9 research outputs found
Role of Synthesis Method on Luminescence Properties of Europium(II, III) Ions in β‑Ca<sub>2</sub>SiO<sub>4</sub>: Probing Local Site and Structure
The europium ion
probes the symmetry disorder in the crystal structure, although the
distortion due to charge compensation in the case of aliovalent dopant
remains interesting, especially preparation involves low and high
temperatures. This work studies the preparation of the β-Ca<sub>2</sub>SiO<sub>4</sub> (from here on C<sub>2</sub>S) particle from
Pechini (C<sub>2</sub>SP) and hydrothermal (C<sub>2</sub>SH) methods,
and its luminescence variance upon doping with Eu<sup>2+</sup> and
Eu<sup>3+</sup> ions. The blue shift of the charge-transfer band (CTB)
in the excitation spectra indicates a larger Eu<sup>3+</sup>–O<sup>2–</sup> distance in Eu<sup>3+</sup> doped C<sub>2</sub>SH.
The changes in vibrational frequencies due to stretching and bending
vibrations in the FTIR and the Raman spectra and binding energy shift
in the XPS analysis confirmed the distorted SiO<sub>4</sub><sup>4–</sup> tetrahedra in C<sub>2</sub>SH. The high hydrothermal temperature
and pressure produce distortion, which leads to symmetry lowering
although doping of aliovalent ion may slightly change the position
of the Ca atoms. The increasing asymmetry ratio value from C<sub>2</sub>SP to C<sub>2</sub>SH clearly indicates that the europium ion stabilized
in a more distorted geometry. It is also supported by Judd–Ofelt
analysis. The concentration quenching and site-occupancy of Eu<sup>3+</sup> ions in two nonequivalent sites of C<sub>2</sub>S were discussed.
The charge state and concentration of europium ions in C<sub>2</sub>SP and C<sub>2</sub>SH were determined using X-ray photoelectron
spectroscopy measurements. The C<sub>2</sub>S particles were studied
by X-ray powder diffraction, FTIR, Raman, BET surface area, TGA/DTA,
electron microscopy, XPS, and luminescence spectroscopy. The impact
of citrate ion on the morphology and particle size of C<sub>2</sub>SH has been hypothesized on the basis of the microscopy images. This
study provides insights that are needed for further understanding
the structure of C<sub>2</sub>S and thereby improves the applications
in optical and biomedical areas and cement hydration
Preparation and Optical Properties of Nd:Bi<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> Laser Crystal with Disordered Structure and Attractive Multiwavelength Emission Characteristics
Laser crystals with multiwavelength emission characteristics
are
potential light sources for terahertz radiation. Herein, the pure
and Nd-doped Bi2Ti2O7 (BTO) laser
crystals with sizes up to 16 × 13 × 5 mm3 were
successfully grown using the flux method in the KF-B2O3–CaBi4Ti4O15 growth
system. The crystal structure, ideal morphology, chemical, mechanical,
and thermal properties, optical transmission and Raman spectra, refractive
index, absorption, and fluorescence spectra, as well as fluorescence
lifetimes, were systematically studied. Besides, the spectral parameters
of Nd3+ ions in the BTO crystal were systematically calculated
based on the Judd–Ofelt theory. The Nd:BTO crystal has a wide
transmittance range (0.44–7.30 μm), a small coefficient
of thermal expansion (5.80 × 10–6 K–1), and a large absorption full width at half-maximum (fwhm) (31.2
nm) at around ∼804 nm, making it more potential for use in
high-power laser systems. Moreover, fluorescence spectra show four
emission peaks at 1054, 1062, 1104, and 1112 nm. The strong multiwavelength
emission property makes Nd:BTO a promising laser crystal, serving
as a potential light source for terahertz radiation
Preparation and Optical Properties of Nd:Bi<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> Laser Crystal with Disordered Structure and Attractive Multiwavelength Emission Characteristics
Laser crystals with multiwavelength emission characteristics
are
potential light sources for terahertz radiation. Herein, the pure
and Nd-doped Bi2Ti2O7 (BTO) laser
crystals with sizes up to 16 × 13 × 5 mm3 were
successfully grown using the flux method in the KF-B2O3–CaBi4Ti4O15 growth
system. The crystal structure, ideal morphology, chemical, mechanical,
and thermal properties, optical transmission and Raman spectra, refractive
index, absorption, and fluorescence spectra, as well as fluorescence
lifetimes, were systematically studied. Besides, the spectral parameters
of Nd3+ ions in the BTO crystal were systematically calculated
based on the Judd–Ofelt theory. The Nd:BTO crystal has a wide
transmittance range (0.44–7.30 μm), a small coefficient
of thermal expansion (5.80 × 10–6 K–1), and a large absorption full width at half-maximum (fwhm) (31.2
nm) at around ∼804 nm, making it more potential for use in
high-power laser systems. Moreover, fluorescence spectra show four
emission peaks at 1054, 1062, 1104, and 1112 nm. The strong multiwavelength
emission property makes Nd:BTO a promising laser crystal, serving
as a potential light source for terahertz radiation
Legislative Documents
Also, variously referred to as: House bills; House documents; House legislative documents; legislative documents; General Court documents
Different views of the casting mold sherd.
<p>(A-F) Six faces of the casting mold sherd.</p
EDS results of the elemental analysis of the casting mold sherd.
<p>EDS results of the elemental analysis of the casting mold sherd.</p
Map of the Shang Dynasty and location of Daxinzhuang.
<p>Both Yin Ruins and Daxinzhuang sites are marked in the map. Reprinted from [<a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0174057#pone.0174057.ref011" target="_blank">11</a>] under a CC BY license, with permission from [Lamassu Design], original copyright [2009].</p
AMS-<sup>14</sup>C dating of archaeological pig bone.
<p>AMS-<sup>14</sup>C dating of archaeological pig bone.</p
X-ray fluorescence mapping of copper and iron mapping in front decoration and back groove.
<p>(A) A groove is labelled by a white rectangle on the back of the casting mold sherd. One red dashed line indicates the deepest position in the groove. (B) X-ray fluorescence mapping of the copper on the back and a white dashed line encircles the groove. (C) X-ray fluorescence mapping of the iron on the back and a black dashed line encircles the groove. One side of the deepest line shows a gathering of iron, and on the other side, this reverses. (D) A probing range is labelled by a white rectangle on the front of the casting mold sherd. (E), (F) X-ray fluorescence mapping on the front decoration of copper and iron, respectively. Both elements have an uneven distribution and some correspondence to the profile of decorated patterns.</p