Effect of Bi3+ addition on the upconversion luminescence properties of NaYbF4:Er

In this study, Bi³⁺ incorporation in NaYbF₄:Er lattice and its influence on upconversion luminescence properties have been investigated in detail using techniques such as temperature‐dependent luminescence, Fourier transform infrared spectroscopy and X‐ray diffraction (XRD). The study was carried out to develop phosphors with improved upconversion luminescence. From photoluminescence and lifetime measurements it is inferred that luminescence intensity from NaYbF₄:Er increases with Bi³⁺ addition. The sample containing 50 at.% Bi³⁺ ions exhibited optimum upconversion luminescence. Increased distance between Yb³⁺–Yb³⁺ and Er³⁺–Er³⁺ due to Bi³⁺ incorporation into the lattice and associated decrease in the extent of dipolar interaction/self‐quenching are responsible for increase in lifetime values and luminescence intensities from Er³⁺ ions. Incorporation of Bi³⁺ into NaYbF₄:Er lattice reduced self‐quenching among Yb³⁺–Yb³⁺ions and this facilitated energy transfer from Yb³⁺ to Er³⁺. This situation also explains decrease in the extent of temperature‐assisted quenching of emission from thermally coupled ²H_11/2 and ⁴S_3/2 levels of Er³⁺. Based on Rietveld refinement of XRD patterns it was confirmed that a maximum of 10 at.% of Bi³⁺added was incorporated into the NaYbF₄:Er lattice and the remaining complex co‐exists as a BiOF phase. These results are of significant interest in the area of development of phosphors based on Yb³⁺–Er³⁺ upconversion luminescence.     

Enhanced green emissions of Er3+/Yb3+ co‐doped Gd2(MoO4)3 by co‐excited up‐conversion processes

Improving the emission from rare earth ions doped materials is of great importance to broaden their application in bio‐imaging, photovoltaics and temperature sensing. The green emissions of Gd₂(MoO₄)₃:Er³⁺/Yb³⁺ powder upon co‐excitation with 980 and 808 nm lasers were investigated in this paper. Distinct enhancement of green emissions was observed compared with single laser excitation. Based on the energy level structure of Er³⁺, the enhancement mechanism was discussed. Moreover, the result of temperature‐dependent enhancement revealed that the enhancement factor reached its maximum (2.5) as the sample heated to 120°C, which is due to the competition of two major thermal effects acting in the co‐excited up‐conversion processes. In addition, the same enhancement of green emissions was also observed in Gd₂(MoO₄)₃:Er³⁺ powder and NaYF₄:Er³⁺/Yb³⁺ powder.     

Down-conversion luminescence and temperature sensing characteristics of LaSrGaO4:Er3+

Erbium(III) ion (Er³⁺) has abundant energy levels that can emit light covering a quite broad wavelength range in many hosts. Here we synthesized LaSrGaO₄:Er³⁺ phosphors by a high-temperature solid-state method. Upon excitation at the ultraviolet (UV) band, LaSrGaO₄:Er³⁺ phosphors could emit green, red and near-infrared emission simultaneously. The temperature dependent emission characteristics of the as-prepared samples was then studied and two kinds of luminescent ratiometric thermometry were constructed. The first one is on the basis of two green emission bands that stems from the ²H_11/2 → ⁴I_15/2 and ⁴S_3/2 → ⁴I_15/2 transitions of Er³⁺. The intensity ratio between these two emission bands was found to follow well with the Boltzmann distribution, and its maximum relative sensitivity was calculated to be 0.84% K⁻¹ at 299 K. The other one depends on the ⁴F_9/2 → ⁴I_15/2 transition of Er³⁺ and self-luminescence of the host LaSrGaO₄, considering that these two emission lines have different temperature response. The relative sensitivity of this type of luminescence intensity ratio (LIR) thermometry could reach 1.86% K⁻¹ at 299 K, we have successfully developed materials with one of the largest relative sensitivities to date, which provides some basis for the subsequent development of a new type of non-contact temperature sensor.     

Preparation and up‐conversion luminescence properties of LaOBr:Yb3+/Er3+ nanofibers via electrospinning

LaOBr:Yb³⁺/Er³⁺ nanofibers were synthesized for the first time by calcinating electrospun PVP/[La(NO₃)₃ + Er(NO₃)₃ + Yb(NO₃)₃ + NH₄Br] composites. The morphology and properties of the final products were investigated in detail using scanning electron microscopy (SEM), energy dispersion spectroscopy (EDS), X‐ray diffractometry (XRD) and fluorescence spectroscopy. The results indicate that LaOBr:Yb³⁺/Er³⁺ nanofibers are tetragonal in structure with a space group of P4/nmm. The diameter of LaOBr:Yb³⁺/Er³⁺ nanofibers is ~ 147 nm. Under the excitation of a 980‐nm diode laser, LaOBr:Yb³⁺/Er³⁺ nanofibers emit strong green and red up‐conversion emission centering at 519, 541 and 667 nm, ascribed to the ²H_11/2, ⁴S_3/2 → ⁴I_15/2 and ⁴ F_9/2 → ⁴I_15/2 energy‐level transitions of Er³⁺ ions, respectively. The up‐conversion luminescent mechanism of LaOBr:Yb³⁺/Er³⁺ nanofibers is advanced. Moreover, near‐infrared emission of LaOBr:Yb³⁺/Er³⁺ nanofibers is obtained under the excitation of a 532‐nm laser. The formation mechanism of LaOBr:Yb³⁺/Er³⁺ nanofibers is proposed. LaOBr:Yb³⁺/Er³⁺ nanofibers could be important up‐conversion luminescent materials. Copyright © 2014 John Wiley & Sons, Ltd.     

Photoluminescence properties of rare‐earth‐doped (Er3+,Yb3+) Y2O3 nanophosphors by a combustion synthesis method

In this work, we report the synthesis of Y₂O₃:Er³⁺, Y₂O₃:Yb³⁺ and Y₂O₃:Er³⁺,Yb³⁺ nanophosphors by the combustion synthesis method using urea as fuel. The doping agents were incorporated in the form of erbium nitrate and ytterbium nitrate. X‐Ray diffraction (XRD) patterns revealed that the synthesized particles have a body‐centered cubic structure with space group Ia‐3. The photoluminescence (PL) properties were investigated after UV and infrared irradiation at room temperature. A strong characteristic emission of Er³⁺ and Yb³⁺ ions was identified, and the influence of doping concentration on the PL properties was systematically studied. Energy transfer from Yb³⁺ to Er³⁺ ions was observed in Y₂O₃ nanophosphors. The obtained result may be useful in potential applications such as bioimaging. Copyright © 2015 John Wiley & Sons, Ltd.     

Thermoluminescence dosimetric attributes of Yb3+-doped BaO–ZnO–LiF–B2O3 glass material after Er3+ co-doping

Motivated by our previous study on Sm³⁺ ions as thermoluminescence (TL) sensitizers to the BaO–ZnO–LiF–B₂O₃–Yb₂O₃ glass system, in the current study we examined the effect of Er³⁺ ion co-doping on the TL characteristics of this glass system. The 4f–4f electronic transitions of the Er³⁺ and Yb³⁺ ions were confirmed via the optical absorption spectrum. Notably, the use of Yb³⁺–Er³⁺ ions failed to improve the TL intensity, sensitivity, and trap density. However, they enabled the glass system to function as an activator–quencher system. The linearity range and effective atomic number remained unaffected after co-doping. In addition, the problem of anomalous fading caused a remnant signal of just 58% after a week of storage of the Yb³⁺ monodoped glass. This was resolved by the optimum co-doping of Er³⁺ ions to achieve an 89% signal. The co-doping of Er³⁺ ions to the BaO–ZnO–LiF–B₂O₃–Yb₂O₃ glass system regulated its thermal stability and therefore supplemented its potential for radiation monitoring in food processing and retrospective dosimetry.     

Structural characterization of Er3+,Yb3+‐doped Gd2O3 phosphor,synthesized using the solid‐state reaction method,and its luminescence behavior

We report the synthesis and structural characterization of Er³⁺,Yb³⁺‐doped Gd₂O₃ phosphor. The sample was prepared using the conventional solid‐state reaction method, which is the most suitable method for large‐scale production. The prepared phosphor sample was characterized using X‐ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), Fourier transform infrared spectroscopy (FTIR), thermoluminescence (TL), photoluminescence (PL) and CIE techniques. For PL studies, the excitation and emission spectra of Gd₂O₃ phosphor doped with Er³⁺ and Yb³⁺ were recorded. The excitation spectrum was recorded at a wavelength of 551 nm and showed an intense peak at 276 nm. The emission spectrum was recorded at 276 nm excitation and showed peaks in all blue, green and red regions, which indicate that the prepared phosphor may act as a single host for white light‐emitting diode (WLED) applications, as verified by International de I'Eclairage (CIE) techniques. From the XRD data, the calculated average crystallite size of Er³⁺ and Yb³⁺‐doped Gd₂O₃ phosphor is ~ 38 nm. A TL study was carried out for the phosphor using UV irradiation. The TL glow curve was recorded for UV, beta and gamma irradiations, and the kinetic parameters were also calculated. In addition, the trap parameters of the prepared phosphor were also studied using computerized glow curve deconvolution (CGCD). Copyright © 2015 John Wiley & Sons, Ltd.     

Spectral‐converting study of Ba9–3(m+n)/2ErmYbnY2Si6O24 (m = 0.005 – 0.2, n = 0 – 0.3) orthosilicate phosphors

Optical materials composed of Ba_9–3(m+n)/2Er_mYb_nY₂Si₆O₂₄ (m = 0.005–0.2, n = 0–0.3) were prepared using a solid‐state reaction. The X‐ray diffraction patterns of the obtained phosphors were examined to index the peak positions. The photoluminescence (PL) excitation and emission spectra of the Er³⁺‐activated phosphors and the critical emission quenching as a function of Er³⁺ content in the Ba_9–3m/2Er_mY₂Si₆O₂₄ structure were monitored. The spectral conversion properties of Er³⁺ and Er³⁺–Yb³⁺ ions doped in Ba₉Y₂Si₆O₂₄ phosphors were elucidated under diode‐laser irradiation at 980 nm. Up‐conversion emission spectra and the dependence of the emission intensity on pump power for the Ba_8.55Er_0.1Yb_0.2Y₂Si₆O₂₄ phosphor were investigated. The desired up‐conversion of the emitted light, which passed through the green, yellow, orange and red regions of the spectrum, was achieved through the use of appropriate Er³⁺ and/or Yb³⁺ concentrations in the host structure and 980 nm excitation light. The up‐conversion mechanism in the phosphors is described by an energy‐level schematic. Copyright © 2015 John Wiley & Sons, Ltd.     

Spectroscopic investigations of Er(3+) :CdO-Bi(2) O(3) -B(2) O(3) glasses

This article reports on the optical properties of Er³⁺ ions doped CdO–Bi₂O₃–B₂O₃ (CdBiB) glasses. The materials were characterized by optical absorption and emission spectra. By using Judd–Ofelt theory, the intensity parameters Ω_λ (λ = 2, 4, 6) and also oscillatory strengths were calculated from the absorption spectra. The results were used to compute the radiative properties of Er³⁺:CdBiB glasses. The concentration quenching and energy transfer from Yb³⁺–Er³⁺ were explained. The stimulated emission cross‐section, full width at half maximum (FWHM) and FWHM × values are also calculated for all the Er³⁺:CdBiB glasses. Copyright © 2011 John Wiley & Sons, Ltd.     

Upconverted photoluminescence in Ho3+ and Yb3+ codoped Gd2O3 nanocrystals with and without Li+ ions

The upconversion photoluminescence of Ho³⁺ ion sensitized by Yb³⁺ ion in Ho³⁺/Yb³⁺codoped Gd₂O₃ nanocrystals with and without Li⁺ is investigated in this paper. Strong fluorescence in the green (534–570 nm) and red (635–674 nm) regions of the spectrum has been observed, arising from the ⁵F₄/⁵S₂ → ⁵I₈ and ⁵F₅ → ⁵I₈ transitions of Ho³⁺ ion, respectively. Yb³⁺ ion is considered to be a better sensitizer for catching enough pumping energy and transferring considerable energy to Ho³⁺ in the Ho³⁺/Yb³⁺system. The upconversion intensity emitted by Ho³⁺ is greatly enhanced when Li⁺ is added to the Ho³⁺/Yb³⁺ codoped Gd₂O₃ nanocrystals.     

The structure and luminescence properties of Mn2+/Eu2+/Er3+‐doped MgO‐Ga2O3‐SiO2 glasses and glass‐ceramics

The MgO–Ga₂O₃–SiO₂ glasses and glass‐ceramics samples doped with Eu²⁺/Mn²⁺/Er³⁺ and heated in reductive atmosphere were prepared by the sol–gel method. The structure, morphology and the luminescence properties were studied using X‐ray diffraction, high‐resolution transmission electron microscope, fluorescence spectra, and up‐conversion emission. The luminescence characteristics of doped ions could be influenced by temperature and matrix component. The characteristic emission of Mn²⁺, Eu²⁺ and Er³⁺ were seen and the energy transfer efficiency from Eu²⁺ to Mn²⁺ was enhanced as Mn²⁺ concentration was increased. In addition, the two‐photon process was determined for the Er³⁺‐doped samples.     

Erbium(III) ion-doped borate-based glasses for 1.53 μm broad band applications

Novel erbium(III) ion-doped borate-based glasses (Er³⁺:BCNF) by conventional melt-quenching technique were designed and synthesized. The glasses were characterized for their structural, vibrational and spectroscopic properties. The nephelauxetic ratio, bonding parameters, and Judd–Ofelt (JO) intensity parameters (Ω_λ λ = 2, 4 and 6) were determined by using absorption spectrum of 1 mol% Er₂O₃ doped glass. These JO parameters were utilized to derive radiative properties for various excited states of erbium(III) ions. Emission cross-section for ⁴I_13/2 → ⁴I_15/2 transition of erbium(III) ions was computed through McCumber theory. The decay curves for (²H_11/2, ⁴S_3/2) and ⁴I_13/2 levels were recorded and analysed. All the results of Er³⁺:BCNF glasses revealed that the studied glasses are efficient and thermally stable and could be suitable for display devices, optical amplification and green laser applications.     

Tunable multicolor and white‐light upconversion luminescence in Yb3+/Tm3+/Ho3+ tri‐doped NaYF4 micro‐crystals

NaYF₄ micro‐crystals with various concentrations of Yb³⁺/Tm³⁺/Ho³⁺ were prepared successfully via a simple and reproducible hydrothermal route using EDTA as the chelating agent. Their phase structure and surface morphology were studied using powder X‐ray diffraction (XRD) and scanning electron microscopy (SEM). The XRD patterns revealed that all the samples were pure hexagonal phase NaYF₄. SEM images showed that Yb³⁺/Tm³⁺/Ho³⁺ tri‐doped NaYF₄ were hexagonal micro‐prisms. Upconversion photoluminescence spectra of Yb³⁺/Tm³⁺/Ho³⁺ tri‐doped NaYF₄ micro‐crystals with various dopant concentrations under 980 nm excitation with a 665 mW pump power were studied. Tunable multicolor (purple, purplish blue, yellowish green, green) and white light were achieved by simply adjusting the Ho³⁺ concentration in 20%Yb³⁺/1%Tm³⁺/xHo³⁺ tri‐doped NaYF₄ micro‐crystals. Furthermore, white‐light emissions could be obtained using different pump powers in 20%Yb³⁺/1%Tm³⁺/1%Ho³⁺ tri‐doped NaYF₄ micro‐crystals at 980 nm excitation. The pump power‐dependent intensity relationship was studied and relevant energy transfer processes were discussed in detail. The results suggest that Yb³⁺/Tm³⁺/Ho³⁺ tri‐doped NaYF₄ micro‐crystals have potential applications in optoelectronic devices such as photovoltaic, plasma display panel and white‐light‐emitting diodes. Copyright © 2014 John Wiley & Sons, Ltd.     

Enhancement of near‐infrared up‐conversion and blue down‐conversion luminescence in LuNbO4:Yb3+,Tm3+ with Ga3+ and Ta5+ substitutions

Under a 980‐nm excitation, the up‐conversion (UC) spectra of LuNbO₄:Yb³⁺,Tm³⁺ powders exhibited predominantly near‐infrared bands (~805 nm) of Tm³⁺ through an energy transfer process from Yb³⁺ to Tm³⁺. Regarding the down‐conversion (DC) luminescence of the powders, the photoluminescence excitation spectra consisted of a broad charge transfer band (270 nm) due to [NbO₄]^3? and sharp band (360 nm) of Tm³⁺, while the corresponding emission spectra exhibited a blue emission at 458 nm. Upon substitution of Ga³⁺ and Ta⁵⁺ for Lu³⁺ and Nb⁵⁺, respectively, both UC and DC luminescence properties were significantly enhanced. For the Ga³⁺ substitution, the increased emission intensity could be explained by the crystal field asymmetry surrounding the Tm³⁺ ions induced by the large difference in ionic radius between Ga³⁺ and Lu³⁺. For the Ta⁵⁺ substitution, we believe that an M′‐LuTaO₄ substructure was formed in the host, which led to the formation of a TaO₆ octahedral coordination instead of a NbO₄ tetrahedral coordination. Consequently, the crystal symmetry of the local structure was modified, and thus the UC and DC luminescence properties were enhanced. The dual‐mode (UC and DC) luminescence demonstrates that LuNbO₄:Yb³⁺,Tm³⁺ has a great potential in the fields of temperature sensing probes, anti‐counterfeiting, and bioapplications.     

Nd3+‐Yb3+/Nd3+‐Yb3+‐Li+ co‐doped Gd2O3 phosphors for up and down conversion luminescence

Frequency up‐conversion (UC) emission from the Nd³⁺‐Yb³⁺/Nd³⁺‐Yb³⁺‐Li⁺ co‐doped gadolinium oxide (Gd₂O₃) phosphors prepared by the solution combustion technique in the visible range have been studied by using 980 nm near infrared (NIR) laser diode excitation. The crystalline structure and formation of the cubic phase has been confirmed with the help of X‐ray diffraction (XRD) studies. XRD peak shifts have been found towards the lower diffraction angle side in the case of the Nd³⁺‐Yb³⁺‐Li⁺ co‐doped phosphors. Surface morphology and particle size information have been observed by using field emission scanning electron microscopy (FESEM) and transmission electron microscopy (TEM) analysis. Down‐conversion emission study under 351 nm excitation in the visible region for the Nd³⁺‐Yb³⁺/Nd³⁺‐Yb³⁺‐Li⁺ co‐doped phosphors has been performed. The UC emission bands lying in the green and red region arising from the Nd³⁺ ions have been enhanced by ~260 times, ~113 times due to incorporation of Li⁺ ions in the Nd³⁺‐Yb³⁺ co‐doped phosphors. Photometric characterization has been done for the Nd³⁺‐Yb³⁺/Nd³⁺‐Yb³⁺‐Li⁺ co‐doped phosphors. The present study suggests the capability of the synthesized phosphors in near‐infrared (NIR) to visible upconverter and luminescent device applications.     

Synthesis and characterization of KCe(PO3)4 doped with some lanthanide activators

KCe(PO₃)₄ doped with Dy³⁺,Tb³⁺,Yb³⁺and Nd³⁺ phosphors were synthesized by a solid state diffusion method. The prepared samples were characterized by X‐ray diffraction and photoluminescence. KCe(PO₃)₄ exhibits emission in ultraviolet (UV) region which indicates weak Ce³⁺–Ce³⁺ interaction. The Ce³⁺–Ce³⁺energy transfer is not efficient. In light of this, energy transfer from Ce³⁺ to other lanthanides like Dy³⁺, Tb³⁺,Yb³⁺ and Nd³⁺ is rather surprising.     

Influence of Er3+ concentration on the photoluminescence characteristics and excitation mechanism of Gd2O3:Er3+ phosphor synthesized via a solid‐state reaction method

An Er³⁺‐doped phosphor of Gd₂O₃ (Gd₂O₃:Er³⁺) was prepared using a conventional solid‐state reaction method. The structure and particle size were determined from X‐ray powder diffraction measurements. The average particle size of the phosphor was in between 20 and 50 nm. The particle size and structure of the phosphor were further confirmed by transmission electron microscopy (TEM) analysis. Luminescence spectra were recorded under excitation wavelengths of 275, 380, 515 and 980 nm. The visible upconversion and downconversion luminescence spectra of the Gd₂O₃:Er³⁺ phosphor were investigated as a function of Er³⁺ ion concentration. The upconverted emission at 980 nm excitation shows enhanced red emission with respect to green emission as the dopant concentration increased. Similar results were observed for downconversion emission under 275 and 380 nm excitation wavelengths. The mechanisms responsible for populating the ⁴S_3/2 and ⁴ F_9/2 levels, for green and red emissions, respectively, are different for different excitations and for different concentrations of Er³⁺. Copyright © 2014 John Wiley & Sons, Ltd.     

Photoluminescence and thermoluminescence properties of pure and rare-earth-doped ZrO2 prepared by Pechini-type sol–gel

In this article, photoluminescence (PL) and thermoluminescence (TL) properties of ZrO₂, ZrO₂:Dy³⁺, ZrO₂:Dy³⁺–Gd³⁺, ZrO₂:Dy³⁺–Yb³⁺, ZrO₂:Dy³⁺–Er³⁺, and ZrO₂:Dy³⁺–Sm³⁺ phosphors synthesized by the Pechini method were investigated. The crystal structure, thermal properties, morphology, PL and TL properties were investigated using X-ray powder diffraction (XRD), differential thermal analysis/thermogravimetric analysis (DTA/TGA), scanning electron microscopy (SEM), PL and TL, respectively. The room temperature emission bands corresponding to ⁴F_9/2 → ⁶H_J (J = 9/2, 11/2, 13/2 and 15/2) transitions of Dy³⁺ ions were measured. The phosphors were analysed using T_m–T_STOP, variable dose, and computerized glow curve fitting methods. Reusability, dose–response, and fading characteristics were investigated. The phosphors have a natural TL emission that vanished by heating treatment. Moreover, new peaks with similar properties to the natural emissions were observed after high-dose irradiation and long-term fading experiments. The glow curves of the phosphors have 13 individual peaks and many low- and high-temperature satellite peaks. The origin of the peaks is ZrO₂ host material and doping with rare-earth ions (Gd³⁺, Dy³⁺, Yb³⁺, Er³⁺ and Sm³⁺) does not lead to a new glow peak. The dopants cause drastic changes in individual peak intensities of ZrO₂.The initial fading rates of all the phosphors are relatively fast, but they slow down as time goes on.     

Pure red upconverted and near-infrared luminescence properties of Er3+-doped SnO2 nanocrystals for lighting applications

Tin oxide (SnO₂) nanocrystalline powders doped with erbium ion (Er³⁺) in different molar ratios (0, 3, 5, and 7 mol%) were prepared using a solid-state reaction technique. These samples were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM), ultraviolet-visible absorption, visible upconversion, and near-infrared luminescence techniques. XRD analysis revealed the tetragonal rutile structure of SnO₂ and the average crystallite size was about 32 nm. From Tauc's plots, it was confirmed that the substitution of Er³⁺ ions into the SnO₂ host lattice resulted in the narrowing its band gap. Optical absorption bands at 520 and 654 nm correspond to the 4f electron transitions of Er³⁺ further confirming visible light absorption. Infrared luminescence spectra showed a broad band centred at 1536 nm which is assigned to the ⁴I_13/2 → ⁴I_15/2 transition of Er³⁺. Visible upconverted emission spectra under 980 nm excitation exhibit a strong red luminescence with a main peak at 672 nm which is attributed to the ⁴F_9/2 → ⁴I_15/2 transition of Er³⁺. Power-dependent upconversion spectra confirmed that two photons participated in the upconversion mechanism. Enhancement in the intensities of both visible and infrared luminescence was observed when raising the concentration. The results pave the way for the potential applications of these nanocrystalline powders in energy harvesting applications such as infrared light upconverting layer in solar cells, light emitting diodes, infrared broadband sources and amplifiers, and biological labelling.