scholarly journals Dynamical Properties of (1-x)(Na0.5Bi0.5)TiO3-xBaTiO3 Single Crystals Studied by Broadband Inelastic Light Scattering

2009 ◽  
Vol 34 (1) ◽  
pp. 35-38 ◽  
Author(s):  
Yosuke Onda ◽  
Shinya Tsukada ◽  
Yuki Hidaka ◽  
Seiji Kojima
Keyword(s):  
Light Scattering ◽  
Single Crystals ◽  
Inelastic Light Scattering ◽  
Dynamical Properties

Anisotropy of Optical and Electron Transport Properties of Atomic Ordering in CdGeAs2

1999 ◽  
Vol 607 ◽  
Author(s):  
B. H. Bairamov ◽  
N. Fernelius ◽  
G. Irmer ◽  
J. Monecke ◽  
I. K. Polushina ◽  
...  
Keyword(s):  
Light Scattering ◽  
Single Crystals ◽  
Wide Band ◽  
Optical Quality ◽  
Surface Barrier ◽  
Optical Phonons ◽  
High Optical Quality ◽  
Inelastic Light Scattering ◽  
Linearly Polarized ◽  
Electron Transport Properties

AbstractInelastic light scattering by optical phonons and the temperature dependent electrical conductivity, Hall constant and photosensitivity were studied in oriented CdGeAs2 crystals grown by ultra-low gradient freeze technique from near-stoichiometric melts. Observation of the clear polarization dependence of the inelastic light scattering spectra by optical phonons combined with the absence of any dependence of the intensity and frequency shift of the observed lines with mapping measurements in 300 μm steps indicated the high optical quality and homogeneity of these single crystals. It is shown that surface-barrier structures using these single crystals may be used as wide-band detectors for natural light, as well as selective photoanalyzers for linearly polarized radiation.

Dynamical properties of cubr2aqueous solutions by inelastic light scattering

1982 ◽  
Vol 12 (1) ◽  
pp. 69-80 ◽  
Author(s):  
F. Aliotta ◽  
G. Maisano ◽  
P. Migliardo ◽  
C. Vasi
Keyword(s):  
Light Scattering ◽  
Inelastic Light Scattering ◽  
Dynamical Properties

RESONANT PROPERTIES OF INELASTIC LIGHT SCATTERING IN Bi2Sr2CaCu2O8-x SUPERCONDUCTING SINGLE CRYSTALS

1992 ◽  
Vol 06 (18) ◽  
pp. 1137-1143 ◽  
Author(s):  
O. V. MISOCHKO ◽  
A. KH. ARSLANBEKOV
Keyword(s):  
Light Scattering ◽  
Raman Scattering ◽  
Single Crystals ◽  
Inelastic Light Scattering ◽  
Similar Character ◽  
Electronic Scattering

The resonant properties of Raman scattering in Bi 2 Sr 2 CaCu 2 O 8-x single crystals for four diagonal phonons and electronic scattering as well have been investigated for different polarizations. The resonance profiles for the phonons were of similar character, but the resonant profiles of the two components of electronic scattering, by contrast, were different.

scholarly journals Study of the superconducting gap inRNi2B2C(R=Y,Lu)single crystals by inelastic light scattering

2000 ◽  
Vol 62 (2) ◽  
pp. 1291-1295 ◽  
Author(s):  
In-Sang Yang ◽  
M. V. Klein ◽  
S. L. Cooper ◽  
P. C. Canfield ◽  
B. K. Cho ◽  
...  
Keyword(s):  
Light Scattering ◽  
Single Crystals ◽  
Superconducting Gap ◽  
Inelastic Light Scattering

An unified approach to inelastic light scattering in Keldysh–Schwinger functional integral formalism

2015 ◽  
Vol 29 (07) ◽  
pp. 1550040 ◽  
Author(s):  
Hyun Cheol Lee
Keyword(s):  
Light Scattering ◽  
Cross Sections ◽  
Golden Rule ◽  
Functional Integral ◽  
Integral Formalism ◽  
Inelastic Light Scattering ◽  
Scattering Geometry ◽  
The One ◽  
Resonant Part ◽  
Functional Integral Formalism

We propose a theoretical framework which can treat the nonresonant and the resonant inelastic light scattering on an equal footing in the form of correlation function, employing Keldysh–Schwinger functional integral formalism. The interference between the nonresonant and the resonant process can be also incorporated in this framework. This approach is applied to the magnetic Raman scattering of two-dimensional antiferromagnetic insulators. The entire set of the scattering cross-sections are obtained at finite temperature, the result for the resonant part agrees with the one obtained by the conventional Fermi golden rule at zero temperature. The interference contribution is shown to be very sensitive to the scattering geometry and the band structure.

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