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Table 1 Slip systems in FCC crystals with their slip plane and Burgers vector b and their Schmid-Boas (SB) notation. The column \(\mathcal {G}^{i}\) lists glissile reactions between slip-system pairs that produce a dislocation on slip system i. Also listed are the Schmid factors Si for four loading orientations: [0 0 1], [1 1 1], [0 1 1] and [4 9 10]

From: Slip-free multiplication and complexity of dislocation networks in FCC metals

Index i

Slip plane

b

SB index i

\(\mathcal {G}^{i}\)

\(S_{i}^{[001]}\)

\(S_{i}^{[111]}\)

\(S_{i}^{[011]}\)

\(S_{i}^{[4\,9\,10]}\)

1

\(\left (\bar {1} 1 1\right)\)

\(\frac {1}{2}\left [0 \bar {1} 1\right ]\)

A2

A3+D6, A6+C3

0.41

0.00

0.00

0.03

2

\(\left (\bar {1} 1 1\right)\)

\(\frac {1}{2}[1 0 1]\)

A3

A2+D6, A6+B2

0.41

0.27

0.41

0.43

3

\(\left (\bar {1} 1 1\right)\)

\(\frac {1}{2}{[1 1 0]}\)

A6

A2+C3, A3+B2

0.00

0.27

0.41

0.40

4

(111)

\(\frac {1}{2}\left [0 \bar {1} 1\right ]\)

B2

B4+C5, B5+D4

0.41

0.00

0.00

0.04

5

(111)

\(\frac {1}{2}\left [\bar {1} 0 1\right ]\)

B4

A2+B5, B2+C5

0.41

0.00

0.41

0.29

6

(111)

\(\frac {1}{2}\left [\bar {1} 1 0\right ]\)

B5

A2+B4, B2+D4

0.00

0.00

0.41

0.24

7

\(\left (\bar {1} \bar {1} 1\right)\)

\(\frac {1}{2}{[0 1 1]}\)

C1

A3+C5, B5+C3

0.41

0.27

0.00

0.12

8

\(\left (\bar {1} \bar {1} 1\right)\)

\(\frac {1}{2}{[1 0 1]}\)

C3

B5+C1, C5+D1

0.41

0.27

0.00

0.09

9

\(\left (\bar {1} \bar {1} 1\right)\)

\(\frac {1}{2}\left [\bar {1} 1 0\right ]\)

C5

A3+C1, C3+D1

0.00

0.00

0.00

0.03

10

\(\left (1 \bar {1} 1\right)\)

\(\frac {1}{2}{[0 1 1]}\)

D1

A6+D4, B4+D6

0.41

0.27

0.00

0.20

11

\(\left (1 \bar {1} 1\right)\)

\(\frac {1}{2}\left [\bar {1} 0 1\right ]\)

D4

A6+D1, C1+D6

0.41

0.00

0.00

0.06

12

\(\left (1 \bar {1} 1\right)\)

\(\frac {1}{2}{[1 1 0]}\)

D6

B4+D1, C1+D4

0.00

0.27

0.00

0.13