same composition. The presence of the Eu3+ and Er3+ ions at the 1 mol% doping level, and the present particle size (200 nm) do not appear to affect the ferro-to-paraelectric phase transition temperature typical of undoped SBN50 single crystals, as detected from anomalies in the dependence of the position of the Raman peak around 635 cm?1 as a function of the temperature.  相似文献   

9.
The Bi–Tm–Er co-doped SiO2–Al2O3–La2O3 (SAL) glasses, which exhibited a broadband near-infrared (NIR) emission, were investigated by the optical absorption and photoluminescence spectra. A super broadband NIR emission extending from 0.95 to 1.6 μm with a full-width at half-maximum (FWHM) of 430 nm which covered the whole O, E, S, C and L bands, was observed in Bi–Tm–Er co-doped samples under 808 nm excitation, as a result of the overlap of the Bi-related emission band (centered at 1270 nm) and the emission from Tm3+ 3H43F4 transition (1450 nm) as well as Er3+ 4I13/24I15/2 transition (1545 nm). In addition, a super broadband emission with amplitude relatively flat from 0.95 to 2.1 μm has been observed. The possible energy transfer between Bi-related centers, Tm3+ ions and Er3+ ions was proposed.  相似文献   

10.
Photoluminescence (PL) properties of Er-doped β-FeSi2 (β-FeSi2:Er) and Er-doped Si (Si:Er) grown by ion implantation were investigated. In PL measurements at 4.2 K, the β-FeSi2:Er showed the 1.54 μm PL due to the intra-4f shell transition of 4I13/24I15/2 in Er3+ ions without a defect-related PL observed in Si:Er. In the dependence of the PL intensity on excitation photon flux density, the obtained optical excitation cross-section σ in β-FeSi2:Er (σ=7×10−17 cm2) is smaller than that in Si:Er (σ=1×10-15 cm2). In the time-resolved PL and the temperature dependence of the PL intensity, the 1.54 μm PL in β-FeSi2:Er showed a longer lifetime and larger activation energies for non-radiative recombination (NR) processes than Si:Er. These results revealed that NR centers induced by ion implantation damage were suppressed in β-FeSi2:Er, but the energy back transfer from Er3+ to β-FeSi2 was larger than Si:Er.  相似文献   

11.
Efficient Er3+:Y2O3 phosphor is synthesized by the sol–gel method. Rate equations for Er3+ energy level populations are used to investigate pump power and temperature dependences of upconversion intensity as well as the fluorescence decay profiles. Excited state absorption cross section of Er3+ 4I13/2 of 6.8×10?27 m2 and cross relaxation rate of 6200 s?1 are determined from comparison between theoretical predictions and experimental data. In addition, it is found that effect of temperature on the phonon-assistant absorption cannot be neglected. This work provides references for the prediction of the upconversion behavior in Er3+ singly doped matrix.  相似文献   

12.
This paper reports on the thermo (TL), iono (IL) and photoluminescence (PL) properties of nanocrystalline CaSiO3:Eu3+ (1–5 mol %) bombarded with 100 MeV Si7+ ions for the first time. The effect of different dopant concentrations and influence of ion fluence has been discussed. The characteristic emission peaks 5D07FJ (J=0, 1, 2, 3, 4) of Eu3+ ions was recorded in both PL (1×1011–1×1013 ions cm?2) and IL (4.16×1012–6.77×1012 ions cm?2) spectra. It is observed that PL intensity increases with ion fluence, whereas in IL the peaks intensity increases up to fluence 5.20×1012 ions cm?2, then it decreases. A well resolved TL glow peak at ~304 °C was recorded in all the ion bombarded samples at a warming rate of 5 °C s?1. The TL intensity is found to be maximum at 5 mol% Eu3+ concentration. Further, TL intensity increases sub linearly with shifting of glow peak towards lower temperature with ion fluence.  相似文献   

13.
A series of Cr,Er:Gd3Ga5O12 crystals with high concentrations of Er3 + were grown by Czochralski method. The absorption spectra, the up-conversion, near infrared (NIR) and mid-infrared (Mid-IR) luminescence spectra as well as the luminescence decay curves of Er: 4I13/2 and 4I11/2 levels were measured at room temperature. The spectroscopic properties of Cr,Er:Gd3Ga5O12 crystals and Cr–Er energy transfer processes were investigated. The spectroscopy of the Er3 +:4I11/2  4I13/2 transition was centralized to discuss, and the important optical parameters including luminescence lifetimes and the Cr–Er energy transfer efficiency are presented. Based on the comprehensive spectral analyses, 0.6 at.%Cr/50 at.%Er:GGG crystal is preferred as candidate of potential xenon lamp pumped ~ 2.7 μm laser in this work.  相似文献   

14.
(5.0%)Er3+:Y3Al5O12/Pt-(TiO2-Ta2O5) powder, as a high effective sonocatalyst, was prepared using sol-gel and calcination method. Then it was characterized by X-ray diffractometer (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM) and energy dispersive X-ray spectroscopy (EDX). In order to evaluate the sonocatalytic activity of the prepared (5.0%)Er3+:Y3Al5O12/Pt-(TiO2-Ta2O5) powder, the sonocatalytic decomposition of ametryn was studied. In addition, some influencing factors such as different Ti/Ta molar ratios on the sonocatalytic activity of the prepared (5.0%)Er3+:Y3Al5O12/Pt-(TiO2-Ta2O5) powder, catalyst added amount with ultrasonic irradiation time and used times on the sonocatalytic decomposition efficiency were examined by using ion chromatogram determination. The experimental results showed that the best sonocatalytic decomposition ratio of ametryn were 77.50% based on the N atom calculation and 95.00% based on the S atom calculation, respectively, when the conditions of 10.00 mg/L initial concentration, 1.00 g/L prepared (5.0%)Er3+:Y3Al5O12/Pt-(TiO2-Ta2O5) powder (Ti/Ta = 1.00:0.25 heat-treated at 550 °C for 3.0 h) added amount, 150 min ultrasonic irradiation (40 kHz frequency and 300 W output power), 100 mL total volume and 25–28 °C temperature were adopted. Therefore, the (5.0%)Er3+:Y3Al5O12/Pt-(TiO2-Ta2O5) composite nanoparticles could be considered as an effective sonocatalyst for decomposition of ametryn in aqueous solution.  相似文献   

15.
《Journal of luminescence》2003,65(2-4):127-133
BaMgAl10O17:Eu2+ (BAM) blue phosphor particles with improved photoluminescence (PL) intensity under vacuum ultraviolet (VUV) excitation were prepared by a spray pyrolysis process. In order to improve the PL intensity, Er3+ and Nd3+ ions were used as co-doping elements. The VUV characteristics of BAM:Eu2+, M+ (M=Er, Nd) were monitored with varying the Er3+ and Nd3+ content in order to find the optimal co-doping concentration when they were prepared by spray pyrolysis. It was found that doping Er3+ or Nd3+ enhances the PL intensity of BAM:Eu2+ blue phosphor particles. In particular, the M3+ doping effect on the PL intensity was pronounced when the prepared BAM:Eu2+, M3+ particles were excited by 172 nm VUV. The maximum intensity was obtained when the M3+ content was 1.0 at% with respect to Ba element. The PL intensity of BAM:Eu2+, M+ (M=Er3+, Nd3+) particles was also further improved by producing them in a spherical shape, which was successfully achieved by controlling the spray solution. The optimized BAM:Eu2+, M+ particles had about 10% higher PL intensity than that of the commercial particles, which are made by a conventional solid-state reaction.  相似文献   

16.
The (GdxY1?x)2O3: Er3+, Yb3+ [x=0.0, 0.1, 0.5, 0.9, 1.0] phosphor samples with 0.5 mol% concentration of Er3+ and 3.0 mol% of Yb3+, have been prepared using combustion route. The effect of variation of composition on the morphology, crystallinity and photoluminescence characteristics of the material has been investigated. The samples were post-heated at a temperature 1200 °C, for 5 h. We find systematic color tunability from red to green with an increase of Gd2O3 content in Y2O3 lattice. Further, the post-heated samples show an enhancement of fluorescence intensity for more than fifteen times. The samples were characterized by X-ray diffraction (XRD), scanning electron microscope (SEM), photoluminescence measurement and Fourier transform infrared (FTIR) techniques in order to find out the structural changes in host lattice. An increase in crystallite size has been marked with increasing Gd content while FTIR analysis explains the reason of variation in the fluorescence of rare earth ions in different host matrices.  相似文献   

17.
Er3+ doped niobic-tungsten–tellurite glasses doped with concentration of Er3+ ion up to 3 wt% were fabricated. The effect of Er3+ doping concentration on thermal stability and optical properties was investigated in order to obtain the most suitable rare earth content for developing 1.5 μm compact fiber amplifier pumped with a commercial telecom 980 nm laser diode. The maximum doping concentration allowed was found to be around 1.77×1020 ions/cm3, for which a broad 1.5 μm emission spectra of 65 nm FWHM and a lifetime of 3.4 ms for the 4I13/2 level was measured.  相似文献   

18.
In this paper, optical glass nanocomposites (nanoparticles sizes up to 100 nm) with composition TeO2–WO3–PbO–xEr2O3–yPr6O11 (x = 0.30 mol%, y = 0.70 mol%) embedded into polymer matrices was reported. The two types of polymers chosen for present study were: photopolymer oligoetheracryalte (OEA) and polymethylmethacrylate (PMMA), respectively. The incorporation of the titled nanoparticles into the polymer matrices is analyzed optically. The fluorescence spectra of the nanocomposites were compared with the fluorescence spectra of bulk glasses. Based on the comparison of Er3 + and Pr3 + ions' energy level schemes, possible energy transfer processes were identified. The prepared glasses are promising candidates for the white light emitting diodes applications.  相似文献   

19.
SrY2−x(MoO4)4:Er3+/Yb3 phosphors with doping concentrations of Er3+ and Yb3+ (x = Er3+ + Yb3+, Er3+ = 0.05, 0.1, 0.2 and Yb3+ = 0.2, 0.45) have been successfully synthesized by a cyclic microwave-modified sol–gel method, and the upconversion photoluminescence properties have been investigated. Well-crystallized particles showed a fine and homogeneous morphology with particle sizes of 1–3 μm. Under excitation at 980 nm, SrY2(MoO4)4:Er3+/Yb3+ particles exhibited a strong 525-nm, weak 550-nm emission bands in the green region, and a very weak 655-nm emission band in the red region. The possible mechanism of the green and red emissions was discussed in detail under consideration of a two-photon process. The Raman spectra of the particles indicated the presence of strong peaks at both higher and lower frequencies.  相似文献   

20.
Transparent phosphate glass ceramics co-doped with Er3+ and Yb3+ in the system P2O5Li2OCaF2TiO2 were successfully synthesized by melt-quenching and subsequent heating. Formation of the nanocrystals was confirmed by X-ray powder diffraction. Judd–Ofelt analyses of Er3+ ions in the precursor glasses and glass ceramics were performed to evaluate the intensity parameters Ω2,4,6. Under 975 nm excitation, intense upconversion (UC) and infrared emission (1545 nm) were observed in the glass ceramics by efficient energy transfer from Yb3+ to Er3+. The luminescence processes were explained and the emission cross section was calculated by Fuchtbauer–Ladenburg (F–L) formula. The results confirm the potential applications of Er3+/Yb3+ co-doped glass ceramics as laser and fiber amplifier media.  相似文献   

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