Search results for "Absorption"

Photostimulated emission of KBr—In previously exposed to UV- or X-radiation

1995

Abstract We have performed a photostimulated luminescence (PSL) study of a KBr—In crystal previously irradiated in the exciton fundamental absorption band. It is shown that the PSL arises from three types of close defect pair. It is also shown that one of these three kinds of defect pairs is {F, In2+}, whereas the electron centre of the two other pairs has a more complex nature.

<title>Nature of fundamental absorption edge of WO<formula><inf><roman>3</roman></inf></formula></title&…

1997

The fundamental absorption edge of amorphous, polycrystalline and crystalline tungsten trioxide (WO3) thin films obtained by different techniques (thermal evaporation, rf plasma sputtering, chemical gas transport) was investigated. Special attention was paid to correct measurements of absorption values of all WO3 thin films taking into account the scattered light, interference effects and reflection losses. The indirect edge at 2.70 eV was determined for crystalline WO3, but for crystal WO3:Ti the direct edge in the same place (2.72 eV) was found. For polycrystalline WO3 thin film first edge transition located at 2.76 eV had a quadratic dependence similar to the amorphous film at a higher p…

Optical Properties of Natural and Synthetic Beryl Crystals

2015

The results of investigation of photoluminescence and UV-Visible absorption spectra of natural beryl crystals from Ural Mountains before and after fast neutron irradiation and synthetic crystal grown in Belarus and Russia are presented. Photoluminescence (PL) spectra of synthetic beryl crystals contain a broad band with maxima 740 nm excited both by UV light (λex = 260 nm, 271 nm) and laser excitation (λex =263 nm). This band is connected with Fe 2+ ions. The temperature lowering down to 8 K leads to appearance of narrow lines in the 680 - 720 nm regions. Emission lines observed in the luminescence spectra are connected with electron transition 2 Eg→ 4 A2g of the Cr 3+ ions: R-lines (682.5 …

Transient Optical Absorption and Luminescence in Calcium Tungstate Crystal

2001

<title>Optical properties of hydrogen-containing MgO crystal</title>

2008

The photoluminescence (PL), its excitation (PLE) and absorption spectra in ultraviolet, visible and infrared (UV-VIS-IR) regions were used to investigate the MgO single crystals irradiated by fast neutrons. It is shown that the photoluminescence band of the MgO crystals at 730 nm belongs to the hydrogen-containing complex centers V-OH-Fe3+, which are transformed during the irradiation with fast neutrons. The behavior of the PL band 730 nm after fast neutron irradiation depends on the iron-chromium concentration. It is found that the fast neutron irradiation produces the interstitial proton H+i and the Mg(OH)2 microphase.© (2008) COPYRIGHT SPIE--The International Society for Optical Engineer…

Photostimulated processes in the CsI-Tl crystal after UV irradiation

1997

The photostimulated luminescence is studied for CsI-Tl crystal after irradiation with ultraviolet light in the 80 - 300 K temperature range. The PSL creation spectrum coincides with the D absorption band at 80 K. Three bands are observed in the stimulation spectra at 80 K: 1400, 950, and 600 nm. The 1400 and 950 nm stimulation bands are presumably explained as optical transitions in the Tl 0 and V k centers situated in the spatial correlated pairs. The stimulation at 600 nm band is ascribed to the unperturbed Tl 0 centers.

Emission of real phonons due to electron’s self-dressing in a covalent crystal

2011

A slow monoelectronic excitation in a covalent crystal at the temperature T=0 is analyzed. The interaction with zero-point longitudinal acoustic phonons leads to the formation of a dressed electronic state at an energy level lower than that of the initial bare state. This aspect of the dressing process is described here by hypothesizing that the excess of energy is released with the emission of real phonons. Specifically, this paper considers the transition probability from the bare monoelectronic state to a dressed state of the electron accompanied by real phonons and a deformation field. The spectrum of the real phonons emitted during the electronic self-dressing is calculated by applying…

X-ray-absorption spectroscopy ofNd3+-exchanged β-alumina crystal

1996

The results of x-ray-absorption spectroscopy investigations of ${\mathrm{Nd}}^{3+}$ ions in a nearly fully exchanged (93%) sodium \ensuremath{\beta}-alumina crystal are reported. The ${\mathrm{Nd}}^{3+}$ local environment is reconstructed using a multishell best fit procedure and is compared with existing structural models. The experimental extended x-ray-absorption fine-structure (EXAFS) spectra are also compared with model ab initio FEFF6 calculations based on the x-ray-diffraction data for the ${\mathrm{Nd}}^{3+}$ ions located at the BR(2d) and interstitial A(6h) sites of \ensuremath{\beta}-alumina. Neodymium ions are mainly found near the BR(2d) sites of the conduction plane, where they…

Factors affecting the UV-Transparency of Molecular Sieves

1994

The optical properties in the UV-region of several types of molecular sieves were studied. The initial onset of absorption around 280 nm which was observed for basically all samles synthesized without special precautions is not due to an early onset of band gap absorption, but might be correlated to the crystal size as well as structural defects within the crystals, e.g. E'-center or peroxy-radical. Using template free synthesis procedures which lead to small crystals containing few defect sites, we were able to synthesize molevular sieves which were almost completely transparent down to 200 nm. Such crystals can become very important in the development of technical luminophores.

Ab initio calculations of the Ni K ‐edge XANES in Ni c Mg 1‐c O solid solutions

2005

An interpretation of the Ni K-edge X-ray absorption near edge structure (XANES) in pure NiO and NicMg1-cO solid solutions is given based on three types of ab initio theoretical calculations: the full-multiple-scattering (FMS) approach, the finite difference method (FDM) and the full potential linear muffin-tin orbital (FP-LMTO) method within the LSDA+U approach. The first two methods differ in the cluster potential approximation: the spherically symmetric muffin-tin potential is used in the FMS approach, whereas a non-muffin-tin numerical potential makes the core of the FDM. We found that the FMS and FDM techniques allow rather accurate description of the experimental XANES signal especiall…