scholarly journals Dielectric tensor of monoclinic Ga2O3 single crystals in the spectral range 0.5–8.5 eV

APL Materials ◽  
2015 ◽  
Vol 3 (10) ◽  
pp. 106106 ◽  
Author(s):  
C. Sturm ◽  
J. Furthmüller ◽  
F. Bechstedt ◽  
R. Schmidt-Grund ◽  
M. Grundmann
2017 ◽  
Vol 111 (8) ◽  
pp. 082102 ◽  
Author(s):  
C. Sturm ◽  
R. Schmidt-Grund ◽  
V. Zviagin ◽  
M. Grundmann

2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Viktorija Pankratova ◽  
Anna P. Kozlova ◽  
Oleg A. Buzanov ◽  
Kirill Chernenko ◽  
Roman Shendrik ◽  
...  

AbstractCerium doped Gd3Ga3Al2O12 (GGAG) single crystals as well as GGAG:Ce single crystals co-doped by divalent (Mg2+, Ca2+) and tetravalent (Zr4+, Ti4+) ions have been studied by means of time-resolved luminescence as well as the excitation luminescence spectroscopy in vacuum ultraviolet (VUV) and soft X-ray (XUV) spectral range. Tunable laser excitation was applied for time-resolved experiments in order to obtain luminescence decay curves under excitations in Ce3+, Gd3+ and excitonic absorption bands. The influence of the co-dopant ions on the Ce3+ luminescence decay kinetics is elucidated. The fastest luminescence decay was observed for the Mg2+ co-doped crystals under any excitation below bandgap energy indicating the perturbation of the 5d states of Ce3+ by Mg2+ ions. Synchrotron radiation was utilized for the luminescence excitation in the energy range from 4.5 to 800 eV. Special attention was paid to the analysis of Ce3+ excitation spectra in VUV and XUV spectral range where multiplication of electronic excitation (MEE) processes occur. Our results demonstrated that GGAG:Ce single crystals co-doped by Mg2+ ions as well as the GGAG:Ce crystal annealed in vacuum reveal the most efficient excitation of Ce3+ emission in VUV-XUV excitation range. The role of intrinsic defects in MEE processes in the co-doped as well as in the annealed GGAG:Ce single crystals is discussed.


2012 ◽  
Vol 190 ◽  
pp. 273-276 ◽  
Author(s):  
A.A. Makhnev ◽  
L.V. Nomerovannaya ◽  
Natalia N. Loshkareva ◽  
A.M. Balbashov

The optical properties of single crystals of the hexagonal manganites RMnO3 (R = Ho, Tm, Yb) have been investigated by spectroscopic ellipsometry in the spectral range 0.6-5.0 eV. The measurements show a strong anisotropy of the diagonal elements of the dielectric tensor. It has been demonstrated that the optical absorption edge for the polarization Ec was determined by the intense band of O(2p)Mn (3d) transition centered near 1.6 eV, whereas this band for the polarization Ec was strongly suppressed and shifted toward higher energies by 0.15-0.20 eV. The spectral dependences of the ε1(E) and ε2(E) for HoMnO3, TmMnO3 and YbMnO3 single crystals were qualitatively similar. The broad absorption band at E<1.0 eV clearly appears at the energies below the fundamental absorption edge of all of study compounds. It is possible, the origin of the near-infrared ε2(E) absorption is associated with 4f-4f transitions of R3+ ions.


1988 ◽  
Vol 133 (3) ◽  
pp. 163-166 ◽  
Author(s):  
A.F. Goncharov ◽  
G.N. Zhizhin ◽  
S.A. Kiselev ◽  
L.A. Kuzik ◽  
V.A. Yakovlev

2019 ◽  
Vol 127 (10) ◽  
pp. 532
Author(s):  
С.Д. Абдурахмонов ◽  
В.С. Горелик

AbstractOvertone bands in the spectral range of 1300−1920 cm^–1 have been found in Raman scattering spectrum of lithium tantalate single crystals. The Raman spectra were recorded in the 180° scattering geometry. The intensity of overtone transitions differs for different samples and, in some cases, is comparable with the Raman scattering intensity at the fundamental modes of a lithium tantalate single crystal.


2014 ◽  
Vol 33 (1) ◽  
pp. 27 ◽  
Author(s):  
Vladimir Ivanovski

Investigation of polarized IR reflectance spectra of single crystals is important in the course of obtaining vibrational, optical and dielectric properties of solid state samples.  Diffraction X-ray methods are usually employed for crystal orientation. In this work, two IR reflectance methods are proposed as a supplement in testing the orientation of the <em>b</em> crystal axis and by that the <em>ac</em> crystal plane, in respect to the morphology of monoclinic single crystals. The methods were tested on two Tutton salt single crystals: K<sub>2</sub>Ni(SO<sub>4</sub>)<sub>2</sub>·6H<sub>2</sub>O and K<sub>2</sub>Ni(SeO<sub>4</sub>)<sub>2</sub>·6H<sub>2</sub>O and were further compared with the cross-polarization IR reflectance method. Both methods rely on the symmetry and optical properties of monoclinic single crystals. One of them takes into account the fact that one of the principal axes of the dielectric tensor is symmetry fixed, while the other employs the conditions for the appearance of an isosbestic-like point i.e. isosbestic-like region in the polarized IR reflectance spectra of single crystals with low symmetry.


Author(s):  
А.В. Телегин ◽  
Ю.П. Сухоруков ◽  
В.Д. Бессонов ◽  
С.В. Наумов

The spectral, temperature and field dependences of the Faraday effect for single crystals of ferrimagnetic spinel CoFe2O4 are studied in the infrared range. It is shown that the magneto-optical q-factor of CoFe2O4 varies from -600/dB до +200/dB in the spectral range from 1.5 μm to 10 μm and weakly depends on temperature from 200 K to 300 K. The physical mechanisms responsible for the observed Faraday effect are proposed.


2021 ◽  
Vol 129 (6) ◽  
pp. 773
Author(s):  
И.А. Каплунов ◽  
Г.И. Кропотов ◽  
В.Е. Рогалин ◽  
А.А. Шахмин

The spectral dependences of the transmittance of CsI, AgCl, KRS-5 and KRS-6 single crystals in the infrared (IR) and terahertz (THz) ranges have been measured. The spectral dependences of the absorption (attenuation) coefficient of these crystals were calculated in the spectral range of 200–3000 μm. It was found, that these crystals are transparent in the millimeter range, which makes it possible to use materials when working with THz radiation. It should be noted that, in contrast to the IR spectral region, the optical quality of the surface of the crystal samples practically does not affect the transmission in the millimeter range.


2007 ◽  
Vol 102 (2) ◽  
pp. 023107 ◽  
Author(s):  
S. Tavazzi ◽  
L. Silvestri ◽  
M. Campione ◽  
A. Borghesi ◽  
A. Papagni ◽  
...  

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