THE HIGH PRESSURE BEHAVIOR OF Mo2GaC AND Mo2Ga2C

Mark Nikolaevsky 1 Roee Friedman 2,3 Mishael Hornik 2,4 Sankalp Kota 5 Joseph Halim 5 El'ad Nisan Caspi 1 Michel Barsoum 5 Martin Dahlqvist 6 Johanna Rosen 6 Aviva Melchior 1
1Physics Department, Nuclear Research Center Negev, Beer-Sheva, Israel
2Physics Department, Israel Atomic Energy Commission, Tel Aviv, Israel
3School of Physics and Astronomy, Tel Aviv Univesity, Tel Aviv, Israel
4Physics Department, Ben-Gurion University of the Negev, Beer-Sheva, Israel
5Department of Physics, Drexel University, Philadelphia, Pennsylvania, USA
6Department of Physics, Chemistry and Biology, Linkoping University, Linkoping, Sweden

Mn+1AXn (MAX) phases with n=1-3 are a class of hexagonal nanolaminated materials, where M is an early transition metal, A is a main group element, and X is C or N. They are characterized by slabs of carbide or nitride (Mn+1Xn) separated by monolayers of pure A element. Having this layered structure the MAX phases exhibit a combination of the properties of both ceramic and metallic compounds, making them attractive for many technological applications. Mo2GaC and Mo2Ga2C are of great interest because of their structural similarity; Mo2Ga2C is also laminated, but it contains a Ga double-layer interleaving between the Mo2C blocks, instead of a Ga monolayer in Mo2GaC.

The mechanical properties and structural evolution under pressure of both Mo2GaC and Mo2Ga2C were calculated by first-principles [1, 2]. For both compounds a substantial difference in the compressibilities along the axes was found – the a axis is much softer than the c axis. For Mo2GaC the compressibility anomaly of c is closely reflected by the internal coordinate shift of Mo atom that shows three different slopes within 0–15, 20–60, and 70–100 GPa, respectively [1]. For Mo2Ga2C, a phase transition is predicted at 48 GPa with an increase of c and a decrease in a [2].

The current work concentrates in experimental investigation of the high pressure behavior of Mo2GaC and Mo2Ga2C. XRD measurements of samples loaded in diamond anvil cells were used to retrieve the structure of the compounds under pressure. The experimental results will be compared to the theoretical predictions.

1. Q.-H. Gao et. al., J. Appl. Phys. 119, 015901 (2016).

2. Z.-J. Yang et. al.,Mod. Phys. Lett. B30, 1650105 (2016).









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