Effect of pressure on the structure of Fe–N alloys formed by solid-state reaction

2001 ◽  
Vol 16 (9) ◽  
pp. 2583-2590 ◽  
Author(s):  
B. Yao ◽  
L. Liu ◽  
S. E. Liu ◽  
X. Hu ◽  
W. H. Su

Fe–N alloys with crystalline structures different from those obtained at atmospheric pressure were produced by solid-state reaction between Fe and amorphous boron nitride under high pressure. Two new paramagnetic Fe–N phases were obtained at temperatures above 800 K under pressures between 2.0 and 4.0 GPa. One is of cubic structure with lattice constant of 6.114 Å, and another is of orthorhombic structure with lattice constants of a = 4 8.443, b = 4 4.749, and c 4 3.993 Å. ε–Fe3Nx with N contents of 18.1 to 21.4 at.%, which could not be obtained at atmospheric pressure, was produced at pressures of 3.0 to 4.0 GPa and temperatures of 690 to 800 K. The mechanism of formation of ε–Fe3Nx under high pressure is discussed.

2004 ◽  
Vol 384 (1-2) ◽  
pp. 268-273 ◽  
Author(s):  
J.G. Tao ◽  
B. Yao ◽  
J.H. Yang ◽  
S.J. Zhang ◽  
K. Zhang ◽  
...  

2021 ◽  
Vol 31 (3) ◽  
pp. 415-418
Author(s):  
Vladimir Yu. Osipov ◽  
Fedor M. Shakhov ◽  
Nikolai M. Romanov ◽  
Kazuyuki Takai

2014 ◽  
Vol 979 ◽  
pp. 220-223
Author(s):  
Piyamas Chainok ◽  
Supphadate Sujinnapram ◽  
Tunyanop Nilkamjon ◽  
Sermsuk Ratreng ◽  
Kiattipong Somsri ◽  
...  

In this research, the Y123 (YBa2Cu3Ox) and Y134 (YBa3Cu4Ox) superconductors were synthesized by solid state reaction and melt process, respectively. The crystal structure of all the samples were then determined using the Rietveld full-profile analysis method to indicate orthorhombic structure. The resistivity measurements showing Tc onset of Y123 lower than Y134 for solid state reaction but higher than Y134 melt process. However, the critical temperature off-set of Y134 has lower than of Y123. The SEM and EDX show that all samples were inhomogeneous. The SEM micrograph for solid state reaction Y123 has many pores between the grain and the grain size clearly demonstrated and bigger than Y134. It was seen that these pores are party eliminated in melt process samples. FTIR spectra detected the trace of carbonate residue in all samples.


2003 ◽  
Vol 15 (14) ◽  
pp. 2744-2751 ◽  
Author(s):  
Takashi Taniguchi ◽  
Koji Kimoto ◽  
Masataka Tansho ◽  
Shigeo Horiuchi ◽  
Shinobu Yamaoka

1978 ◽  
Vol 33 (2) ◽  
pp. 146-148 ◽  
Author(s):  
Hk. Müller-Buschbaum ◽  
M. Harder

Single crystals of the compound Ba2Fe11Al11O34 were prepared by solid state reaction (1700 °C) of BaO-Fe2O3-Al2O3 mixtures. The crystal structure was investigated by X-ray data (space group D46h-P63/mmc, lattice constants: a = 565.3, c = 2281.0 pm). Ba2Fe11Al11O34 is isotypic with Na2O · 11 Al2O3, the structure of β-alumina


2007 ◽  
Vol 63 (11) ◽  
pp. i191-i191 ◽  
Author(s):  
P. Armand ◽  
D. Granier ◽  
A. van der Lee

The cubic structure of trirubidium molybdophosphate, Rb3[PMo12O40], contains α-type Keggin [PMo12O40]3− anions and Rb+ counter-ions located in orthogonally intersecting channels. The P and Rb atoms are located on special positions with site symmetries \overline{4}3m and \overline{4}2.m, respectively. The three-dimensional arrangement is isostructural with that found in, for example, X 3[PMo12O40], with X = K, NH4 and H3O, or X 3[PW12O40] and X 4[SiW12O40], with X = Ag and Tl. The compound was crystallized using a typical high-temperature solid-state reaction with GaPO4 and X 3Mo3O10 (X = Rb or Li) as starting materials.


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