Final Magnetic Moment0.005 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingNM |
Formation Energy / Atom-3.526 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.011 eVThe 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. |
Density5.00 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToNa9Sr2Nd9Ti20O60 + SrTiO3 |
Band Gap1.791 eVIn 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. |
Hermann MauguinP421m [113] |
HallP 4 2ab |
Point Group42m |
Crystal Systemtetragonal |
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%)
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 30.8 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 277.6 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 154.2 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 215.9 |
GaN (mp-804) | <1 1 0> | <0 0 1> | 339.3 |
SiO2 (mp-6930) | <1 1 0> | <0 0 1> | 246.8 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 215.9 |
DyScO3 (mp-31120) | <0 1 1> | <0 0 1> | 215.9 |
DyScO3 (mp-31120) | <1 0 0> | <0 0 1> | 308.5 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 61.7 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 154.2 |
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 154.2 |
LaAlO3 (mp-2920) | <1 0 0> | <0 0 1> | 215.9 |
LaAlO3 (mp-2920) | <1 0 1> | <0 0 1> | 154.2 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 154.2 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 246.8 |
CeO2 (mp-20194) | <1 1 0> | <0 0 1> | 215.9 |
CeO2 (mp-20194) | <1 1 1> | <0 0 1> | 154.2 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 246.8 |
GaN (mp-804) | <1 0 1> | <0 0 1> | 339.3 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 246.8 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 277.6 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 277.6 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 154.2 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 215.9 |
CdS (mp-672) | <1 0 0> | <0 0 1> | 308.5 |
LiF (mp-1138) | <1 0 0> | <0 0 1> | 154.2 |
YVO4 (mp-19133) | <0 0 1> | <0 0 1> | 246.8 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 277.6 |
Te2Mo (mp-602) | <1 0 1> | <0 0 1> | 277.6 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 154.2 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 154.2 |
GaSe (mp-1943) | <0 0 1> | <0 0 1> | 154.2 |
GaSe (mp-1943) | <1 0 0> | <0 0 1> | 277.6 |
GaSe (mp-1943) | <1 0 1> | <0 0 1> | 277.6 |
BN (mp-984) | <0 0 1> | <0 0 1> | 215.9 |
BN (mp-984) | <1 0 0> | <0 0 1> | 277.6 |
BN (mp-984) | <1 1 0> | <0 0 1> | 308.5 |
BN (mp-984) | <1 1 1> | <0 0 1> | 246.8 |
MoS2 (mp-1434) | <0 0 1> | <0 0 1> | 215.9 |
Al (mp-134) | <1 0 0> | <0 0 1> | 277.6 |
Al (mp-134) | <1 1 0> | <0 0 1> | 154.2 |
Al (mp-134) | <1 1 1> | <0 0 1> | 215.9 |
LiGaO2 (mp-5854) | <0 0 1> | <0 0 1> | 277.6 |
LiGaO2 (mp-5854) | <0 1 0> | <0 0 1> | 339.3 |
LiGaO2 (mp-5854) | <1 0 0> | <0 0 1> | 215.9 |
LiGaO2 (mp-5854) | <1 0 1> | <0 0 1> | 92.5 |
TeO2 (mp-2125) | <0 1 0> | <0 0 1> | 277.6 |
TeO2 (mp-2125) | <0 1 1> | <0 0 1> | 154.2 |
SiC (mp-7631) | <0 0 1> | <0 0 1> | 308.5 |
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.
Once you have registered you can also "vote" for full calculation of this material's elastic properties.
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
SrTiO3 (mp-4651) | 0.2875 | 0.000 | 3 |
KMnF3 (mp-644332) | 0.3176 | 0.002 | 3 |
CaSiO3 (mp-3382) | 0.2863 | 0.244 | 3 |
BaZrO3 (mp-1019544) | 0.3076 | 0.000 | 3 |
SrHfO3 (mp-13108) | 0.2892 | 0.033 | 3 |
Sr9LaTi10O30 (mp-695042) | 0.2387 | 0.000 | 4 |
BaPrMn2O6 (mp-19274) | 0.3362 | 0.031 | 4 |
BaLa(CoO3)2 (mp-24855) | 0.3342 | 0.109 | 4 |
BaNdMn2O6 (mp-25004) | 0.3330 | 0.040 | 4 |
Sr2MgOsO6 (mp-1078180) | 0.2957 | 0.000 | 4 |
Mn4N (mp-637576) | 0.6280 | 1.992 | 2 |
Fe2O3 (mp-1068212) | 0.6234 | 0.860 | 2 |
Fe4P (mp-20885) | 0.6367 | 0.686 | 2 |
Ni4O (mp-1094082) | 0.6379 | 1.732 | 2 |
Ni4N (mp-1094090) | 0.6379 | 0.067 | 2 |
Ba3La7Mn2(Co4O15)2 (mp-694945) | 0.3802 | 0.225 | 5 |
NaSr2LaTi4O12 (mp-694876) | 0.3374 | 0.013 | 5 |
NaSr3LaTi5O15 (mp-40830) | 0.3368 | 0.000 | 5 |
NaLaMgWO6 (mp-566983) | 0.3698 | 0.027 | 5 |
Ba3La7Mn(Co3O10)3 (mp-704461) | 0.3757 | 0.147 | 5 |
Na5Ca2Ce3Ti8Nb2O30 (mp-721094) | 0.3653 | 0.065 | 6 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Na_pv Sr_sv Nd_3 Ti_pv O |
Final Energy/Atom-8.0444 eV |
Corrected Energy-845.6587 eV
Uncorrected energy = -804.4387 eV
Composition-based energy adjustment (-0.687 eV/atom x 60.0 atoms) = -41.2200 eV
Corrected energy = -845.6587 eV
|
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)