random selection: La-Si-P (794 entries found)
Displaying 12 entries out of 12 entries found.
Crystallographic data Sstructural stability [Footnotes] Magnetic properties [Footnotes, magnetic units] Methods References
Materials ID Formula Formula units per cell Atomic sites per cell Crystal system Space group [Number] Formation energy (eV/atom) Energy relative to convex hull (eV/atom) Structure search Averaged magnetic moment (μB/atom) Magnetic polarization, Js (T) Methods References
REMD-156 La6Si2P 2 18 orthorhombic C222 [21] -0.539 0.169 ML 0.00 0.00 DFT WX
REMD-202 La6Si2P 4 36 monoclinic Pm [6] -0.615 0.092 ML 0.00 0.00 DFT WX
REMD-246 La6Si2P 2 18 orthorhombic Amm2 [38] -0.449 0.259 ML 0.00 0.00 DFT WX
REMD-257 La6Si2P 1 9 tetragonal P4/mmm [123] -0.330 0.377 ML 0.00 0.00 DFT WX
REMD-380 La6Si2P 1 9 triclinic P1 [1] -0.451 0.257 ML 0.00 0.00 DFT WX
REMD-362 La6Si2P 1 9 hexagonal P6/mmm [191] -0.079 0.628 ML 0.00 0.00 DFT WX
REMD-680 La6Si2P 4 36 orthorhombic Pbam [55] -0.465 0.242 ML 0.00 0.00 DFT WX
REMD-613 La6Si2P 4 36 orthorhombic Pbam [55] -0.492 0.215 ML 0.00 0.00 DFT WX
REMD-653 La6Si2P 4 36 orthorhombic Pbam [55] -0.493 0.215 ML 0.00 0.00 DFT WX
REMD-683 La6Si2P 4 36 orthorhombic Pbam [55] -0.418 0.289 ML 0.00 0.00 DFT WX
REMD-693 La6Si2P 1 9 hexagonal P-62m [189] -0.655 0.052 ML 0.00 0.00 DFT WX
REMD-749 La6Si2P 1 9 triclinic P1 [1] -0.634 0.074 ML 0.00 0.00 DFT WX

Footnotes:
  1. Formation energy:
    We perform DFT calculations to calculate the total enegies of all the structures. The formation energy is computed with respect to a linear combination of the total energies of reference elemental phases. When the formation energies are plotted as a function of chemical composition, a set of stable compounds forms a convex hull, which represents a boundary (theoretical lower limit) in a compositional phase diagram. Metastable compounds lie above the hull, and the energy relative to the hull (distance to the hull) is a useful quantity to examine the metastability of a new compound. The lower the formation energy above the convex hull, the more likely it is for the material to exist.

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