k - IUCr Journals

0k - phase I (Cmc21, 295 K)
1
3
5
→ k
bI*
cI*
h + k = 2n + 1, absent (C lattice)
1k - phase I (Cmc21, 295 K)
2
4
6
→ k
bI*
cI*
h + k = 2n + 1, absent (C lattice)
2k - phase I (Cmc21, 295 K)
1
3
5
→ k
bI*
cI*
h + k = 2n + 1, absent (C lattice)
3k - phase I (Cmc21, 295 K)
2
4
6
→ k
bI*
cI*
h + k = 2n + 1, absent (C lattice)
h0 - phase I (Cmc21, 295 K)
1 3 5 7 9
→ h
aI*
cI*
h + k = 2n + 1, absent (C lattice)
h1 - phase I (Cmc21, 295 K)
2 4 6 8 10
→ h
aI*
cI*
h + k = 2n + 1, absent (C lattice)
h2 - phase I (Cmc21, 295 K)
1 3 5 7 9
→ h
aI*
cI*
h + k = 2n + 1, absent (C lattice)
h3 - phase I (Cmc21, 295 K)
2 4 6 8 10
→ h
aI*
cI*
h + k = 2n + 1, absent (C lattice)
hk0 - phase I (Cmc21, 295 K)
2 4 6 8 10
→ h
aI*
1
2
3
4
5
6
↓
k
bI*
h + k = 2n + 1, absent (C lattice)
hk1 - phase I (Cmc21, 295 K)
2 4 6 8 10
→ h
aI*
1
2
3
4
5
6
↓
k
bI*
h + k = 2n + 1, absent (C lattice)
hk2 - phase I (Cmc21, 295 K)
2 4 6 8 10
→ h
aI*
1
2
3
4
5
6
↓
k
bI*
h + k = 2n + 1, absent (C lattice)
hk3 - phase I (Cmc21, 295 K)
2 4 6 8 10
→ h
aI*
1
2
3
4
5
6
↓
k
bI*
h + k = 2n + 1, absent (C lattice)
0k - phase II (Pbc21, 210 K)
1
3
5
→ k
bII*
cII*
h + k = 2n, systematically stronger
h + k = 2n + 1, systematically weaker
1k - phase II (Pbc21, 210 K)
2
4
6
→ k
bII*
cII*
h + k = 2n, systematically stronger
h + k = 2n + 1, systematically weaker
2k - phase II (Pbc21, 210 K)
1
3
5
→ k
bII*
cII*
h + k = 2n, systematically stronger
h + k = 2n + 1, systematically weaker
3k - phase II (Pbc21, 210 K)
2
4
6
→ k
bII*
cII*
h + k = 2n, systematically stronger
h + k = 2n + 1, systematically weaker
h0 - phase II (Pbc21, 210 K)
1 3 5 7 9
→ h
aII*
cII*
h + k = 2n, systematically stronger
h + k = 2n + 1, systematically weaker
h1 - phase II (Pbc21, 210 K)
2 4 6 8 10
→ h
aII*
cII*
h + k = 2n, systematically stronger
h + k = 2n + 1, systematically weaker
h2 - phase II (Pbc21, 210 K)
1 3 5 7 9
→ h
aII*
cII*
h + k = 2n, systematically stronger
h + k = 2n + 1, systematically weaker
h3 - phase II (Pbc21, 210 K)
2 4 6 8 10
→ h
aII*
cII*
h + k = 2n, systematically stronger
h + k = 2n + 1, systematically weaker
hk0 - phase II (Pbc21, 210 K)
2 4 6 8 10
→ h
aII*
1
2
3
4
5
6
↓
k
bII*
h + k = 2n, systematically stronger
h + k = 2n + 1, systematically weaker
hk1 - phase II (Pbc21, 210 K)
2 4 6 8 10
→ h
aII*
1
2
3
4
5
6
↓
k
bII*
h + k = 2n, systematically stronger
h + k = 2n + 1, systematically weaker
hk2 - phase II (Pbc21, 210 K)
2 4 6 8 10
→ h
aII*
1
2
3
4
5
6
↓
k
bII*
h + k = 2n, systematically stronger
h + k = 2n + 1, systematically weaker
hk3 - phase II (Pbc21, 210 K)
2 4 6 8 10
→ h
aII*
1
2
3
4
5
6
↓
k
bII*
h + k = 2n, systematically stronger
h + k = 2n + 1, systematically weaker
0k - phase III (Pbn21, 110 K)
4
8
12
→ k
bIII*
cIII*
1k - phase III (Pbn21, 110 K)
2
6
8
→ k
bIII*
cIII*
2k - phase III (Pbn21, 110 K)
4
8
12
→ k
bIII*
cIII*
3k - phase III (Pbn21, 110 K)
2
6
8
→ k
bIII*
cIII*
h0 - phase III (Pbn21, 110 K)
aIII*
cIII*
h1 - phase III (Pbn21, 110 K)
aIII*
cIII*
h2 - phase III (Pbn21, 110 K)
aIII*
cIII*
h3 - phase III (Pbn21, 110 K)
aIII*
cIII*
hk0 - phase III (Pbn21, 110 K)
aIII*
bIII*
hk1 - phase III (Pbn21, 110 K)
aIII*
bIII*
hk2 - phase III (Pbn21, 110 K)
aIII*
bIII*
hk3 - phase III (Pbn21, 110 K)
aIII*
bIII*