Structural features of the congruently melting compounds MLi (NO3)2 (M=K, Rb, Cs) inferred from their Raman spectra

1999 ◽  
Vol 60 (3) ◽  
pp. 317-324 ◽  
Author(s):  
Kangcheng Xu ◽  
Yang Chen
1998 ◽  
Vol 47 (3) ◽  
pp. 417-422 ◽  
Author(s):  
Sh. Sh. Nabiev ◽  
I. I. Ostroukhova ◽  
N. V. Revina ◽  
L. P. Sukhanov

1992 ◽  
Vol 279 ◽  
Author(s):  
A. PéRez-Rodríguez ◽  
A. Romano-Rodríguez ◽  
J. R. Morante ◽  
J. Esteve ◽  
J. Montserrat

ABSTRACTIn this work Si samples implanted with nitrogen (N+ or N2+) at a dose of 1017 cm−2 are characterized by Raman spectroscopy and cross section transmission electron microscopy (XTEM). The correlation between the Raman spectra obtained with different excitation wavelengths and XTEM observations allows to determine the structural features related to the layers contributing to the total spectra. The evolution of these features with the annealing treatments (up to 1150°C) is studied. The results obtained show, after the annealing treatment at the highest temperature, the presence of silicon nitride precipitates in the silicon subsurface region, and the formation of a nitrogen rich polycrystalline Si layer with Si3N4 grains. The Raman spectra from the subsurface region show a remaining shift of -0.15 cm−1 when compared to the spectra from unimplanted Si. This shift, together with the similar shape of both Raman lines, suggests the presence in this region of an average tensile stress of 37.5 MPa.


2008 ◽  
Vol 105 (6) ◽  
pp. 913-918 ◽  
Author(s):  
P. G. Chufyrev ◽  
N. V. Sidorov ◽  
M. N. Palatnikov ◽  
A. A. Yanichev

2015 ◽  
Vol 1806 ◽  
pp. 1-6
Author(s):  
Sergey Mamedov

ABSTRACTTiO2 nanopowders obtained using different methods with the mean size of 5, 15, and 30 nm have been investigated by Raman spectroscopy in wide spectral range. Nano-size of TiO2 crystals lead to a shift and broadening of the first-order Raman lines through a relaxation of the q = 0 selection rule and effects on to the position, width and asymmetry of a Raman bands. The details of the evolution of the 142.9 cm-1 Raman line shape on the size and distributions of the nanopowders are presented and discussed in frame of confined phonons model. Analysis of Raman spectra shows that structural characteristics of nanopowders may be different even size of the nanopowders is the same. Structural features of the material depend on preparation methods/conditions and can be extracted from Raman spectra of the material.


1977 ◽  
Vol 32 (12) ◽  
pp. 1393-1399 ◽  
Author(s):  
Gert Heller ◽  
Jürgen Zambelli

Perhydrolysis of the trimethyl ester of boric acid with Η2O2/Η2Ο (85:15 by weight) in butanolic solvents in the presence of lithium- or cesium-tert-butylate in certain molar ratios yields Li2[B2(O2)2(OH)4 or Cs2[B2(O2)2(OH)4].In methanol in the presence of MX2, where M = Ca, Sr or Ba and X = N-methylacetamide depending on the experimental conditions M[B2(O2)2(OH)4] · n CH3OH, M[B2(O2)2(OH)2(OOH)2] · CH3OH or a compound with a chain structure (anion C) are obtained. Perhydrolysis with H2O2/ H2O (98:2 by weight) yields Sr[B2(O2)2(OOH)4] · CH3OH, Ba[B2(O2)2(OOH)4] · CH3OH or Ba[B2(O2)2(OOH)4] · 2 H2O2.Based on IR spectra and Raman spectra the structural features of these salts are discussed.


2008 ◽  
Author(s):  
P. Chufyrev ◽  
N. Sidorov ◽  
M. Palatnikov ◽  
K. Bormanis

1971 ◽  
Vol 44 (1) ◽  
pp. 71-86 ◽  
Author(s):  
J. L. Koenig ◽  
M. M. Coleman ◽  
J. R. Shelton ◽  
P. H. Starmer

Abstract We have demonstrated that good quality Raman spectra can be obtained from vulcanizates prepared from cis-l,4-polybutadiene. Furthermore, significant differences are seen in the spectra of extracted vulcanizates prepared from various recipes. Tentative assignments have been made for many of the following Raman lines observed in the spectra. 1. The 1633, 1187, 734, and 720 cm−1 lines are thought to be associated with dialkenyl sulfide crosslinks. 2. Lines occurring at 440 and 505 cm−1 are assigned to polysulfidic and disulfidic structures respectively. 3. The 635, 690, and 708 cm−1 lines are thought to be associated with cyclic sulfides. In particular, the 635 cm−1 line with six membered thioalkenes, the 690 cm−1 line with five membered thioalkanes and the 708 cm−1 line with five membered thioalkenes. 4. Pendent side groups derived from TMTD are thought to have lines occurring at 1142 and 577 cm−1. Other lines occurring in the Raman spectra of the vulcanizates examined cannot be assigned with the same degree of confidence. The line occurring at 1606 cm−1 may be associated with conjugation but further work is necessary to verify it. The recipes chosen do not necessarily reflect those used currently in industry but were designed to accentuate certain structural features in the network. Consequently, the weak band at 1587 cm−1, observed only in systems with large amounts of TMTD and associated with vinyl thioether type structures, should not be overemphasized. Lines occurring at 558, 852, and 872 cm−1 are unassigned at present. Although the initial results are encouraging, it must be stated that many problems exist. Due to difficulties associated with fluorescence and degradation, Raman spectra of many important rubber systems will be difficult to obtain. Low levels of fluorescence cause serious problems when weak lines are present and when quantitative measurements of line intensities are made.


2013 ◽  
Vol 854 ◽  
pp. 111-115 ◽  
Author(s):  
Alexander Stronski

Defect configuration of Ge5As37S58chalcogenide glasses was studied by positron annihilation lifetime spectra (PALS). Size of nanovoids was determined using Liaos formula for radius of nanovoids in spherical approximation. Peculiarities of structural features were obtained from Raman spectra.


Author(s):  
O.C. de Hodgins ◽  
K. R. Lawless ◽  
R. Anderson

Commercial polyimide films have shown to be homogeneous on a scale of 5 to 200 nm. The observation of Skybond (SKB) 705 and PI5878 was carried out by using a Philips 400, 120 KeV STEM. The objective was to elucidate the structural features of the polymeric samples. The specimens were spun and cured at stepped temperatures in an inert atmosphere and cooled slowly for eight hours. TEM micrographs showed heterogeneities (or nodular structures) generally on a scale of 100 nm for PI5878 and approximately 40 nm for SKB 705, present in large volume fractions of both specimens. See Figures 1 and 2. It is possible that the nodulus observed may be associated with surface effects and the structure of the polymers be regarded as random amorphous arrays. Diffraction patterns of the matrix and the nodular areas showed different amorphous ring patterns in both materials. The specimens were viewed in both bright and dark fields using a high resolution electron microscope which provided magnifications of 100,000X or more on the photographic plates if desired.


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