\textrm{La}_{2}\textrm{CoMnO}_{6}, RT + HT
Contents
\(\textrm{La}_{2}\textrm{CoMnO}_{6}\), RT \(+\) HT¶
Target
Another compound, from another family: the same parent phase
Another High Temperature Distorted Phase:
Finding the Transformation Matrix
Steps
AMPLIMODES for FullProf with the standard: previous parent phase, as usual
Use STRUCTURE RELATIONS: Transformation Matrix
AMPLIMODES with standard: parent phase from the paper
Take the structure from the paper¶
# P 1 21/n 1
014
5.5251 5.4875 7.7786 90.000 89.940 90.000
6
Mn 1 2a 0.00000 0.00000 0.00000
Co 1 2b 0.00000 0.00000 0.50000
La 1 4e -0.00660 0.46450 0.74990
O 1 4e -0.27710 0.21680 -0.03620
O 2 4e -0.79820 0.29420 0.04000
O 3 4e 0.07530 0.01280 0.75800
# P 1 21/c 1
014
7.7786 5.4875 9.5459 90.00 144.63 90.00
6
Mn 1 2a 0.000000 0.000000 0.000000
Co 1 2b 0.500000 0.000000 0.000000
La 1 4e 0.756500 0.464500 0.006600
O 1 4e 0.240900 0.216800 0.277100
O 2 4e 0.838200 0.294200 0.798200
O 3 4e 0.682700 0.012800 -0.075300
…go through \(I\frac{2}{m}\)
# C 1 2/m 1
012
9.8516 5.6861 5.7021 90.00 125.41 90.00
5
Sb 1 2d -0.500000 0.000000 -0.500000
Sc 1 2a 0.000000 0.000000 0.000000
Sr 1 4i -0.249400 0.000000 0.249910
O 1 4i -0.255990 0.000000 -0.304570
O 2 8j -0.023630 0.255510 0.232860
Find the Transformation Matrix with STRUCTURE RELATIONS¶
Lattice Pseudosymmetry
[ Data obtained via CCTBX library ]Result for pseudosymmetry search
Formulae
Input of the program
Initial structure:12 9.8516 5.6861 5.7021 90.00 125.41 90.00 5 Sb 1 2d -0.500000 0.000000 -0.500000 Sc 1 2a 0.000000 0.000000 0.000000 Sr 1 4i -0.249400 0.000000 0.249910 O 1 4i -0.255990 0.000000 -0.304570 O 2 8j -0.023630 0.255510 0.232860Maximum tolerance: 2
Summary search results
Pseudosymmetry search among minimal supergroups within the specialized normalizer and compatible with possible high symmetry lattices.Case # | Supergroup G | Index i | Index ik | (P,p) | Tr. Matrix | Δmax | umax |
---|---|---|---|---|---|---|---|
1 | R-3m (166) | 3 | 1 | 2a+b,-b,-2/3a-1/3b-1/3c ; 0,0,0 |
[ 2 0 -2/3 ] [ 0] [ 1 -1 -1/3 ] [ 0] [ 0 0 -1/3 ] [ 0] |
0.4313 | 0.2726 |
2 | R-3m (166) | 3 | 1 | 2a+b,-b,-2/3a-1/3b-1/3c ; 1,1/2,0 |
[ 2 0 -2/3 ] [ 1] [ 1 -1 -1/3 ] [ 1/2] [ 0 0 -1/3 ] [ 0] |
>tol | - |
Idealized structures
1# Supergroup R-3m (166): 2a+b,-b,-2/3a-1/3b-1/3c ; 0,0,0 and index 3
Displacements:Atom | Idealized Coordinates | ux | uy | uz | |u| |
---|---|---|---|---|---|
Sb1 | (0.5000, 0.0000, 0.5000) | 0.000000 | 0.000000 | 0.000000 | 0.0000 |
Sc1 | (0.0000, 0.0000, 0.0000) | 0.000000 | 0.000000 | 0.000000 | 0.0000 |
Sr1 | (0.7500, 0.0000, 0.2499) | 0.000630 | 0.000000 | 0.000000 | 0.0062 |
O1 | (0.7440, 0.0000, 0.7432) | 0.000007 | 0.000000 | -0.047807 | 0.2726 |
O2 | (0.0004, 0.2556, 0.2568) | -0.024013 | -0.000103 | -0.023903 | 0.1928 |
NOTE: ux, uy and uz are given in relative units. |u| is the absolute displacement given in Å
Idealized structure (subgroup setting):
12 9.8516 5.6861 5.7021 90.00 125.41 90.00 5 Sb 1 2d 0.500000 0.000000 0.500000 Sc 1 2a 0.000000 0.000000 0.000000 Sr 1 4i 0.749970 0.000000 0.249910 O 1 4i 0.744003 0.000000 0.743237 O 2 8j 0.000383 0.255613 0.256763Idealized structure (supergroup setting):
166 5.6874 5.6861 13.9422 90.00 89.79 119.99 4 Sb 1 3b 0.666667 0.333333 0.833333 Sc 1 3a 0.000000 0.000000 0.000000 Sr 1 6c 0.333333 0.666667 0.916697 O 1 18h 0.992515 0.496257 0.752254Notes:
- Idealized structure with space group 166 related with the given by the transformation 2a+b,-b,-2/3a-1/3b-1/3c ; 0,0,0 and index 3
- Cell parameters have not been symmetrized. They may include in general some symmetry breaking strain, to be removed by hand.
- Some problems might be present in the assignment of Wyckoff positions of the idealized orbits due to the decimal point errors.
AMPLIMODES for FullProf with standard, previous parent¶
225
8.087481 8.087481 8.087481 90.00000 90.00000 90.00000
4
Mn 1 4a 0.000000 0.000000 0.000000
Co 1 4b 0.500000 0.500000 0.500000
La 1 8c 0.250000 0.250000 0.250000
O 1 24e 0.254100 0.000000 0.000000
# R -3 m
166
5.6874 5.6861 13.9422 90.00 89.79 119.99
4
Mn 1 3b 0.666667 0.333333 0.833333
Co 1 3a 0.000000 0.000000 0.000000
La 1 6c 0.333333 0.666667 0.916697
O 1 18h 0.992515 0.496257 0.752254
2a+b,-b,-2/3a-1/3b-1/3c; 0 0 0