Encyclopedia of Crystallographic Prototypes

AFLOW Prototype: A2BC_tI8_119_ac_b_d-001

If you are using this page, please cite:
H. Eckert, S. Divilov, M. J. Mehl, D. Hicks, A. C. Zettel, M. Esters. X. Campilongo and S. Curtarolo, The AFLOW Library of Crystallographic Prototypes: Part 4. Submitted to Computational Materials Science.

Links to this page

https://aflow.org/p/4BRY
or https://aflow.org/p/A2BC_tI8_119_ac_b_d-001
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Mn$_{2}$RhSn Tetragonal Heusler Structure: A2BC_tI8_119_ac_b_d-001

Picture of Structure; Click for Big Picture
Prototype Mn$_{2}$RhSn
AFLOW prototype label A2BC_tI8_119_ac_b_d-001
ICSD none
Pearson symbol tI8
Space group number 119
Space group symbol $I\overline{4}m2$
AFLOW prototype command aflow --proto=A2BC_tI8_119_ac_b_d-001
--params=$a, \allowbreak c/a$

Other compounds with this structure

Mn$_{2}$PtIn,  Mn$_{3}$Ga,  Rh$_{2}$CrSn,  Rh$_{2}$FeSn,  Mn$_{2-x}$Rh$_{1+x}$Sn,  Mn$_{2}$Rh$_{x}$Co$_{1-x}$Sn


  • (Alijani, 2013) describe this as a tetragonal inverse Heusler compound. This is likely an idealized version of the structure, as the atoms are all assumed to sit on high-symmetry Wyckoff positions.

\[ \begin{array}{ccc} \mathbf{a_{1}}&=&- \frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{2}a \,\mathbf{\hat{y}}+\frac{1}{2}c \,\mathbf{\hat{z}}\\\mathbf{a_{2}}&=&\frac{1}{2}a \,\mathbf{\hat{x}}- \frac{1}{2}a \,\mathbf{\hat{y}}+\frac{1}{2}c \,\mathbf{\hat{z}}\\\mathbf{a_{3}}&=&\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{2}a \,\mathbf{\hat{y}}- \frac{1}{2}c \,\mathbf{\hat{z}} \end{array}\]

Basis vectors

Lattice coordinates Cartesian coordinates Wyckoff position Atom type
$\mathbf{B_{1}}$ = $0$ = $0$ (2a) Mn I
$\mathbf{B_{2}}$ = $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{2}$ = $\frac{1}{2}c \,\mathbf{\hat{z}}$ (2b) Rh I
$\mathbf{B_{3}}$ = $\frac{3}{4} \, \mathbf{a}_{1}+\frac{1}{4} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ = $\frac{1}{2}a \,\mathbf{\hat{y}}+\frac{1}{4}c \,\mathbf{\hat{z}}$ (2c) Mn II
$\mathbf{B_{4}}$ = $\frac{1}{4} \, \mathbf{a}_{1}+\frac{3}{4} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ = $\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{4}c \,\mathbf{\hat{z}}$ (2d) Sn I

References

  • V. Alijani, O. Meshcheriakova, J. Winterlik, G. Kreiner, G. H. Fecher, and C. Felser, Increasing Curie temperature in tetragonal Mn$_{2}$RhSn Heusler compound through substitution of Rh by Co and Mn by Rh, J. Appl. Phys. 113, 063904 (2013), doi:10.1063/1.4791564.

Prototype Generator

aflow --proto=A2BC_tI8_119_ac_b_d --params=$a,c/a$

Species:

Running:

Output: