22 research outputs found
Electronic Spectra and Crystal-Field Analysis of Europium in Hexanitritolanthanate Systems
The luminescence spectra of Eu<sup>3+</sup> at a <i>T</i><sub><i>h</i></sub> point-group site in the hexanitritolanthanate
systems Cs<sub>2</sub>NaEuÂ(<sup>14</sup>NO<sub>2</sub>)<sub>6</sub>, Cs<sub>2</sub>NaEuÂ(<sup>15</sup>NO<sub>2</sub>)<sub>6</sub>, Rb<sub>2</sub>NaEuÂ(<sup>14</sup>NO<sub>2</sub>)<sub>6</sub>, Cs<sub>2</sub>LiEuÂ(<sup>14</sup>NO<sub>2</sub>)<sub>6</sub>, and Cs<sub>2</sub>NaYÂ(<sup>14</sup>NO<sub>2</sub>)<sub>6</sub>:Eu<sup>3+</sup> have
been recorded between 19 500 and 10 500 cm<sup>–1</sup> at temperatures down to 3 K. The spectra comprise magnetic-dipole-allowed
zero phonon lines, odd-parity metal–ligand vibrations, internal
anion vibrations, and lattice modes, with some weak vibrational progressions
based upon vibronic origins. With the aid of density functional theory
calculations, the vibrational modes in the vibronic sidebands of transitions
have been assigned. The two-center transitions involving NO<sub>2</sub><sup>–</sup> stretching and scissoring modes are most prominent
for the <sup>5</sup>D<sub>0</sub> → <sup>7</sup>F<sub>2</sub> hypersensitive transition. The onset of NO<sub>2</sub><sup>–</sup> triplet absorption above 20 000 cm<sup>–1</sup> restricts
the derived Eu<sup>3+</sup> energy-level data set to the <sup>7</sup>F<sub><i>J</i></sub> (<i>J</i> = 0–6)
and <sup>5</sup>D<sub>0,1</sub> multiplets. A total of 21 levels have
been included in crystal-field energy-level calculations of Eu<sup>3+</sup> in Cs<sub>2</sub>NaEuÂ(NO<sub>2</sub>)<sub>6</sub>, using
seven adjustable parameters, resulting in a mean deviation of ∼20
cm<sup>–1</sup>. The comparison of our results is made with
Eu<sup>3+</sup> in the double nitrate salt. In both cases, the fourth-rank
crystal field is comparatively weaker than that in europium hexahaloelpasolites
What Factors Affect the <sup>5</sup>D<sub>0</sub> Energy of Eu<sup>3+</sup>? An Investigation of Nephelauxetic Effects
Relationships
involving the interelectronic repulsion parameters, <i>F</i><sup><i>k</i></sup> (<i>k</i> = 2,
4, 6), the spin–orbit coupling constant, ζ<sub>f</sub>, and <i>J</i>-mixing, with the <sup>5</sup>D<sub>0</sub>–<sup>7</sup>F<sub>0</sub> energy, <i>E</i>, have
been investigated for Eu<sup>3+</sup> using various approaches. First,
the linear relationship between <i>E</i> and the <sup>7</sup>F<sub>1</sub> splitting (or the second rank crystal field parameter)
is shown to be applicable not only to glasses but also to solid-state
crystalline systems with Eu<sup>3+</sup> site symmetry of <i>C</i><sub>2</sub>, <i>C</i><sub>2<i>v</i></sub>, or lower. In these cases, the change in <sup>5</sup>D<sub>0</sub>–<sup>7</sup>F<sub>0</sub> energy is mainly due to
the <i>J</i>-mixing effect of <sup>7</sup>F<sub><i>J</i></sub> (<i>J</i> = 2, 4, 6: most notably <i>J</i> = 2) which depresses <sup>7</sup>F<sub>0</sub>, whereas
the <sup>5</sup>D<sub>0</sub> energy is relatively constant. The <sup>5</sup>D<sub>0</sub>–<sup>7</sup>F<sub>0</sub> energy also
depends upon certain energy parameters in the Hamiltonian, in particular, <i>F</i><sup><i>k</i></sup> and ζ<sub>f</sub>.
Model calculations show that increase in <i>F</i><sup>4</sup> or <i>F</i><sup>6</sup> produces an increase in <i>E</i>, whereas increase in <i>F</i><sup>2</sup> produces
a decrease in <i>E</i>. An increase in ζ<sub>f</sub> produces a decrease in <i>E</i>. These findings are rationalized.
Most previous 4f<sup>6</sup> crystal field calculations have only
considered the F and D terms of Eu<sup>3+</sup> so that the Slater
parameters are not well-determined. More reliable energy level data
sets and crystal field calculations for Eu<sup>3+</sup> with fluoride,
oxide, or chloride ligands have been selected, and certain of these
have been repeated since most previous calculations have errors in
matrix elements. The fitted Slater parameters have been corrected
for the effects of three-body Coulomb interactions. Some systems do
not follow the ligand trend F ∼ O > Cl for Slater and spin–orbit
parameters. From the limited data available, the average values of
the corrected Slater parameters are greater for fluoride compared
with chloride ligands, but the differences are comparable with the
standard deviations of the parameters. There is no clear nephelauxetic
series for these three types of ligands, with respect to spin–orbit
coupling. Previous correlations of <i>E</i> with various
parameters are of limited value because the <sup>5</sup>D<sub>0</sub>–<sup>7</sup>F<sub>0</sub> energy difference not only depends
upon the <i>F</i><sup><i>k</i></sup> and ζ<sub>f</sub> parameters but in addition is sensitive to the importance
of <i>J</i>-mixing for low symmetry systems
Ce–O Covalence in Silicate Oxyapatites and Its Influence on Luminescence Dynamics
Cerium substituting gadolinium in
Ca<sub>2</sub>Gd<sub>8</sub>(SiO<sub>4</sub>)<sub>6</sub>O<sub>2</sub> occupies two intrinsic sites of distinct coordination. The coexistence
of an ionic bonding at a 4F site and an ionic–covalent mixed
bonding at a 6H site in the same crystalline compound provides an
ideal system for comparative studies of ion–ligand interactions.
Experimentally, the spectroscopic properties and photoluminescence
dynamics of this white-phosphor are investigated. An anomalous thermal
quenching of the photoluminescence of Ce<sup>3+</sup> at the 6H site
is analyzed. Theoretically, ab initio calculations are conducted to
reveal the distinctive properties of the Ce–O coordination
at the two Ce<sup>3+</sup> sites. The calculated eigenstates of Ce<sup>3+</sup> at the 6H site suggest a weak Ce–O covalent bond
formed between Ce<sup>3+</sup> and one of the coordinated oxygen ions
not bonded with Si<sup>4+</sup>. The electronic energy levels and
frequencies of local vibrational modes are correlated with specific
Ce–O pairs to provide a comparative understanding of the site-resolved
experimental results. On the basis of the calculated results, we propose
a model of charge transfer and vibronic coupling for interpretation
of the anomalous thermal quenching of the Ce<sup>3+</sup> luminescence.
The combination of experimental and theoretical studies in the present
work provides a comprehensive understanding of the spectroscopy and
luminescence dynamics of Ce<sup>3+</sup> in crystals of ionic–covalent
coordination
Energetic, Optical, and Electronic Properties of Intrinsic Electron-Trapping Defects in YAlO<sub>3</sub>: A Hybrid DFT Study
The formation energies of cation
antisite defects (Y<sub>Al</sub> and Al<sub>Y</sub>), oxygen vacancies
(V<sub>O</sub>), and nearest-neighbor defect complexes (Y<sub>Al</sub>–Al<sub>Y</sub> and Y<sub>Al</sub>–V<sub>O</sub>) in
various charge states in the YAlO<sub>3</sub> crystal are calculated
using density functional theory (DFT) with a modified PBE0 hybrid
functional containing 32% Hartree–Fock (HF) exchange. It is
found that the formation of Y<sub>Al</sub> is more energetically favorable
than Al<sub>Y</sub> under oxygen-poor condition, consistent with the
fact that the latter was not observed in experiments. On the basis
of calculated optical transition energies associated with the excitons
trapped at Y<sub>Al</sub>, V<sub>O</sub>, and Y<sub>Al</sub>–V<sub>O</sub>, the two emission bands observed under excitonic excitation
at low temperature are identified. Electronic properties of Y<sub>Al</sub>–V<sub>O</sub> complexes in the neutral and singly
negative charge states are finally investigated. It shows that the
extra electron added into the negative charge state is mainly localized
at 4d orbitals of Y<sub>Al</sub> with a two-component feature of its
density distribution extending axially along the Y<sub>Al</sub>–V<sub>O</sub> direction
Electronic Structure and Site Occupancy of Lanthanide-Doped (Sr, Ca)<sub>3</sub>(Y, Lu)<sub>2</sub>Ge<sub>3</sub>O<sub>12</sub> Garnets: A Spectroscopic and First-Principles Study
Photoluminescence
excitation (PLE) and emission spectra (PL) of
undoped (Sr, Ca)<sub>3</sub>(Y, Lu)<sub>2</sub>Ge<sub>3</sub>O<sub>12</sub> as well as Eu<sup>3+</sup>- and Ce<sup>3+</sup>-doped samples
have been investigated. The PL spectra show that Eu<sup>3+</sup> enters
into both dodecahedral (Ca, Sr) and octahedral (Y, Lu) sites. Ce<sup>3+</sup> gives two broad excitation bands in the range of 200–450
nm. First-principle calculations for Ce<sup>3+</sup> on both dodecahedral
and octahedral sites provide sets of 5d excited level energies that
are consistent with the experimental results. Then the vacuum referred
binding energy diagrams for (Sr, Ca)<sub>3</sub>(Y, Lu)<sub>2</sub>Ge<sub>3</sub>O<sub>12</sub> have been constructed with the lanthanide
dopant energy levels by utilizing spectroscopic data. The Ce<sup>3+</sup> 5d excited states are calculated by first-principles calculations.
Thermoluminescence (TL) glow curves of (Ce<sup>3+</sup>, Sm<sup>3+</sup>)-codoped (Sr, Ca)<sub>3</sub>(Y, Lu)<sub>2</sub>Ge<sub>3</sub>O<sub>12</sub> samples show a good agreement with the prediction of lanthanide
trapping depths derived from the energy level diagram. Finally, the
energy level diagram is used to explain the low thermal quenching
temperature of Ce<sup>3+</sup> and the absence of afterglow in (Sr,
Ca)<sub>3</sub>(Y, Lu)<sub>2</sub>Ge<sub>3</sub>O<sub>12</sub>
Temperature and Eu<sup>2+</sup>-Doping Induced Phase Selection in NaAlSiO<sub>4</sub> Polymorphs and the Controlled Yellow/Blue Emission
The union of temperature-dependent
phase transition and relating
structural transformation via modification of chemical compositions
is of fundamental importance for the discovery of new materials or
their functional properties optimization. Herein, the synthesis temperature
and Eu<sup>2+</sup>-doping content induced phase selection and variations
of the local structures in nepheline, low-carnegieite and high-carnegieite
types of NaAlSiO<sub>4</sub> polymorphs were studied in detail. The
luminescence of Eu<sup>2+</sup> in low-carnegieite and nepheline phases
shows blue (460 nm) and yellow (540 nm) broad-band emissions, respectively,
under near-ultraviolet excitation. The photoluminescence evolution
can be triggered by the different synthesis temperatures in relation
to the Eu<sup>2+</sup>-doping concentration, as corroborated by density
functional theory calculations on the local coordination structures
and corresponding mechanical stabilities in terms of the Debye temperature.
The fabricated white light-emitting diode device with high color rendering
index demonstrates that the multicolor phosphors from one system provides
a new gateway for the photoluminescence tuning
Mechanical Properties, Electronic Structures, and Potential Applications in Lithium Ion Batteries: A First-Principles Study toward SnSe<sub>2</sub> Nanotubes
First-principles calculations were
carried out to investigate the mechanical and electronic properties
as well as the potential application of SnSe<sub>2</sub> nanotubes.
It was found that the mechanical properties are closely dependent
on diameter and chirality: the Young’s modulus (<i>Y</i>) increases with the enlargement of diameter and converges to the
monolayer limit when the diameter reaches a certain degree; with a
comparable diameter, the armchair nanotube has a larger Young’s
modulus than the zigzag one. The significantly higher Young’s
modulus of SnSe<sub>2</sub> nanotubes with the larger diameter demonstrates
that the deformation does not easily occur, which is beneficial to
the application as anode materials in lithium ion batteries because
a large volume expansion during charge–discharge cycling will
result in serious pulverization of the electrodes and thus rapid capacity
degradation. On the other hand, band structure calculations unveiled
that SnSe<sub>2</sub> nanotubes display a diversity of electronic
properties, which are also diameter- and chirality-dependent: armchair
nanotubes (ANTs) are indirect bandgap semiconductors, and the energy
gaps increase monotonously with the increase of tube diameter, while
zigzag nanotubes (ZNTs) are metals. The metallic SnSe<sub>2</sub> ZNTs
exhibit terrific performance for the adsorption and diffusion of Li
atom, thus they are very promising as anode materials in the Li-ion
batteries
Eu<sup>2+</sup> Site Preferences in the Mixed Cation K<sub>2</sub>BaCa(PO<sub>4</sub>)<sub>2</sub> and Thermally Stable Luminescence
Site preferences of dopant Eu<sup>2+</sup> on the locations of
K<sup>+</sup>, Ba<sup>2+</sup>, and Ca<sup>2+</sup> in the mixed cation
phosphate K<sub>2</sub>BaCaÂ(PO<sub>4</sub>)<sub>2</sub> (KBCP) are
quantitatively analyzed via a combined experimental and theoretical
method to develop a blue-emitting phosphor with thermally stable luminescence.
Eu<sup>2+</sup> ions are located at K2 (M2) and K3 (M3) sites of KBCP,
with the latter occupation relatively more stable than the former,
corresponding to emissions at 438 and 465 nm, respectively. KBCP:Eu<sup>2+</sup> phosphor exhibits highly thermal stable luminescence even
up to 200 °C, which is interpreted as due to a balance between
thermal ionization and recombination of Eu<sup>2+</sup> 5d excited-state
centers with the involvement of electrons trapped at crystal defect
levels. Our results can initiate more exploration of activator site
engineering in phosphors and therefore allow predictive control of
photoluminescence tuning and thermally stable luminescence for emerging
applications in white LEDs
Eu<sup>2+</sup> Site Preferences in the Mixed Cation K<sub>2</sub>BaCa(PO<sub>4</sub>)<sub>2</sub> and Thermally Stable Luminescence
Site preferences of dopant Eu<sup>2+</sup> on the locations of
K<sup>+</sup>, Ba<sup>2+</sup>, and Ca<sup>2+</sup> in the mixed cation
phosphate K<sub>2</sub>BaCaÂ(PO<sub>4</sub>)<sub>2</sub> (KBCP) are
quantitatively analyzed via a combined experimental and theoretical
method to develop a blue-emitting phosphor with thermally stable luminescence.
Eu<sup>2+</sup> ions are located at K2 (M2) and K3 (M3) sites of KBCP,
with the latter occupation relatively more stable than the former,
corresponding to emissions at 438 and 465 nm, respectively. KBCP:Eu<sup>2+</sup> phosphor exhibits highly thermal stable luminescence even
up to 200 °C, which is interpreted as due to a balance between
thermal ionization and recombination of Eu<sup>2+</sup> 5d excited-state
centers with the involvement of electrons trapped at crystal defect
levels. Our results can initiate more exploration of activator site
engineering in phosphors and therefore allow predictive control of
photoluminescence tuning and thermally stable luminescence for emerging
applications in white LEDs
A Theoretical Study on the Structural and Energy Spectral Properties of Ce<sup>3+</sup> Ions Doped in Various Fluoride Compounds
Geometry optimization and wave function-based complete-active-space
self-consistent field-embedded cluster calculations have been performed
for a series of Ce<sup>3+</sup>-doped fluoride compounds (CaF<sub>2</sub>, YF<sub>3</sub>, LaF<sub>3</sub>, KMgF<sub>3</sub>, LiYF<sub>4</sub>, K<sub>2</sub>YF<sub>5</sub>, and KY<sub>3</sub>F<sub>10</sub>) to investigate local coordination structures, crystal field parameters,
and 5d<sup>1</sup> energy-level structures of doping Ce<sup>3+</sup> ions. The crystal-field parameters of Ce<sup>3+</sup> are extracted
from the calculated energies and wave functions. The calculated crystal-field
parameters and 5d<sup>1</sup> energy-level structures show excellent
consistency with the experimental results. Our calculations show that
the onset of 4f → 5d absorption, which is important in phosphors
and scintillators, can be well-predicted. Apart from that, the distortion
of local structure due to doping, the wave functions, and the crystal-field
parameters of 4f<sup>1</sup> and 5d<sup>1</sup> states of Ce<sup>3+</sup> in the hosts can be obtained. Those can seldom be obtained by fitting
empirical crystal-field Hamiltonian to experimental data but are required
by some detailed theoretical analysis, such as the calculation of
transition intensities and hyperfine splittings. The obtained crystal-field
parameters of Ce<sup>3+</sup> may also be useful for other lanthanide
ions in the same hosts