10 research outputs found

    On Doping Eu<sup>3+</sup> in Sr<sub>0.99</sub>La<sub>1.01</sub>Zn<sub>0.99</sub>O<sub>3.495</sub>: The Photoluminescence, Population Pathway, De-Excitation Mechanism, and Decay Dynamics

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    Eu<sup>3+</sup>, with the 4f<sup>6</sup> electronic configuration, generally exhibits bright red f-f emissions arising from its <sup>5</sup>D<sub>0</sub> multiplet, and Eu<sup>3+</sup> doped phosphors have attracted lots of attention for applications in lighting and display fields. However, the electron population mechanisms between relevant Eu<sup>3+</sup> excited states as well as charge-transfer state (CTS) still need to be further clarified since the puzzles on these issues limit the exploration of new luminescent materials and the improvement of the luminescence efficiency of the potential phosphors. In this work, a series of Sr<sub>0.99</sub>[La<sub>(1–<i>x</i>)</sub>Eu<sub><i>x</i></sub>]<sub>1.01</sub>Zn<sub>0.99</sub>O<sub>3.495</sub> phosphors was prepared by a high-temperature solid-state reaction technique and was characterized by X-ray diffraction (XRD) measurements at different temperatures, infrared (IR) spectrum, and diffusion reflectance spectra (DRS) at room temperature (RT). The temperature-, doping concentration-, and excitation wavelength-dependent luminescence properties were systematically studied to clarify the population pathway, de-excitation mechanism, and decay dynamics of Eu<sup>3+</sup> in this low-phonon-frequency compound. The impacts of cross relaxation (CR) and multiphonon relaxation (MPR) processes on the luminescence and decay spectra were investigated in detail. The special coordination polyhedron around Eu<sup>3+</sup> played a dominant role in the intense Eu<sup>3+ 5</sup>D<sub>0</sub>–<sup>7</sup>F<sub>4</sub> emission. The CTS peaks shifted to longer wavelengths with increasing temperatures, which seems to relate to the lattice expansion at higher temperatures

    First-Principles Screening and Design of Novel Triphenylamine-Based D−π–A Organic Dyes for Highly Efficient Dye-Sensitized Solar Cells

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    We screen a series of π-conjugated bridge groups and design a range of metal-free organic donor−π–acceptor (D−π–A) <b>SPL101</b>–<b>SPL108</b> dyes based on the experimentally synthesized <b>C217</b> dye for highly efficient dye-sensitized solar cells (DSSC) using density functional theory (DFT) and time-dependent DFT (TDDFT), and further calculate their physical and electronic properties, including geometrical structures, electronic cloud distribution, molecular orbital energy levels, absorption spectra, light harvesting efficiency (LHE), driving force of injection (Δ<i>G</i><sub>inj</sub>) and regeneration (Δ<i>G</i><sub>reg</sub>), and electron dipole moment (μ<sub>normal</sub>). Results reveal that the π-conjugated bridge groups in <b>SPL103</b> and <b>SPL104</b> are promising functional groups for D−π–A organic dyes. In particular,<b> SPL106 </b>and<b> SPL108</b> have not only smaller energy gaps, higher molar extinction coefficients, and 128 and 143 nm redshifts, but also a broader absorption spectrum covering the entire visible range up to the near-IR region of 1200 nm compared to <b>C217</b> dye

    Structure Refinement and Two-Center Luminescence of Ca<sub>3</sub>La<sub>3</sub>(BO<sub>3</sub>)<sub>5</sub>:Ce<sup>3+</sup> under VUV–UV Excitation

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    A series of Ca<sub>3</sub>La<sub>3(1–<i>x</i>)</sub>Ce<sub>3<i>x</i></sub>(BO<sub>3</sub>)<sub>5</sub> phosphors were prepared by a high-temperature solid-state reaction technique. Rietveld refinement was performed using the powder X-ray diffraction (XRD) data, which shows occupation of Ce<sup>3+</sup> on both Ca<sup>2+</sup> and La<sup>3+</sup> sites with a preferred location on the La<sup>3+</sup> site over the Ca<sup>2+</sup> site. The prepared samples contain minor second phase LaBO<sub>3</sub> with contents of ∼0.64–3.27 wt % from the Rietveld analysis. LaBO<sub>3</sub>:1%Ce<sup>3+</sup> was prepared as a single phase material and its excitation and emission bands were determined for identifying the influence of impurity LaBO<sub>3</sub>:Ce<sup>3+</sup> luminescence on the spectra of the Ca<sub>3</sub>La<sub>3(1–<i>x</i>)</sub>Ce<sub>3<i>x</i></sub>(BO<sub>3</sub>)<sub>5</sub> samples. The luminescence properties of Ca<sub>3</sub>La<sub>3(1–<i>x</i>)</sub>Ce<sub>3<i>x</i></sub>(BO<sub>3</sub>)<sub>5</sub> samples under vacuum ultraviolet (VUV) and UV excitation were investigated, which exhibited two-center luminescence of Ce<sup>3+</sup>, assigned to the Ce(1)<sup>3+</sup> center in the La<sup>3+</sup> site and Ce(2)<sup>3+</sup> center in the Ca<sup>2+</sup> site, taking into account the spectroscopic properties and the Rietveld refinement results. The influences of the doping concentration and the excitation wavelength on the luminescence of Ce<sup>3+</sup> in Ca<sub>3</sub>La<sub>3(1–<i>x</i>)</sub>Ce<sub>3<i>x</i></sub>(BO<sub>3</sub>)<sub>5</sub> are discussed together with the decay characteristics

    Structure Refinement and Two-Center Luminescence of Ca<sub>3</sub>La<sub>3</sub>(BO<sub>3</sub>)<sub>5</sub>:Ce<sup>3+</sup> under VUV–UV Excitation

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    A series of Ca<sub>3</sub>La<sub>3(1–<i>x</i>)</sub>Ce<sub>3<i>x</i></sub>(BO<sub>3</sub>)<sub>5</sub> phosphors were prepared by a high-temperature solid-state reaction technique. Rietveld refinement was performed using the powder X-ray diffraction (XRD) data, which shows occupation of Ce<sup>3+</sup> on both Ca<sup>2+</sup> and La<sup>3+</sup> sites with a preferred location on the La<sup>3+</sup> site over the Ca<sup>2+</sup> site. The prepared samples contain minor second phase LaBO<sub>3</sub> with contents of ∼0.64–3.27 wt % from the Rietveld analysis. LaBO<sub>3</sub>:1%Ce<sup>3+</sup> was prepared as a single phase material and its excitation and emission bands were determined for identifying the influence of impurity LaBO<sub>3</sub>:Ce<sup>3+</sup> luminescence on the spectra of the Ca<sub>3</sub>La<sub>3(1–<i>x</i>)</sub>Ce<sub>3<i>x</i></sub>(BO<sub>3</sub>)<sub>5</sub> samples. The luminescence properties of Ca<sub>3</sub>La<sub>3(1–<i>x</i>)</sub>Ce<sub>3<i>x</i></sub>(BO<sub>3</sub>)<sub>5</sub> samples under vacuum ultraviolet (VUV) and UV excitation were investigated, which exhibited two-center luminescence of Ce<sup>3+</sup>, assigned to the Ce(1)<sup>3+</sup> center in the La<sup>3+</sup> site and Ce(2)<sup>3+</sup> center in the Ca<sup>2+</sup> site, taking into account the spectroscopic properties and the Rietveld refinement results. The influences of the doping concentration and the excitation wavelength on the luminescence of Ce<sup>3+</sup> in Ca<sub>3</sub>La<sub>3(1–<i>x</i>)</sub>Ce<sub>3<i>x</i></sub>(BO<sub>3</sub>)<sub>5</sub> are discussed together with the decay characteristics

    Rational Design of Dithienopicenocarbazole-Based Dyes and a Prediction of Their Energy-Conversion Efficiency Characteristics for Dye-Sensitized Solar Cells

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    A series of metal-free organic donor–acceptor (D–A) derivatives (<b>ME01</b>–<b>ME06</b>) of the known dye <b>C281</b> were designed using first-principles calculations in order to evaluate their potential for applications in dye-sensitized solar cells (DSSCs). Their physical and electronic properties were calculated using density functional theory (DFT) and time-dependent density functional theory (TD-DFT). These include molecular properties that are required to assess the feasibility of a dye to function in DSSCs: UV–vis absorption spectra, light-harvesting efficiency (LHE), and driving forces of electron injection (<i>Δ<i>G</i></i><sub>inj</sub>). <b>ME01</b>, <b>ME02</b>, and <b>ME04</b> are predicted to exhibit broad absorption optical spectra that cover the entire visible range, rendering these three dyes promising DSSC prospects. Device-relevant calculations on these three short-listed dyes and the parent dye <b>C281</b> were then performed, whereupon the dye molecules were adsorbed onto anatase TiO<sub>2</sub> surfaces to form the DSSC working electrode. Associated DSSC device characteristics of this dye···TiO<sub>2</sub> interfacial structure were determined. These include the light-harvesting efficiency, the number of injected electrons, the electron-injection lifetime, and the quantum-energy alignment of the adsorbed dye molecule to that of its device components. In turn, these calculated parameters enabled the derivation of the DSSC device performance parameters: short-circuit current density, <i>J</i><sub>SC</sub>, incident photon-to-electron conversion efficiency, IPCE, and open-circuit voltage, <i>V</i><sub>OC</sub>. Thus, we demonstrate a systematic <i>ab initio</i> approach to screen rationally designed D–A dyes with respect to their potential applicability in high-performance DSSC devices

    Optical Properties of Ce-Doped Li<sub>4</sub>SrCa(SiO<sub>4</sub>)<sub>2</sub>: A Combined Experimental and Theoretical Study

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    Investigation of optical properties of Ce<sup>3+</sup>-activated phosphors is not only of practical importance for various applications but also of fundamental importance for providing a basis to understand relevant properties of other lanthanide ions in the same host. We report herein a combined experimental and theoretical study of optical properties of Ce<sup>3+</sup> in Li<sub>4</sub>SrCa­(SiO<sub>4</sub>)<sub>2</sub>. Photoluminescence properties of the material prepared by a solid-state reaction method are investigated with excitation energies in the vacuum-ultraviolet (VUV) to ultraviolet (UV) range at low temperatures. The band maxima in the excitation spectra are assigned with respect to 4f → 5d transitions of Ce<sup>3+</sup> at the Sr and Ca sites, from comparison between experimental and <i>ab initio</i> predicted transition energies. As a result of the two-site occupation, the material displays luminescence at 300–500 nm with a high thermal quenching temperature (>500 K), consistent with the calculated large gaps (∼1.40 eV) between the emitting 5d levels and the bottom of the host conduction band. On the basis of experimental and calculated results for Ce<sup>3+</sup> in Li<sub>4</sub>SrCa­(SiO<sub>4</sub>)<sub>2</sub>, the energy-level diagram for the 4f ground states and the lowest 5d states of all trivalent and divalent lanthanide ions at the Sr and Ca sites of the same host is constructed and discussed in association with experimental findings

    Vacuum Referred Binding Energy Scheme, Electron–Vibrational Interaction, and Energy Transfer Dynamics in BaMg<sub>2</sub>Si<sub>2</sub>O<sub>7</sub>:Ln (Ce<sup>3+</sup>, Eu<sup>2+</sup>) Phosphors

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    The host structure and the synchrotron radiation VUV–UV luminescence properties of samples BaMg<sub>2</sub>Si<sub>2</sub>O<sub>7</sub> (BMSO):Ln (Ce<sup>3+</sup>, Eu<sup>2+</sup>) at different doping levels and different temperatures were investigated in detail. Three important aspects are studied to elucidate the luminescence properties of samples: (1) the vacuum referred binding energy (VRBE) scheme is constructed with the electron binding in the BMSO host bands and in the Ce<sup>3+</sup> and Eu<sup>2+</sup> impurity levels with the aim to explain the different thermal stabilities of Ce<sup>3+</sup> and Eu<sup>2+</sup> emissions; (2) the electron–vibrational interaction analysis on the narrow Eu<sup>2+</sup> emission indicates a weak electron–phonon interaction in the current case; (3) by using three models (Inokuti–Hirayama, Yokota–Tanimoto, and Burshteĭn models) at different conditions, the energy transfer dynamics between Ce<sup>3+</sup> and Eu<sup>2+</sup> was analyzed. It reveals that the energy transfer from Ce<sup>3+</sup> to Eu<sup>2+</sup> via electric dipole–dipole (EDD) interaction is dominant while energy migration between Ce<sup>3+</sup> is negligible. Finally, the X-ray excited luminescence spectra of samples BMSO:Ce<sup>3+</sup>/Eu<sup>2+</sup> are collected to evaluate their possible scintillator applications

    Excitation Wavelength Dependent Luminescence of LuNbO<sub>4</sub>:Pr<sup>3+</sup>î—¸Influences of Intervalence Charge Transfer and Host Sensitization

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    A series of LuNbO<sub>4</sub>:Pr<sup>3+</sup> phosphors was prepared by a solid-state reaction method at high-temperature. Rietveld refinements were performed based on powder X-ray diffraction (XRD) data. Diffuse reflectance spectra (DRS), UV–vis photoluminescence (PL), time-resolved emission spectra (TRES), and fluorescence decays were utilized to study the luminescence and host sensitization processes of Pr<sup>3+</sup> in LuNbO<sub>4</sub>. Excitation wavelength dependent luminescence of LuNbO<sub>4</sub>:Pr<sup>3+</sup> was investigated and explained in consideration of the processes of nonradiation relaxation via cross-relaxation, multiphonon relaxation, and crossover to the intervalence charge transfer (IVCT) state. Furthermore, the host sensitization of Pr<sup>3+</sup> emission in LuNbO<sub>4</sub> was confirmed and the energy transfer efficiency from host to Pr<sup>3+</sup> increased with increasing Pr<sup>3+</sup> doping concentration/temperature. Because the change of emission intensities for both blue from the host and red from <sup>1</sup>D<sub>2</sub> is sensitive to temperature, a large variation of emission color is observed between RT and 500 K

    The Effect of Sr<sup>2+</sup> on Luminescence of Ce<sup>3+</sup>-Doped (Ca,Sr)<sub>2</sub>Al<sub>2</sub>SiO<sub>7</sub>

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    A series of Ce<sup>3+</sup>-doped (Ca,Sr)<sub>2</sub>Al<sub>2</sub>SiO<sub>7</sub> phosphors with different Ce<sup>3+</sup> and Ca<sup>2+</sup>/Sr<sup>2+</sup> concentrations were prepared by a high temperature solid-state reaction technique. To get insight into the structure–luminescence relationship, the impact of incorporation of Sr<sup>2+</sup> on structure of (Ca,Sr)<sub>2</sub>Al<sub>2</sub>SiO<sub>7</sub> was first investigated via Rietveld refinement of high quality X-ray diffraction (XRD) data, and then the VUV–UV excitation and UV–vis emission spectra of (Ca,Sr)<sub>2</sub>Al<sub>2</sub>SiO<sub>7</sub>:Ce<sup>3+</sup> were collected at low temperature. The results reveal that the crystal structure evolution of (Ca,Sr)<sub>2</sub>Al<sub>2</sub>SiO<sub>7</sub>:Ce<sup>3+</sup> has influences on band gaps and Ce<sup>3+</sup> luminescence properties including 4f–5d<sub><i>i</i></sub> (<i>i</i> = 1–5) transition energies, radiative lifetime, emission intensity, quantum efficiency, and thermal stability. Moreover, the influence of Sr<sup>2+</sup> content on the energy of Eu<sup>3+</sup>–O<sup>2–</sup> charge-transfer states (CTS) in (Ca,Sr)<sub>2</sub>Al<sub>2</sub>SiO<sub>7</sub>:Eu<sup>3+</sup> was studied in order to construct vacuum referred binding energy (VRBE) schemes with the aim to further understand the luminescence properties of (Ca,Sr)<sub>2</sub>Al<sub>2</sub>SiO<sub>7</sub>:Ce<sup>3+</sup>. Finally, X-ray excited luminescence (XEL) spectra were measured to evaluate the possibility of (Ca,Sr)<sub>2</sub>Al<sub>2</sub>SiO<sub>7</sub>:Ce<sup>3+</sup> as a scintillation material

    High Light Yield of Sr<sub>8</sub>(Si<sub>4</sub>O<sub>12</sub>)Cl<sub>8</sub>:Eu<sup>2+</sup> under X‑ray Excitation and Its Temperature-Dependent Luminescence Characteristics

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    In this work, we first investigate the relationship between temperature and lattice parameters by means of Rietveld refinement and then demonstrate its impact on the luminescence peak position of Eu<sup>2+</sup> in Sr<sub>8</sub>(Si<sub>4</sub>O<sub>12</sub>)­Cl<sub>8</sub>. It is found that with increases in temperature, lattice expansion takes place without significant distortion of the coordination around Eu<sup>2+</sup>. As a result, the crystal field splitting of the Eu<sup>2+</sup> 5d state decreases. At the same time, with the experimental data of the full width at half-maximum of Eu<sup>2+</sup> emission at different temperatures and the infrared spectrum, the effective phonon frequency is evaluated and the main vibration motions are determined using first-principles calculation. Due to the high light yield under X-ray excitation and the excellent thermal stability of luminescence intensity and decay, a further optimized sample Sr<sub>7.7</sub>Eu<sub>0.3</sub>(Si<sub>4</sub>O<sub>12</sub>)­Cl<sub>8</sub> could be a potential scintillation material
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