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表1 fcc结构材料的滑移系

Table 1 Slip systems of the fcc crystal

α	$M_{s} = m_{s}^{α} \otimes n_{s}^{α}$	α	$M_{s} = m_{s}^{α} \otimes n_{s}^{α}$
1	$[01 \bar{1}] \otimes (111) / \sqrt[]{6}$	7	$[011] \otimes (1 \bar{1} 1) / \sqrt[]{6}$
2	$[10 \bar{1}] \otimes (111) / \sqrt[]{6}$	8	$[10 \bar{1}] \otimes (1 \bar{1} 1) / \sqrt[]{6}$
3	$[1 \bar{1} 0] \otimes (111) / \sqrt[]{6}$	9	$[110] \otimes (1 \bar{1} 1) / \sqrt[]{6}$
4	$[01 \bar{1}] \otimes (\bar{1} 11) / \sqrt[]{6}$	10	$[011] \otimes (11 \bar{1}) / \sqrt[]{6}$
5	$[101] \otimes (\bar{1} 11) / \sqrt[]{6}$	11	$[101] \otimes (11 \bar{1}) / \sqrt[]{6}$
6	$[110] \otimes (\bar{1} 11) / \sqrt[]{6}$	12	$[1 \bar{1} 0] \otimes (11 \bar{1}) / \sqrt[]{6}$