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1.
Single crystals of dysprosium-doped gadolinium orthovanadate (Dy:GdVO4) were successfully grown by the floating zone method and their fluorescence properties were investigated. The as-grown crystals did not contain any macroscopic defects such as cracks and inclusions for any Dy-concentration of up to 4 at%. Every crystal showed optical homogeneity under observation with a polarizing microscope; that is, no low-angle grain boundaries and growth striations were detected. In the visible region, two distinct fluorescence bands were observed around 480 and 575 nm, corresponding to 4F9/26H15/2 and 4F9/26H13/2 transitions, respectively. The excitation spectrum for the emission of 573 nm indicates the possibility to use a commercially available laser diode of 450 nm as a pumping source for solid-state yellow laser.  相似文献   

2.
Dysprosium (Dy) doped La3Ga5.5Nb0.5O14 single crystals were grown by the traditional Czochralski method along z‐axis. The structure of the crystal has been studied by X‐ray powder diffraction method, and the unit‐cell parameters are calculated to be a=8.22070 Å, c=5.12533 Å and V=299.965 Å3. The segregation coefficient of Dy3+ in La3Ga5.5Nb0.5O14 crystal was measured by X‐ray fluorescence analysis. For 1 mol% doping level in the melt, the distribution coefficient of Dy3+ was determined to be 0.341 wt%. Specific heat, thermal expansion and transmission spectrum of Dy: La3Ga5.5Nb0.5O14 single crystals have been measured. The fluorescence spectra of Dy3+: La3Ga5.5Nb0.5O14 crystals were measured at room temperature, and there were four emission transitions occurring at 479, 576, 662 and 754 nm, respectively. The fluorescent lifetimes measurement results show 1.0% Dy: La3Ga5.5Nb0.5O14 possesses shorter fluorescence decay time (303.4 μs) than does 1.0%Dy:LGS (436.12 μs). (© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

3.
This paper reports crystal growth and optical characteristics of dysprosium (Dy3+) and erbium (Er3+) doped mid‐infrared laser crystal ternary‐potassium‐lead‐chloride (KPb2Cl5). Two transparent crystals with good optical quality have been grown successfully by using the Bridgman technique,the largest crystal size reaches up to ∅︁10×60mm2. Measurements of X‐ray diffraction(XRD) and absorption spectra were carried out. Based on Judd‐Ofelt theory, the intensity parameters Ωt(t=2,4,6), the experimental and theoretical oscillator strengths have been obtained.The intensity parameters Ωt(t=2,4,6) of Er3+:KPb2Cl5 were calculated to be Ω2=5.10×10‐20 cm2, Ω4=1.25×10‐20 cm2, Ω6=0.83×10‐20 cm2, and the values for Dy3+:KPb2Cl5 were calculated to be Ω2=6.26×10‐20 cm2, Ω4=2.45×10‐20 cm2, Ω6=0.04×10‐20 cm2 respectively. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

4.
A Tm,Ho:CaYAlO4 single crystal was grown using the Czochralski (CZ) method. The absorption spectra, the fluorescence spectrum around 2 μm, the upconversion spectrum and energy‐transfer (ET) schemes between Tm3+ ions and Ho3+ ions have been studied. The crystal boule was free from cracks, inclusions and scattering centers. The broad FWHM of the 797‐nm absorption band (with E//c polarization is 19 nm and with E//a polarization is 18 nm), the large emission bandwidth (about 600 nm) and the intense ET from Tm3+ ions to Ho3+ ions make Tm,Ho:CaYAlO4 a promising media for tunable and ultrashort pulses.  相似文献   

5.
The spin‐Hamiltonian parameters (g factors g, g and hyperfine structure constants 161A, 161A, 163A, 163A) for 161Dy3+ and 161Dy3+ isotopes in the trigonal 12‐fold coordinated La3+ site of La2Mg3(NO3)12·24H2O crystal are calculated from a diagonalization (of energy matrix) method. In the method, the Zeeman and hyperfine interaction terms are added to the conventional Hamiltonian used in the studies of crystal‐field energy levels, and a 66×66 energy matrix concerning the ground multiplet 6H15/2 and the first to fifth excited multiplets 6H13/2, 6H11/2, 6H9/2, 6H7/2 and 6H5/2 are applied. The calculated results are discussed. (© 2010 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

6.
In this work, Ce:YAG crystal with the size of ?4 in was successfully grown by the TGT method. The optical and scintillation properties of as-grown Ce:YAG crystals were investigated. Three obvious absorption bands at 223, 340 and 460 nm and two weak color-center absorption bands at 296 and 370 nm are observed in as-grown Ce:YAG crystal. Fluorescence with an emission peak at 398 nm is observed due to the color centers, and absorption bands of the color centers can be eliminated by annealing in O2 or H2 atmosphere at 1673 K for 24 h. Yellow-green fluorescence centered at 530 nm is found when the crystal was excited at 460 nm and the 530 nm excitation spectrum shows two peaks at 340 and 460 nm. X-ray fluorescence spectrum of as-grown crystal shows three emission peaks at 300, 360 and 530 nm. An average light output of 1360 phe/MeV and a single exponential decay with the decay time constant of 62.97 ns are found in as-grown Ce:YAG crystal.  相似文献   

7.
The photoluminescence properties of different concentrations of Sm3+ ions doped sodium fluoroborate (SFB) glasses of composition Na2O–LaF3–CaF2–AlF3–B2O3–SmF3 have been investigated. The energy level analysis is carried out using free-ion Hamiltonian model. The Judd–Ofelt intensity parameters are used to evaluate the laser characteristic parameters such as spontaneous transition probability, radiative lifetime and fluorescence branching ratio for 4G5/2  6HJ (J = 5/2, 7/2, 9/2 and 11/2) emission transitions of Sm3+ ion. The principal photoluminescence transitions of interest are identified by recording the emission spectra for different Sm3+ ion concentrations and measuring their emission cross-sections, integrated absorption cross-sections and optical gain parameters. The decay profiles from the 4G7/2 excited manifold state to its lower lying energy levels have been recorded by monitoring the excitation and emission wavelengths at 402 and 600 nm, respectively. The dependence of effective fluorescence lifetime on the Sm3+ concentration is also discussed.  相似文献   

8.
The BaY2F8 crystals doped with different concentrations of Tm3+ ions were prepared by the temperature gradient technique (TGT). X‐ray powder diffraction was applied to analyze the phase. The cracking phenomenon along (010) and (100) planes of the crystals grown by temperature gradient technique was studied on the basis of the structure of BaY2F8 crystals. The absorption spectra were measured and investigated in the ultraviolet‐visible and near‐infrared ranges at room temperature. Several characteristic absorption bands of Tm3+‐doped BaY2F8 crystal were observed. The emission and excitation spectra were obtained and investigated at room temperature and 12 K, showing the characteristic emission peaks of Tm3+ ions. The temperature dependence of Photoluminescence curve was also investigated in the range of 12–296 K. The luminescence intensity of emission bands decreased with increasing temperature, while the effective bandwidth increased. The up‐conversion spectrum excited at 650 nm was recorded and up‐conversion mechanism was analyzed in detail. The result showed the purple, green and yellow emissions corresponding to 3P13F3, 1D23H5 and 3P01G4 transitions, respectively.  相似文献   

9.
Recharging processes of chromium ions were investigated for Mg2SiO4:Mg, Cr single crystals using annealing in O2 and in air and γ‐irradiation, as compare to YAG :Ca, Cr single crystals. The formation of tetravalent Cr ions in the Mg2SiO4 :Mg, Cr is related not only to the initial Cr content in the melt, oxygen partial pressure and O2‐ vacancy existing in the crystal, but also to the external field such as γ‐irradiation. The additional absorption after γ‐irradiation shows the decrease in intensity of the absorption of Cr3+ and Cr4+ ions in some part of the spectrum and increase in the other giving evidence on recharging effects between Cr3+ and Cr4+. There arises also color centers observed between 380 nm and 570 nm that may participate in energy transfer of any excitation to Cr4+ giving rise to Cr4+ emission. Opposite to forsterite crystal, absorption spectrum of YAG:Ca, Cr crystal after γ‐irradiation reveals only increase in the absorption of the Cr bands. The observed behavior of the absorption spectrum of YAG:Ca, Cr crystal under influence of γ‐irradiation suggests that γ‐irradiation ionizes only Cr ions. (© 2005 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

10.
Sm‐doped CaNb2O6 (CaNb2O6:Sm) phosphor thin films were prepared by radio‐frequency magnetron sputtering on sapphire substrates. The thin films were grown at several growth temperatures and subsequently annealed at 800 °C in air. The crystallinity, surface morphology, optical transmittance, and photoluminescence of the thin films were investigated by X‐ray diffraction, scanning electron microscopy, ultraviolet‐visible spectrophotometry, and fluorescence spectrophotometry, respectively. All of the thin films showed a main red emission radiated by the transition from the 4G5/2 excited state to the 6H9/2 ground state of the Sm3+ ions and several weak bands under ultraviolet excitation with a 279 nm wavelength. The optimum growth temperature for depositing the high‐quality CaNb2O6:Sm thin films, which was determined from the luminescence intensity, was found to be 400 °C, where the thin film exhibited an orthorhombic structure with a thickness of 370 nm, an average grain size of 220 nm, a band gap energy of 3.99 eV, and an average optical transmittance of 85.9%. These results indicate that the growth temperature plays an important role in controlling the emission intensity and optical band gap energy of CaNb2O6:Sm thin films.  相似文献   

11.
Photoluminescence properties of Sm3+, Dy3+, and Tm3+-doped transparent oxyfluoride silicate glass ceramics containing CaF2 nanocrystals were reported. Emission bands of 4G5/2  6H5/2 (562 nm), 4G5/2  6H7/2 (598 nm), 4G5/2  6H9/2 (645 nm) and 4G5/2  6H11/2 (706 nm) for the Sm3+: glass and glass ceramic, with an excitation at 6H5/2  4F7/2 (402 nm) have been recorded. Of them, 4G5/2  6H7/2 (598 nm) has shown a bright orange emission. With regard to the Dy3+: glass, a bright fluorescent yellow emission at 575 nm (4F9/2  6H13/2) and blue emission at 481 nm (4F9/2  6H15/2) have been observed, apart from 662 nm (4F9/2  6H11/2) emission transition with an excitation at 386 nm (6H15/2  4I13/2 + 4F7/2) wavelength. Emission bands of 1G4  3F4 (650 nm) and 1G4  3H5 (795 nm) transitions for the Tm3+: glass and glass ceramic, with an excitation at 3H6  1G4 (467 nm) have been observed. Of them, 1G4  3F4 (650 nm) has shown bright red emission. Decay lifetime measurements were also carried out for all the observed Sm3+, Dy3+, and Tm3+-doped glass and glass ceramic emission bands.  相似文献   

12.
Nd‐doped gadolinium aluminium tetraborate, NdxGd1‐xAl3(BO3)4 (NGAB), crystallizes with x = 0.1 in the trigonal system with point group 32, conforming space group R32. They were grown using flux method, of large sizes and good optical quality. The unit cell constants were a = 0.93057 (6) and c = 0.72481 (3) nm, and z = 1. The measured absorption of the NGAB is compared to Judd‐Ofelt (JO) theory. When applied, the JO theory of parity‐forbidden electric‐dipole transitions of rare earth ions on noncentrosymmetric sites demonstrates good agreement. A measured band gap of the eigentransition was about 4.00 eV. The fitted intensity parameters Ot (t = 2, 4, and 6) were 2.446 × 10‐20, 2.266 × 10‐20 and 2.598 × 10‐20 cm2. Both the emission properties of the sub‐stable 4F3/2 state with the level lifetime of 506.20 μs and a fluorescence spectrum corresponding to the transition 4F3/24I11/2 were studied. The results indicate the pass band of laser for potential applications in practice.  相似文献   

13.
Perfect single crystals of cadmium oxalate trihydrate have been grown using the slow and controlled reaction between Cd+2 and (C2O4)‐2 ions in agar‐agar gel, resulting in the formation of insoluble product Cd(COO)2.3H2O. The optimum growth parameters have been determined. The variation of magnetic moment of the grown crystals under an applied static magnetic field is studied and the material is found to be diamagnetic. The polarizability is found sensitive to optical band gap. An empirical relation between magnetic susceptibility and electronic polarizability has been established. Optical absorption spectra of the sample recorded in the range 200‐2500 nm reveal transitions involving absorption and emission of phonons. The detailed study supports the existence of allowed direct and indirect allowed gaps in the material. The direct allowed transition prevails in the region of relatively higher photon energy. Some feeble disorder in the crystal is conceived to be present. (© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

14.
A neodymium doped Ca5(BO3)3F single crystal with size up to 51×48×8 mm3 has been grown by the top seeded solution growth (TSSG) technique with a Li2O‐B2O3‐LiF flux. The spectra of absorption and fluorescence were measured at room temperature. According to Judd‐Ofelt (J‐O) theory, the spectroscopic parameters were calculated and the J‐O parameters Ω2, Ω4, Ω6 were obtained as follows: Ω2 = 1.41×10−20cm2, Ω4 = 3.18×10−20cm2, Ω6 = 2.11×10−20cm2. The room temperature fluorescence lifetime of NCBF was measured to be 51.8 μs. According to the J‐O paramenters, the emission probabilities of transitions, branching ratios, the radiative lifetime and the quantum efficiency from the Nd3+ 4F3/2 metastable state to lower lying J manifolds were also obtained. In comparasion with other Nd‐doped borate crystals, the calculated and experimental parameters show that NCBF is a promising SFD crystal.  相似文献   

15.
The optical properties of Tm:ZBLAN glass have been simulated. The simulated optical spectra agreed substantially with the observed spectra. The population of the energy levels of the Tm3+ ion under dual-wavelength excitation for upconversion emission and amplification was evaluated by solving the rate equation with the simulated transition probabilities and spectral shapes of the transitions of which the initial levels were from the 3H6 to 3P2 levels. The large population of the 1G4 level, which is the upper level for 480 nm laser oscillation, was estimated for the conditions of laser oscillation at room temperature. We also proposed new combinations of the excitation wavelengths for the amplification of the 1470 nm signal.  相似文献   

16.
The effect of lead oxide (PbO) on optical properties of Dy3+-doped PbO–H3BO3–TiO2–AlF3 (LBTAFDy) glasses is investigated. The LBTAFDy glasses were prepared with different PbO contents ranging from 30 to 60 mol%. The Judd–Ofelt intensity parameters (Ωλ = 2, 4, 6) are obtained by the least square fit analysis. It is found that the Ω2 parameter and yellow-to-blue intensity ratio (Y/B) of the Dy3+ emission depend on the PbO content in LBTAFDy glass. The structural asymmetry around the Dy3+ ion and the DyO covalency are responsible for the changes in Ω2 parameter and Y/B ratio. The variation of decay time of 4F9/2 emission level with the PbO content also supports the changes in structural asymmetry and DyO covalency in LBTAFDy glass.  相似文献   

17.
L‐Valinium picrate (C5H12NO2)+. (C6H2N3O7), a non‐linear optical material from the amino acid family which has large second harmonic generation (SHG) efficiency, was grown by slow evaporation method. Characterization of the crystals was made using single crystal X‐ray diffraction. The functional groups and the modes of vibrations were found by using the Fourier transform infrared (FTIR) spectroscopy. The second harmonic generation (SHG) conversion efficiency was investigated using the Kurtz and Perry method. The SHG conversion efficiency is 60 times higher than that of the standard KDP and 8 times higher than that of the standard Urea and the optical transparency was analyzed using UV‐visible‐NIR absorption spectrum. The structural features of the material leading to the large SHG efficiency are discussed. Microhardness and dielectric studies were also carried out. (© 2008 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

18.
The mixed rare earth oxide (Dy1‐xErx)2O3 (0.0 ≤ x ≤ 1.0) were synthesized by a sol–gel process. X‐ray and neutron diffraction data were collected and crystal structure and microstructure analyses were performed using Rietveld refinement method. All samples were found to have the same crystal structure and formed solid solutions over the whole range of x. Preferential cationic distribution is found for all samples but with different extent with Dy3+ preferring the 8b among the two non‐equivalent sites 8b and 24d of the space group Ia3. The lattice parameter is found to vary linearly with the composition x and a systematic variation is found in the r.m.s microstrain . Magnetization measurements were done in the temperature range 5‐300 K and a behavior in accordance with Curie‐Weiss law was found. Anomalous concentration dependence is found in magnetic susceptibility which is ascribed to the concentration dependence of effective crystal field combined with the contribution of 4I15/2 and 6H15/2 manifold at elevated temperature. The effective magnetic moments μeff is found to decrease linearly with composition parameter x, except for sample x=0.5 where the magnetization is enhanced. The Curie‐Weiss paramagnetic temperatures indicated antiferromagnetic interaction. These magnetic results are discussed in view of the cationic distribution. (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

19.
A novel terbium coordination polymer {[Tb(TCB)1/2(H2TCB)1/2(H2O)](H2O)2}n (H2TCB = 1, 2, 4, 5‐benzenetetracarboxylic acid) ( 1 ) has been hydrothermally synthesized and determined by single crystal X‐ray diffraction method, which features a very interesting three‐dimensional framework with large packing cavities. It crystallizes in the monoclinic space group P21/n with a = 1.0723(4) nm, b = 0.7168(3) nm, c = 1.7155(6) nm, β = 97.079(4)°, V = 1.3086(8) nm3, Z = 4, and final R1 = 0.0203, wR2 = 0.0404. In 1, the protonated carboxylate groups are free, the other carboxylate groups are bonded to Tb3+ ion in three modes: the chelating bidentate, the bridging bidentate and bridging tridentate. Moreover each Tb3+ ion is coordinated by nine oxygen atoms from six carboxylate groups and one water molecule respectively to complete a deformed tricapped trigonal prismatic geometry. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

20.
Nonlinear optical (NLO) crystal of thiourea mixed cadmium–lead chloride dihydrate Cd[(PbCl3)(NH2CSNH2)].2H2O (TCCPC) have been grown in solution by slow evaporation technique at room temperature. The powder X‐ray diffraction pattern has been recorded and indexed. The UV‐Vis‐NIR transmittance and FT‐IR spectrum have been recorded in the range 200‐1090 nm and 400‐4000 cm‐1, respectively. The lower cut‐off wavelength is 280 nm in the UV region, which is higher than that of pure Cd(PbCl3) (CCPC) crystal. The presence of functional groups has been confirmed by FT‐IR analysis. The TCCPC crystal was characterized by SEM and EDX spectrum. The second harmonic generation (SHG) of the thiourea mixed cadmium–lead chloride (TCCPC) crystal is demonstrated by the Kurtz Perry method using Nd:YAG laser and the results confirm that the grown crystal is roughly three times more efficient than ADP. (© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

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