Low-temperature thermoluminescence in CaGa2S4:Eu

In the last years many insulating and semiconducting materials activated with rare-earth elements were found to exhibit phosphorescence and thermoluminescence properties, and are attracting increasing interest due to the variety of application of long-lasting phosphors. In this work we studied the phosphorescence decay and thermoluminescence properties of CaGa₂S₄:Eu²⁺ as a function of temperature in the 9-325 K range. The comparison between spectra recorded as a function of time delay from the excitation pulse at different temperatures indicates that long-lasting emissions peaked at about 2.2 eV occurs at Eu²⁺ sites. Thermoluminescence glow curve is characterized by five components at 69, 98, 145, 185 and 244 K. Experimental data are discussed in the framework of generalized order of kinetic model and allow to estimate the activation energies of trapping defects. The origin of glow components at 69, 98, 145 and 244 K is correlated to trapping defects induced by Eu²⁺ doping, while the component at 185 K is attributed to a continuous distribution of defects.     

Cr-related centers in Gd3Ga5O12 polycrystals

The luminescence excitation spectra, emission spectra under photo- and X-ray excitation, luminescence decay kinetics and thermostimulated luminescence (TSL) of Gd₃Ga₅O₁₂ garnet (GGG) polycrystalline samples have been investigated. It was established that the spectrum of Cr³⁺ ion emission were present in all TSL peaks. The activation energies of traps that are responsible for appearance of TSL in the region 295-600 K were estimated. It is shown that delocalization of electrons from the Cr³⁺e traps leads to the appearance of thermoluminescence (TL) glow peak at 390 K. The nature of other TSL peaks is discussed. The influence of visible light on the TSL intensity of the preliminary X-ray-irradiated samples is shown.     

A novel blue-emitting long-lasting proyphosphate phosphor Sr2P2O7:Eu,Y

By introducing the Y³⁺ into Sr₂P₂O₇:Eu²⁺, we successfully prepared a kind of new phosphor with blue long-lasting phosphorescence by the high-temperature solid-state reaction method. In this paper, the properties of Sr₂P₂O₇:Eu²⁺,Y³⁺ were investigated utilizing XRD, photoluminescence, luminescence decay, long-lasting phosphorescence and thermoluminescence (TL) spectra. The phosphor emitted blue light that was related to the 4f⁶5d¹-⁸S_7/2 transition of Eu²⁺. The bright blue phosphorescence could be observed by naked eyes even 8 h after the excitation source was removed. Two TL peaks at 317 and 378 K related to two types of defects appeared in the TL spectrum. By analyzing the TL curve the depths of traps were calculated to be 0.61 and 0.66 eV. Also, the mechanism of LLP was discussed in this report.     

Relaxation kinetics of Sm: Ce-doped CaS phosphors

Different samples of calcium sulphide (CaS):CaS(Sm) and CaS(Sm,Ce) phosphors have been prepared. To study the phosphorescence decay systematically, the samples were excited to a saturation using 259 nm line of xenon lamp and phosphorescence emission was monitored for a wavelength 569 nm of samarium. The trap depth has been evaluated by analyzing the decay curves. The observed decay could be explained satisfactorily by assuming a superposition scheme. The thermoluminescence properties of the doped CaS phosphors are also investigated in detail by computerized deconvolution technique of the glow curves obtained by UV irradiation.     

Study of Vκ centers in CsI crystal

V_κ centers have been observed in CsI doped with Na⁺ and Tl⁺ after X-ray irradiation at LHeT using optical and EPR techniques. It is shown that they are oriented along [100] directions. By studying thermoluminescence two types of thermal migration have been found, one due to linear displacement of the centers along the cubic axis and the other due to 90° rotations. They correspond to two glow peaks at 60 and 90° K respectively.     

Luminescence of Ca-doped (Y1-x, Gdx)2O2S

Broad-band yellow luminescence peaking around 575–595 nm has been found in Ca-doped (Y_1-x, Gd_x)₂O₂S. The doping of Ca into Y₂O₂S with the concentration up to 1 mol% is possible. At the optimum concentration (about 0.2 mol%), the cathodoluminescence brightness of Ca-doped Y₂O₂S is 10% of that of yellow-emitting (Zn, Cd)S: Ag.The emission peak is 575 nm in Y₂O₂S: Ca and 595 nm in Gd₂O₂S: Ca. The phosphor exhibits strong thermoluminescence after UV excitation at 77 K. In (Y_1-x, Gd_x)₂O₂S, neither emission spectra nor the temperatures of thermal glow peak depend on x, indicating localized characters of the traps concerned. The photoluminescence is slow in buildup and persistent in decay. These results are explained by a model: the substitution of Y(Gd) by Ca creates acceptor levels in which holes are captured, giving rise to subsequent radiative recombination with excited electrons. Trapped electrons recombine with mobile holes nonradiatively, but exhibit thermoluminescence with high efficiency when they are thermally released.     

Correlated ESR, PL and TL studies on Sr5(PO4)3Cl:Eu thermoluminescence dosimetry phosphor

Electron spin resonance (ESR), thermoluminescence and photoluminescence studies in Eu²⁺ activated Sr₅(PO₄)₃Cl phosphor are reported in this paper. The Sr₅(PO₄)₃Cl:Eu²⁺ phosphor is twice as sensitive as the conventional CaSO₄:Dy phosphor used in thermoluminescence dosimetry of ionizing radiations. It has a linear response, simple glow curve, emission peaking at 456 nm. The defect centers formed in the Sr₅(PO₄)₃Cl:Eu²⁺phosphor are studied by using the technique of ESR. A dominant TL glow peak at 430 K with a smaller shoulder at 410 K is observed in the phosphor. ESR studies indicate the presence at three centers at room temperature. Step annealing measurements show a connection between one of the centers and the dominant glow peak at 430 K. The 430 K TL peak is well correlated with center I, which is tentatively identified as (PO₄)²⁻ radical.     

Effect of RE as a co-dopant in long-lasting phosphorescence CdSiO3:Mn (RE=Y, La, Gd, Lu)

Effect of RE³⁺ as a co-dopant in long-lasting phosphorescence CdSiO₃:Mn²⁺ (RE=Y, La, Gd, Lu) has been investigated. A longer orange emitting phosphorescence phenomenon was observed in the co-doped CdSiO₃:Mn²⁺,RE³⁺ phosphors after exciting with ultraviolet (UV) light. The luminescence properties, including photoluminescence (PL) spectra and thermoluminescence (TL) spectra, as well as the afterglow decay curves, were studied. The results revealed that one of the origins of the improvement is due to nonequivalent substitution to produce more e-traps, and energy transfer from Gd³⁺ to Mn²⁺ to boost the performance of CdSiO₃:Mn²⁺,Gd³⁺. Role of RE³⁺ co-doped into CdSiO₃:Mn²⁺ matrix and the possible long-lasting phosphorescence process are discussed in this paper.     

Thermoluminescent properties of a Li2O-B2O3-Al2O3 glass system doped with CaF2 and Mn

A Li₂O-B₂O₃-Al₂O₃ glass system doped with CaF₂ and Mn was synthesized by fusion and its physical properties were investigated using thermoluminescence (TL) and differential thermal analysis (DTA) techniques. The TL glow curve peaks, resulting from this analysis, are characteristic of metastable levels intrinsic to CaF₂ crystals that have undergone γ-ray irradiation from a colbalt-60 (⁶⁰Co) source. This provides evidence of CaF₂ crystal formation in the glass system. Furthermore, the TL glow peak at about 480 K was stable at room temperature, sensitive to ⁶⁰Co γ-rays and showed good linearity with doses ranging from 3 Gy to approximately 100 Gy, and consequently could be used to quantify radiation doses. High quality synthesis of these crystals permits control of their thermoluminescent properties.     

Thermoluminescence of rare earth activated CdSO4, SrSO4 and BaSO4

The thermoluminescence (TL) of rare earth (RE) activated sulfates of Cd, Sr and Ba was studied above room temperature. Many of the phosphors prepared exhibit an extremely bright TL following X-irradiation (most notably with Sm, Eu, Tb, Dy and Tm dopants), having an efficiency comparable to that of the highest sensitivity phosphors available for TL dosimetry, and exhibiting activator-induced glow peaks between 405 and 480°K. In a given lattice, the RE³⁺ ions produce a characteristic glow peak at the same temperature (independent of the particular RE ion), whereas Eu²⁺ produces a single glow peak at a different temperature. A decrease in glow peak temperature with increasing interatomic spacing was observed in the homologous SrSO₄-BaSO₄ system - this shift being most pronounced in the Eu²⁺ -doped materials. TL emission spectra were obtained for trivalent Sm, Tb, Dy and Tm and for divalent Eu in these sulfates (and also in CaSO₄).     

Blue-emitting long-lasting phosphor, Sr3Al10SiO20:Eu,Ho

A novel blue-emitting long-lasting phosphor Sr₃Al₁₀SiO₂₀:Eu²⁺,Ho³⁺ is prepared by the conventional high-temperature solid-state technique and their luminescent properties are investigated. XRD, photoluminescence (PL) and thermoluminescence (TL) are used to characterize the synthesized phosphors. These phosphors are well crystallized by calcinations at 1500-1600 °C for 3 h. The phosphor emits blue light and shows long-lasting phosphorescence after it is excited with 254/365 nm ultraviolet light. TL curves reveal the introduction of Ho³⁺ ions into the Sr₃Al₁₀SiO₂₀:Eu²⁺ host produces a highly dense trap level at appropriate depth, which is the origin of the long-lasting phosphorescence in this kind of material. The long-lasting phosphorescence lasts for nearly 6 h in the light perception of the dark-adapted human eye (0.32 mcd/m²). All the results indicate that this phosphor has promising potential practical applications.     

EPR,thermoluminescence, and thermally stimulated conductivity in BaWO4 crystals

In BaWO₄ crystals electrons and holes trapped at WO₄ complexes are identified by electron paramagnetic resonance (EPR) after X-irradiation at T = 80 K. The thermal decay of the intrinsic hole centres at about 100 K is accompanied by a simultaneous decrease of electron traps (WO₄)^3- and glow maxima of thermoluminescence (TL) and of thermally stimulated conductivity (TSC). This connection is explained by a thermally activated hopping of the $\text{(WO}{}_4\text{)}\text{3-}\text{2}$ hole centres followed by radiative recombination with electron traps (WO₄)^3-. A qualitative kinetic calculation based upon EPR data and the shift between TL and TSC glow peak confirms this model.     

Polarization of thermoluminescence of various scheelites

The polarization of the thermoluminescence of various scheelite type single crystals being correlated with the thermal decay of intrinsic hole centres has been measured. The crystals show partial z-polarization of the thermoluminescence. The degree of polarization of the glow light increases with increasing compression of the anionic XO^2-₄ complexes in different crystals. A model explaining the results on the basis of the term diagram of a single oxocomplex is presented.     

α-Al2O3单晶的热释光和光释光特性

研究了纯α-Al₂O₃单晶的热释光发光曲线和三维发光谱，以及光释光衰变曲线，对它们的发光机理和剂量学特性进行了分析和讨论.实验观察到α-Al₂O₃单晶β射线照射后立即测量的热释光发光曲线，有峰温为76℃和207℃两个发光峰.经γ射线照射数小时后测量的三维发光谱，只有峰温207℃波长为416 nm发光峰，它与α-Al₂O₃:C晶体的发光波长基本相同，是受热激发到导带的电子与F< 关键词： 2O₃')" href="#">α-Al₂O₃ 三维发光谱 TL/OSL剂量响应     

Structural analysis, TSL studies and evaluation of trapping parameters of Cu activated CaSO4

The XRD and SEM and TSL studies of the as prepared pure, Cu and Mn doped CaSO₄ have been carried out. From the comparative TSL studies it has been seen that the 137 °C glow peak of CaSO₄:Cu is superior to undoped and Mn doped CaSO₄ compounds as well as other Cu doped alkaline earth sulphates. Evaluation of trapping parameters of the most intensive glow peak Cu (0.5 mol%) doped CaSO₄ is accomplished by a technique named isothermal luminescence decay method and comparison of these parameters with the previously calculated trapping parameters by glow curve shape method (Chen’s method) have been done. It is observed that the most intensive glow peak of Cu doped CaSO₄ is found to obey second order kinetics, because of availability of vacant traps for retrapping to take place. Moreover the effect of various doping concentration of Cu on the TSL glow curve and reproducibility of Cu doped CaSO₄ has also studied.     

Thermoluminescence and isothermal decay of luminescence in x-irradiated urea and thiourea

Experiments have been performed on the thermoluminescence and the isothermal decay of luminescence of both urea and thiourea crystals excited by X-rays at low temperature. The analysis of the isothermal decay curves has been performed assuming that the light emission consists of a sum of exponential decays with different time constants τ_i. Taking into account the dependence of τ_i from temperature, the values of thermal activation energies of the trapping centres involved in the luminescence process are obtained. In addition, the analysis of the glow curve, that has been performed through three different methods, allowed to obtain the values of some parameters related to the thermoluminescence process, such as the thermal activation energy E, the frequency factor s and the ration A/B between the retrapping and recombination probabilities. These results agree well enough with those from the isothermal decay analysis. A comparison has been made between the results for urea and for thiorea. Some topics concerned with the nature of the defects responsible for the luminescence process in these substances are also investigated.     

Dosimetric properties of rare earth doped LiCaBO3 thermoluminescence phosphors

Lithium Calcium borate (LiCaBO₃) polycrystalline thermoluminescence (TL) phosphor doped with rare earth (RE³⁺) elements has been synthesized by high temperature solid state diffusion reaction. The reaction has produced a very stable crystalline LiCaBO₃:RE³⁺ phosphors. Among these RE³⁺ doped phosphors thulium doped material showed maximum TL sensitivity with favorable glow curve shape. TL glow curve of gamma irradiated LiCaBO₃:Tm³⁺ samples had shown two major well-separated glow peaks at 230 and 430 °C. The glow peak at 430 °C is almost thrice the intensity of the glow peak at 230 °C. The TL sensitivity of the phosphor to gamma radiation was about eight times that of TLD-100 (LiF). Photoluminescence and TL emission spectra showed the characteristic Tm³⁺ peaks. TL response to gamma radiation dose was linear up to 10³ Gy. Post-irradiation TL fading on storage in room temperature and elevated temperatures was studied in LiCaBO₃:Tm³⁺ phosphor.     

Cr+ centres in mixed polytype ZnS single crystal

The glow peaks of mixed polytype ZnS: Cu, Cr, Cl crystals were identified as produced by three Cr⁺ centres observed by electron paramagnetic resonance (EPR): one cubic (C) and two axial (H₁ and H₂). The characteristics of these centres were partly found by the methods of interrupted thermoluminescence, infrared stimulation, “thermo-EPR” (variation of the EPR signal with heating of a previously excited crystal) and also by decay of glow areas and of the three Cr⁺EPR signals after excitation at different temperatures. Moreover, these measurements showed the important part played by the non-thermal emptying of the Cr⁺ traps. This emptying occurs through photoexcitation of the trapped electrons by the reabsorbed luminescence light or through recombination of these electrons with free holes. Both of these processes diminish the efficiency of phosphorescence when the crystal is cooled; so it was necessary to take them into account when analysing the experimental results. The percentage of H₁ and H₂ found by EPR and luminescence is in agreement with the percentage of the hexagonalicity as found from the birefringence measurements. The crystal field calculation gives account of three centres in such a mixed polytype crystal.     

Effect of doping on the luminescence properties of Li2B4O7

In this work, we have investigated the influence of doping agents on the luminescence properties of multiply doped Li₂B₄O₇ and the temperature lag between TSL materials and the heating element. The results of thermoluminescence studies show that the Ag doping leads to the appearance of a new glow curve peak at 165 °C and the increasing sensitivity of Li₂B₄O₇:Cu,Ag,P is correlated with copper and phosphate concentrations. Under the excitation at 245 nm the emission spectra show maxima at 365 and 450 nm in the ceramic, crystal and glass. The low energy shift in the latter system might be related to the local structural distortion in the glass around Cu⁺ ions.     

Isothermal stability of colour centers in microcrystalline powder of NaCl:KCl

A correlation between thermoluminescence and isothermal decay of colouration in NaCl:KCl microcrystalline powder is reported. No isothermal bleaching of colouration is observed for all the compositions. However, a rapid isothermal decay is seen in K₉₅N₅Cl and K₉₀Na₁₀Cl, when the first of the two glow peaks is thermally bleached. It is suggested that the interaction between colour centers and dislocations is inhibited upon mixing.