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1.
A new blue-emitting phosphor LiCaPO4: Eu2+ was synthesized by solid state reaction at a relatively low temperature of 900 °C. It gives a single intense emission band centering at 470 nm, which corresponds to the 4f65d1→4f7 transition of Eu2+. The dependence of luminescence intensities on Eu2+ concentration was investigated. The phosphor, with a single excitation band extending from 250 to 400 nm, could be efficiently excited by near-ultraviolet light-emitting diodes and is believed to be a promising blue-emitting phosphor for white light-emitting diodes.  相似文献   

2.
Green-emitting phosphor Na2Ba2Si2O7:Eu2+ has been synthesized by a conventional high-temperature solid-state reaction. The phase structure and luminescence properties are characterized by the X-ray powder diffraction, diffuse reflectance spectra, photoluminescence excitation and emission spectra, temperature-dependent emission spectra, respectively. It can be efficiently excited in the wavelength range of 325–400 nm and consists of a strong broad green band centered at about 501 nm, which is ascribed to 4f66s05d1 → 4f76s25d0 transition of Eu2+. The critical quenching concentration of Eu2+ in the Na2Ba2Si2O7 host is about 0.8 mol % and corresponding quenching behavior is ascribed to be electric dipole–dipole interaction. Furthermore, the phosphor has good thermal stability property, and the activation energy for thermal quenching is calculated as 0.34 eV.  相似文献   

3.
The 4f65d1(e)→4f7 emission (normal) of Eu2+ in SrF2 and normal and anomalous emissions of Eu2+ in BaF2 are studied as a function of pressure and temperature. Although in BaF2 both emissions (anomalous and normal) shift with pressure in the same spectral direction (a red shift), the anomalous emission converts to the normal emission when the pressure increases to 33 kbar. Considering the dependence of BaF2:Eu2+ luminescence on the pressure and temperature we have found that spectral transformation takes place due to a smooth pressure-induced level crossing at approximately the same pressure as the phase transition.  相似文献   

4.
Eutectic crystal of 0.5% Eu-doped 30LaAlO3–70Al2O3 (vol %) was prepared by micro-pulling down (μ-PD) technique under nitrogen atmosphere. Being excited at a wavelength of 320 nm, the crystal exhibited intense emission band with a maximum at 450 nm which is corresponding to 4f65d-4f7(8S7/2) transitions of Eu2+. The decay time and fluorescence quantum efficiency (QE) were determined to be about 475 ns and 60%, respectively. When alpha-ray excited the crystal, both Eu2+ 4f65d-4f7(8S7/2) and Eu3+ 4f6-4f6 (5D0-7F1,2) emission peaks were observed at 435 nm and 600 nm. By the pulse height spectra, the relative scintillation light yield of the crystal was about 4% compared with that of BGO commercial scintillator.  相似文献   

5.
The blue-emitting phosphors of Eu2+-doped Na2CaMg(PO4)2 were prepared by high-temperature solid-state reaction. The crystal phase formation was confirmed by X-ray powder diffraction measurement. The luminescence properties were investigated by photoluminescence excitation and emission spectra. The phosphor exhibited the blue luminescence due to the 4f65d1→4f7 transition of Eu2+ ions under the excitation of near UV light. The influence of temperature on the luminescence intensities and decay lifetimes of Eu2+ was investigated. An unusual increase of the decay lifetimes of the 4f65d emission of Eu2+ ion is observed in Na2CaMg(PO4)2 from 10 K to room temperature. The thermal stability of the luminescence of Eu2+-doped Na2CaMg(PO4)2 was discussed.  相似文献   

6.
Green phosphor compositions MgxSr1−xAl2O4:Eu, Nd (with x=0.05-0.25) were prepared by solid state reaction method. The effect of Mg substitution on photoluminescence characteristics was investigated. The photoluminescence show intense green emission for MgSrAl2O4:Eu2+, Nd3+ with long persistence. This green emission corresponds to transitions from 4f65d1 to 4f7 of Eu2+ ion. Comparative analysis of the excitation and emission spectra were used to evaluate the crystal field splitting of the 5d states of Eu2+ and the parameters of electron-vibrational interaction, such as Huang-Rhys factor, effective phonon energy, and zero-phonon line position.  相似文献   

7.
The excitation and emission spectra of octahedrally coordinated europium ion (Eu2+) ions in Cs2M2+P2O7 (M2+=Ca, Sr) are reported and discussed. The remarkable features of the Eu2+ luminescence in these phosphate materials include (a) very large Stokes shift of emission (∼1 eV), (b) high luminescence quenching temperature, and (c) unusually low energy of the emitted photons for Eu2+ luminescence in phosphate-based materials. The broad emission bands of Eu2+ in Cs2CaP2O7 and Cs2SrP2O7 peak at 607 and 563 nm, respectively. The Stokes shift, crystal field splitting, centroid shift and the red shift of the Eu2+ 4f65d1 electronic configuration have been estimated from the relevant optical data. The radiative lifetime of the Eu2+ emission in Cs2M2+P2O7 is ∼1.2 μs. The nature of the Eu2+ emission in Cs2M2+P2O7 is discussed and arguments are presented to associate the luminescence with an extreme case of normal 4f65d1→4f7[8S7/2] emission.  相似文献   

8.
The optical properties of SrSi2AlO2N3 doped with Eu2+ and Yb2+ are investigated towards their applicability in LEDs. The Eu2+-doped material shows emission in the green, peaking around 500 nm. The emission is ascribed to the 4f65d1–4f7 transition on Eu2+. In view of the too low quantum efficiency and the considerable thermal quenching of the emission at the operation temperature of high power LED (>1W/mm2) this phosphor is only suitable for application in low power LEDs. The Yb2+ emission shows an anomalously red-shifted emission compared to Eu2+, which is characterized by a larger FWHM, a larger Stokes shift and lower thermal quenching temperature. The emission is ascribed to self-trapped exciton emission. The Yb2+ activated phosphor is found to be unsuitable for the use in any phosphor-converted LEDs.  相似文献   

9.
Eu2+-activated Sr2LiSiO4F phosphors were synthesized at 900°C by solid-state reaction in reducing atmosphere, and their photoluminescence (PL) properties were systematically investigated by diffuse reflection spectra, PL excitation and emission spectra, and by the fluorescence decay curve. Sr2LiSiO4F:Eu2+ emits intense green light at 520 nm originating from the 5d14f6−4f7 transition of Eu2+ under 365 nm n-UV excitation. The PL excitation spectrum matches the emission from n-UV chips. These materials could be promising green phosphors for use in generating white light in phosphor-converted white light-emitting-diodes (LEDs).  相似文献   

10.
The nonstationary behavior of Eu2+ and Sm2+ photoluminescence in continuously optically pumped CaF2:RE2+-CdF2superlattices was considered. The transient character of the photoluminescence is due to spontaneous electron tunneling from the excited 4f5d states into the conduction band of the adjacent CdF2 layer. Coupled balance equations were constructed and numerically analyzed. It is shown that photoionization energies of the 4f5d states can be derived from the experimentally measured variation of the photoluminescence intensity in superlattices with CaF2 and CdF2 layers 10 to 20 monolayers thick.  相似文献   

11.
The reflection and luminescence excitation spectra of CaF2 crystals containing europium ions in divalent (Eu2+) and trivalent (Eu3+) states were measured in the range from 4 to 16 eV. It was established that, in CaF2 : Eu3+ crystals, luminescence of Eu3+ ions (the f-f transitions) is effectively excited both in the charge-transfer band (at ~8 eV) and in the region of the 4f–5d transitions (at ~10 eV) but is virtually not excited in the fundamental region of the crystal (at an energy higher than 10.5 eV). Luminescence of Eu2+ ions (the 427-nm band) in CaF2 : Eu3+ is effectively excited in the fundamental region of the crystal; i.e., luminescence of divalent europium ions occurs through the trapping mechanism. Emission of Eu2+ ions in CaF2 : Eu2+ crystals is characterized by the excitation band at an energy of 5.6 eV (the 4f → 5d,t 2g transitions), as well as by the exciton and interband luminescence excitations. The results obtained and data available in the literature are used to construct the energy level diagram with the basic electron transitions in the CaF2 : Eu crystals.  相似文献   

12.
A mechanism of direct excited exchange between the nearest Eu2+ ions in Eu-chalcogenides caused by simultaneous electron 4f7 → 4f65d1 transitions on both ions is proposed. The wavefunctions are considered, the energy spectrum is found, and the form of effective spin-Hamiltonian is determined for the Eu2+ ? Eu2+ “molecule” in crystal field of D2h symmetry. The change of effective exchange integral between nearest Eu2+ ions in a series of Eu-chalcogenides is discussed briefly.  相似文献   

13.
Emission related to rare earth ions in solids takes place usually due to 4fn→4fn and 4fn−15d1→4fn internal transitions. In the case of band to band excitation the effective energy transfer from the host to optically active impurity is required. Among other processes one of the possibilities is capturing of the electron at the excited state and the hole at the ground state of impurity.The latest results on high pressure investigations of luminescence related to Pr3+ and Eu2+ in different lattices are briefly reviewed. The influence of pressure on anomalous luminescence and 4fn−15d1→4fn luminescence in BaSrF2:Eu2+ and LiBaF3:Eu2+ systems and Pr3+ 4fn→4fn emission quenching is presented and discussed. A theoretical model describing the impurity-trapped exciton as a system where a hole is localized at the impurity and an electron is captured by Coulomb potential at Rydberg-like states is developed. The results show the importance of local lattice relaxation for the creation of stable impurity-trapped exciton states. The ligands shifts create a potential barrier that controls the effect of mixing between the Rydberg-like electron and localized electron wave functions.  相似文献   

14.
In this work, we made five samples of SrAl2O4: Eu2+, Dy3+, the α phase and β phase SrAl2O4:Eu2+,Dy3+ powder and pellet samples, and α phase single crystal. We have measured the emission spectra of all the samples. All the emission peaks are around 520 nm, which correspond to the transition from 4f65d1(2Eg) to 4f7(8S7/2) of Eu2+ in SrAl2O4 host. The intensity of emission of the β phase is stronger than that of the α phase. We believe that it is because the Eu2+ ions have occupied the two types of sites in the α phase SrAl2O4 host and the lifetime of the transition of Eu2+ in the A site is longer than that in the B site. This result also proves that the β phase of the material is brighter than the α phase. In addition, the β phase can be achieved by quenching technique.  相似文献   

15.
Luminescence of yttrium-aluminum garnet Y3Al5O12: Eu,Si samples is studied. It is found that luminescence is associated with Eu2+ ions, but does not correspond to intracenter 4f 65d 1–4f 7 transitions. Measurements of the excited state lifetime point to the luminescence mechanism involving charge-transfer states.  相似文献   

16.
We have succeeded in developing a new elasticoluminescent (elastico-L) material SrMg2(PO4)2:Eu (SMPE), which emits purple light clearly observable with the naked eye. SMPE can be synthesized at a firing temperature, which is several hundred degrees Kelvin lower than that for other materials of this group. Based on a comparison between elastico-L emission spectrum and photoluminescence spectrum, the emission was identified to be due to electron transition from an excited state 4f65d1 to the ground state 4f7 in Eu2+ ions. While the emission gradually decayed as stress was applied repeatedly, it recovered completely upon irradiation with UV light (365 nm). This behavior, characteristic to elastico-L materials of the defect-controlled type, suggests that deep charge traps are involved in the emission process. In this paper, the elastico-L mechanism in SMPE is discussed in detail with reference to its thermoluminescence and electroluminescence spectra.  相似文献   

17.
Spectroscopic investigations are presented of KMgF3:Eu2+ crystal under high hydrostatic pressure from ambient to 310 kbar. The sample was excited by 30 ps pulses generated by optical parametric generator (OPG) system with wavelength controlled between 210 and 325 nm. The Grüneisen parameters of individual phonons are obtained from the pressure shift of the Eu2+ emission related to the 6P7/28S7/2 transition accompanied by phonon sideband. The luminescence decays exponentially for the pressure below 135 kbar with lifetime of 3.30 ms and slightly nonexponential above 135 kbar, while the average decay time is nearly independent of the pressure. The results obtained for KMgF3:Eu2+ are compared with those for LiBaF3:Eu2+ in which the 6P7/28S7/2 emission is replaced by the broadband emission of the 4f65d1→4f7 transition at high hydrostatic pressure.  相似文献   

18.
Transparent Eu2+/Mn2+ co-doped new glass ceramics (GC) containing β-Zn2SiO4 nanocrystals were prepared under a reduced atmosphere. The optical properties of these samples have been investigated. The emission spectra of Eu2+/Mn2+ co-doped glass ceramics show two broadband peakings at 458 and 560 nm under ultraviolet radiation, which can be attributed to 4f65d1→4f7 transition of Eu2+ and 4T1(4G)6A1(6S) transition of Mn2+, respectively. Energy transfer (ET) from Eu2+ to Mn2+ is discovered by directly observing significant overlap of the excitation spectrum of Mn2+ and the emission spectrum of Eu2+. ET from Eu2+ to Mn2+ in glass ceramics is further confirmed by fluorescence studies performed on the samples with various activator (Mn2+) concentrations. The optimal composition generates white light with chromaticity coordinates (0.291, 0.344). The results indicate that Eu2+/Mn2+ co-doped glass ceramics is potential material for white light-emitting diodes (LEDs).  相似文献   

19.
The luminescence and scintillation properties of Cs2LiLuCl6:0.5%Ce3+ are presented. Special attention is devoted to a 9.4 ns fast emission at 275 nm that can only be excited via the highest cubic field 5de state of Ce. Contrary to Cs3LuCl6 and Cs2LiYCl6, where the same type of fast emission was observed, the emission in Cs2LiLuCl6 is still observed at room temperature. Assuming that the 5de state is located inside the host conduction band (CB), we propose that the emission originates from a mixed state at or just below the bottom of the CB and ends at the 4f ground state of Ce3+. To proof this model we studied the thermal quenching of the anomalous luminescence and performed X-ray photoelectron spectroscopy. A model for a temperature-activated energy transfer from the anomalous state to the lowest 5dt excited state of Ce3+ explains most of the results. Besides the 275 nm emission, the material shows 5dt-4f Ce3+ emission at 370 and 406 nm and 2 ns fast core-valence luminescence when excited with 16-22 eV photons. The scintillation properties of Cs2LiLuCl6:Ce are briefly discussed.  相似文献   

20.
Investigations of EuGa2S4 have been done on the photoluminescence (PL) related to the transition between 4f65d and 4f7 configuration of the Eu2+ ion and its excitation (PLE) spectra, Raman scattering and infrared absorption. The energies of phonons coupled to the ground and the excited states of the transition are analyzed to be 34 and 19 meV from the shapes of the PL and PLE bands, respectively. The former corresponds to the energy of the Raman line showing the highest intensity. The latter is close to the value obtained from analysis of the temperature dependence of the half width of the PL band. These correspondences indicate that the relevant emission of EuGa2S4 surely has phonon-terminated character.  相似文献   

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