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The absolute structure has been determined for MnSi with data collected using synchrotron radiation with E = 78.3 keV (0.158 Å). At this energy, the resonant scattering contribution from MnSi is very small (f′Mn = −0.0397, f′′Mn = 0.0385, f′Si = −0.0197, f′′Si = 0.0027), but the large number of observed Bijvoet differences together with a wide Q range make absolute structure determination possible. A comparison with the data collected at E = 18 keV (0.68 Å) (f′Mn = 0.2858, f′′Mn = 0.6739, f′Si = 0.0653, f′′Si = 0.0646) for the same crystal shows the correctness of the absolute structure measured at the higher energy. A similar data collection has also been done at E = 65.3 keV (0.19 Å) for a single crystal of Fe0.7Co0.3Si with known absolute structure. In all cases, the absolute structure was correctly determined by analysing the statistical distribution of the chirality measure. Statistical descriptors of the refinements, the Flack parameter and the distribution of Parsons quotients are discussed for all presented experiments.
Supporting information
CCDC references: 1474065; 1474066; 1474067
For all compounds, program(s) used to refine structure: SHELXL2014/7 (Sheldrick, 2014).
Crystal data top
MnSi | Dx = 5.808 Mg m−3 |
Mr = 83.03 | Synchrotron radiation, λ = 0.68894 Å |
Cubic, P213 | Cell parameters from 715 reflections |
a = 4.5622 (3) Å | θ = 4.3–32.3° |
V = 94.96 (2) Å3 | µ = 12.76 mm−1 |
Z = 4 | T = 293 K |
F(000) = 156 | Block, metallic dark grey |
Data collection top
Pilatus@SNBL diffractometer | 127 reflections with I > 2σ(I) |
Radiation source: ESRF bending magnet | Rint = 0.026 |
Silicon monochromator | θmax = 32.3°, θmin = 6.1° |
φ scan | h = −6→6 |
797 measured reflections | k = −7→7 |
127 independent reflections | l = −6→6 |
Refinement top
Refinement on F2 | w = 1/[σ2(Fo2) + (0.053P)2] where P = (Fo2 + 2Fc2)/3 |
Least-squares matrix: full | (Δ/σ)max < 0.001 |
R[F2 > 2σ(F2)] = 0.036 | Δρmax = 0.96 e Å−3 |
wR(F2) = 0.074 | Δρmin = −1.29 e Å−3 |
S = 1.34 | Extinction correction: SHELXL-2014/7 (Sheldrick 2014, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
127 reflections | Extinction coefficient: 0.63 (11) |
8 parameters | Absolute structure: Flack x determined using 46 quotients [(I+)-(I-)]/[(I+)+(I-)]
(Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259). |
0 restraints | Absolute structure parameter: 0.06 (2) |
Special details top
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes)
are estimated using the full covariance matrix. The cell esds are taken
into account individually in the estimation of esds in distances, angles
and torsion angles; correlations between esds in cell parameters are only
used when they are defined by crystal symmetry. An approximate (isotropic)
treatment of cell esds is used for estimating esds involving l.s. planes. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Mn01 | 0.13683 (11) | 0.13683 (11) | 0.13683 (11) | 0.0169 (5) | |
Si02 | 0.8453 (2) | 0.8453 (2) | 0.8453 (2) | 0.0182 (5) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Mn01 | 0.0169 (5) | 0.0169 (5) | 0.0169 (5) | 0.00003 (11) | 0.00003 (11) | 0.00003 (11) |
Si02 | 0.0182 (5) | 0.0182 (5) | 0.0182 (5) | −0.0007 (2) | −0.0007 (2) | −0.0007 (2) |
Geometric parameters (Å, º) top
Mn01—Si02i | 2.304 (2) | Si02—Mn01xiii | 2.304 (2) |
Mn01—Si02ii | 2.3977 (13) | Si02—Mn01xiv | 2.3977 (13) |
Mn01—Si02iii | 2.3977 (13) | Si02—Mn01xv | 2.3977 (13) |
Mn01—Si02iv | 2.3977 (13) | Si02—Mn01xvi | 2.3977 (13) |
Mn01—Si02v | 2.5482 (9) | Si02—Mn01xvii | 2.5482 (9) |
Mn01—Si02vi | 2.5482 (9) | Si02—Mn01xviii | 2.5482 (9) |
Mn01—Si02vii | 2.5482 (9) | Si02—Mn01xix | 2.5482 (9) |
Mn01—Mn01viii | 2.7980 (2) | Si02—Si02xx | 2.8200 (4) |
Mn01—Mn01ix | 2.7980 (2) | Si02—Si02xxi | 2.8200 (4) |
Mn01—Mn01x | 2.7980 (2) | Si02—Si02xxii | 2.8200 (4) |
Mn01—Mn01xi | 2.7980 (2) | Si02—Si02xxiii | 2.8200 (4) |
Mn01—Mn01xii | 2.7980 (2) | Si02—Si02xxiv | 2.8200 (4) |
| | | |
Si02i—Mn01—Si02ii | 73.68 (2) | Mn01xiii—Si02—Mn01xiv | 137.64 (3) |
Si02i—Mn01—Si02iii | 73.68 (2) | Mn01xiii—Si02—Mn01xv | 137.64 (3) |
Si02ii—Mn01—Si02iii | 112.431 (17) | Mn01xiv—Si02—Mn01xv | 71.39 (5) |
Si02i—Mn01—Si02iv | 73.68 (2) | Mn01xiii—Si02—Mn01xvi | 137.64 (3) |
Si02ii—Mn01—Si02iv | 112.431 (17) | Mn01xiv—Si02—Mn01xvi | 71.39 (5) |
Si02iii—Mn01—Si02iv | 112.431 (17) | Mn01xv—Si02—Mn01xvi | 71.39 (5) |
Si02i—Mn01—Si02v | 140.288 (13) | Mn01xiii—Si02—Mn01xvii | 70.22 (4) |
Si02ii—Mn01—Si02v | 69.45 (2) | Mn01xiv—Si02—Mn01xvii | 114.19 (4) |
Si02iii—Mn01—Si02v | 107.34 (6) | Mn01xv—Si02—Mn01xvii | 134.54 (5) |
Si02iv—Mn01—Si02v | 134.54 (5) | Mn01xvi—Si02—Mn01xvii | 68.826 (14) |
Si02i—Mn01—Si02vi | 140.288 (13) | Mn01xiii—Si02—Mn01xviii | 70.22 (4) |
Si02ii—Mn01—Si02vi | 134.54 (5) | Mn01xiv—Si02—Mn01xviii | 134.54 (5) |
Si02iii—Mn01—Si02vi | 69.45 (2) | Mn01xv—Si02—Mn01xviii | 68.826 (14) |
Si02iv—Mn01—Si02vi | 107.34 (6) | Mn01xvi—Si02—Mn01xviii | 114.19 (4) |
Si02v—Mn01—Si02vi | 67.19 (2) | Mn01xvii—Si02—Mn01xviii | 109.17 (4) |
Si02i—Mn01—Si02vii | 140.288 (13) | Mn01xiii—Si02—Mn01xix | 70.22 (4) |
Si02ii—Mn01—Si02vii | 107.34 (6) | Mn01xiv—Si02—Mn01xix | 68.826 (14) |
Si02iii—Mn01—Si02vii | 134.54 (5) | Mn01xv—Si02—Mn01xix | 114.19 (4) |
Si02iv—Mn01—Si02vii | 69.45 (2) | Mn01xvi—Si02—Mn01xix | 134.54 (5) |
Si02v—Mn01—Si02vii | 67.19 (2) | Mn01xvii—Si02—Mn01xix | 109.17 (4) |
Si02vi—Mn01—Si02vii | 67.19 (2) | Mn01xviii—Si02—Mn01xix | 109.17 (4) |
Si02i—Mn01—Mn01viii | 115.22 (3) | Mn01xiii—Si02—Si02xx | 54.69 (5) |
Si02ii—Mn01—Mn01viii | 91.74 (2) | Mn01xiv—Si02—Si02xx | 91.202 (14) |
Si02iii—Mn01—Mn01viii | 54.31 (2) | Mn01xv—Si02—Si02xx | 162.01 (4) |
Si02iv—Mn01—Mn01viii | 155.83 (4) | Mn01xvi—Si02—Si02xx | 108.02 (5) |
Si02v—Mn01—Mn01viii | 53.04 (4) | Mn01xvii—Si02—Si02xx | 56.405 (10) |
Si02vi—Mn01—Mn01viii | 50.79 (5) | Mn01xviii—Si02—Si02xx | 124.87 (9) |
Si02vii—Mn01—Mn01viii | 104.47 (4) | Mn01xix—Si02—Si02xx | 52.76 (4) |
Si02i—Mn01—Mn01ix | 115.22 (3) | Mn01xiii—Si02—Si02xxi | 54.69 (5) |
Si02ii—Mn01—Mn01ix | 54.31 (2) | Mn01xiv—Si02—Si02xxi | 162.01 (4) |
Si02iii—Mn01—Mn01ix | 155.83 (4) | Mn01xv—Si02—Si02xxi | 108.02 (5) |
Si02iv—Mn01—Mn01ix | 91.74 (2) | Mn01xvi—Si02—Si02xxi | 91.202 (14) |
Si02v—Mn01—Mn01ix | 50.79 (5) | Mn01xvii—Si02—Si02xxi | 52.76 (4) |
Si02vi—Mn01—Mn01ix | 104.47 (4) | Mn01xviii—Si02—Si02xxi | 56.405 (10) |
Si02vii—Mn01—Mn01ix | 53.04 (4) | Mn01xix—Si02—Si02xxi | 124.87 (9) |
Mn01viii—Mn01—Mn01ix | 103.16 (3) | Si02xx—Si02—Si02xxi | 89.93 (8) |
Si02i—Mn01—Mn01x | 115.22 (3) | Mn01xiii—Si02—Si02xxii | 54.69 (5) |
Si02ii—Mn01—Mn01x | 155.83 (4) | Mn01xiv—Si02—Si02xxii | 108.02 (5) |
Si02iii—Mn01—Mn01x | 91.74 (2) | Mn01xv—Si02—Si02xxii | 91.202 (14) |
Si02iv—Mn01—Mn01x | 54.31 (2) | Mn01xvi—Si02—Si02xxii | 162.01 (4) |
Si02v—Mn01—Mn01x | 104.47 (4) | Mn01xvii—Si02—Si02xxii | 124.87 (9) |
Si02vi—Mn01—Mn01x | 53.04 (4) | Mn01xviii—Si02—Si02xxii | 52.76 (4) |
Si02vii—Mn01—Mn01x | 50.79 (5) | Mn01xix—Si02—Si02xxii | 56.405 (10) |
Mn01viii—Mn01—Mn01x | 103.16 (3) | Si02xx—Si02—Si02xxii | 89.93 (8) |
Mn01ix—Mn01—Mn01x | 103.16 (3) | Si02xxi—Si02—Si02xxii | 89.93 (8) |
Si02i—Mn01—Mn01xi | 58.99 (3) | Mn01xiii—Si02—Si02xxiii | 110.85 (6) |
Si02ii—Mn01—Mn01xi | 54.31 (2) | Mn01xiv—Si02—Si02xxiii | 51.63 (5) |
Si02iii—Mn01—Mn01xi | 132.62 (4) | Mn01xv—Si02—Si02xxiii | 57.79 (3) |
Si02iv—Mn01—Mn01xi | 58.13 (3) | Mn01xvi—Si02—Si02xxiii | 111.37 (9) |
Si02v—Mn01—Mn01xi | 107.58 (4) | Mn01xvii—Si02—Si02xxiii | 161.21 (3) |
Si02vi—Mn01—Mn01xi | 155.59 (4) | Mn01xviii—Si02—Si02xxiii | 88.16 (3) |
Si02vii—Mn01—Mn01xi | 88.646 (19) | Mn01xix—Si02—Si02xxiii | 56.405 (10) |
Mn01viii—Mn01—Mn01xi | 146.033 (7) | Si02xx—Si02—Si02xxiii | 107.98 (2) |
Mn01ix—Mn01—Mn01xi | 60.0 | Si02xxi—Si02—Si02xxiii | 143.97 (4) |
Mn01x—Mn01—Mn01xi | 109.230 (4) | Si02xxii—Si02—Si02xxiii | 60.0 |
Si02i—Mn01—Mn01xii | 58.99 (3) | Mn01xiii—Si02—Si02xxiv | 110.85 (6) |
Si02ii—Mn01—Mn01xii | 58.13 (3) | Mn01xiv—Si02—Si02xxiv | 57.79 (3) |
Si02iii—Mn01—Mn01xii | 54.31 (2) | Mn01xv—Si02—Si02xxiv | 111.37 (9) |
Si02iv—Mn01—Mn01xii | 132.62 (4) | Mn01xvi—Si02—Si02xxiv | 51.63 (5) |
Si02v—Mn01—Mn01xii | 88.646 (19) | Mn01xvii—Si02—Si02xxiv | 56.405 (10) |
Si02vi—Mn01—Mn01xii | 107.58 (4) | Mn01xviii—Si02—Si02xxiv | 161.21 (3) |
Si02vii—Mn01—Mn01xii | 155.59 (4) | Mn01xix—Si02—Si02xxiv | 88.16 (3) |
Mn01viii—Mn01—Mn01xii | 60.0 | Si02xx—Si02—Si02xxiv | 60.0 |
Mn01ix—Mn01—Mn01xii | 109.230 (4) | Si02xxi—Si02—Si02xxiv | 107.98 (2) |
Mn01x—Mn01—Mn01xii | 146.033 (7) | Si02xxii—Si02—Si02xxiv | 143.97 (4) |
Mn01xi—Mn01—Mn01xii | 95.84 (3) | Si02xxiii—Si02—Si02xxiv | 108.05 (6) |
Symmetry codes: (i) x−1, y−1, z−1; (ii) −x+1, y−1/2, −z+1/2; (iii) −x+1/2, −y+1, z−1/2; (iv) x−1/2, −y+1/2, −z+1; (v) x−1/2, −y+3/2, −z+1; (vi) −x+1, y−1/2, −z+3/2; (vii) −x+3/2, −y+1, z−1/2; (viii) −x, y+1/2, −z+1/2; (ix) x+1/2, −y+1/2, −z; (x) −x+1/2, −y, z+1/2; (xi) −x+1/2, −y, z−1/2; (xii) x−1/2, −y+1/2, −z; (xiii) x+1, y+1, z+1; (xiv) −x+1, y+1/2, −z+1/2; (xv) x+1/2, −y+1/2, −z+1; (xvi) −x+1/2, −y+1, z+1/2; (xvii) x+1/2, −y+3/2, −z+1; (xviii) −x+1, y+1/2, −z+3/2; (xix) −x+3/2, −y+1, z+1/2; (xx) −x+2, y+1/2, −z+3/2; (xxi) −x+3/2, −y+2, z+1/2; (xxii) x+1/2, −y+3/2, −z+2; (xxiii) −x+2, y−1/2, −z+3/2; (xxiv) −x+3/2, −y+2, z−1/2. |
Crystal data top
MnSi | Dx = 5.793 Mg m−3 |
Mr = 83.03 | Cell parameters from 14604 reflections |
Cubic, P213 | θ = 2.0–19.9° |
a = 4.5662 (1) Å | µ = 0.26 mm−1 |
V = 95.21 (1) Å3 | T = 293 K |
Z = 4 | Block, metallic dark grey |
F(000) = 156 | |
Data collection top
Huber χ at ID11@ESRF diffractometer | θmax = 15.2°, θmin = 1.7° |
φ scan | h = −15→14 |
12145 measured reflections | k = −15→15 |
12145 independent reflections | l = −15→15 |
11972 reflections with I > 2σ(I) | |
Refinement top
Refinement on F2 | 0 restraints |
Least-squares matrix: full | w = 1/[σ2(Fo2) + (0.0218P)2 + 0.0116P] where P = (Fo2 + 2Fc2)/3 |
R[F2 > 2σ(F2)] = 0.015 | (Δ/σ)max < 0.001 |
wR(F2) = 0.037 | Δρmax = 0.59 e Å−3 |
S = 1.08 | Δρmin = −1.39 e Å−3 |
12145 reflections | Absolute structure: Flack x determined using 529 quotients [(I+)-(I-)]/[(I+)+(I-)]
(Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259). |
7 parameters | Absolute structure parameter: −0.02 (12) |
Special details top
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes)
are estimated using the full covariance matrix. The cell esds are taken
into account individually in the estimation of esds in distances, angles
and torsion angles; correlations between esds in cell parameters are only
used when they are defined by crystal symmetry. An approximate (isotropic)
treatment of cell esds is used for estimating esds involving l.s. planes. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Mn01 | 0.13688 (2) | 0.13688 (2) | 0.13688 (2) | 0.004460 (10) | |
Si02 | −0.15445 (4) | −0.15445 (4) | −0.15445 (4) | 0.00570 (3) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Mn01 | 0.004460 (10) | 0.004460 (10) | 0.004460 (10) | −0.000040 (10) | −0.000040 (10) | −0.000040 (10) |
Si02 | 0.00570 (3) | 0.00570 (3) | 0.00570 (3) | −0.00061 (3) | −0.00061 (3) | −0.00061 (3) |
Geometric parameters (Å, º) top
Mn01—Si02 | 2.3040 (3) | Si02—Mn01x | 2.4015 (2) |
Mn01—Si02i | 2.4014 (2) | Si02—Mn01xi | 2.4015 (2) |
Mn01—Si02ii | 2.4014 (2) | Si02—Mn01xii | 2.4015 (2) |
Mn01—Si02iii | 2.4014 (2) | Si02—Mn01ix | 2.5494 (1) |
Mn01—Si02iv | 2.5495 (1) | Si02—Mn01vii | 2.5494 (1) |
Mn01—Si02v | 2.5495 (1) | Si02—Mn01viii | 2.5494 (1) |
Mn01—Si02vi | 2.5495 (1) | Si02—Si02i | 2.8220 (1) |
Mn01—Mn01vii | 2.8004 (1) | Si02—Si02ii | 2.8220 (1) |
Mn01—Mn01viii | 2.8004 (1) | Si02—Si02iii | 2.8220 (1) |
Mn01—Mn01ix | 2.8004 (1) | Si02—Si02x | 2.8220 (1) |
Mn01—Mn01v | 2.8004 (1) | Si02—Si02xi | 2.8220 (1) |
Mn01—Mn01vi | 2.8004 (1) | | |
| | | |
Si02—Mn01—Si02i | 73.666 (2) | Mn01—Si02—Mn01x | 137.680 (5) |
Si02—Mn01—Si02ii | 73.666 (2) | Mn01—Si02—Mn01xi | 137.680 (5) |
Si02i—Mn01—Si02ii | 112.418 (2) | Mn01x—Si02—Mn01xi | 71.333 (7) |
Si02—Mn01—Si02iii | 73.666 (2) | Mn01—Si02—Mn01xii | 137.680 (5) |
Si02i—Mn01—Si02iii | 112.418 (2) | Mn01x—Si02—Mn01xii | 71.333 (7) |
Si02ii—Mn01—Si02iii | 112.418 (2) | Mn01xi—Si02—Mn01xii | 71.333 (7) |
Si02—Mn01—Si02iv | 140.278 (2) | Mn01—Si02—Mn01ix | 70.270 (6) |
Si02i—Mn01—Si02iv | 134.507 (7) | Mn01x—Si02—Mn01ix | 114.152 (5) |
Si02ii—Mn01—Si02iv | 69.425 (3) | Mn01xi—Si02—Mn01ix | 68.819 (2) |
Si02iii—Mn01—Si02iv | 107.420 (10) | Mn01xii—Si02—Mn01ix | 134.507 (7) |
Si02—Mn01—Si02v | 140.278 (2) | Mn01—Si02—Mn01vii | 70.270 (6) |
Si02i—Mn01—Si02v | 107.420 (10) | Mn01x—Si02—Mn01vii | 68.819 (2) |
Si02ii—Mn01—Si02v | 134.507 (7) | Mn01xi—Si02—Mn01vii | 134.507 (7) |
Si02iii—Mn01—Si02v | 69.425 (3) | Mn01xii—Si02—Mn01vii | 114.152 (5) |
Si02iv—Mn01—Si02v | 67.207 (3) | Mn01ix—Si02—Mn01vii | 109.211 (6) |
Si02—Mn01—Si02vi | 140.278 (2) | Mn01—Si02—Mn01viii | 70.270 (6) |
Si02i—Mn01—Si02vi | 69.425 (3) | Mn01x—Si02—Mn01viii | 134.507 (7) |
Si02ii—Mn01—Si02vi | 107.420 (10) | Mn01xi—Si02—Mn01viii | 114.152 (5) |
Si02iii—Mn01—Si02vi | 134.507 (7) | Mn01xii—Si02—Mn01viii | 68.819 (2) |
Si02iv—Mn01—Si02vi | 67.207 (3) | Mn01ix—Si02—Mn01viii | 109.211 (6) |
Si02v—Mn01—Si02vi | 67.207 (3) | Mn01vii—Si02—Mn01viii | 109.211 (6) |
Si02—Mn01—Mn01vii | 58.974 (3) | Mn01—Si02—Si02i | 54.750 (9) |
Si02i—Mn01—Mn01vii | 58.090 (5) | Mn01x—Si02—Si02i | 107.985 (7) |
Si02ii—Mn01—Mn01vii | 54.334 (4) | Mn01xi—Si02—Si02i | 161.951 (7) |
Si02iii—Mn01—Mn01vii | 132.594 (5) | Mn01xii—Si02—Si02i | 91.184 (2) |
Si02iv—Mn01—Mn01vii | 107.552 (6) | Mn01ix—Si02—Si02i | 124.980 (15) |
Si02v—Mn01—Mn01vii | 155.640 (6) | Mn01vii—Si02—Si02i | 56.3960 (10) |
Si02vi—Mn01—Mn01vii | 88.669 (3) | Mn01viii—Si02—Si02i | 52.817 (7) |
Si02—Mn01—Mn01viii | 58.974 (3) | Mn01—Si02—Si02ii | 54.750 (9) |
Si02i—Mn01—Mn01viii | 54.334 (4) | Mn01x—Si02—Si02ii | 91.184 (2) |
Si02ii—Mn01—Mn01viii | 132.594 (5) | Mn01xi—Si02—Si02ii | 107.985 (7) |
Si02iii—Mn01—Mn01viii | 58.090 (5) | Mn01xii—Si02—Si02ii | 161.951 (7) |
Si02iv—Mn01—Mn01viii | 155.640 (6) | Mn01ix—Si02—Si02ii | 56.3960 (10) |
Si02v—Mn01—Mn01viii | 88.669 (3) | Mn01vii—Si02—Si02ii | 52.817 (7) |
Si02vi—Mn01—Mn01viii | 107.552 (6) | Mn01viii—Si02—Si02ii | 124.980 (15) |
Mn01vii—Mn01—Mn01viii | 95.826 (4) | Si02i—Si02—Si02ii | 90.020 (12) |
Si02—Mn01—Mn01ix | 58.974 (3) | Mn01—Si02—Si02iii | 54.750 (9) |
Si02i—Mn01—Mn01ix | 132.594 (5) | Mn01x—Si02—Si02iii | 161.951 (7) |
Si02ii—Mn01—Mn01ix | 58.090 (5) | Mn01xi—Si02—Si02iii | 91.184 (2) |
Si02iii—Mn01—Mn01ix | 54.334 (4) | Mn01xii—Si02—Si02iii | 107.985 (7) |
Si02iv—Mn01—Mn01ix | 88.669 (3) | Mn01ix—Si02—Si02iii | 52.817 (7) |
Si02v—Mn01—Mn01ix | 107.552 (6) | Mn01vii—Si02—Si02iii | 124.980 (15) |
Si02vi—Mn01—Mn01ix | 155.640 (6) | Mn01viii—Si02—Si02iii | 56.3960 (10) |
Mn01vii—Mn01—Mn01ix | 95.826 (4) | Si02i—Si02—Si02iii | 90.020 (12) |
Mn01viii—Mn01—Mn01ix | 95.826 (4) | Si02ii—Si02—Si02iii | 90.020 (12) |
Si02—Mn01—Mn01v | 115.212 (3) | Mn01—Si02—Si02x | 110.920 (9) |
Si02i—Mn01—Mn01v | 155.872 (5) | Mn01x—Si02—Si02x | 51.584 (8) |
Si02ii—Mn01—Mn01v | 91.709 (4) | Mn01xi—Si02—Si02x | 111.274 (14) |
Si02iii—Mn01—Mn01v | 54.333 (4) | Mn01xii—Si02—Si02x | 57.758 (4) |
Si02iv—Mn01—Mn01v | 53.091 (6) | Mn01ix—Si02—Si02x | 161.178 (4) |
Si02v—Mn01—Mn01v | 50.756 (7) | Mn01vii—Si02—Si02x | 56.3960 (10) |
Si02vi—Mn01—Mn01v | 104.492 (4) | Mn01viii—Si02—Si02x | 88.197 (4) |
Mn01vii—Mn01—Mn01v | 146.0300 (10) | Si02i—Si02—Si02x | 60.0 |
Mn01viii—Mn01—Mn01v | 109.2 | Si02ii—Si02—Si02x | 108.006 (3) |
Mn01ix—Mn01—Mn01v | 60.0 | Si02iii—Si02—Si02x | 144.009 (6) |
Si02—Mn01—Mn01vi | 115.212 (3) | Mn01—Si02—Si02xi | 110.920 (9) |
Si02i—Mn01—Mn01vi | 54.333 (4) | Mn01x—Si02—Si02xi | 57.758 (4) |
Si02ii—Mn01—Mn01vi | 155.872 (5) | Mn01xi—Si02—Si02xi | 51.584 (8) |
Si02iii—Mn01—Mn01vi | 91.709 (4) | Mn01xii—Si02—Si02xi | 111.274 (14) |
Si02iv—Mn01—Mn01vi | 104.492 (4) | Mn01ix—Si02—Si02xi | 56.3960 (10) |
Si02v—Mn01—Mn01vi | 53.091 (6) | Mn01vii—Si02—Si02xi | 88.197 (4) |
Si02vi—Mn01—Mn01vi | 50.756 (7) | Mn01viii—Si02—Si02xi | 161.177 (4) |
Mn01vii—Mn01—Mn01vi | 109.2 | Si02i—Si02—Si02xi | 144.009 (6) |
Mn01viii—Mn01—Mn01vi | 60.0 | Si02ii—Si02—Si02xi | 60.0 |
Mn01ix—Mn01—Mn01vi | 146.0300 (10) | Si02iii—Si02—Si02xi | 108.006 (4) |
Mn01v—Mn01—Mn01vi | 103.169 (3) | Si02x—Si02—Si02xi | 107.985 (9) |
Symmetry codes: (i) x+1/2, −y−1/2, −z; (ii) −x, y+1/2, −z−1/2; (iii) −x−1/2, −y, z+1/2; (iv) x+1/2, −y+1/2, −z; (v) −x, y+1/2, −z+1/2; (vi) −x+1/2, −y, z+1/2; (vii) −x+1/2, −y, z−1/2; (viii) −x, y−1/2, −z+1/2; (ix) x−1/2, −y+1/2, −z; (x) −x, y−1/2, −z−1/2; (xi) −x−1/2, −y, z−1/2; (xii) x−1/2, −y−1/2, −z. |
Crystal data top
Co0.30Fe0.70Si | Dx = 6.298 Mg m−3 |
Mr = 84.86 | Cell parameters from 5730 reflections |
Cubic, P213 | θ = 1.7–19.6° |
a = 4.4732 (5) Å | µ = 0.48 mm−1 |
V = 89.51 (3) Å3 | T = 120 K |
Z = 4 | Block, metallic dark grey |
F(000) = 161 | |
Data collection top
Huber χ at ID11@ESRF diffractometer | θmax = 19.7°, θmin = 1.7° |
φ scan | h = −14→14 |
8860 measured reflections | k = −14→15 |
8860 independent reflections | l = −12→12 |
8781 reflections with I > 2σ(I) | |
Refinement top
Refinement on F2 | 0 restraints |
Least-squares matrix: full | w = 1/[σ2(Fo2) + (0.0331P)2 + 0.1327P] where P = (Fo2 + 2Fc2)/3 |
R[F2 > 2σ(F2)] = 0.024 | (Δ/σ)max < 0.001 |
wR(F2) = 0.062 | Δρmax = 0.99 e Å−3 |
S = 1.06 | Δρmin = −2.26 e Å−3 |
8860 reflections | Absolute structure: Flack x determined using 509 quotients [(I+)-(I-)]/[(I+)+(I-)]
(Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259). |
7 parameters | Absolute structure parameter: −0.08 (10) |
Special details top
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes)
are estimated using the full covariance matrix. The cell esds are taken
into account individually in the estimation of esds in distances, angles
and torsion angles; correlations between esds in cell parameters are only
used when they are defined by crystal symmetry. An approximate (isotropic)
treatment of cell esds is used for estimating esds involving l.s. planes. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | Occ. (<1) |
Fe01 | 0.13757 (2) | 0.13757 (2) | 0.13757 (2) | 0.00264 (2) | 0.6999 |
Co01 | 0.13757 (2) | 0.13757 (2) | 0.13757 (2) | 0.00264 (2) | 0.3 |
Si01 | 0.84218 (7) | 0.84218 (7) | 0.84218 (7) | 0.00333 (5) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Fe01 | 0.00264 (2) | 0.00264 (2) | 0.00264 (2) | 0.00004 (2) | 0.00004 (2) | 0.00004 (2) |
Co01 | 0.00264 (2) | 0.00264 (2) | 0.00264 (2) | 0.00004 (2) | 0.00004 (2) | 0.00004 (2) |
Si01 | 0.00333 (5) | 0.00333 (5) | 0.00333 (5) | −0.00021 (5) | −0.00021 (5) | −0.00021 (5) |
Geometric parameters (Å, º) top
Fe01—Si01i | 2.2886 (6) | Si01—Co01xi | 2.2886 (6) |
Fe01—Si01ii | 2.3348 (5) | Si01—Fe01xi | 2.2886 (6) |
Fe01—Si01iii | 2.3348 (5) | Si01—Co01xii | 2.3348 (5) |
Fe01—Si01iv | 2.3348 (5) | Si01—Fe01xii | 2.3348 (5) |
Fe01—Si01v | 2.5023 (4) | Si01—Co01xiii | 2.3348 (5) |
Fe01—Si01vi | 2.5023 (4) | Si01—Co01xiv | 2.3348 (5) |
Fe01—Si01vii | 2.5023 (4) | Si01—Fe01xiii | 2.3348 (5) |
Fe01—Fe01viii | 2.7439 (3) | Si01—Fe01xiv | 2.3348 (5) |
Fe01—Co01viii | 2.7439 (3) | Si01—Co01xv | 2.5023 (4) |
Fe01—Fe01ix | 2.7439 (3) | Si01—Fe01xv | 2.5023 (4) |
Fe01—Co01ix | 2.7439 (3) | Si01—Co01xvi | 2.5023 (4) |
Fe01—Co01x | 2.7439 (3) | Si01—Co01xvii | 2.5023 (4) |
| | | |
Si01i—Fe01—Si01ii | 73.624 (5) | Co01xi—Si01—Fe01xi | 0.0 |
Si01i—Fe01—Si01iii | 73.624 (5) | Co01xi—Si01—Co01xii | 137.274 (9) |
Si01ii—Fe01—Si01iii | 112.381 (4) | Fe01xi—Si01—Co01xii | 137.274 (9) |
Si01i—Fe01—Si01iv | 73.624 (5) | Co01xi—Si01—Fe01xii | 137.3 |
Si01ii—Fe01—Si01iv | 112.381 (4) | Fe01xi—Si01—Fe01xii | 137.274 (9) |
Si01iii—Fe01—Si01iv | 112.381 (4) | Co01xii—Si01—Fe01xii | 0.0 |
Si01i—Fe01—Si01v | 140.265 (3) | Co01xi—Si01—Co01xiii | 137.274 (9) |
Si01ii—Fe01—Si01v | 69.788 (6) | Fe01xi—Si01—Co01xiii | 137.274 (9) |
Si01iii—Fe01—Si01v | 106.615 (18) | Co01xii—Si01—Co01xiii | 71.973 (13) |
Si01iv—Fe01—Si01v | 135.236 (12) | Fe01xii—Si01—Co01xiii | 71.973 (13) |
Si01i—Fe01—Si01vi | 140.265 (3) | Co01xi—Si01—Co01xiv | 137.274 (9) |
Si01ii—Fe01—Si01vi | 135.236 (12) | Fe01xi—Si01—Co01xiv | 137.274 (9) |
Si01iii—Fe01—Si01vi | 69.788 (6) | Co01xii—Si01—Co01xiv | 71.973 (13) |
Si01iv—Fe01—Si01vi | 106.615 (18) | Fe01xii—Si01—Co01xiv | 71.973 (13) |
Si01v—Fe01—Si01vi | 67.228 (5) | Co01xiii—Si01—Co01xiv | 71.973 (13) |
Si01i—Fe01—Si01vii | 140.265 (3) | Co01xi—Si01—Fe01xiii | 137.3 |
Si01ii—Fe01—Si01vii | 106.615 (18) | Fe01xi—Si01—Fe01xiii | 137.274 (9) |
Si01iii—Fe01—Si01vii | 135.236 (12) | Co01xii—Si01—Fe01xiii | 72.0 |
Si01iv—Fe01—Si01vii | 69.788 (6) | Fe01xii—Si01—Fe01xiii | 71.973 (13) |
Si01v—Fe01—Si01vii | 67.228 (5) | Co01xiii—Si01—Fe01xiii | 0.0 |
Si01vi—Fe01—Si01vii | 67.228 (5) | Co01xiv—Si01—Fe01xiii | 72.0 |
Si01i—Fe01—Fe01viii | 58.806 (6) | Co01xi—Si01—Fe01xiv | 137.3 |
Si01ii—Fe01—Fe01viii | 132.366 (10) | Fe01xi—Si01—Fe01xiv | 137.274 (9) |
Si01iii—Fe01—Fe01viii | 58.374 (9) | Co01xii—Si01—Fe01xiv | 72.0 |
Si01iv—Fe01—Fe01viii | 54.014 (7) | Fe01xii—Si01—Fe01xiv | 71.973 (13) |
Si01v—Fe01—Fe01viii | 155.349 (10) | Co01xiii—Si01—Fe01xiv | 72.0 |
Si01vi—Fe01—Fe01viii | 88.480 (5) | Co01xiv—Si01—Fe01xiv | 0.0 |
Si01vii—Fe01—Fe01viii | 108.214 (11) | Fe01xiii—Si01—Fe01xiv | 71.973 (13) |
Si01i—Fe01—Co01viii | 58.806 (6) | Co01xi—Si01—Co01xv | 69.717 (11) |
Si01ii—Fe01—Co01viii | 132.366 (10) | Fe01xi—Si01—Co01xv | 69.717 (11) |
Si01iii—Fe01—Co01viii | 58.374 (9) | Co01xii—Si01—Co01xv | 69.018 (3) |
Si01iv—Fe01—Co01viii | 54.014 (7) | Fe01xii—Si01—Co01xv | 69.018 (3) |
Si01v—Fe01—Co01viii | 155.349 (10) | Co01xiii—Si01—Co01xv | 135.237 (12) |
Si01vi—Fe01—Co01viii | 88.480 (5) | Co01xiv—Si01—Co01xv | 114.331 (9) |
Si01vii—Fe01—Co01viii | 108.214 (11) | Fe01xiii—Si01—Co01xv | 135.237 (12) |
Fe01viii—Fe01—Co01viii | 0.000 (5) | Fe01xiv—Si01—Co01xv | 114.331 (9) |
Si01i—Fe01—Fe01ix | 58.806 (6) | Co01xi—Si01—Fe01xv | 69.7 |
Si01ii—Fe01—Fe01ix | 54.014 (7) | Fe01xi—Si01—Fe01xv | 69.717 (11) |
Si01iii—Fe01—Fe01ix | 132.366 (10) | Co01xii—Si01—Fe01xv | 69.0 |
Si01iv—Fe01—Fe01ix | 58.374 (9) | Fe01xii—Si01—Fe01xv | 69.018 (3) |
Si01v—Fe01—Fe01ix | 108.214 (11) | Co01xiii—Si01—Fe01xv | 135.2 |
Si01vi—Fe01—Fe01ix | 155.349 (10) | Co01xiv—Si01—Fe01xv | 114.3 |
Si01vii—Fe01—Fe01ix | 88.480 (5) | Fe01xiii—Si01—Fe01xv | 135.237 (12) |
Fe01viii—Fe01—Fe01ix | 95.601 (8) | Fe01xiv—Si01—Fe01xv | 114.331 (9) |
Co01viii—Fe01—Fe01ix | 95.6 | Co01xv—Si01—Fe01xv | 0.0 |
Si01i—Fe01—Co01ix | 58.806 (6) | Co01xi—Si01—Co01xvi | 69.717 (11) |
Si01ii—Fe01—Co01ix | 54.014 (7) | Fe01xi—Si01—Co01xvi | 69.717 (11) |
Si01iii—Fe01—Co01ix | 132.366 (10) | Co01xii—Si01—Co01xvi | 135.237 (12) |
Si01iv—Fe01—Co01ix | 58.374 (9) | Fe01xii—Si01—Co01xvi | 135.237 (12) |
Si01v—Fe01—Co01ix | 108.214 (11) | Co01xiii—Si01—Co01xvi | 114.331 (9) |
Si01vi—Fe01—Co01ix | 155.349 (10) | Co01xiv—Si01—Co01xvi | 69.018 (3) |
Si01vii—Fe01—Co01ix | 88.480 (5) | Fe01xiii—Si01—Co01xvi | 114.331 (9) |
Fe01viii—Fe01—Co01ix | 95.601 (8) | Fe01xiv—Si01—Co01xvi | 69.018 (3) |
Co01viii—Fe01—Co01ix | 95.601 (8) | Co01xv—Si01—Co01xvi | 108.648 (11) |
Fe01ix—Fe01—Co01ix | 0.000 (5) | Fe01xv—Si01—Co01xvi | 108.648 (11) |
Si01i—Fe01—Co01x | 58.806 (6) | Co01xi—Si01—Co01xvii | 69.717 (11) |
Si01ii—Fe01—Co01x | 58.374 (9) | Fe01xi—Si01—Co01xvii | 69.717 (11) |
Si01iii—Fe01—Co01x | 54.014 (7) | Co01xii—Si01—Co01xvii | 114.331 (9) |
Si01iv—Fe01—Co01x | 132.366 (10) | Fe01xii—Si01—Co01xvii | 114.331 (9) |
Si01v—Fe01—Co01x | 88.480 (5) | Co01xiii—Si01—Co01xvii | 69.018 (3) |
Si01vi—Fe01—Co01x | 108.214 (11) | Co01xiv—Si01—Co01xvii | 135.237 (12) |
Si01vii—Fe01—Co01x | 155.349 (10) | Fe01xiii—Si01—Co01xvii | 69.018 (3) |
Fe01viii—Fe01—Co01x | 95.601 (7) | Fe01xiv—Si01—Co01xvii | 135.237 (12) |
Co01viii—Fe01—Co01x | 95.601 (7) | Co01xv—Si01—Co01xvii | 108.648 (11) |
Fe01ix—Fe01—Co01x | 95.601 (8) | Fe01xv—Si01—Co01xvii | 108.648 (11) |
Co01ix—Fe01—Co01x | 95.601 (8) | Co01xvi—Si01—Co01xvii | 108.648 (11) |
Symmetry codes: (i) x−1, y−1, z−1; (ii) x−1/2, −y+1/2, −z+1; (iii) −x+1, y−1/2, −z+1/2; (iv) −x+1/2, −y+1, z−1/2; (v) −x+3/2, −y+1, z−1/2; (vi) x−1/2, −y+3/2, −z+1; (vii) −x+1, y−1/2, −z+3/2; (viii) x−1/2, −y+1/2, −z; (ix) −x, y−1/2, −z+1/2; (x) −x+1/2, −y, z−1/2; (xi) x+1, y+1, z+1; (xii) x+1/2, −y+1/2, −z+1; (xiii) −x+1, y+1/2, −z+1/2; (xiv) −x+1/2, −y+1, z+1/2; (xv) −x+1, y+1/2, −z+3/2; (xvi) x+1/2, −y+3/2, −z+1; (xvii) −x+3/2, −y+1, z+1/2. |
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