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Structural, Elastic, and Electronic Properties of Antiperovskite Chromium-Based Carbides ACCr3 (A = Al and Ga)

DOI: 10.1155/2013/136274

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Abstract:

We theoretically investigated antiperovskite chromium-based carbides ACCr3 through the first-principles calculation based on density functional theory (DFT). The structure optimization shows that the lattice parameter of ACCr3 is basically proportional to the radius of A-site elements. The calculated formation energies show that AlCCr3 and GaCCr3 can be synthesized at ambient pressure and are stable with nonmagnetic ground states. Based on the calculation of elastic constants, some elastic, mechanical, and thermal parameters are derived and discussed. AlCCr3 and GaCCr3 show ductile natures and may have similar thermal properties. From the analysis of the electronic structures, it was found that there are electron and hole bands that cross the Fermi level for AlCCr3 and GaCCr3, indicating multiple-band natures. The Fermi level locates at the vicinity of the density of states (DOSs) peak, which leads to a large DOS at Fermi level dominated by Cr-3d electrons. The band structures of AlCCr3 and GaCCr3 are very similar to those of the superconducting antiperovskite MgCNi3. The similarity may make AlCCr3 and GaCCr3 behave superconductively, which needs to be further investigated in theoretical and experimental studies. 1. Introduction Recently, antiperovskite compounds AXM3 (A, main group elements; X, carbon, boron, or nitrogen; M, transition metal) have attracted considerable attention. Due to the high concentration of transition metals in a cell, it can be deduced that interesting properties will be found in the family of compounds. In the antiperovskites family, nickel-based and manganese-based antiperovskites were extensively studied. Abundant physical properties were shown in the two kinds of compounds, such as superconductivity [1–3], giant magnetoresistance (MR) [4, 5], large negative magnetocaloric effect (MCE) [6, 7], giant negative thermal expansion [8, 9], magnetostriction [10], and nearly zero temperature coefficient of resistivity [11, 12]. But there are only a few reports about other 3d-metal-based antiperovskites so far. The difficulty restricting researchers is the exploration of new materials that can be experimentally synthesized. Therefore, theoretical investigations on these potential 3d-metal-based antiperovskites are useful to find the easily prepared stable materials and explore the new physical properties. In the earlier years, researchers have found that in chromium compounds there are varieties of interesting physical properties. Many of chromium alloys such as Cr-Ru, Cr-Rh, and Cr-Ir alloys show superconductivity [13]. And it was

References

[1]  T. He, Q. Huang, A. P. Ramirez et al., “Superconductivity in the non-oxide perovskite MgCNi3,” Nature, vol. 411, no. 6833, pp. 54–56, 2001.
[2]  M. Uehara, T. Yamazaki, T. K?ri, T. Kashida, Y. Kimishima, and I. Hase, “Superconducting properties of CdCNi3,” Journal of the Physical Society of Japan, vol. 76, no. 3, Article ID 034714, 2007.
[3]  M. Uehara, A. Uehara, K. Kozawa, and Y. Kimishima, “New antiperovskite-type superconductor ZnNyNi3,” Journal of the Physical Society of Japan, vol. 78, no. 3, 2009.
[4]  K. Kamishima, T. Goto, H. Nakagawa et al., “Giant magnetoresistance in the intermetallic compound Mn3GaC,” Physical Review B, vol. 63, no. 2, Article ID 024426, 2001.
[5]  Y. B. Li, W. F. Li, W. J. Feng, Y. Q. Zhang, and Z. D. Zhang, “Magnetic, transport and magnetotransport properties of Mn3+xSn1-xC and Mn3ZnySn1-yC compounds,” Physical Review B, vol. 72, no. 2, Article ID 024411, 2005.
[6]  T. Tohei, H. Wada, and T. Kanomata, “Negative magnetocaloric effect at the antiferromagnetic to ferromagnetic transition of Mn3GaC,” Journal of Applied Physics, vol. 94, no. 3, pp. 1800–1802, 2003.
[7]  M. H. Yu, L. H. Lewis, and A. R. Moodenbaugh, “Large magnetic entropy change in the metallic antiperovskite Mn3GaC,” Journal of Applied Physics, vol. 93, no. 12, pp. 10128–10130, 2003.
[8]  K. Takenaka and H. Takagi, “Giant negative thermal expansion in Ge-doped anti-perovskite manganese nitrides,” Applied Physics Letters, vol. 87, no. 26, Article ID 261902, pp. 1–3, 2005.
[9]  K. Takenaka, K. Asano, M. Misawa, and H. Takagi, “Negative thermal expansion in Ge-free antiperovskite manganese nitrides: tin-doping effect,” Applied Physics Letters, vol. 92, no. 1, Article ID 011927, 2008.
[10]  K. Asano, K. Koyama, and K. Takenaka, “Magnetostriction in Mn3 CuN,” Applied Physics Letters, vol. 92, no. 16, Article ID 161909, 2008.
[11]  E. O. Chi, W. S. Kim, and N. H. Hur, “Nearly zero temperature coefficient of resistivity in antiperovskite compound CuNMn3,” Solid State Communications, vol. 120, no. 7-8, pp. 307–310, 2001.
[12]  J. C. Lin, B. S. Wang, P. Tong et al., “Tunable temperature coefficient of resistivity in C- and Co-doped CuNMn3,” Scripta Materialia, vol. 65, no. 5, pp. 452–455, 2011.
[13]  B. T. Matthias, T. H. Geballe, V. B. Compton, E. Corenzwit, and G. W. Hull, “Superconductivity of chromium alloys,” Physical Review, vol. 128, no. 2, pp. 588–590, 1962.
[14]  Y. Nishihara, Y. Yamaguchi, T. Kohara, and M. Tokumoto, “Itinerant-electron antiferromagnetism and superconductivity in bcc Cr-Re alloys,” Physical Review B, vol. 31, no. 9, pp. 5775–5781, 1985.
[15]  Y. Nishihara, Y. Yamaguchi, M. Tokumoto, K. Takeda, and K. Fukamichi, “Superconductivity and magnetism of bcc Cr-Ru alloys,” Physical Review B, vol. 34, no. 5, pp. 3446–3449, 1986.
[16]  H. L. Alberts, D. S. McLachlan, T. Germishuyse, and M. Naidoo, “Superconductivity and antiferromagnetism in Cr-Mo-Ru alloys,” Journal of Physics, vol. 3, no. 12, pp. 1793–1800, 1991.
[17]  B. Wiendlocha, J. Tobola, S. Kaprzyk, and D. Fruchart, “Electronic structure, superconductivity and magnetism study of Cr3GaN and Cr3RhN,” Journal of Alloys and Compounds, vol. 442, no. 1-2, pp. 289–291, 2007.
[18]  H. M. Tütüncü and G. P. Srivastava, “Phonons and superconductivity in the cubic perovskite Cr3RhN,” Journal of Applied Physics, vol. 112, no. 9, Article ID 093914, 2012.
[19]  P. E. Bl?chl, “Projector augmented-wave method,” Physical Review B, vol. 50, no. 24, pp. 17953–17979, 1994.
[20]  M. Torrent, F. Jollet, F. Bottin, G. Zérah, and X. Gonze, “Implementation of the projector augmented-wave method in the ABINIT code: application to the study of iron under pressure,” Computational Materials Science, vol. 42, no. 2, pp. 337–351, 2008.
[21]  X. Gonze, J. M. Beuken, R. Caracas et al., “First-principles computation of material properties: the ABINIT software project,” Computational Materials Science, vol. 25, no. 3, pp. 478–492, 2002.
[22]  X. Gonze, B. Amadon, P. M. Anglade et al., “ABINIT: first-principles approach to material and nanosystem properties,” Computer Physics Communications, vol. 180, no. 12, pp. 2582–2615, 2009.
[23]  X. Gonze, G. M. Rignanese, M. Verstraete et al., “A brief introduction to the ABINIT software package,” Zeitschrift fur Kristallographie, vol. 220, no. 5-6, pp. 558–562, 2005.
[24]  J. P. Perdew, K. Burke, and M. Ernzerhof, “Generalized gradient approximation made simple,” Physical Review Letters, vol. 77, no. 18, pp. 3865–3868, 1996.
[25]  H. J. Monkhorst and J. D. Pack, “Special points for Brillouin-zone integrations,” Physical Review B, vol. 13, no. 12, pp. 5188–5192, 1976.
[26]  F. Birch, “Finite elastic strain of cubic crystals,” Physical Review, vol. 71, no. 11, pp. 809–824, 1947.
[27]  F. D. Murnaghan, Finite Deformation of An Elastic Solid, Dover Publications, New York, NY, USA, 1951.
[28]  J. Zhao, J. M. Winey, and Y. M. Gupta, “First-principles calculations of second- and third-order elastic constants for single crystals of arbitrary symmetry,” Physical Review B, vol. 75, no. 9, Article ID 094105, 2007.
[29]  R. Hill, “The elastic behaviour of a crystalline aggregate,” Proceedings of the Physical Society A, vol. 65, no. 5, pp. 349–354, 1952.
[30]  D. C. Wallace, Thermodynamics of Crystals, John Wiley & Sons, New York, NY, USA, 1972.
[31]  D. J. Green, An Introduction to the Mechanical Properties of Ceramics, Cambridge University Press, Cambridge, UK, 1998.
[32]  R. E. Newnham, Properties of Materials; Anisotropy, Symmetry, Structure, Oxford University Press, New York, NY, USA, 2005.
[33]  D. G. Pettifor, “Theoretical predictions of structure and related properties of intermetallics,” Materials Science and Technology, vol. 8, no. 4, pp. 345–349, 1992.
[34]  S. Pugh, “Relations between the elastic moduli and the plastic properties of polycrystalline pure metals,” Philosophical Magazine Series, vol. 7, no. 45, pp. 823–843, 1954.
[35]  J. Haines, J. M. Léger, and G. Bocquillon, “Synthesis and design of superhard materials,” Annual Review of Materials Research, vol. 31, pp. 1–23, 2001.
[36]  V. Kanchana, “Mechanical properties of Ti3AlX (X?=?C, N): Ab initio study,” Europhysics Letters, vol. 87, no. 2, p. 26006, 2009.
[37]  S. Mollah, “The physics of the non-oxide perovskite superconductor MgCNi3,” Journal of Physics Condensed Matter, vol. 16, no. 43, pp. R1237–R1276, 2004.
[38]  W. L. McMillan, “Transition temperature of strong-coupled superconductors,” Physical Review, vol. 167, no. 2, pp. 331–344, 1968.
[39]  J. H. Shim, S. K. Kwon, and B. I. Min, “Electronic structures of antiperovskite superconductors MgXNi3 (X?=?B, C, and N),” Physical Review B, vol. 64, no. 18, Article ID 180510, 2001.

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