Encyclopedia of Crystallographic Prototypes

AFLOW Prototype: AB_hP4_186_b_a-001

This structure originally had the label AB_hP4_186_b_a. 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/QUDC
or https://aflow.org/p/AB_hP4_186_b_a-001
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Original BN ($B12$) Structure (Obsolete): AB_hP4_186_b_a-001

Picture of Structure; Click for Big Picture
Prototype BN
AFLOW prototype label AB_hP4_186_b_a-001
Strukturbericht designation $B12$
ICSD none
Pearson symbol hP4
Space group number 186
Space group symbol $P6_3mc$
AFLOW prototype command aflow --proto=AB_hP4_186_b_a-001
--params=$a, \allowbreak c/a, \allowbreak z_{1}, \allowbreak z_{2}$

  • This is the BN structure found in (Ewald, 1931) p. 95 and (Wilson, 1961) 125-126. (Pease, 1950) later determined that the true boron nitride structure is what is now known as the $B_{k}$ structure. We leave this structure here for historical reasons. It is crystallographically equivalent to, and hence a binary representation of, the buckled graphite structure.
  • Space group $P6_{3}mc$ #186 does not specify the origin of the $z$-axis. Here we chose $z_{1} = 0$ for the boron (2a) site.

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

Basis vectors

Lattice coordinates Cartesian coordinates Wyckoff position Atom type
$\mathbf{B_{1}}$ = $z_{1} \, \mathbf{a}_{3}$ = $c z_{1} \,\mathbf{\hat{z}}$ (2a) N I
$\mathbf{B_{2}}$ = $\left(z_{1} + \frac{1}{2}\right) \, \mathbf{a}_{3}$ = $c \left(z_{1} + \frac{1}{2}\right) \,\mathbf{\hat{z}}$ (2a) N I
$\mathbf{B_{3}}$ = $\frac{1}{3} \, \mathbf{a}_{1}+\frac{2}{3} \, \mathbf{a}_{2}+z_{2} \, \mathbf{a}_{3}$ = $\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{\sqrt{3}}{6}a \,\mathbf{\hat{y}}+c z_{2} \,\mathbf{\hat{z}}$ (2b) B I
$\mathbf{B_{4}}$ = $\frac{2}{3} \, \mathbf{a}_{1}+\frac{1}{3} \, \mathbf{a}_{2}+\left(z_{2} + \frac{1}{2}\right) \, \mathbf{a}_{3}$ = $\frac{1}{2}a \,\mathbf{\hat{x}}- \frac{\sqrt{3}}{6}a \,\mathbf{\hat{y}}+c \left(z_{2} + \frac{1}{2}\right) \,\mathbf{\hat{z}}$ (2b) B I

References

  • A. Brager, X-ray examination of the structure of boron nitride, Acta Physicochimica URSS 7, 699–706 (1937).
  • R. S. Pease, Crystal Structure of Boron Nitride, Nature 165, 722–723 (1950), doi:10.1038/165722b0.
  • P. P. Ewald and C. Hermann, eds., Strukturbericht 1913-1928 (Akademische Verlagsgesellschaft M. B. H., Leipzig, 1931).

Found in

  • A. J. C. Wilson, ed., Structure Reports for 1947–1948, Structure Reports, vol. 18 (N.V.A. Oosthoek's Uitgevers, Utrecht, 1961).

Prototype Generator

aflow --proto=AB_hP4_186_b_a --params=$a,c/a,z_{1},z_{2}$

Species:

Running:

Output: