29 research outputs found
Thermal and luminescent properties of M2Zn(VO3) 4 (M = Rb, Cs)
We have developed processes for the synthesis of the Rb 2Zn(VO3)4 and Cs2Zn(VO 3)4 tetrametavanadates. Rb2Zn(VO 3)4 has been prepared by solid-state reaction (350 C) between presynthesized RbVO3 and ZnV2O6 powders, and Cs2Zn(VO3)4 has been prepared by the Pechini method (sol-gel process). Both metavanadates crystallize in monoclinic symmetry (sp. gr. P21/m). Thermochemical characterization results demonstrate that the vanadates undergo complex transformations during heating to 450 C and subsequent cooling. As a result, the materials are in a nonequilibrium state at room temperature and consist of both the parent double metavanadates and their peritectic decomposition products. We believe that the formation of the structure of the M2Zn(VO3)4 compounds from their melts is a kinetically hindered process. These compounds are structurally stable only at temperatures below 369 (Rb2Zn(VO 3)4) or 420 C (Cs2Zn(VO3) 4). We have measured for the first time the diffuse reflectance and photoluminescence excitation spectra of the two tetrametavanadates in their emission range and their photoluminescence spectra at various excitation wavelengths and determined their chromaticity coordinates. Their X-ray luminescence and scintillation decay characteristics have been determined for the first time under pulsed electron beam excitation. The electron excitation dissipation processes in the cesium and rubidium compounds are shown to be similar. We discuss the origin of the emission bands in the mixed vanadates and their potential application areas. Β© 2013 Pleiades Publishing, Ltd
Time-Resolved Vacuum Ultraviolet Spectroscopy of Er3+ ions in the SrF2 Crystal
The photoluminescence and photoexcitation spectra as well as the luminescence decay kinetics of Er3+ ions in the visible ultraviolet and vacuum ultraviolet (VUV) regions have been studied by the method of low-temperature, time-resolved VUV-spectroscopy on excitation by synchrotron radiation. In the VUV spectral region of the luminescence of SrF2:1% Er3+, the 146.5-nm band with a time of decay of less than 0.6 nsec was revealed together with the well-known emission band at 164.3 nm (decay constant in the microsecond range). Its possible nature is discussed. The specific features of the formation of photoexcitation spectra of the f-f and f-d transitions in the Er3+ ion are considered. Competition between the processes of excitation of f-f and d-f luminescence has been revealed. It manifests itself in the inverse relationship of their photoexcitation spectra in a range of energies of incident photons that are close to the position of the 4fn-15d configuration levels. Β© 2005 Springer Science+Business Media, Inc.This work was carried out with the support of grants from the Russian Fundamental Research Foundation (05-02-16530), "Universities of Russia (UR 02.01.433), Ural Scientific Center Promising Materials" CRDF (EK-005-XI), and partially from BMBF (05KS8GMD/1)
Vacuum Ultraviolet Excitation of Rare-Earth ion Luminescence in Strontium Fluoride Crystals
The photoexcitation spectra (70-280 nm) of the Eu 3+, Tb 3+, Dy 3+, Er 3+, and Tm 3+ ion luminescence in strontium fluoride crystals are studied at 8 and 295 K by vacuum ultraviolet spectroscopy using synchrotron-radiation excitation. The processes of transfer of the excitation energy to the impurity centers as well as the relaxation mechanisms of the excited high-energy states of the rare-earth ions are analyzed. The bands corresponding to the interconfiguration 4f-5d transitions and the charge-transfer bands are identified in the photoexcitation luminescence spectra. Β©2005 Springer Science+Business Media, Inc.The present work was supported in part by the Russian Foundation for Basic Research (Grant 05-02-16530), by the Program βRussian Universitiesβ (Grant UR.02.01.433), by REC-005 (ΠΠ-005-XI), and BMBF (05KS8GMD/1)
Structure and luminescent properties of Cs2Sr(VO3)(4): Mn2+
We have developed a procedure for thermally stimulated synthesis of a cesium strontium metavanadate, Cs 2Sr(VO 3) 4:Mn 2+ (0.01, 0.50, 1.00, 5.00 at % Mn 2+), using MnO-containing starting mixtures. The EPR spectrum of the material containing 0.01 at % Mn 2+ shows a hyperfine structure due to the incorporation of a small amount of manganese into the diamagnetic double metavanadate host. The luminescent and optical properties of Cs 2Sr(VO 3) 4:Mn 2+ depend on manganese content. In contrast to higher doping levels, doping with 0.01 at % Mn 2+ increases the integrated emission intensity of the vanadate by 10% and improves its chromaticity characteristics (approaching them to those of white light). We assume that this is due to the reduction in the density of vacancy-type growth defects, such as oxygen vacancies. Β© Pleiades Publishing, Ltd., 2012
Spacer-armed copper(ii) complexes with benzenecarboxylic acids and trifluoroacetylacetone aroylhydrazones
RESEARCHING THE PROCESS OF HOLLOW PROFILE SETTING- PRESSING OF A COMPOSITE MATERIAL BASED ON METALLIC POWDERS
The paper presents the researching processes of hollow profile setting-pressing of a composite material based on "iron-copper" metallic powders and the improving of the quality by increas- ing the homogeneity of properties
INORGANIC SCINTILLATOR
FIELD: selective detection and displaying of heavy-density pulse electron beams in background Ξ±-, Ξ²-, Ξ³ radiation of nuclides, in particular, for electron beams generated by heavy-current amplifiers of electrons. SUBSTANCE: method involves usage of semiconductor crystals of HgI2 (red tetragonal modification) as inorganic scintillator.EFFECT: increased efficiency for detection of heavy-density electron beams, practical insensitivity to Ξ±-, Ξ²-, Ξ³- radiation of nuclides.ΠΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅: Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΈΠ·Π±ΠΈΡΠ°ΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ Π΄Π΅ΡΠ΅ΠΊΡΠΎΡΠ° Π΄Π»Ρ Π²ΠΈΠ·ΡΠ°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΈ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠΉ ΡΠ΅Π³ΠΈΡΡΡΠ°ΡΠΈΠΈ ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΡΡ
ΠΏΡΡΠΊΠΎΠ² ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ² Π²ΡΡΠΎΠΊΠΎΠΉ ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΠΈ Π½Π° ΡΠΎΠ½Π΅ Ξ±-, Ξ²-, Ξ³ - ΡΠ΄Π΅ΡΠ½ΡΡ
ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΠΉ ΡΠ°Π΄ΠΈΠΎΠ½ΡΠΊΠ»ΠΈΠ΄ΠΎΠ² Π² ΡΠ°ΡΡΠ½ΠΎΡΡΠΈ, Π΄Π»Ρ Π²ΠΈΠ·ΡΠ°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΈ ΡΠ΅Π³ΠΈΡΡΡΠ°ΡΠΈΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΡ
ΠΏΡΡΠΊΠΎΠ², ΡΠΎΠ·Π΄Π°Π²Π°Π΅ΠΌΡΡ
ΡΠΈΠ»ΡΠ½ΠΎΡΠΎΡΠ½ΡΠΌΠΈ ΡΡΠΊΠΎΡΠΈΡΠ΅Π»ΡΠΌΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ² Π½Π°Π½ΠΎ- ΠΈ ΠΏΠΈΠΊΠΎΡΠ΅ΠΊΡΠ½Π΄Π½ΠΎΠ³ΠΎ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π°. Π‘ΡΡΠ½ΠΎΡΡΡ ΠΈΠ·ΠΎΠ±ΡΠ΅ΡΠ΅Π½ΠΈΡ: ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΈΠ·Π²Π΅ΡΡΠ½ΡΡ
ΠΏΠΎΠ»ΡΠΏΡΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠΎΠ²ΡΡ
ΠΊΡΠΈΡΡΠ°Π»Π»ΠΎΠ² ΠΈΠΎΠ΄ΠΈΠ΄Π° ΡΡΡΡΠΈ HgI2 (ΠΊΡΠ°ΡΠ½ΠΎΠΉ ΡΠ΅ΡΡΠ°Π³ΠΎΠ½Π°Π»ΡΠ½ΠΎΠΉ ΠΌΠΎΠ΄ΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ) Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ Π½Π΅ΠΎΡΠ³Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΡΠΈΠ½ΡΠΈΠ»Π»ΡΡΠΎΡΠ°, ΠΎΠ±Π»Π°Π΄Π°ΡΡΠ΅Π³ΠΎ Π²ΡΡΠΎΠΊΠΎΠΉ ΡΡΠΈΠ½ΡΠΈΠ»Π»ΡΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡΡ CΠΎΡΠ½ ΠΏΡΠΈ ΡΠ΅Π³ΠΈΡΡΡΠ°ΡΠΈΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΡ
ΠΏΡΡΠΊΠΎΠ² Π²ΡΡΠΎΠΊΠΎΠΉ ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΠΈ ΠΈ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈ Π½Π΅ ΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΠΊΠ°ΠΊ ΡΡΠΈΠ½ΡΠΈΠ»Π»ΡΡΠΎΡ ΠΊ ΡΠ΄Π΅ΡΠ½ΡΠΌ Ξ±-, Ξ²-, Ξ³- ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡΠΌ ΡΠ°Π΄ΠΈΠΎΠ½ΡΠΊΠ»ΠΈΠ΄ΠΎΠ²
METHOD OF COLORING NATURAL BERYL CRYSTALS AND ARTICLES MADE THEREFROM
FIELD: gem treatment. SUBSTANCE: method of coloring natural beryl crystals and articles (jeweler's insertions) to improve their color (simulation of emerald) involves irradiation of natural beryl crystals with ionizing radiation and heat treatment and is distinguished with that thermally treated crystals are submitted to a secondary irradiation, the both irradiation steps being effected with 6-8 MeV electron beam at fluency 10 15-2,5β’1016 electrons per 1 sq.cm, whereas heat treatment is carried out via slow heating and cooling (2-2.5 deg./h) and exposure to 160-170 C for 1-2 h. EFFECT: improved quality of color.ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ ΡΠΏΠΎΡΠΎΠ± ΠΎΠΊΡΠ°ΡΠΈΠ²Π°Π½ΠΈΡ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΎΠ² ΠΏΡΠΈΡΠΎΠ΄Π½ΠΎΠ³ΠΎ Π±Π΅ΡΠΈΠ»Π»Π° ΠΈ ΠΈΠ·Π΄Π΅Π»ΠΈΠΉ ΠΈΠ· Π½ΠΈΡ
/ΡΠ²Π΅Π»ΠΈΡΠ½ΡΡ
Π²ΡΡΠ°Π²ΠΎΠΊ/ Π΄Π»Ρ ΡΠ»ΡΡΡΠ΅Π½ΠΈΡ ΠΊΠ°ΡΠ΅ΡΡΠ²Π° ΠΈΡ
ΠΎΠΊΡΠ°ΡΠΊΠΈ - ΠΎΠΊΡΠ°ΡΠΈΠ²Π°Π½ΠΈΡ ΠΏΠΎΠ΄ ΠΈΠ·ΡΠΌΡΡΠ΄. Π‘ΠΏΠΎΡΠΎΠ± Π²ΠΊΠ»ΡΡΠ°Π΅Ρ ΠΎΠ±Π»ΡΡΠ΅Π½ΠΈΠ΅ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΎΠ² ΠΏΡΠΈΡΠΎΠ΄Π½ΠΎΠ³ΠΎ Π±Π΅ΡΠΈΠ»Π»Π° ΠΈΠΎΠ½ΠΈΠ·ΠΈΡΡΡΡΠΈΠΌ ΠΈ ΠΈΡ
ΡΠ΅ΡΠΌΠΎΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΡ ΠΈ ΠΎΡΠ»ΠΈΡΠ°Π΅ΡΡΡ ΡΠ΅ΠΌ, ΡΡΠΎ ΡΠ΅ΡΠΌΠΎΠΎΠ±ΡΠ°Π±ΠΎΡΠ°Π½Π½ΡΠ΅ ΠΊΡΠΈΡΡΠ°Π»Π»Ρ ΠΏΠΎΠ΄Π²Π΅ΡΠ³Π°ΡΡ Π²ΡΠΎΡΠΈΡΠ½ΠΎΠΌΡ ΠΎΠ±Π»ΡΡΠ΅Π½ΠΈΡ, ΠΏΡΠΈΡΠ΅ΠΌ ΠΏΠ΅ΡΠ²ΠΈΡΠ½ΠΎΠ΅ ΠΈ Π²ΡΠΎΡΠΈΡΠ½ΠΎΠ΅ ΠΎΠ±Π»ΡΡΠ΅Π½ΠΈΠ΅ ΠΏΡΠΎΠ²ΠΎΠ΄ΡΡ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΠΌ ΠΏΡΡΠΊΠΎΠΌ Ρ ΡΠ½Π΅ΡΠ³ΠΈΠ΅ΠΉ 6-8 ΠΡΠ ΠΈ ΡΠ»ΡΠ΅Π½ΡΠΎΠΌ 1015 - 2,5 β’ 1016 ΡΠ»Π΅ΠΊΡΡΠΎΠ½ /ΡΠΌ2/ ΠΏΡΠΈ ΠΊΠ°ΠΆΠ΄ΠΎΠΌ ΠΎΠ±Π»ΡΡΠ΅Π½ΠΈΠΈ/, Π° ΡΠ΅ΡΠΌΠΎΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΡ Π²Π΅Π΄ΡΡ ΠΌΠ΅Π΄Π»Π΅Π½Π½ΡΠΌ Π½Π°Π³ΡΠ΅Π²ΠΎΠΌ ΠΈ ΠΎΡ
Π»Π°ΠΆΠ΄Π΅Π½ΠΈΠ΅ΠΌ /2-2,5 Π³ΡΠ°Π΄/ΡΠ°Ρ/ Ρ Π²ΡΠ΄Π΅ΡΠΆΠΊΠΎΠΉ ΠΏΡΠΈ 160-170oC Π² ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ 1-2 ΡΠ°ΡΠΎΠ²