Table 3 System sizes and integration parameters used in this study. In each case, simulations were performed using the number of atoms indicated as Nj + 1 (=2N j ).

From: No system-size anomalies in entropy of bcc iron at Earth’s inner-core conditions

j

bcc

hcp

N j  → Nj + 1

Supercell

λ m

n λ

N j  → Nj + 1

Supercell

λ m

n λ

0

512 → 1024

8 × 8 × (4 → 8)

19.0

227

192 → 384

6 × 4 × (2 → 4)

19.0

201

1

1024 → 2048

(8 → 16) × 8 × 8

19.0

130

384 → 768

(6 → 12) × 4 × 4

19.0

111

2

2048 → 4096

16 × (8 → 16) × 8

10.0

52

768 → 1 536

12 × (4 → 8) × 4

10.0

50

3

4096 → 8192

16 × 16 × (8 → 16)

10.0

43

1536 → 3072

12 × 8 × (4 → 8)

9.6

41

4

8192 → 16384

(16 → 32) × 16 × 16

10.0

42

3072 → 6144

(12 → 24) × 8 × 8

9.6

41

5

16384 → 32768

32 × (16 → 32) × 16

10.0

7

6144 → 12288

24 × (8 → 16) × 8

9.6

20

6

32768 → 65536

32 × 32 × (16 → 32)

8.4

5

12288 → 24576

24 × 16 × (8 → 16)

9.6

14

  1. Integration is performed for λ from 0 to λm, using n λ steps, and yields ΔA(N j ) ≡ A(Nj + 1) − A(N j ). For hcp, λ steps are equally spaced, but in bcc the separation varies along the path.