Tags: Strontium gallium indium (11/4/3)

Material Details

Final Magnetic Moment
0.000 μB

Calculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit.

Magnetic Ordering
Formation Energy / Atom
-0.357 eV

Calculated formation energy from the elements normalized to per atom in the unit cell.

Energy Above Hull / Atom
0.001 eV

The energy of decomposition of this material into the set of most stable materials at this chemical composition, in eV/atom. Stability is tested against all potential chemical combinations that result in the material's composition. For example, a Co2O3 structure would be tested for decomposition against other Co2O3 structures, against Co and O2 mixtures, and against CoO and O2 mixtures.

3.96 g/cm3

The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%)

Decomposes To
Sr28In11 + Sr8Ga7 + SrIn
Band Gap
0.015 eV

In general, band gaps computed with common exchange-correlation functionals such as the LDA and GGA are severely underestimated. Typically the disagreement is reported to be ~50% in the literature. Some internal testing by the Materials Project supports these statements; typically, we find that band gaps are underestimated by ~40%. We additionally find that several known insulators are predicted to be metallic.

Space Group

Hermann Mauguin
Fm3m [225]
-F 4 2 3
Point Group
Crystal System
We have not yet calculated a detailed bandstructure for this material
  • Cu
  • Ag
  • Mo
  • Fe

Calculated powder diffraction pattern; note that peak spacings may be affected due to inaccuracies in calculated cell volume, which is typically overestimated on average by 3% (+/- 6%)

X-Ray Absorption Spectra


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FWHM: 0 eV

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Download FEFF Input parameters.

Warning: These results are intended to be semi-quantitative in that corrections, such as edge shifts and Debye-Waller damping, have not been included.


A full elastic tensor has not been calculated for this material. Registered users can view statistical-learning-based predictions of this material's bulk and shear moduli.

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Similar Structures

Explanation of similarity distance measure: Documentation.
material # of elements distance
ZrFe12Si2B (mp-653838) 4 1.1622
Ce3Mn(Al3Cu)8 (mp-669550) 4 1.0367
LiMgH6Ir (mp-866640) 4 1.2492
Dy4In(NiGe2)2 (mp-20748) 4 1.2464
Ho4In(NiGe2)2 (mp-13510) 4 1.2525
Sr11In7 (mp-642322) 2 0.2790
Cd5Cu2 (mp-30696) 2 0.9109
In3Au7 (mp-567550) 2 0.9242
RbHg11 (mp-11953) 2 0.9182
Ca11Ga7 (mp-30474) 2 0.2406
Sr11Al4In3 (mp-642031) 3 0.1613
Sr11Ga4Sn3 (mp-567959) 3 0.1356
Sr17(Li2Hg3)3 (mp-866669) 3 0.7933
Sr21In8Pb7 (mp-642281) 3 0.3842
Sr11Al4Sn3 (mp-571154) 3 0.2482
Ba2CaCuSb2F14 (mvc-1743) 5 1.6233
Ba2La2Mn(WO6)2 (mp-566048) 5 1.5136
TiNb2Zn(PbO3)4 (mp-684721) 5 1.5858
LaTiNbBi2O9 (mp-636654) 5 1.5625
Ba3CaZrWO9 (mp-736122) 5 1.5943
Pu (mp-542606) 1 1.2878
Ta (mp-569794) 1 1.2832
Ta (mp-42) 1 1.3108
U (mp-93) 1 1.3818
Co (mp-669382) 1 1.3115
Na2Ca9NdY5HoF41 (mp-720432) 6 1.9488
Ba3LaZnReWO12 (mp-705508) 6 1.6405
Na5Ca2Ce3Ti8Nb2O30 (mp-721094) 6 1.8761
CrH36C12S6(ClO2)3 (mp-25498) 6 1.9551
NaH12C4S2BrO2 (mp-555975) 6 1.9175
SbTe7SXeCl(OF4)9 (mp-560359) 7 2.2481
SbTe7SXeCl(OF4)9 (mp-581488) 7 2.1551
BaH2C4S4N2(O3F4)3 (mp-554761) 7 2.2769
K2Mo2H12C4N(OF3)3 (mp-744190) 7 2.1364
RbBiAs6H24C8(S6N)2 (mp-556621) 7 2.0669
NaCa3UH16C3SO25F (mp-707264) 8 2.9658
NaAl6Fe3Si6B3H3O30F (mp-863289) 8 2.8826
FeP2H24C8S4NClO4 (mp-744839) 8 2.5819
CoP2H24C8S4NClO4 (mp-746679) 8 2.5680
GaCoPH18C9NCl2O3 (mp-605176) 8 2.3914
Scroll to show top 5 similar elemental, binary, ternary, quaternary, etc. structures.

Calculation Summary

Structure Optimization

Run Type
Energy Cutoff
520 eV
# of K-points
U Values
VASP PAW: Sr_sv In_d Ga_d
Final Energy/Atom
-2.5133 eV
Corrected Energy
-90.4789 eV
-90.4789 eV = -90.4789 eV (uncorrected energy)

Detailed input parameters and outputs for all calculations

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  • 159150

Displaying lattice parameters for primitive cell; note that calculated cell volumes are typically overestimated on average by 3% (+/- 6%). Note the primitive cell may appear less symmetric than the conventional cell representation (see "Structure Type" selector below the 3d structure)