Encyclopedia of Crystallographic Prototypes

AFLOW Prototype: AB_hP2_187_a_d-001

This structure previously used the label(s) AB_hP2_187_d_a. Calls to these addresses will be redirected here.

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Tungsten Carbide (WC, $B_{h}$) Structure: AB_hP2_187_a_d-001

Picture of Structure; Click for Big Picture
Prototype CW
AFLOW prototype label AB_hP2_187_a_d-001
Strukturbericht designation $B_{h}$
ICSD 15406
CCDC 1596158
Pearson symbol hP2
Space group number 187
Space group symbol $P\overline{6}m2$
AFLOW prototype command aflow --proto=AB_hP2_187_a_d-001
--params=$a, \allowbreak c/a$

Other compounds with this structure

AgN,  AlSn,  AuC,  BIr,  CdN,  CrAs,  CrC,  CrN,  HfC,  HfS,  HfSe,  HfTe,  IrB,  IrC,  IrN,  LaC,  MoC,  MoN,  MoP,  NbC,  NbN,  NbS,  OsB,  OsC,  PbS,  PdN,  PrN,  PtC,  ReB,  ReC,  ReN,  RhN,  RuC,  RuN,  TaAs,  TaC,  TaN,  TaS,  TcB,  TcN,  TeZr,  TiO,  TiS,  TiSe,  TiTe,  VN,  WC,  WN,  YN,  ZrN,  ZrS,  ZrSe,  ZrTe


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

Basis vectors

Lattice coordinates Cartesian coordinates Wyckoff position Atom type
$\mathbf{B_{1}}$ = $0$ = $0$ (1a) C I
$\mathbf{B_{2}}$ = $\frac{1}{3} \, \mathbf{a}_{1}+\frac{2}{3} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ = $\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{\sqrt{3}}{6}a \,\mathbf{\hat{y}}+\frac{1}{2}c \,\mathbf{\hat{z}}$ (1d) W I

References

Found in

  • W. B. Pearson, The Crystal Chemistry and Physics of Metals and Alloys (Wiley Interscience, New York, London, Sydney, Tornoto, 1972).

First cited in

  • 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)

Geometry files


Prototype Generator

aflow --proto=AB_hP2_187_a_d --params=$a,c/a$

Species:

Running:

Output: