Two-dimensional focusing X-ray optics: application of anisotropic elasticity theory for characterization of bent crystals

1994 ◽  
Vol 27 (6) ◽  
pp. 971-979 ◽  
Author(s):  
F. N. Chukhovskii ◽  
W. Z. Chang ◽  
E. Förster
2012 ◽  
Vol 600 ◽  
pp. 174-177 ◽  
Author(s):  
Jian Fei Xia ◽  
Zong Hua Wang ◽  
Yan Zhi Xia ◽  
Fei Fei Zhang ◽  
Fu Qiang Zhu ◽  
...  

Zirconia-graphene composite (ZrO2-G) has been successfully synthesized via decomposition of ZrOCl2•6H2O in a water-isopropanol system with dispersed graphene oxide (GO) utilizing Na2S as a precursor could enable the occurrence of the deposition of Zr4+ and the deoxygenation of GO at the same time. Transmission electron microscopy (TEM), Fourier transform infrared spectroscopy (FT-IR) and X-ray diffraction (XRD) techniques were used to characterize the samples. It was found that graphene were fully coated with ZrO2, and the ZrO2 existing in tetragonal phase, which resulted in the formation of two-dimensional composite.


2010 ◽  
Vol 65 (1) ◽  
pp. 90-94 ◽  
Author(s):  
Thomas Harmening ◽  
Rainer Pöttgen

Samples of EuRu4B4 and of the new boride EuRuB4 were prepared from europium, RuB, and RuB4 precursor alloys, respectively, in sealed tantalum tubes in an induction furnace. EuRu4B4 crystallizes with the LuRu4B4 structure, a = 748.1(1), c = 1502.3(4) pm. The structure of EuRuB4 was refined on the basis of X-ray diffractometer data: Pbam, a = 599.7(1), b = 1160.7(3), c = 358.06(7) pm, wR2 = 0.0691, 474 F2 values, and 38 variables. The four crystallographically independent boron sites build up layers which consist of almost regular pentagons and heptagons which sandwich the ruthenium and europium atoms, respectively. Within the two-dimensional [B4] networks each boron atom has a slightly distorted trigonal-planar boron coordination with B-B distances in the range 172 - 186 pm. Temperature-dependent 151Eu Mössbauer spectra show stable trivalent europium for EuRu4B4 and EuRuB4


Author(s):  
Claudio Ferrari ◽  
Riccardo Lolli ◽  
Bianca Salmaso ◽  
Giovanni Pareschi ◽  
Gianpiero Tagliaferri ◽  
...  
Keyword(s):  
X Ray ◽  

2016 ◽  
Vol 41 (2) ◽  
pp. 281 ◽  
Author(s):  
Istvan Mohacsi ◽  
Ismo Vartiainen ◽  
Manuel Guizar-Sicairos ◽  
Petri Karvinen ◽  
Vitaliy A. Guzenko ◽  
...  

2010 ◽  
Vol 65 (9) ◽  
pp. 1173-1176 ◽  
Author(s):  
Zhi-Guo Kong ◽  
Xiao-Yuan Ma ◽  
Zhan-Lin Xu

The title complex, [Mn2(glu)(L)2(HL)2]・0.5H2O (H2glu = glutaric acid, HL = 2-(2-chloro-6-fluorophenyl)-1Himidazo[ 4,5-f][1,10]phenanthroline) has been synthesized using a hydrothermal method and characterized by elemental analysis, IR spectroscopy and single-crystal X-ray diffraction. Crystal data: C162H88Cl8F8Mn4N32O9, triclinic, space group P1¯, a = 14.932(5), b = 16.414(5), c = 17.891(5) Å , α = 115.851(5), β = 91.288(5), γ = 112.894(5)◦, V = 3536.4(19) Å3, Z = 1. Compound 1 exhibits 1D chains which are further stacked by C-H...π interactions to give two-dimensional supramolecular layers.


2016 ◽  
Author(s):  
Frank Seiboth ◽  
Maik Kahnt ◽  
Maria Scholz ◽  
Martin Seyrich ◽  
Felix Wittwer ◽  
...  

1989 ◽  
Vol 160 ◽  
Author(s):  
David D. Allred ◽  
Qi Wang ◽  
Jesus Gonzalez-Hernandez

AbstractLaser Raman spectroscopy has been found to be useful for characterizing amorphous semiconductor multilayers, especially the interfaces of multilayers. Recently, we have extended this technique to the characterization of magnetron sputtered multilayers commonly used as reflectors in soft x-ray optics. Unlike the multilayers previously studied which contained only semiconductors and dielectrics, these are generally semiconductor/metal multilayers. We report here on the Raman characterization of the most common class of multilayers used in soft x-ray optics, those that contain a high density metal like tungsten interspersed with layers of carbon. In all of the metal/carbon multilayers the dominate feature in the Raman spectra is due to a-C. The a-C spectra consists of a broad peak at about 1560 cm-1 (G-peak) and a shoulder at about 1400 cm-1 (D-peak). This can be deconvoluted with Gaussian line shapes to yield two peaks (one at about 1560 to 1570 cm-1 and the other at about 1380 to 1420 cm-1). Among the W/C multilayer samples peak positions and relative magnitudes changed little with carbon thickness over the range of 1 to 12 nm. Significant differences are, however, seen as the identity of the metal component is altered or, especially, as the preparations are varied. For example, the intensity ratio of the D-peak to G-peak was much larger for multilayer samples prepared under conditions of good plasma confinement.


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