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 Papers published during 2009:  part Ⅲ 

 

     31.Zirconium Aluminum Carbides: New Precursors for Synthesizing ZrO2–Al2O3 Composites

          L.F. He, Y.W. Bao, Y.C. Zhou, J. Am. Ceram. Soc., 92 [11] 2751–2758 (2009)

Abstract

ZrO2–Al2O3 nanocrystalline powders have been synthesized by oxidizing ternary Zr2Al3C4 powders. The simultaneous oxidation of Al and Zr in Zr2Al3C4 results in homogeneous mixture of ZrO2 and Al2O3 at nanoscale. Bulk nano- and submicrocomposites were prepared by hot-pressing as-oxidized powders at 1100oC–1500oC. The composition and microstructure evolution during sintering was investigated by XRD, Raman spectroscopy, SEM, and TEM. The crystallite size of ZrO2 in the composites increased from 7.5 nm for as-oxidized powders to about 0.5 lm at 1500 oC, while the tetragonal polymorph gradually converted to monolithic one with increasing crystallite size. The Al2O3 in the composites transformed from an amorphous phase in as oxidized powders to h phase at 1100 oC and a phase at higher temperatures. The hardness of the composite increased from 2.0 GPa at 1100 oC to 13.5 GPa at 1400 oC due to the increase of density.

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     32. High-temperature powder x-ray diffraction experiments and ab initio calculation of Ti3AlC2

          H. B. Zhang, X. Wu, Klaus Georg Nickel, J. X. Chen, Volker Presser1,  J. Appl. Phys.,  106(2009):013519

Abstract

The structural stability of the layered ternary carbide Ti3AlC2 was studied up to 35 GPa using x-ray diffraction with a Merrill–Basset-type diamond anvil cell and ab initio calculations. The structure P63 /mmc was stable in the present pressure range without any phase transition. The Birch–Murnaghan equation of state was employed to fit the experimental pressure-volume date, from which the isothermal bulk modulus of Ti3AlC2 was determined as 156±5 GPa, which was also supported by theoretical results. In addition, theoretical calculations described anisotropic pressure dependences of the lattice parameters, electronic structure, and bonding properties of Ti3AlC2.

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