A Practical Approach to Low Temperature Microscopy and X-Ray Microanalysis

2000 ◽  
Vol 6 (S2) ◽  
pp. 306-307
Author(s):  
Patrick Echlin

Water is the most abundant and most important molecule in the hydrosphere, outer lithosphere and the biosphere of our planet. It is also the most abundant and energetically the least expensive building block of living material, forms an integral parts of natural inorganic matrices such as soil and is a constituent of many synthetic organic materials such as paints and polymers. Paradoxically, water does not exist naturally, in the pure state. Water, when converted to the solid state, can provide the perfect matrix in which we may observe the structure and study the in situ chemistry of hydrated samples. We will consider the nature of this solid matrix, and its constituent components in a range of sample, and show how it may be formed, manipulated, examined and analysed. In the short amount of time and space available, one can do little more than highlight the main features of the subject.

2004 ◽  
Vol 59 (6) ◽  
pp. 635-638 ◽  
Author(s):  
Norbert W. Mitzel ◽  
Udo Losehand

The compounds (H3C)2S, (H3Si)2S and (H3Ge)2S have been crystallised in situ on a diffractometer and their crystal structures determined by low-temperature X-ray diffraction. The molecules are present as monomers in the crystals. The aggregation of the molecules through secondary intermolecular contacts in the crystal is different: (H3C)2S is weakly associated into dimers by S···S contacts, whereas (H3Si)2S and (H3Ge)2S form Si···S and Ge···S contacts in an ice-analogous aggregation motif. Important geometry parameters are (H3C)2S: C-S 1.794(av) Å , C-S-C 99.2(1)°; (H3Si)2S: Si- S 2.143(1) Å , Si-S-Si 98.4°; (H3Ge)2S Ge-S 2.223(2) and 2.230(2) Å , Ge-S-Ge 98.2(1)◦.


2018 ◽  
Vol 51 (4) ◽  
pp. 1133-1140 ◽  
Author(s):  
Andrea Quintero ◽  
Patrice Gergaud ◽  
Joris Aubin ◽  
Jean-Michel Hartmann ◽  
Vincent Reboud ◽  
...  

The Ni/Ge0.9Sn0.1 solid-state reaction was monitored by combining in situ X-ray diffraction, in-plane reciprocal space map measurements and in-plane pole figures. A sequential growth was shown, in which the first phase formed was an Ni-rich phase. Then, at 518 K, the mono-stanogermanide phase Ni(Ge0.9Sn0.1) was observed. This phase was stable up to 873 K. Special attention has been given to the nature and the crystallographic orientation of the Ni-rich phase obtained at low temperature. It is demonstrated, with in-plane pole figure measurements and simulation, that it was the ∊-Ni5(Ge0.9Sn0.1)3 metastable phase with a hexagonal structure.


2011 ◽  
Vol 21 (15) ◽  
pp. 5604 ◽  
Author(s):  
Zonghai Chen ◽  
Yang Ren ◽  
Yan Qin ◽  
Huiming Wu ◽  
Shengqian Ma ◽  
...  

2011 ◽  
Vol 40 (26) ◽  
pp. 6961 ◽  
Author(s):  
Gang Lian ◽  
Xiao Zhang ◽  
Miao Tan ◽  
Shunjie Zhang ◽  
Deliang Cui ◽  
...  

2016 ◽  
Vol 52 (66) ◽  
pp. 10144-10146 ◽  
Author(s):  
Felix Hanke ◽  
Sarah Hindley ◽  
Anthony C. Jones ◽  
Alexander Steiner

X-ray structures and DFT calculations show that the HT phase is of Me2Cd is two-dimensionally disordered, while the LT phase is ordered. Both phases contain linearly coordinated cadmium atoms; methyl groups are staggered in the HT form and eclipsed in the LT-form.


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