2008
DOI: 10.1016/j.physc.2007.08.004
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Structural, elastic and electronic properties of superconducting anti-perovskites MgCNi3, ZnCNi3 and CdCNi3 from first principles

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Cited by 54 publications
(29 citation statements)
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“…The suggested lattice constant is perfect between our GGA and LDA results, just like the same cases for isostructural MgCNi 3 [11] and CdCNi 3 whose theoretical data are compared with experimental data [8]. For CdCNi 3 , our results are consistent with the Uehara et al experimental results [8], the present B 0 and B 0 are very close to the Wu et al [7] while have some difference with the Shein et al calculations [9]. It is easily found that almost all the theoretical calculations for the lattice constants by GGA are overestimated, and those by LDA are underestimated.…”
Section: Structure and Equation Of Statesupporting
confidence: 90%
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“…The suggested lattice constant is perfect between our GGA and LDA results, just like the same cases for isostructural MgCNi 3 [11] and CdCNi 3 whose theoretical data are compared with experimental data [8]. For CdCNi 3 , our results are consistent with the Uehara et al experimental results [8], the present B 0 and B 0 are very close to the Wu et al [7] while have some difference with the Shein et al calculations [9]. It is easily found that almost all the theoretical calculations for the lattice constants by GGA are overestimated, and those by LDA are underestimated.…”
Section: Structure and Equation Of Statesupporting
confidence: 90%
“…Up to now, most of experimental and theoretical investigations have been focused on superconductivity, density of states (DOS) and energy bands of MCNi 3 [2][3][4][5][6][7][8][9][10][11]. Park et al [3] found that the experimental data on ZnCNi 3 shows that the Fermi level density of states is smaller than that of MgCNi 3 , and argued that a strongly depressed DOS at the Fermi level could be responsible for pushing the transition temperature of ZnCNi 3 below 2 K. Uehara et al [8] observed that CdCNi 3 is a superconductor with T c = 2.5-3.2 K. Moreover, the available experimental and theoretical data have shown that the physical properties of MgCNi 3 material are very sensitive to external pressure, such as the superconducting transition temperature T c , electronic and elastic properties [10,11].…”
Section: Introductionmentioning
confidence: 99%
“…Thus, the difference in the effect of the pressure between the two materials can be understood qualitatively. For CdCNi 3 , a bulk modulus of 153 GPa was predicted [9,10]. Therefore, in CdCNi 3 the largest pressure effect is expected among the three antiperovskite superconductors.…”
Section: Introductionmentioning
confidence: 94%
“…In the antiperovskite superconductor ZnNNi 3 , the effect of the pressure is very small (0.0023 K/GPa). With regard to the bulk modulus, 204 GPa for ZnNNi 3 and 171 GPa for MgCNi 3 were calculated [9,10]. MgCNi 3 is "softer" than ZnNNi 3 .…”
Section: Introductionmentioning
confidence: 99%
“…Experimental investigations include photoemission and x-ray absorption measurements. 8 On the theoretical side, it includes the self-consistent tightbinding linear muffin-tin orbital (TB LMTO), 9 the linear muffin tin orbital (LMTO) method, 4,10 the full-potential augmented plane wave (FLAPW) method, 11,12 and densityfunctional theory within the local-density approximation. 11,[13][14][15] These experimental and theoretical studies showed that the significant feature of the electronic structure of MgCNi 3 is an extended van Hove singularity which creates a large density of states (DOS) just below the Fermi level.…”
Section: Introductionmentioning
confidence: 99%