Hostname: page-component-78c5997874-s2hrs Total loading time: 0 Render date: 2024-11-19T03:48:56.385Z Has data issue: false hasContentIssue false

Trend in crystal structure of layered ternary T-Al-C carbides (T = Sc, Ti, V, Cr, Zr, Nb, Mo, Hf, W, and Ta)

Published online by Cambridge University Press:  31 January 2011

Jingyang Wang*
Affiliation:
Shenyang National Laboratory for Materials Science, Institute of Metal Research, Chinese Academy of Sciences, Shenyang 110016, China; and International Centre for Materials Physics, Institute of Metal Research, Chinese Academy of Sciences, Shenyang 110016, China
Yanchun Zhou
Affiliation:
Shenyang National Laboratory for Materials Science, Institute of Metal Research, Chinese Academy of Sciences, Shenyang 110016, China
Ting Liao
Affiliation:
Shenyang National Laboratory for Materials Science, Institute of Metal Research, Chinese Academy of Sciences, Shenyang 110016, China; and Graduate School of Chinese Academy of Sciences, Beijing 100039, China
Zhijun Lin
Affiliation:
Shenyang National Laboratory for Materials Science, Institute of Metal Research, Chinese Academy of Sciences, Shenyang 110016, China; and Graduate School of Chinese Academy of Sciences, Beijing 100039, China
*
a)Address all correspondence to this author. e-mail: [email protected]
Get access

Abstract

Layered ternary T-Al-C ceramics containing early transition metal Sc, Zr, and Hf, crystallize with the TnAl3Cn+2 formula, while others containing neighbor elements Ti, V, Cr, Nb, Mo, W, and Ta yield the Tn+1AlCn formula. Ternary TnAl3Cn+2 ceramics are structurally characterized by NaCl-type TC slabs being separated by Al4C3-type AlC layers. In the present study, we suggest that the ability of forming the TnAl3Cn+2 carbide could be traced back to the structure mismatches between the TC, Al4C3 and TnAl3Cn+2 compounds. Ternary carbides following the TnAl3Cn+2 formula experience small lattice mismatches and strain energies. Moreover, the discrepancy between crystal structures of TnAl3Cn+2 and Tn+1AlCn is interpreted by lattice mismatch and the produced strain energy for the ternary T-Al-C ceramics. We also present close relationships between the atomic radii of transition metal and lattice mismatch, as well as the strain energy. The proposed method is not only helpful to explain the trend in crystal structure of T-Al-C based ceramics, but may be also general to predict the crystal structure of layered compounds constructed by alternatively stacked structural units.

Type
Articles
Copyright
Copyright © Materials Research Society 2007

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

1Nowotny, H.Windisch, S.: High temperature compounds. Annual Rev. Mater. Sci. 3, 171 1973CrossRefGoogle Scholar
2Gesing, T.M.Jeitschko, W.: The crystal structures of Zr3Al3C5, ScAl3C3, and UAl3C3 and their relation to the structures of U2Al3C4and Al4C3. J. Solid State Chem. 140, 396 1998CrossRefGoogle Scholar
3Schuster, J.C.Nowotny, H.: Investigations of the ternary systems (Zr, H, Nb, Ta)-Al-C and studies on complex carbides. Z. Metallkd. 71, 341 1980Google Scholar
4Fukuda, K., Mori, S.Hashimoto, S.: Crystal structure of Zr2Al3C4. J. Am. Ceram. Soc. 88, 3528 2005CrossRefGoogle Scholar
5Schuster, J.C., Nowotny, H.Vaccaro, C.: The ternary systems: Cr-Al-C, V-Al-C, and Ti-Al-C and the behavior of H-phases (M2AlC). J. Solid State Chem. 32, 213 1980CrossRefGoogle Scholar
6Wang, J.Y., Zhou, Y.C., Lin, Z.J., Liao, T.He, L.F.: First-principles prediction of mechanical properties and electronic structure of ternary aluminum carbide Zr3Al3C5. Phys. Rev. B 73, 134107 2006CrossRefGoogle Scholar
7Lin, Z.J., Zhuo, M.J., He, L.F., Zhou, Y.C., Li, M.S.Wang, J.Y.: Atomic-scale microstructures of Zr2Al3C4 and Zr3Al3C5 ceramics. Acta Mater. 54, 3843 2006CrossRefGoogle Scholar
8Barsoum, M.W.: The MN+1AXN phases: A new class of solid. Prog. Solid State Chem. 28, 201 2000CrossRefGoogle Scholar
9Wang, J.Y.Zhou, Y.C.: Dependence of elastic stiffness on electronic band structure of nanolaminate M 2AlC (M=Ti, V, Nb, and Cr) ceramics. Phys. Rev. B 69, 214111 2004CrossRefGoogle Scholar
10Wang, J.Y., Zhou, Y.C., Lin, Z.J., Meng, F.L.Li, F.: Raman active phonon modes and heat capacities of Ti2AlC and Cr2AlC ceramics: First-principles and experimental investigations. Appl. Phys. Lett. 86, 101902 2005CrossRefGoogle Scholar
11Segall, M.D., Lindan, P.L.D., Probert, M.J., Pickard, C.J., Hasnip, P.J., Clark, S.J.Payne, M.C.: First-principles simulation: Ideas, illustrations and the CASTEP code. J. Phys.: Condens. Matter 14, 2717 2002Google Scholar
12Vanderbilt, D.: Soft self-consistent pseudopotentials in a generalized eigenvalue formalism. Phys. Rev. B 41, 7892 1990CrossRefGoogle Scholar
13Perdew, J.P., Chevary, J.A., Vosko, S.H., Jackson, K.A., Pederson, M.R., Singh, D.J.Fiolhais, C.: Atoms, molecules, solids, and surfaces: Applications of the generalized gradient approximation for exchange and correlation. Phys. Rev. B 46, 6671 1992CrossRefGoogle ScholarPubMed
14Monkhorst, H.J.Pack, J.D.: Special points for Brillouin-zone integrations. Phys. Rev. B 16, 1748 1977Google Scholar
15Pfrommer, B.G., Côté, M., Louie, S.G.Cohen, M.L.: Relaxation of crystals with the quasi-newton method. J. Comp. Phys. 131, 233 1997CrossRefGoogle Scholar
16Milman, V.Warren, M.C.: Elasticity of hexagonal BeO. J. Phys.: Condens. Matter 13, 241 2001Google Scholar
17Shen, J.Y., Johnston, S., Shang, S.L.Anderson, T.: Calculated strain energy of hexagonal epitaxial thin films. J. Cryst. Growth 240, 6 2002CrossRefGoogle Scholar
18Yu, R., He, L.L.Ye, H.Q.: Effects of Si and Al on twin boundary energy of TiC. Acta Mater. 51, 2477 2003CrossRefGoogle Scholar