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Next: 3.1.24 IBRAV=213 base-centered monoclinic(C)(底心単斜格子(C)) Up: 3.1 Input of lattice Previous: 3.1.22 IBRAV=13 base-centered monoclinic(B)(底心単斜格子(B))


3.1.23 IBRAV=113 base-centered monoclinic(C)(底心単斜格子(C))

CELLDM(1) $=a$, CELLDM(2) $=b/a$, CELLDM(3) $=c/a$,
CELLDM(4) $=\cos{\beta} (0 < \beta < 180^{\circ})$, $\Omega=abc\sin{\beta}/2$
$({\bf a}_{1},{\bf a}_{2},{\bf a}_{3})= ({\bf x},{\bf y},{\bf z})
\left(
\beg...
...c\cos{\beta} \\
b/2 & b/2 & 0 \\
0 & 0 & c\sin{\beta}
\end{array} \right)$
$({\bf b}_{1},{\bf b}_{2},{\bf b}_{3})= \frac{2 \pi}{a}
({\bf x},{\bf y},{\bf ...
... \frac{\cos{\beta}}{\sin{\beta}} & \frac{a}{c\sin{\beta}}
\end{array} \right)$
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Next: 3.1.24 IBRAV=213 base-centered monoclinic(C)(底心単斜格子(C)) Up: 3.1 Input of lattice Previous: 3.1.22 IBRAV=13 base-centered monoclinic(B)(底心単斜格子(B))
Copyright (C), Tatsuki Oda (oda@cphys.s.kanazawa-u.ac.jp, Kanazawa University)