26 research outputs found
Insight into the Relationship between Crystal Structure and Crystal-Field Splitting of Ce<sup>3+</sup> Doped Garnet Compounds
The common understanding
of the negative relationship between bond
lengths and crystal-field splitting (CFS) is renewed by Ce<sup>3+</sup> doped garnets in this work. We represent the contradictory relationship
between structure data and spectroscopic crystal-field splitting in
detail. A satisfactory explanation is given by expressing crystal-field
splitting in terms of crystal-field parameters, on the basis of structural
data. The results show that not only the bond length, but also the
geometrical configuration have influence on the magnitude of crystal-field
splitting. Also it is found that the ligand oxygen behaves differently
with regard to multiple site substitution in garnet structure
Host Dependency of Boundary between Strong and Weak Crystal Field Strength of Cr<sup>3+</sup> Luminescence
Cr3+ doped near-infrared phosphors hold significant
applications and generate considerable research interest. The critical
parameter for assessing the strength of the crystal field for Cr3+ in the Tanabe–Sugano diagram is the boundary value
of Dq/B, representing the ratio of crystal field splitting to the
Racah parameter B. Nevertheless, there are conflicting values for
this parameter, as reported in various studies, such as 2.1, 2.2,
and 2.3 for C/B = 4.5–4.8. Moreover, some Cr3+ doped
phosphors with wide-band emissions exhibit a Dq/B value that falls
within the region of a contradictory strong field. In this study,
we numerically determine the boundary value of Dq/B, which distinguishes
between strong and weak fields. The results then demonstrate a dependence
on the host material and are correlated with the values of Racah parameters
B and C. This work resolves the inconsistency between the boundary
values of Dq/B and the emission profile of Cr3+, providing
researchers with a more profound comprehension of Cr3+ luminescence
Insight into the Controlled Synthesis of Cu<sub>2</sub>Zn(Ge,Sn)S<sub>4</sub> Nanoparticles with Selective Grain Size
Controlled synthesis of
absorber materials Cu<sub>2</sub>ZnGeS<sub>4</sub> (CZGS) has been
performed using different Ge precursors, including GeCl<sub>4</sub> and the self-synthesized Ge complexes with Ge-glycolic acid (denoted
as Ge-Gly), Ge-tartaric acid (denoted as Ge-Tar), and Ge-citric acid
(denoted as Ge-Cit). The grain size of as-prepared CZGS nanocrystals
(NCs) is dependent on the Ge precursors. All four Ge precursors enabled
the wurtzstannite CZGS phase formation. The Ge-Cit precursor led to
the formation of monodispersed NCs owing to the fact that the undissolved
metal-Cit complex in OLA absorbed the small CZSG NCs and avoided the
irregular crystalline behavior. The other three precursors induced
two different sizes, and the corresponding reaction mechanism has
been proposed. Moreover, the Cu<sub>2</sub>ZnGe<sub>1–<i>x</i></sub>Sn<sub><i>x</i></sub>S<sub>4</sub> NCs
with different Ge/Sn ratios were prepared using the Ge-Cit precursor,
verifying the general effect on the phase formation and selective
grain sizes. The compositional effect on the band gap variation and
morphologies of Cu<sub>2</sub>ZnGe<sub>1–<i>x</i></sub>Sn<sub><i>x</i></sub>S<sub>4</sub> was also studied
Controllable Synthesis and Optical Properties of ZnS:Mn<sup>2+</sup>/ZnS/ZnS:Cu<sup>2+</sup>/ZnS Core/Multishell Quantum Dots toward Efficient White Light Emission
The
ability to control dopants and defects, as well as the core/shell
structures, of quantum dots (QDs) is an essential nanotechnology to
modify and optimize their photoluminescence properties. Herein, the
optimized ZnS:Mn<sup>2+</sup>/ZnS/ZnS:Cu<sup>2+</sup>/ZnS core/multishell
QDs have been prepared, and their luminescence properties depending
on the ratios of the starting materials and the injection temperature
of an extra sulfur source were discussed; finally the white light
can be possibly obtained by mixing the blue light (emission peak at
450 nm originating from Cu<sup>2+</sup> dopants or emission peaks
at 405 and 430 nm corresponding to a defect emission center) and orange
light (emission peak at 585 nm from Mn<sup>2+</sup> dopants). As a
controlled synthesis comparison, the optimum core/shell structures
and key synthesis parameters have been determined, and the quantum
yield (QY) of the as-obtained ZnS:Mn<sup>2+</sup>/ZnS/ZnS:Cu<sup>2+</sup>/ZnS core/multishell white light emitting QDs without defect emission
was determined to be 38%. The practical white light device prototype
has been also fabricated and the CIE color coordinate of (0.32, 0.34)
with a warm white light has been realized upon the excitation of the
commercial 370 nm UV LED chip, which demonstrated potential application
for micro/nano optical functional devices
Ethylenediamine-Assisted Hydrothermal Synthesis of NaCaSiO<sub>3</sub>OH: Controlled Morphology, Mechanism, and Luminescence Properties by Doping Eu<sup>3+</sup>/Tb<sup>3+</sup>
This
paper demonstrates a facile hydrothermal method using ethylenediamine
(EDA) as a “shape modifier” for the controlled synthesis
of rod bunch, decanedron, spindle, flakiness, and flowerlike NaCaSiO<sub>3</sub>OH microarchitectures. The set of experimental conditions
is important to obtain adjustable shape and size of NaCaSiO<sub>3</sub>OH particles, as the change in either the amount of EDA/H<sub>2</sub>O or reaction time, or the amount of NaOH. Accordingly, the crystal
growth mechanism during the synthesis process is proposed, and it
is found that the EDA, acting as the chelating agent and shape modifier,
plays a crucial role in fine-tuning the NaCaSiO<sub>3</sub>OH morphology.
Morphology evolution process of flowerlike NaCaSiO<sub>3</sub>OH as
a function of NaOH is also explained in detail. Eu<sup>3+</sup>/Tb<sup>3+</sup> doped NaCaSiO<sub>3</sub>OH samples exhibit strong red and
green emission under ultraviolet excitation, corresponding to the
characteristic electronic transitions of Eu<sup>3+</sup> and Tb<sup>3+</sup>. These results imply
that the morphology-tunable NaCaSiO<sub>3</sub>OH:Eu<sup>3+</sup>/Tb<sup>3+</sup> microarchitectures with tunable luminescence properties
are expected to have promising applications for micro/nano optical
functional devices
Luminescence Tuning, Thermal Quenching, and Electronic Structure of Narrow-Band Red-Emitting Nitride Phosphors
Exploring
high-performance narrow-band red-emitting phosphor is an important
challenge for improving white light LEDs. Here, on the basis of three
interesting nitride phosphors with similar vierer rings framework
structure, two phosphor series, Eu<sup>2+</sup>-doped Sr(LiAl)<sub>1–<i>x</i></sub>Mg<sub>2<i>x</i></sub>Al<sub>2</sub>N<sub>4</sub> and Sr(LiAl<sub>3</sub>)<sub>1–<i>y</i></sub>(Mg<sub>3</sub>Si)<sub><i>y</i></sub>N<sub>4</sub> (<i>x</i>, <i>y</i> = 0–1), are
successfully synthesized by a solid state reaction. They show narrow-band
red emission with tunable emission peaks from 614 to 658 nm and 607
to 663 nm. The varying luminescence behaviors with composition and
structure are discussed based on centroid shift, crystal field splitting
and Stokes shift. On the basis of experimental data, we construct
the host referred binding energy (HRBE) and vacuum referred binding
energy (VRBE) schemes of divalent/trivalent lanthanide-doped end-member
compounds, and further give thermal quenching mechanism of these series
phosphors
Structural Phase Transformation and Luminescent Properties of Ca<sub>2–<i>x</i></sub>Sr<sub><i>x</i></sub>SiO<sub>4</sub>:Ce<sup>3+</sup> Orthosilicate Phosphors
The
orthosilicate phosphors demonstrate great potential in the field of
solid-state lighting, and the understanding of the structure–property
relationships depending on their versatile polymorphs and chemical
compositions is highly desirable. Here we report the structural phase
transformation of Ca<sub>2–<i>x</i></sub>Sr<sub><i>x</i></sub>SiO<sub>4</sub>:Ce<sup>3+</sup> phosphor by Sr<sup>2+</sup> substituting for Ca<sup>2+</sup> within 0 ≤ <i>x</i> < 2. The crystal structures of Ca<sub>2–<i>x</i></sub>Sr<sub><i>x</i></sub>SiO<sub>4</sub>:Ce<sup>3+</sup> are divided into two groups, namely, β phase (0 ≤ <i>x</i> < 0.15) and α′ phase (0.18 ≤ <i>x</i> < 2), and the phase transition (β → α′)
mechanism originated from the controlled chemical compositions is
revealed. Our findings verified that the phase transition <i>Pnma</i> (α′-phase) ↔ <i>P</i>2<sub>1</sub>/<i>n</i> (β-phase) can be ascribed
to the second-order type, and Sr<sup>2+</sup> ions in Ca<sub>2–<i>x</i></sub>Sr<sub><i>x</i></sub>SiO<sub>4</sub> preferentially
occupy the seven-coordinated Ca<sup>2+</sup> sites rather than the
eight-coordinated sites with increasing Sr<sup>2+</sup> content, which
was reflected from the Rietveld refinements and further clarified
through the difference of the Ca–O bond length in the two polymorphs
of Ca<sub>2</sub>SiO<sub>4</sub>. The emission peaks of Ce<sup>3+</sup> shift from 417 to 433 nm in the composition range of 0 ≤ <i>x</i> ≤ 0.8, and the difference in the decay curves can
also verify the phase transformation process. Thermal quenching properties
of selected Ca<sub>2–<i>x</i></sub>Sr<sub><i>x</i></sub>SiO<sub>4</sub>:Ce<sup>3+</sup> samples were evaluated,
and the results show that the integral emission intensities at 200
°C maintain >90% of that at room temperature suggesting superior
properties for the application as white light-emitting diodes (w-LEDs)
phosphors
Near-Infrared Luminescence and Color Tunable Chromophores Based on Cr<sup>3+</sup>-Doped Mullite-Type Bi<sub>2</sub>(Ga,Al)<sub>4</sub>O<sub>9</sub> Solid Solutions
Cr<sup>3+</sup>-activated mullite-type Bi<sub>2</sub>Ga<sub>(4‑<i>x</i>)</sub>Al<sub><i>x</i></sub>O<sub>9</sub> (<i>x</i> = 0, 1, 2, 3, and 4) solid solutions were prepared
by the solid state reaction, and their spectroscopic properties were
investigated in conjunction with the structural evolution. Under excitation
at 610 nm, Bi<sub>2</sub>[Ga<sub>(4‑<i>y</i>)</sub>Al<sub><i>y</i></sub>]<sub>3.97</sub>O<sub>9</sub>:0.03Cr<sup>3+</sup> (<i>y</i> = 0, 1, 2, 3, and 4) phosphors
exhibited broad-band near-infrared (NIR) emission peaking at ∼710
nm in the range 650–850 nm, and the optimum Cr<sup>3+</sup> concentrations and concentration quenching mechanism were determined.
Except for the interesting NIR emission, the body color changed from
white (at <i>x</i> = 0) to green (at <i>x</i> =
0.08) for Bi<sub>2</sub>Ga<sub>4–<i>x</i></sub>O<sub>9</sub>:<i>x</i>Cr<sup>3+</sup>, and from light yellow
(at <i>x</i> = 0) to deep brown (at <i>x</i> =
0.08) for Bi<sub>2</sub>Al<sub>4–<i>x</i></sub>O<sub>9</sub>:<i>x</i>Cr<sup>3+</sup>, respectively. Moreover,
as a result of variable Al/Ga ratio, the observed body color for Bi<sub>2</sub>[Ga<sub>(4‑<i>y</i>)</sub>Al<sub><i>y</i></sub>]<sub>3.97</sub>O<sub>9</sub>:0.03Cr<sup>3+</sup> (<i>y</i> = 0, 1, 2, 3, and 4) varied from deep brown
to green. The relationship between the observed colors and their diffuse
reflectance spectra were also studied for the understanding of the
different absorption bands. The results indicated that Cr<sup>3+</sup>-doped Bi<sub>2</sub>Ga<sub>(4‑<i>x</i>)</sub>Al<sub><i>x</i></sub>O<sub>9</sub> solid solutions appeared as
the bifunctional materials with NIR phosphors and color-tunable pigments
Near-Infrared Luminescence and Color Tunable Chromophores Based on Cr<sup>3+</sup>-Doped Mullite-Type Bi<sub>2</sub>(Ga,Al)<sub>4</sub>O<sub>9</sub> Solid Solutions
Cr<sup>3+</sup>-activated mullite-type Bi<sub>2</sub>Ga<sub>(4‑<i>x</i>)</sub>Al<sub><i>x</i></sub>O<sub>9</sub> (<i>x</i> = 0, 1, 2, 3, and 4) solid solutions were prepared
by the solid state reaction, and their spectroscopic properties were
investigated in conjunction with the structural evolution. Under excitation
at 610 nm, Bi<sub>2</sub>[Ga<sub>(4‑<i>y</i>)</sub>Al<sub><i>y</i></sub>]<sub>3.97</sub>O<sub>9</sub>:0.03Cr<sup>3+</sup> (<i>y</i> = 0, 1, 2, 3, and 4) phosphors
exhibited broad-band near-infrared (NIR) emission peaking at ∼710
nm in the range 650–850 nm, and the optimum Cr<sup>3+</sup> concentrations and concentration quenching mechanism were determined.
Except for the interesting NIR emission, the body color changed from
white (at <i>x</i> = 0) to green (at <i>x</i> =
0.08) for Bi<sub>2</sub>Ga<sub>4–<i>x</i></sub>O<sub>9</sub>:<i>x</i>Cr<sup>3+</sup>, and from light yellow
(at <i>x</i> = 0) to deep brown (at <i>x</i> =
0.08) for Bi<sub>2</sub>Al<sub>4–<i>x</i></sub>O<sub>9</sub>:<i>x</i>Cr<sup>3+</sup>, respectively. Moreover,
as a result of variable Al/Ga ratio, the observed body color for Bi<sub>2</sub>[Ga<sub>(4‑<i>y</i>)</sub>Al<sub><i>y</i></sub>]<sub>3.97</sub>O<sub>9</sub>:0.03Cr<sup>3+</sup> (<i>y</i> = 0, 1, 2, 3, and 4) varied from deep brown
to green. The relationship between the observed colors and their diffuse
reflectance spectra were also studied for the understanding of the
different absorption bands. The results indicated that Cr<sup>3+</sup>-doped Bi<sub>2</sub>Ga<sub>(4‑<i>x</i>)</sub>Al<sub><i>x</i></sub>O<sub>9</sub> solid solutions appeared as
the bifunctional materials with NIR phosphors and color-tunable pigments