Encyclopedia of Crystallographic Prototypes

AFLOW Prototype: AB2_tI6_139_a_e-001

This structure originally had the label AB2_tI6_139_a_e. Calls to that address will be redirected here.

If you are using this page, please cite:
M. J. Mehl, D. Hicks, C. Toher, O. Levy, R. M. Hanson, G. L. W. Hart, and S. Curtarolo, The AFLOW Library of Crystallographic Prototypes: Part 1, Comp. Mat. Sci. 136, S1-S828 (2017). (doi=10.1016/j.commatsci.2017.01.017)

Links to this page

https://aflow.org/p/NG7F
or https://aflow.org/p/AB2_tI6_139_a_e-001
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MoSi$_{2}$ ($C11_{b}$) Structure: AB2_tI6_139_a_e-001

Picture of Structure; Click for Big Picture
Prototype MoSi$_{2}$
AFLOW prototype label AB2_tI6_139_a_e-001
Strukturbericht designation $C11_{b}$
ICSD 85756
Pearson symbol tI6
Space group number 139
Space group symbol $I4/mmm$
AFLOW prototype command aflow --proto=AB2_tI6_139_a_e-001
--params=$a, \allowbreak c/a, \allowbreak z_{2}$

Other compounds with this structure

AgZr$_{2}$,  AuHf$_{2}$,  AuMn$_{2}$,  AuZr$_{2}$,  BeAu$_{2}$,  CdTi$_{2}$,  CuHf$_{2}$,  CuTl$_{2}$,  CuZr$_{2}$,  DyAg$_{2}$,  DyAu$_{2}$,  DyTl$_{2}$,  ErAu$_{2}$,  GdAg$_{2}$,  GdAu$_{2}$,  HfAu$_{2}$,  LuAu$_{2}$,  MnAu$_{2}$,  MoGe$_{2}$,  MoU$_{2}$,  $\beta$-PdBi$_{2}$,  PdHf$_{2}$,  PdTi$_{2}$,  PtHf$_{2}$,  ReSi$_{2}$,  TaNi$_{2}$,  TiAu$_{2}$,  WSi$_{2}$,  ZrAu$_{2}$,  ZrPd$_{2}$


  • When $c=3a$ and $z_{2}=1/3$ the atoms are on the sites of a body-centered cubic ($A2$) lattice. For MoSi$_{2}$ itself, (Harada, 1998) gives $c/a = 2.45$ and $z_{2}=0.3353$. Other compounds in this structure have very different values of $c/a$ and even $z_{2}$.

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

Basis vectors

Lattice coordinates Cartesian coordinates Wyckoff position Atom type
$\mathbf{B_{1}}$ = $0$ = $0$ (2a) Mo I
$\mathbf{B_{2}}$ = $z_{2} \, \mathbf{a}_{1}+z_{2} \, \mathbf{a}_{2}$ = $c z_{2} \,\mathbf{\hat{z}}$ (4e) Si I
$\mathbf{B_{3}}$ = $- z_{2} \, \mathbf{a}_{1}- z_{2} \, \mathbf{a}_{2}$ = $- c z_{2} \,\mathbf{\hat{z}}$ (4e) Si I

References

  • Y. Harada, M. Morinaga, D. Saso, M. Takata, and M. Sakata, Refinement of crystal structure in MoSi$_2$, Intermetallics 6, 523–527 (1998), doi:10.1016/S0966-9795(97)00102-7.

Prototype Generator

aflow --proto=AB2_tI6_139_a_e --params=$a,c/a,z_{2}$

Species:

Running:

Output: