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Next: 3.1.22 IBRAV=13 base-centered monoclinic(B)(底心単斜格子(B)) Up: 3.1 Input of lattice Previous: 3.1.20 IBRAV=12 simple monoclinic


3.1.21 IBRAV=112 simple monoclinic lattice(単純単斜格子)

CELLDM(1) $=a$, CELLDM(2) $=b/a$, CELLDM(3) $=c/a$,
CELLDM(4) $=\cos{\beta} (0 < \beta < 180^{\circ})$, $\Omega=abc\sin{\beta}$
$({\bf a}_{1},{\bf a}_{2},{\bf a}_{3})= ({\bf x},{\bf y},{\bf z})
\left(
\beg...
...0 & c\cos{\beta} \\
0 & b & 0 \\
0 & 0 & c\sin{\beta}
\end{array} \right)$
$({\bf b}_{1},{\bf b}_{2},{\bf b}_{3})= \frac{2 \pi}{a}
({\bf x},{\bf y},{\bf ...
...rac{\cos{\beta}}{\sin{\beta}} & 0 & \frac{a}{c\sin{\beta}}
\end{array} \right)$
Calculation example(計算例):solid oxyden$\alpha$phase(Anti-ferromagnetic)(固体酸素$\alpha$相(反強磁性))
next up previous contents index
Next: 3.1.22 IBRAV=13 base-centered monoclinic(B)(底心単斜格子(B)) Up: 3.1 Input of lattice Previous: 3.1.20 IBRAV=12 simple monoclinic
Copyright (C), Tatsuki Oda (oda@cphys.s.kanazawa-u.ac.jp, Kanazawa University)