High-pressure Phase Transition and Properties of Cu3N: An Experimental and Theoretical Study

被引:19
作者
Wosylus, Aron [2 ]
Schwarz, Ulrich [2 ]
Akselrud, Lev [2 ]
Tucker, Matt G. [3 ]
Hanfland, Michael [4 ]
Rabia, Kaneez [5 ]
Kuntscher, Christine [5 ]
von Appen, Joerg [6 ]
Dronskowski, Richard [6 ]
Rau, Dieter [1 ]
Niewa, Rainer [1 ]
机构
[1] Univ Stuttgart, Inst Anorgan Chem, D-70569 Stuttgart, Germany
[2] Max Planck Inst Chem Phys Fester Stoffe, D-01187 Dresden, Germany
[3] Rutherford Appleton Lab, ISIS Facil, Didcot OX11 0QX, Oxon, England
[4] European Synchrotron Radiat Facil, F-38043 Grenoble, France
[5] Univ Augsburg, Inst Phys, Lehrstuhl Expt Phys 2, D-86159 Augsburg, Germany
[6] Univ Aachen, Rhein Westfal TH Aachen, Inst Inorgan Chem, D-52074 Aachen, Germany
来源
ZEITSCHRIFT FUR ANORGANISCHE UND ALLGEMEINE CHEMIE | 2009年 / 635卷 / 12期
关键词
INITIO MOLECULAR-DYNAMICS; PHENOMENOLOGICAL MODEL; INDUCED METALLIZATION; POWDER DIFFRACTION; SEMICONDUCTOR;
D O I
10.1002/zaac.200900369
中图分类号
O61 [无机化学];
学科分类号
070301 ; 081704 ;
摘要
In-situ X-ray and neutron diffraction investigations on Cu3N indicate the onset of a high-pressure phase transition at about 5 GPa. The tetragonal cell parameters of the high-pressure phase reveal a discontinuous volume decrease of about 20 %. The phase transition is reversible, with a hysteresis of about 2 GPa. Subsequent ex-situ investigations in a multi-anvil press evidence a reversible re-formation of ambient pressure Cu3N from XRD patterns. The structure refinement with nitrogen atoms disordered in distorted octahedral voids of a tetragonal body-centered copper substructure leads to an occupation of approximately 1/3 and thus to a composition of Cu3N1.0(1). Optical absorption measurements (IR-VIS) up to 10 GPa indicate a semiconductor-metal transition. Density-functional based total energy calculations concerning the proposed high-pressure phase of Cu3N strongly support the experimental findings of a pressure-induced phase transition above 6 GPa to a structure with a copper tetragonal body-centered sublattice and nitrogen atoms in distorted octahedral voids. However, the calculations identify a need for an ordered alternative to provide the tetragonal distortion within the range of the observed c/a ratio. The resulting lattice parameters and the transition pressure fit with the measured data. For the case of an ordered occupation of the copper bct octahedral voids, all observed properties are in good agreement with the calculations.
引用
收藏
页码:1959 / 1968
页数:10
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