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
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
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
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
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
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
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>SrCaÂ(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>SrCaÂ(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
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
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>
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
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>)ÂCl<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>)ÂCl<sub>8</sub> could be a
potential scintillation material