V2AlC, V4AlC3-x (x ≈ 0.31), and V12Al3C8:: Synthesis, crystal growth, structure, and superstructure

被引:123
作者
Etzkorn, Johannes
Ade, Martin
Hillebrecht, Harald
机构
[1] Univ Freiburg, Inst Anorgan & Analyt Chem, D-79104 Freiburg, Germany
[2] Freiburger Mat Forschungszentrum, D-79104 Freiburg, Germany
关键词
D O I
10.1021/ic700382y
中图分类号
O61 [无机化学];
学科分类号
070301 ; 081704 ;
摘要
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 approximate to 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 P6(3)/mmc, Z = 2, and lattice parameters of a = 2.9107(6) A, and c = 13.101(4) A. V4AlC3-x (x approximate to 0.31) represents a 413-phase with space group P6(3)/mmc, Z = 2, a = 2.9302(4) A, and c = 22.745(5) A. The C-deficit is limited to the carbon site of the central layer. V12Al3C8 is obtained at lower temperatures. In the superstructure (P6(3)/mcm, Z = 2, a = 5.0882(7) A, and c = 22.983(5) A) 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 approximate to 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'.
引用
收藏
页码:7646 / 7653
页数:8
相关论文
共 51 条
[1]  
ADE M, 1997, THESIS U FREIBURG GE
[2]  
[Anonymous], 2004, INT TABLES CRYSTAL A
[3]  
Barnighausen H., 1980, Communications in mathematical chemistry, V9, P139, DOI DOI 10.1002/ADFM.201604754
[4]   Dynamic elastic hysteretic solids and dislocations [J].
Barsoum, MW ;
Radovic, M ;
Zhen, T ;
Finkel, P ;
Kalidindi, SR .
PHYSICAL REVIEW LETTERS, 2005, 94 (08)
[5]   The MN+1AXN phases:: A new class of solids;: Thermodynamically stable nanolaminates [J].
Barsoum, MW .
PROGRESS IN SOLID STATE CHEMISTRY, 2000, 28 (1-4) :201-281
[6]  
Barsoum MW, 2001, AM SCI, V89, P334, DOI 10.1511/2001.4.334
[7]   Synthesis and characterization of a remarkable ceramic: Ti3SiC2 [J].
Barsoum, MW ;
ElRaghy, T .
JOURNAL OF THE AMERICAN CERAMIC SOCIETY, 1996, 79 (07) :1953-1956
[8]   CRYSTAL STRUCTURES OF V2C AND TA2C [J].
BOWMAN, AL ;
WALLACE, TC ;
YARNELL, JL ;
WENZEL, RG ;
STORMS, EK .
ACTA CRYSTALLOGRAPHICA, 1965, 19 :6-&
[9]   VALENCE: A program for calculating bond valences [J].
Brown, ID .
JOURNAL OF APPLIED CRYSTALLOGRAPHY, 1996, 29 :479-480
[10]   INORGANIC STRUCTURE TYPES WITH REVISED SPACE-GROUPS .1. [J].
CENZUAL, K ;
GELATO, LM ;
PENZO, M ;
PARTHE, E .
ACTA CRYSTALLOGRAPHICA SECTION B-STRUCTURAL SCIENCE, 1991, 47 :433-439