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MAGNDATA: A Collection of magnetic structures with portable cif-type files

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HoNiO3 (#2.3)

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Magnetic structure with all atoms

Magnetic structure with only magnetic atoms


Reference: M.T. Fernandez-Diaz, J.A. Alonso, M.J. Martinez-Lope, M.T. Casais and J.L. Garcia-Munoz, Physical Review B (2001) 64.
DOI: 10.1103/physrevb.64.144417
Atomic positions from: ICSD #88042

Parent space group (paramagnetic phase): P21/n (#14) (non-standard)
Transformation to a standard setting: (a,b,a+c;0,0,0)
    [View matrix form]
Propagation vector(s):
k1 (1/2, 0, 1/2)
k2 (0, 0, 0)

Transition Temperature: 3 K
Experiment Temperature: 1.5 K

Lattice parameters of the magnetic unit cell:
10.3640 5.5105 14.8467 90.0000 90.0840 90.0000
Transformation from parent structure: (2a,b,2c;0,0,0)
    [View matrix form]

BNS Magnetic Space Group: P21 (#4.7) (non-standard)
    [View symmetry operations]
Transformation to a standard setting: (a/2+c/2,-b,a/2-c/2;7/8,0,1/8)
    [View matrix form]
Systematic absences for this Magnetic Space Group via

Magnetic Point Group: 2.1 (3.1.6)
    [View symmetry operations]
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

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LabelAtom typexyzMultiplicitySymmetry constraints on MMxMyMz|M|
Ho1_1Ho-0.009090.071770.125154mx,my,mz-3.14-6.71-1.57.56
Ho1_2Ho0.490910.071770.125154mx,my,mz-3.14-6.71-1.57.56
Ho1_3Ho0.50909-0.071770.374854mx,my,mz3.146.711.57.56
Ho1_4Ho0.50909-0.07177-0.125154mx,my,mz3.146.711.57.56
Ni1_1Ni0.250000.000000.000004mx,my,mz0.90.01.11.42
Ni1_2Ni0.250000.000000.500004mx,my,mz-0.90.0-1.11.42
Ni2_1Ni0.250000.000000.250004mx,my,mz0.350.0-0.40.53
Ni2_2Ni0.250000.00000-0.250004mx,my,mz-0.350.00.40.53

    [Show all magnetic atoms in unit cell and their moment relations]



Active Irreps:                                           
Irrep decomposition via


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