Incommensurate modulated structure of BaMnF4with monoclinic symmetry at 100 and 210K

Authors:

Sciau, Ph.; Lapasset, J.; Grebille, D.; Berar, J.F.

Journal:

Acta Cryst. B 44 108-116 (1988)

DOI:

https://doi.org/10.1107/S0108768187010280

B-IncStrDB ID: 202EZImNU Entry date: 2010-11-08 Last revision: 2021-12-30

BaMn210

Chemical data


Structural Formula Sum: Ba1 F4 Mn1 [ Help ]

Formula weight: 268.3 Da [ Help ]

Crystallographic data and experimental details


a: 6.01(1) Å [ Help ]

b: 30.32(6) Å [ Help ]

c: 8.44(2) Å [ Help ]

α: 90 ° [ Help ]

β: 90 ° [ Help ]

γ: 90 ° [ Help ]

Volume: 1538(5) Å3 [ Help ]

μ: 6.698 mm-1 [ Help ]

Z: 8 [ Help ]

Cell measurement temperature: 210 K [ Help ]

Crystal system: monoclinic [ Help ]

Superspace group name (WJJ): U:A 21 1 1:1 1 1 [ Help ]

Superspace group name: X21(α00)0 [ Help ]

Symmetry operations of the superspace group: [ Help ]

Operation code Operation in algebraic form
1 x1,x2,x3,x4
2 1/2+x1,-x2,-x3,x4
3 x1,1/2+x2,1/2+x3,x4
4 1/2+x1,1/2-x2,1/2-x3,x4
5 x1,1/2+x2,x3,1/2+x4
6 1/2+x1,1/2-x2,-x3,1/2+x4
7 x1,x2,1/2+x3,1/2+x4
8 1/2+x1,-x2,1/2-x3,1/2+x4

Space group name (H-M): A 21 1 1 [ Help ]

Symmetry operations of the space group: [ Help ]

Operation code Operation in algebraic form
1 x,y,z
2 1/2+x,-y,-z
3 x,1/2+y,1/2+z
4 1/2+x,1/2-y,1/2-z
5 x,1/2+y,z
6 1/2+x,1/2-y,-z
7 x,y,1/2+z
8 1/2+x,-y,1/2-z

Modulation dimension: 1 [ Help ]

Measured independent wave vectors: [ Help ]

Wave vector id q_x q_y q_z
1 0.395 0 0

Refinement details


Refinement remarks: Anisotropic temperature factors refined for reflections with 0.38 [ Help ]

Modulation functions description: Displacive modulation:Fourier series. Up to 2nd-order harmonics. [ Help ]

Structure factors calc. details: Gaussian integration [ Help ]

Nb. of observed reflections: 3844 [ Help ]

R(obs): 0.0561 [ Help ]

Structural Information


Average Structure: [ Help ]

Atom site label Atom symbol Symmetry multiplicity Occupancy x y z Uiso/equiv ADP type
Ba Ba 8 1 0.4480 0.17227(2) 0.2504(2) 0.0100(3) Uani
Mn Mn 8 1 -0.0050(2) 0.20806(3) 0.0015(5) 0.0065(3) Uani
F1 F 8 1 0.1976(7) 0.1500(2) 0.0073(10) 0.009(1) Uani
F2 F 8 1 0.7213(8) 0.1680(2) 0.0056(10) 0.012(1) Uani
F3 F 8 1 0.3347(8) 0.2319(2) 0.0034(12) 0.015(1) Uani
F4 F 8 1 0.0245(10) 0.2110(2) 0.2518(13) 0.027(1) Uani

Fourier Wave Vectors (explicit: q_x,q_y,q_z or coefficients: q_1,q_2,...): [ Help ]

Wave vector code q_x q_y q_z
1 0.395 0 0
2 0.790 0 0

Definition of the displacive (translational) Fourier series: [ Help ]

Modulation code Atom site label Displacement axis Wave vector code
Bax1 Ba x 1
Bax2 Ba x 2
Bay1 Ba y 1
Bay2 Ba y 2
Baz1 Ba z 1
Baz2 Ba z 2
Mnx1 Mn x 1
Mnx2 Mn x 2
Mny1 Mn y 1
Mny2 Mn y 2
Mnz1 Mn z 1
Mnz2 Mn z 2
F1x1 F1 x 1
F1x2 F1 x 2
F1y1 F1 y 1
F1y2 F1 y 2
F1z1 F1 z 1
F1z2 F1 z 2
F2x1 F2 x 1
F2x2 F2 x 2
F2y1 F2 y 1
F2y2 F2 y 2
F2z1 F2 z 1
F2z2 F2 z 2
F3x1 F3 x 1
F3x2 F3 x 2
F3y1 F3 y 1
F3y2 F3 y 2
F3z1 F3 z 1
F3z2 F3 z 2
F4x1 F4 x 1
F4x2 F4 x 2
F4y1 F4 y 1
F4y2 F4 y 2
F4z1 F4 z 1
F4z2 F4 z 2

Displacive (translational) Fourier coefficients: [ Help ]

Modulation code Cosine coefficient Sine coefficient
Bax1 0.0128 0.0141(2)
Bax2 -0.0002(2) 0.0038(3)
Bay1 0.00356(4) 0.00305(4)
Bay2 0.00046(4) 0.00127(3)
Baz1 -0.0009(1) -0.0002(1)
Baz2 0.0006(2) -0.0011(2)
Mnx1 -0.0014(3) -0.0010(3)
Mnx2 0.0003(5) 0.0007(5)
Mny1 0.00016(6) -0.00049(5)
Mny2 0.00066(7) -0.00015(7)
Mnz1 0.0032(2) 0.0005(2)
Mnz2 0.0013(6) -0.0022(5)
F1x1 0.0001(10) -0.0019(11)
F1x2 0.0007(18) -0.0003(18)
F1y1 0.0006(2) -0.0006(2)
F1y2 0.0004(3) -0.0003(3)
F1z1 0.0097(9) 0.0129(8)
F1z2 0.0015(17) -0.0052(17)
F2x1 -0.0061(13) 0.0013(12)
F2x2 -0.0010(18) 0.0028(18)
F2y1 0.0027(3) -0.0011(3)
F2y2 0.0011(3) -0.0001(3)
F2z1 -0.0068(9) -0.0096(9)
F2z2 -0.0022(17) 0.0021(16)
F3x1 -0.0056(13) 0.0013(12)
F3x2 -0.0004(20) -0.0015(22)
F3y1 0.0007(3) -0.0012(3)
F3y2 0.0010(3) 0.0003(3)
F3z1 -0.0237(10) -0.0071(10)
F3z2 0.0015(22) 0.0073(18)
F4x1 0.0248(15) 0.0060(16)
F4x2 -0.0083(24) 0.0015(30)
F4y1 0.0048(4) 0.0079(3)
F4y2 0.0006(4) -0.0013(5)
F4z1 0.0018(12) 0.0009(10)
F4z2 -0.0041(20) -0.0046(20)