Parameter: index = 0.1004
MAGNDATA - Collection of Magnetic Structures
MAGNDATA
Collection of Magnetic Structures
MAGNDATA: A Collection of magnetic structures with portable cif-type files Log in
Magnetic structure with all atoms Magnetic structure with only magnetic atoms
Reference: R. A. Ewings, M. Reehuis, F. Orlandi, P. Manuel, D. D. Khalyavin, A. S. Gibbs, A. D. Fortes, A. Hoser, A. J. Princep, M. Jansen, PHYSICAL REVIEW B (2023) 108 174412DOI: 10.1103/PhysRevB.108.174412 Atomic positions from: same referenceParent space group (paramagnetic phase): Pnam (#62) (non-standard)
Transformation to a standard setting: (a ,-c ,b ;0,0,0)
[View matrix form]
Transformation matrix from the parent setting (a
p ,b
p ,c
p ) to the standard setting of the parent space group (a
pst ,b
pst ,c
pst ):
[Hide] Propagation vector: k1 (0, 0, 0)
Transition Temperature: 10 KExperiment Temperature: 1.5 K
Lattice parameters of the magnetic unit cell:
8.72710 4.39760 7.33860 90.00 90.00 90.00Transformation from parent structure: (a ,b ,c ;0,0,0)
[View matrix form]
Transformation matrix from the setting of the parent structure (a
p ,b
p ,c
p ) to the working setting (a,b,c):
[Hide]
BNS Magnetic Space Group: Pn'a'm' (#62.449) (non-standard)
[View symmetry operations] Symmetry operations of the magnetic space group in the setting used:
N (x,y,z) Seitz notation 1 x,y,z,+1 { 1 | 0 }
2 x+1/2,-y+1/2,-z+1/2,+1 { 2100 | 1/2 1/2 1/2 }
3 -x,-y,z+1/2,+1 { 2001 | 0 0 1/2 }
4 -x+1/2,y+1/2,-z,+1 { 2010 | 1/2 1/2 0 }
5 -x,-y,-z,-1 { -1' | 0 }
6 -x+1/2,y+1/2,z+1/2,-1 { m'100 | 1/2 1/2 1/2 }
7 x,y,-z+1/2,-1 { m'001 | 0 0 1/2 }
8 x+1/2,-y+1/2,z,-1 { m'010 | 1/2 1/2 0 }
[Hide] Transformation to a standard setting: (a ,-c ,b ;0,0,0) [View matrix form]
Transformation matrix from the working setting (a,b,c) to the standard setting of the magnetic space group (a
s ,b
s ,c
s ):
[Hide] Systematic absences for this Magnetic Space Group via Magnetic Point Group: m'm'm' (8.5.28)
[View symmetry operations]
Symmetry operations of the magnetic point group in the setting used:
N (x,y,z) Seitz notation 1 x,y,z,+1 1
2 x,-y,-z,+1 2100
3 -x,-y,z,+1 2001
4 -x,y,-z,+1 2010
5 -x,-y,-z,-1 -1'
6 -x,y,z,-1 m'100
7 x,y,-z,-1 m'001
8 x,-y,z,-1 m'010
[Hide] Symmetry-adapted form of material tensors via Symmetry-adapted form of material tensors for domain-related equivalent structures via Positions and magnetic moments of symmetry independent atoms:
From now on, magnetic atoms are in boldface and colored in red . Magnetic moments are expressed in units of μB [Show only magnetic atoms] Use MVISUALIZE to: [Show all the atoms] Magnetic atoms :
Label Atom type x y z Multiplicity Symmetry constraints on M Mx My Mz |M |
O1 O 0.87470 0.24720 0.15944 8 mx ,my ,mz 0.025 -0.256 0.0 0.26
Non-magnetic atoms :
Label Atom type x y z Multiplicity
Cs1 Cs 0.37930 0.21420 0.75000 4
[Show all atoms in unit cell and their moment relations]
Positions and magnetic moments of all atoms in unit cell, with magnetic moment relations explicitly given:
Magnetic atoms :
Set of atoms in the unit cell related by symmetry with the magnetic atom O1:
Atom x y z Symmetry constraints on M Mx My Mz
1 0.87470 0.24720 0.15944 mx ,my ,mz 0.02500 -0.25600 0.00000 2 0.37470 0.25280 0.34056 mx ,-my ,-mz 0.02500 0.25600 0.00000 3 0.12530 0.75280 0.65944 -mx ,-my ,mz -0.02500 0.25600 0.00000 4 0.62530 0.74720 0.84056 -mx ,my ,-mz -0.02500 -0.25600 0.00000 5 0.12530 0.75280 0.84056 -mx ,-my ,-mz -0.02500 0.25600 0.00000 6 0.62530 0.74720 0.65944 -mx ,my ,mz -0.02500 -0.25600 0.00000 7 0.87470 0.24720 0.34056 mx ,my ,-mz 0.02500 -0.25600 0.00000 8 0.37470 0.25280 0.15944 mx ,-my ,mz 0.02500 0.25600 0.00000
Non-magnetic atoms :
Set of atoms in the unit cell related by symmetry with the atom Cs1:
Atom x y z
1 0.37930 0.21420 0.75000 2 0.87930 0.28580 0.75000 3 0.62070 0.78580 0.25000 4 0.12070 0.71420 0.25000
[Hide]
Label Atom type x y z Multiplicity Symmetry constraints on M Mx My Mz |M |
O1 O 0.87470 0.24720 0.15944 8 mx ,my ,mz 0.025 -0.256 0.0 0.26
[Show all magnetic atoms in unit cell and their moment relations]
Positions and magnetic moments of all atoms in unit cell, with magnetic moment relations explicitly given:
Set of atoms in the unit cell related by symmetry with the magnetic atom O1:
Atom x y z Symmetry constraints on M Mx My Mz
1 0.87470 0.24720 0.15944 mx ,my ,mz 0.02500 -0.25600 0.00000 2 0.37470 0.25280 0.34056 mx ,-my ,-mz 0.02500 0.25600 0.00000 3 0.12530 0.75280 0.65944 -mx ,-my ,mz -0.02500 0.25600 0.00000 4 0.62530 0.74720 0.84056 -mx ,my ,-mz -0.02500 -0.25600 0.00000 5 0.12530 0.75280 0.84056 -mx ,-my ,-mz -0.02500 0.25600 0.00000 6 0.62530 0.74720 0.65944 -mx ,my ,mz -0.02500 -0.25600 0.00000 7 0.87470 0.24720 0.34056 mx ,my ,-mz 0.02500 -0.25600 0.00000 8 0.37470 0.25280 0.15944 mx ,-my ,mz 0.02500 0.25600 0.00000
[Hide] Active Irreps:
label dim. small irrep dim. full irrep action number of modes mGM1-
1
1
primary
2
Comments:
NPD
Position structure from a measurement at 10K
Non-standard Pnam parent setting
The magnetic moments were located at the mass centers of the O2- units and the form factor for s=1/2 O2- ions was used in the fit.
Here, due to format restrictions, the reported for these O2- ions have been halbed and located at each of the reported positions of the oxygen atoms.
The pairs of oxygens forming the O2- ions, are forced by symmetry to have opposite z moments components.
Comments (symmetry):
1k magnetic structure
k-maximal magnetic symmetry
1-dim irrep