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1.
We characterized ZnGa2O4:Mn2+ (ZnGa2O4—zinc gallate) nanophosphor synthesized by the solvothermal method in 1,4-butanediol-containing water to increase the amount of Mn2+ ions incorporated in the ZnGa2O4 matrix without post-heat treatment. We investigated the influence of water content in the solvent on the photoluminescence (PL) intensity and the Mn amount, the latter being measured by X-ray fluorescence analysis and electron paramagnetic resonance spectroscopy. The PL intensity per Mn amount reached the maximum at the 50 wt% water content. The addition of water promotes repeated dissolution and precipitation, resulting in homogeneous Mn2+ distribution in the ZnGa2O4 matrix. This suggests that the solvothermal method in the 1,4-butanediol-water system is useful for increasing the amount of Mn2+ ions incorporated in the ZnGa2O4 matrix without post-heat treatment. At the water content >50 wt%, the decrease in PL intensity is attributed to the optical absorption of the by-product, MnOOH.  相似文献   

2.
The water-soluble Mn2+-doped ZnS quantum dots (Mn:ZnS d-dots) were synthesized by using thioglycolic acid (TGA) as stabilizer in aqueous solutions in air, and characterized by X-ray powder diffraction (XRD), UV-vis absorption spectra and photoluminescence (PL) emission spectroscopy. The sizes of Mn:ZnS d-dots were determined to be about 2 nm using XRD measurements and the UV-vis absorption spectra. It was found that the Mn2+4T1 → 6A1 emission intensity of Mn:ZnS d-dots significantly increased with the increase of Mn2+ concentration, and showed a maximum when Mn2+ doping content was 1.5%. If Mn2+ concentration continued to increase, namely more than 1.5%, the Mn2+4T1 → 6A1 emission intensity would decrease. In addition, the effects of TGA/(Zn + Mn) molar ratio on PL were investigated. It was found that the peak intensity ratio of Mn2+4T1 → 6A1 emission to defect-states emission showed a maximum when the TGA/(Zn + Mn) molar ratio was equal to 1.8.  相似文献   

3.
In this work we synthesized ZnS:Mn2+ nanoparticles by chemical method using PVP (polyvinylpyrrolidone) as a capping agent in aqueous solution. The structure and optical properties of the resultant product were characterized using UV-vis optical spectroscopy, X-ray diffraction (XRD), photoluminescence (PL) and z-scan techniques. UV-vis spectra for all samples showed an excitonic peak at around 292 nm, indicating that concentration of Mn2+ ions does not alter the band gap of nanoparticles. XRD patterns showed that the ZnS:Mn2+ nanoparticles have zinc blende structure with the average crystalline sizes of about 2 nm. The room temperature photoluminescence (PL) spectrum of ZnS:Mn2+ exhibited an orange-red emission at 594 nm due to the 4T1-6A1 transition in Mn2+. The PL intensity increased with increase in the Mn2+ ion concentration. The second-order nonlinear optical properties of nanoparticles were studied using a continuous-wave (CW) He-Ne laser by z-scan technique. The nonlinear refractive indices of nanoparticles were in the order of 10−8 cm2/W with negative sign and the nonlinear absorption indices of these nanoparticles were obtained to be about 10−3 cm/W with positive sign.  相似文献   

4.
ZnS nanoparticles with Mn2+ doping (0.5-20%) have been prepared through a simple chemical method, namely the chemical precipitation method. The structure of the nanoparticles has been analyzed using X-ray diffraction (XRD), scanning electron microscope (SEM), transmission electron microscope (TEM) and UV-vis spectrometer. The size of the particles is found to be 3-5 nm range. Photoluminescence spectra were recorded for undoped ZnS nanoparticles using an excitation wavelength of 320 nm, exhibiting an emission peak centered at around 445 nm. However, from the Mn2+-doped samples, a yellow-orange emission from the Mn2+4T1-6A1 transition is observed along with the blue emission. The prepared Mn2+-doped sample shows efficient emission of yellow-orange light with the peak emission 580 nm with the blue emission suppressed. The maximum PL intensity is observed only at the excitation energy of 3.88 eV (320 nm). Increase in stabilizing time up to 48 h in de-ionized water yields the enhancement of emission intensity of doped (4% Mn2+) ZnS. The correlation made through the concentration of Mn2+ versus PL intensity resulted in opposite trend (mirror image) of blue and yellow emissions.  相似文献   

5.
We have studied photoluminescence (PL) spectrum and dynamics of Cu- and Al-doped ZnS (ZnS:Cu,Al) nanocrystals fabricated by sequential implantation of Zn+, S+, Cu+, and Al+ ions into Al2O3 matrices. These samples exhibit intense green PL under UV light excitation. The space- and time-resolved PL measurements show that the broad green PL is due to the donor–acceptor (DA) pair luminescence of single ZnS:Cu,Al nanocrystals.  相似文献   

6.
《Journal of luminescence》1986,36(2):101-107
Four kinds of Er3+ centers in ZnS:Er3+ thin films have been distinguished by means of laser selective excitation. Their impact cross sections in electroluminescence (EL) and absorption cross sections in photoluminescence (PL) have been compared with each other. The average value of the impact cross section of Er3+ obtained by comparing the EL intensity of Er3+ with that of Mn2+ in ZnS:ErF3, Mn2+ thin films is about 2×10−16 cm2.  相似文献   

7.
《Composite Interfaces》2013,20(7):425-432
Abstract

ZnS nanoparticles and Mn2+-doped ZnS nanoparticles were prepared by a reverse micelle reaction system. In addition, ZnS and Mn2+-doped ZnS nanoparticles were modified with poly(vinyl alcohol) (PVA) and 1-dodecanethiol (C12H25SH). The average particle size of the ZnS sample is determined around 2.3 nm by using the well-known Scherrer equation, which is in accordance with the results obtained from UV–vis and TEM analysis. Fluorescence intensity of the Mn2+-doped ZnS nanoparticles increases with increasing Mn2+ content compared with undoped ZnS nanoparticles, and coating PVA can also make fluorescence intensity increase. Different Zn2+/S2- or C12H25SH/Zn2+ can affect intensity of PL emission peak and its position, which is discussed in this paper.  相似文献   

8.
ZnS nanoparticles with Mn2+ doping (1–2.5%) have been prepared through a simple soft chemical route, namely the chemical precipitation method. The nanostructures of the prepared undoped ZnS and Mn2+-doped ZnS:Mn nanoparticles have been analyzed using X-ray diffraction (XRD), Scanning electron microscope (SEM), transmission electron microscope (TEM) and UV–vis spectrophotometer. The size of the particles is found to be in 2–3 nm range. Room-temperature photoluminescence (PL) spectrum of the undoped sample only exhibits a blue-light emission peaked at ∼365 nm under UV excitation. However, from the Mn2+-doped samples, a yellow-orange emission from the Mn2+ 4T16A1 transition is observed along with the blue emission. The prepared 2.5% Mn2+-doped sample shows efficient emission of yellow-orange light with the peak emission at ∼580 nm with the blue emission suppressed.  相似文献   

9.
Zn1−XMnXS (X=0.85% and 1.26%) nanoparticles have been synthesized using a specially designed equipment and we have studied the influence of doping Mn2+ on the surface energy of ZnS. The high pressure behaviors of ZnS nanocrystals with different dopant contents have been investigated using angle-dispersive synchrotron X-ray powder diffraction up to 45.1 GPa. Theoretical calculations show that doping with Mn2+ increases the surface energy of the nanocrystals. The theoretical result has been further corroborated by our experimental observation of an increase in the phase transition pressure of Mn2+ doped ZnS nanocrystals in diamond-anvil-cell studies.  相似文献   

10.
CdS:Mn2+/ZnS and CdS:Mn2+/CdS core–shell nanoparticles were synthesized in aqueous medium via chemical precipitation method in an ambient atmosphere. Polyvinylpyrrolidone (PVP) was used as a capping agent. The effect of the shell (ZnS and CdS) thickness on CdS:Mn2+ nanoparticles was investigated. Inorganically passivated core/shell nanocrystals having a core (CdS:Mn2+) diameter of 4 nm and a ZnS-shell thickness of ∼0.5 nm exhibited improved PL intensity. Optimum concentration of doping ions (Mn2+) was selected through optical study. For all the core–shell samples two emission peaks were observed, the first one is band edge emission in the lower wavelength side due to energy transfer to the Mn2+ ions in the crystal lattice; the second emission is characteristic peak of Mn2+ ions (4T1 → 6A1). The XRD, TEM and PL results showed that the synthesized core–shell particles were of high quality and monodisperse.  相似文献   

11.
L.Y. Zhu 《Optics Communications》2008,281(9):2548-2551
Ni2+-doped ZrO2 precursor fibers were prepared via sol-gel technique by dry-spinning method and then heat-treated at different temperatures. The surface of the fibers is smooth with uniform diameter and no cracks have been observed by scanning electron microscopy (SEM). The emission intensity reaches a maximum value at 1 mol% Ni2+ because of the concentration quenching. The photoluminescence (PL) relative intensity is apparently intensifying with increasing temperature before 700 °C due to the crystallinity of the ZrO2 lattice improvement. The PL results show that the typical emission center is at 510 nm excited at 315 nm.  相似文献   

12.
A series of Li+ and Eu3+ co-doped double tungstate NaLa(WO4)2 (NLW) red phosphors have been successfully synthesized by an ion exchange method under a hydrothermal condition. The effects of Li+ doping concentration on the crystal structure, morphology and photoluminescence properties were investigated using the XRD, TEM and photoluminescence (PL) measurements. The results reveal that the samples have phase-pure scheelite structure and adopt spherical particle morphology. Furthermore, room temperature PL spectrum shows that the optical brightness is highly dependent on the concentration of doping Li+, which is determined by ion exchange duration and the precursor concentration of LiNO3. As 5% Li+ ions was introduced into the crystal lattice, the emission intensity was enhanced by more than 10-fold as compared with the pristine one. Moreover, the co-doping of Li+ can substantially improve the effective excitation of the NaLa(WO4)2:Eu3+ phosphors under near-UV region.  相似文献   

13.
ZnO:Eu3+, Li+ films prepared by the dip-coating method were characterized by photoluminescence (PL) and electroluminescence (EL). When the ZnO:Eu3+, Li+ films were excited using UV light with energy corresponding to the band-to-band excitation of the host matrix, the PL spectra showed emissions from both ZnO and Eu3+ ions, while their EL spectra showed emissions only from Eu3+ ions, and no emission from ZnO could be detected. It is found that the EL emission intensity B is dependent on the applied voltage, B=Bo exp(−bV−1/2). With increasing frequency, the EL intensity dramatically increases at lower frequencies (<1000 Hz), and then increases gradually at higher frequencies (>1000 Hz).  相似文献   

14.
Undoped and Cu2+ doped (0.2-0.8%) ZnS nanoparticles have been synthesized through chemical precipitation method. Tri-n-octylphosphine oxide (TOPO) and sodium hexametaphosphate (SHMP) were used as capping agents. The synthesized nanoparticles have been analyzed using X-ray diffraction (XRD), transmission electron microscope (TEM), Fourier transform infrared spectrometer (FT-IR), UV-vis spectrometer, photoluminescence (PL) and thermo gravimetric-differential scanning calorimetry (TG-DTA) analysis. The size of the particles is found to be 4-6 nm range. Photoluminescence spectra were recorded for ZnS:Cu2+ under the excitation wavelength of 320 nm. The prepared Cu2+-doped sample shows efficient PL emission in 470-525 nm region. The capped ZnS:Cu emission intensity is enhanced than the uncapped particles. The doping ions were identified by electron spin resonance (ESR) spectrometer. The phase changes were observed in different temperatures.  相似文献   

15.
The effect of K+ ions on GdTaO4:Eu3+ thin-film phosphors was investigated in order to improve their luminescent properties. The GdTaO4:Eu0.1, Kx thin films were synthesized by sol-gel process, and characterized through measuring their microstructure and luminescence. The results indicated that photoluminescence (PL) intensity of GdTaO4:Eu3+ film was improved remarkably by K doping. There were two maxima in the curve of PL intensity against K+ dopant concentration, where one was improved up to 2.1 times at x = 0.001 and the other was enhanced up to 2.7 times at x = 0.05. The first maximum was regarded as the alteration of the local environment surrounding the Eu3+ activator by incorporation of K+ ions, and the second maximum was due to the flux effect. Additionally, the luminescence increased with the increase of firing temperature from 800 °C to 1200 °C.  相似文献   

16.
ZnS and SiO2-ZnS nanophosphors, with or without different concentration of Mn2+ activator ions, were synthesized by using a sol-gel method. Dried gels were annealed at 600 °C for 2 h. Structure, morphology and particle sizes of the samples were determined by using X-ray diffraction (XRD), highresolution transmission electron microscopy (HRTEM) and field emission scanning electron microscopy (FESEM). The diffraction peaks associated with the zincblende and the wurtzite structures of ZnS were detected from as prepared ZnS powders and additional diffraction peaks associated with ZnO were detected from the annealed powders. The particle sizes of the ZnS powders were shown to increase from 3 to 50 nm when the powders were annealed at 600 °C. An UV-Vis spectrophotometer and a 325 nm He-Cd laser were used to investigate luminescent properties of the samples in air at room temperature. The bandgap of ZnS nanoparticles estimated from the UV-Vis data was 4.1 eV. Enhanced orange photoluminescence (PL) associated with 4T16A1 transitions of Mn2+ was observed from as prepared ZnS:Mn2+and SiO2-ZnS:Mn2+ powders at 600 nm when the concentration of Mn2+ was varied from 2-20 mol%. This emission was suppressed when the powders were annealed at 600 °C resulting in two emission peaks at 450 and 560 nm, which can be ascribed to defects emission in SiO2 and ZnO respectively. The mechanism of light emission from Mn2+, the effect of varying the concentration on the PL intensity, and the effect of annealing are discussed.  相似文献   

17.
《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   

18.
Y2O3:Yb3+ nanocrystals codoping with Li+ ions were synthesized by glycine combustion method. Codoping with Li+ ions leads to about 12 times enhancement of the photoluminescence (PL) intensity around 1 μm, in terms of the increased lifetimes at 1026 nm from 0.384 ms to 1.42 ms at room temperature. The enhancement in the PL intensity could be mostly attributed to the modification of the local symmetry around Yb3+ ions by codoping with Li+ ions.  相似文献   

19.
A method of UV spectroscopy was used to measure photoluminescence (PL) spectra and photoluminescence excitation (PLE) spectra in anion-defective alumina crystals exposed to high doses of gamma-radiation. An additional emission band in the range of 1.6–2.75 eV appears in the exposed crystals. Aggregate F2-type centers in different charge states are responsible for this band. It was found that growing intensity of PL aggregate centers occurs at doses corresponding to saturation of dose response and is accompanied by a sharp drop in the intensity of F+-band in the PL spectrum resulting from combination of F+-centers into aggregates. Uncharged F2-centers are formed when electrons are trapped by F2+ and F22+-centers. The main role of F+-centers in radiation-induced transformations of color centers under high-dose irradiation of anion-defective alumina crystals was indicated.  相似文献   

20.
Intense room-temperature photoluminescence (PL) from the UV to the green region was observed from Zr4+-doped silica synthesized by a sol-gel process using tetraethoxysilane as the precursor, followed by thermal treatment at 500 °C in air. The wide PL band can be resolved into three components centered at 3.70, 3.25, and 2.65 eV, respectively. The intensity of the 3.25 and 2.65 eV PL bands was greatly enhanced compared with pure sol-gel silica. The 3.70 eV emission was assigned to non-bridging oxygen hole centers, while the 2.65 eV one originated from neutral oxygen vacancies (VO). The 3.25 eV PL band was most likely associated with E′ centers, as supported by electron spin resonance measurement. It was proposed that the Zr4+-doping leads to oxygen deficiency in the silica, thus resulting in enhancement of the density of VO and E′ center defects.  相似文献   

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