Encyclopedia of Crystallographic Prototypes

AFLOW Prototype: A2B4CD_tI16_82_ac_g_b_d-001

This structure originally had the label A2BCD4_tI16_82_ac_b_d_g. Calls to that address will be redirected here.

If you are using this page, please cite:
D. Hicks, M.J. Mehl, M. Esters, C. Oses, O. Levy, G.L.W. Hart, C. Toher, and S. Curtarolo, The AFLOW Library of Crystallographic Prototypes: Part 3, Comp. Mat. Sci. 199, 110450 (2021). (doi=10.1016/j.commatsci.2021.110450)

Links to this page

https://aflow.org/p/92JU
or https://aflow.org/p/A2B4CD_tI16_82_ac_g_b_d-001
or PDF Version

Kesterite [Cu$_{2}$(Zn,Fe)SnS$_{4}$] Structure: A2B4CD_tI16_82_ac_g_b_d-001

Picture of Structure; Click for Big Picture
Prototype Cu$_{2}$S$_{4}$SnZn
AFLOW prototype label A2B4CD_tI16_82_ac_g_b_d-001
Mineral name kesterite
ICSD 5096
Pearson symbol tI16
Space group number 82
Space group symbol $I\overline{4}$
AFLOW prototype command aflow --proto=A2B4CD_tI16_82_ac_g_b_d-001
--params=$a, \allowbreak c/a, \allowbreak x_{5}, \allowbreak y_{5}, \allowbreak z_{5}$

Other compounds with this structure

Cu$_{2}$ZnSnS$_{4}$


  • The kesterite structure is related to the stannite structure, with differences occurring due to the positioning of the Cu atoms (Hall, 1978). The (2b) Wyckoff position is partially occupied with iron and zinc. We label this site Zn.

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

Basis vectors

Lattice coordinates Cartesian coordinates Wyckoff position Atom type
$\mathbf{B_{1}}$ = $0$ = $0$ (2a) Cu I
$\mathbf{B_{2}}$ = $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{2}$ = $\frac{1}{2}c \,\mathbf{\hat{z}}$ (2b) Sn 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) Cu 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) Zn I
$\mathbf{B_{5}}$ = $\left(y_{5} + z_{5}\right) \, \mathbf{a}_{1}+\left(x_{5} + z_{5}\right) \, \mathbf{a}_{2}+\left(x_{5} + y_{5}\right) \, \mathbf{a}_{3}$ = $a x_{5} \,\mathbf{\hat{x}}+a y_{5} \,\mathbf{\hat{y}}+c z_{5} \,\mathbf{\hat{z}}$ (8g) S I
$\mathbf{B_{6}}$ = $- \left(y_{5} - z_{5}\right) \, \mathbf{a}_{1}- \left(x_{5} - z_{5}\right) \, \mathbf{a}_{2}- \left(x_{5} + y_{5}\right) \, \mathbf{a}_{3}$ = $- a x_{5} \,\mathbf{\hat{x}}- a y_{5} \,\mathbf{\hat{y}}+c z_{5} \,\mathbf{\hat{z}}$ (8g) S I
$\mathbf{B_{7}}$ = $- \left(x_{5} + z_{5}\right) \, \mathbf{a}_{1}+\left(y_{5} - z_{5}\right) \, \mathbf{a}_{2}- \left(x_{5} - y_{5}\right) \, \mathbf{a}_{3}$ = $a y_{5} \,\mathbf{\hat{x}}- a x_{5} \,\mathbf{\hat{y}}- c z_{5} \,\mathbf{\hat{z}}$ (8g) S I
$\mathbf{B_{8}}$ = $\left(x_{5} - z_{5}\right) \, \mathbf{a}_{1}- \left(y_{5} + z_{5}\right) \, \mathbf{a}_{2}+\left(x_{5} - y_{5}\right) \, \mathbf{a}_{3}$ = $- a y_{5} \,\mathbf{\hat{x}}+a x_{5} \,\mathbf{\hat{y}}- c z_{5} \,\mathbf{\hat{z}}$ (8g) S I

References

  • S. Schorr, H.-J. Hoebler, and M. Tovar, A neutron diffraction study of the stannite-kesterite solid solution series, Euro. J. Mineral. 19, 65–73 (2007), doi:10.1127/0935-1221/2007/0019-0065.
  • S. Schoor, The crystal structure of kesterite type compounds: A neutron and X-ray diffraction study, Sol. Energy Mater. Sol. Cells 95, 1482–1488 (2011), doi:10.1016/j.solmat.2011.01.002.

Prototype Generator

aflow --proto=A2B4CD_tI16_82_ac_g_b_d --params=$a,c/a,x_{5},y_{5},z_{5}$

Species:

Running:

Output: