V2AlC, V4AlC3 - x (x ≈ 0.31), and V12Al3C8: Synthesis, Crystal Growth, Structure, and Superstructure
Single crystals of V2AlC and the new carbides V4AlC3 - x and V12Al3C8 were synthesized from metallic melts. V2AlC was formed with an excess of Al, while V4AlC3 - x (x ≈ 0.31) and V12Al3C8 require the addition of cobalt to the melt. All compounds were characterized by XRD, EDX, and WDX measurements....
Saved in:
Published in | Inorganic chemistry Vol. 46; no. 18; pp. 7646 - 7653 |
---|---|
Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
United States
American Chemical Society
03.09.2007
|
Online Access | Get full text |
Cover
Loading…
Summary: | Single crystals of V2AlC and the new carbides V4AlC3 - x and V12Al3C8 were synthesized from metallic melts. V2AlC was formed with an excess of Al, while V4AlC3 - x (x ≈ 0.31) and V12Al3C8 require the addition of cobalt to the melt. All compounds were characterized by XRD, EDX, and WDX measurements. Crystal structures were refined on the basis of single-crystal data. The crystal structures can be explained with a building-block system consisting of two types of partial structures. The intermetallic part with a composition VAl is a two-layer cutting of the hexagonal closest packing. The carbide partial structure is a fragment of the binary carbide VC1 - x containing one or three layers. V2AlC is a H-phase (211-phase) with space group P63/mmc, Z = 2, and lattice parameters of a = 2.9107(6) Å, and c = 13.101(4) Å. V4AlC3 - x (x ≈ 0.31) represents a 413-phase with space group P63/mmc, Z = 2, a = 2.9302(4) Å, and c = 22.745(5) Å. The C-deficit is limited to the carbon site of the central layer. V12Al3C8 is obtained at lower temperatures. In the superstructure (P63/mcm, Z = 2, a = 5.0882(7) Å, and c = 22.983(5) Å) the vacancies on the carbon sites are ordered. The ordering is combined to a small shift of the V atoms. This ordered structure can serve as a structure model for the binary carbides TMC1 - x as well. V4AlC3 - x (x ≈ 0.31) and V12Al3C8 are the first examples of the so-called MAX-phases (MX) n MM‘ (n = 1, 2, 3), where a deficit of X and its ordered distribution in a superstructure is proven, (MX1 - x ) n MM‘. |
---|---|
Bibliography: | istex:411CF5C113151826A02E7F298A8F13F55BA16B1B ark:/67375/TPS-LZ2ZX0J8-T ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 0020-1669 1520-510X |
DOI: | 10.1021/ic700382y |