Small Angle X-Ray Diffraction of Collagen Fibrils Using a Three-Dimensional Imaging Gas Detector

Author(s):  
A. La Monaca ◽  
A. Bigi ◽  
A. Ripamonti ◽  
N. Roveri ◽  
M. Iannuzzi ◽  
...  
Materia Japan ◽  
2007 ◽  
Vol 46 (12) ◽  
pp. 827-827
Author(s):  
Yoshinori Nishino ◽  
Yukio Takahashi ◽  
Tetsuya Ishikawa ◽  
Eiichiro Matsubara

2012 ◽  
Vol 101 (24) ◽  
pp. 244103 ◽  
Author(s):  
D. Hänschke ◽  
L. Helfen ◽  
V. Altapova ◽  
A. Danilewsky ◽  
T. Baumbach

Soft Matter ◽  
2015 ◽  
Vol 11 (23) ◽  
pp. 4572-4575 ◽  
Author(s):  
H. Kikuchi ◽  
S. Izena ◽  
H. Higuchi ◽  
Y. Okumura ◽  
K. Higashiguchi

Ultra-small angle X-ray diffraction patterns of a polymer-stabilized blue phase liquid crystal and a possible three-dimensional giant polymer lattice with body-centered cubic O8− symmetry formed in it.


2019 ◽  
Vol 58 (SL) ◽  
pp. SLLA05 ◽  
Author(s):  
Kenji Ohwada ◽  
Kento Sugawara ◽  
Tomohiro Abe ◽  
Tetsuro Ueno ◽  
Akihiko Machida ◽  
...  

Author(s):  
D. Sayre

Single-particle X-ray diffraction is an extension of X-ray crystallography which allows the specimen to be any small solid-state bounded object; in Shapiroet al.[Proc. Natl Acad. Sci. USA(2005),102, 15343–15346] and Thibaultet al.[Acta Cryst.(2006), A62, 248–261], the reader can find descriptions of a recent StonyBrook/Berkeley/Cornell two-dimensional imaging of a yeast cell by this technique. Our present work is aimed at extending the technique to the three-dimensional imaging of a cell. However, the usual method of doing that, namely rotating the specimen into many orientations in the X-ray beam, has not as yet given sufficiently good three-dimensional diffraction data to allow the work to go forward, the largest problem being the difficulty of preventing unwanted levels of change in the specimen through the extended exposure to a hostile environment of X-rays and, in some cases, high vacuum and/or extreme cold. The present paper discusses possible methods of dealing with this problem.


Author(s):  
David A. Shapiro

In the paper by Sayre [Acta Cryst.(2008), A64, 33–35], a proposal is made to use stereoscopy as a short-term means of overcoming the primarily technological hurdles involved in three-dimensional imaging of the biological cell by soft X-ray diffraction microscopy. This addendum provides a broader perspective on the techniques used by this rapidly maturing community to investigate structural problems in the biological and material sciences.


1996 ◽  
Vol 35 (Part 1, No. 12A) ◽  
pp. 6172-6179 ◽  
Author(s):  
Takashi Itoh ◽  
Hajime Tsuchiya ◽  
Yumi Yoshimura ◽  
Masato Hashimoto ◽  
Takashi Konishi

Author(s):  
James A. Lake

The understanding of ribosome structure has advanced considerably in the last several years. Biochemists have characterized the constituent proteins and rRNA's of ribosomes. Complete sequences have been determined for some ribosomal proteins and specific antibodies have been prepared against all E. coli small subunit proteins. In addition, a number of naturally occuring systems of three dimensional ribosome crystals which are suitable for structural studies have been observed in eukaryotes. Although the crystals are, in general, too small for X-ray diffraction, their size is ideal for electron microscopy.


2015 ◽  
Vol 71 (4) ◽  
pp. 330-337 ◽  
Author(s):  
Sabina Kovač ◽  
Ljiljana Karanović ◽  
Tamara Đorđević

Two isostructural diarsenates, SrZnAs2O7(strontium zinc diarsenate), (I), and BaCuAs2O7[barium copper(II) diarsenate], (II), have been synthesized under hydrothermal conditions and characterized by single-crystal X-ray diffraction. The three-dimensional open-framework crystal structure consists of corner-sharingM2O5(M2 = Zn or Cu) square pyramids and diarsenate (As2O7) groups. Each As2O7group shares its five corners with five differentM2O5square pyramids. The resulting framework delimits two types of tunnels aligned parallel to the [010] and [100] directions where the large divalent nine-coordinatedM1 (M1 = Sr or Ba) cations are located. The geometrical characteristics of theM1O9,M2O5and As2O7groups of known isostructural diarsenates, adopting the general formulaM1IIM2IIAs2O7(M1II= Sr, Ba, Pb;M2II= Mg, Co, Cu, Zn) and crystallizing in the space groupP21/n, are presented and discussed.


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