TY - JOUR
T1 - In situ observation of the reaction of tantalum with nitrogen in a laser heated diamond anvil cell
AU - Friedrich, Alexandra
AU - Winkler, Björn
AU - Bayarjargal, Lkhamsuren
AU - Juarez Arellano, Erick A.
AU - Morgenroth, Wolfgang
AU - Biehler, Jasmin
AU - Schröder, Florian
AU - Yan, Jinyuan
AU - Clark, Simon M.
PY - 2010/7/16
Y1 - 2010/7/16
N2 - Tantalum nitrides were formed by reaction of the elements at pressures between 9(1) and 12.7(5) GPa and temperatures >1600-2000K in the laser-heated diamond anvil cell. The incorporation of small amount of nitrogen in the tantalum structure was identified as the first reaction product on weak laser irradiation. Subsequent laser heating led to the formation of hexagonal β-Ta2Nand orthorhombic η-Ta2N3, whichwas the stable phase at pressures up to 27 GPa and high temperatures. No evidence was found for the presence of ε-TaN, ∂-TaN, δ-TaN, Ta3N5-I or Ta 3N5-II, which was predicted to be the stable phase at P > 17 GPa and T = 2800 K, at the P, T-conditions of this experiment. The bulk modulus of η-Ta2N3 was determined to be B0 = 319(6) GPa from a 2nd order Birch-Murnaghan equation of state fit to the experimental data, while quantum mechanical calculations using the density functional theory gave a bulk modulus of B0 = 348.0(9) GPa for a 2nd-order fit or B0 = 339(1) GPa and B′ = 4.67(9) for a 3rd-order fit. The values show the large incompressibility of this high-pressure phase. From the DFT data the structural compression mechanism could be determined.
AB - Tantalum nitrides were formed by reaction of the elements at pressures between 9(1) and 12.7(5) GPa and temperatures >1600-2000K in the laser-heated diamond anvil cell. The incorporation of small amount of nitrogen in the tantalum structure was identified as the first reaction product on weak laser irradiation. Subsequent laser heating led to the formation of hexagonal β-Ta2Nand orthorhombic η-Ta2N3, whichwas the stable phase at pressures up to 27 GPa and high temperatures. No evidence was found for the presence of ε-TaN, ∂-TaN, δ-TaN, Ta3N5-I or Ta 3N5-II, which was predicted to be the stable phase at P > 17 GPa and T = 2800 K, at the P, T-conditions of this experiment. The bulk modulus of η-Ta2N3 was determined to be B0 = 319(6) GPa from a 2nd order Birch-Murnaghan equation of state fit to the experimental data, while quantum mechanical calculations using the density functional theory gave a bulk modulus of B0 = 348.0(9) GPa for a 2nd-order fit or B0 = 339(1) GPa and B′ = 4.67(9) for a 3rd-order fit. The values show the large incompressibility of this high-pressure phase. From the DFT data the structural compression mechanism could be determined.
UR - http://www.scopus.com/inward/record.url?scp=77954215715&partnerID=8YFLogxK
U2 - 10.1016/j.jallcom.2010.04.113
DO - 10.1016/j.jallcom.2010.04.113
M3 - Article
AN - SCOPUS:77954215715
SN - 0925-8388
VL - 502
SP - 5
EP - 12
JO - Journal of Alloys and Compounds
JF - Journal of Alloys and Compounds
IS - 1
ER -