
The room-temperature structural properties of the RMn2O5 multiferroics have been investigated under pressure, using powder X-ray scattering and density functional theory (DFT) calculations. It was possible to determine the lattice parameters and the main atomic positions as a function of pressure. Good agreement was observed between the X-ray and DFT results for most of the determined crystallographic data. From the DFT calculations, it was possible to infer the pressure evolution of the exchange interactions, and this analysis led to the conclusion that the onset of the q = (½, 0, ½) magnetic structure under pressure is related to the increase in the J1 super-exchange terms (due to the reduction in the Mn—O distances) compared with the Mn—R exchange interactions. In addition, the 1D antiferromagnetic character of the compounds should be reinforced under pressure.
Supporting information
![]() | Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520619007844/ps5078sup1.cif |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S2052520619007844/ps5078Isup2.hkl |
![]() | Zip compressed file https://doi.org/10.1107/S2052520619007844/ps5078sup3.zip |
![]() | Gzipped compressed file https://doi.org/10.1107/S2052520619007844/ps5078sup4.gz |
![]() | Gzipped compressed file https://doi.org/10.1107/S2052520619007844/ps5078sup5.gz |
![]() | Portable Document Format (PDF) file https://doi.org/10.1107/S2052520619007844/ps5078sup6.pdf |
CCDC reference: 1919948
(I) top
Crystal data top
Mn2O5Pr | c = 5.7154 (5) Å |
Mr = 330.78 | V = 374.28 (5) Å3 |
Orthorhombic, Pbam | Z = 4 |
Hall symbol: -P 2 2ab | Mo Kα radiation, λ = 0.710000 Å |
a = 7.5666 (6) Å | T = 300 K |
b = 8.6545 (6) Å |
Data collection top
Homemade diffractometer | Scan method: step |
Radiation source: rotating-anode X-ray tube | 2θmin = 6.287°, 2θmax = 42.360°, 2θstep = 0.009° |
Refinement top
Rp = 1.280 | 3858 data points |
Rwp = 1.729 | 10 parameters |
Rexp = 6.495 | 0 restraints |
RBragg = 2.757 | (Δ/σ)max = 0.002 |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
x | y | z | Uiso*/Ueq | ||
Pr | 0.1457 (3) | 0.1735 (3) | 0.00000 | 0.00000* | |
Mn1 | 0.00000 | 0.50000 | 0.2544 (11) | 0.00000* | |
Mn2 | 0.4114 (6) | 0.3531 (7) | 0.50000 | 0.00000* | |
O1 | 0.00000 | 0.00000 | 0.26905 | 0.00000* | |
O2 | 0.16565 | 0.44544 | 0.00000 | 0.00000* | |
O3 | 0.13373 | 0.43770 | 0.50000 | 0.00000* | |
O4 | 0.40463 | 0.20287 | 0.25507 | 0.00000* |
Geometric parameters (Å, º) top
Pr—O1 | 2.4115 (19) | Mn1—O4 | 1.8983 (1) |
Pr—O2 | 2.436 (3) | Mn2—O1 | 1.9514 (2) |
Pr—O4 | 2.4553 (18) | Mn2—O3 | 2.225 (5) |
Mn1—O2 | 1.977 (5) | Mn2—O4 | 1.911 (4) |
Mn1—O3 | 1.813 (5) | ||
O2—Mn1—O2 | 81.1 (3) | O1—Mn2—O3 | 95.7 (2) |
O2—Mn1—O3 | 96.9 (2) | O1—Mn2—O4 | 87.4 (2) |
O2—Mn1—O3 | 175.7 (2) | O1—Mn2—O4 | 160.5 (2) |
O2—Mn1—O4 | 87.8 (2) | O3—Mn2—O4 | 101.8 (2) |
O2—Mn1—O4 | 90.3 (2) | O4—Mn2—O4 | 97.5 (2) |
O3—Mn1—O3 | 85.3 (3) | Mn2—O1—Mn2 | 98.0 (2) |
O3—Mn1—O4 | 88.4 (2) | Mn1—O2—Mn1 | 98.98 (2) |
O3—Mn1—O4 | 93.5 (2) | Mn1—O3—Mn1 | 94.7 (2) |
O4—Mn1—O4 | 177.5 (2) | Mn1—O3—Mn2 | 132.4 (2) |
O1—Mn2—O1 | 82.5 (2) | Mn1—O4—Mn2 | 125.6 (2) |