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This work is devoted to an investigation of the magnetic properties and thermal behaviour of the natural oxoborates vonsenite and hulsite in the tem­per­ature range 5–500 K. The local environment, the oxidation states of the Fe and Sn atoms, and the charge distribution were determined using Mössbauer spectroscopy and are in accordance with a refinement of the crystal structure of hulsite from single-crystal X-ray diffraction data (SCXRD) in anisotropic approximation for the first time. The magnetic properties were studied by vibrating sample magnetometry (VSM) (5 ≤ T ≤ 400 K) and are reported for the first time for iron-rich hulsite. Both oxoborates show a very complex magnetic behaviour. Cascades of magnetic transitions are revealed and the critical tem­per­atures were determined. The sequences of magnetic transitions in both vonsenite and hulsite with increasing tem­per­ature were found to be as follows: magnetically ordered state → partial magnetic ordering → paramagnetic state. According to X-ray diffraction data (93 ≤ T ≤ 500 K), these processes are accompanied by anomalies in the unit-cell parameters and thermal expansion of the oxoborates at critical tem­per­atures. A strong negative volume thermal expansion is observed for both oxoborates at tem­per­atures below ∼120 K.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520621010866/ra5102sup1.cif
Contains datablocks global, I, II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520621010866/ra5102Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520621010866/ra5102IIsup3.hkl
Contains datablocks II, I

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520621010866/ra5102sup4.pdf
Additional figures and tables

CCDC references: 2116500; 2120235

Computing details top

Data collection: CrysAlis PRO 1.171.39.46 (Rigaku OD, 2018) for (I). Cell refinement: CrysAlis PRO 1.171.39.46 (Rigaku OD, 2018) for (I). Data reduction: CrysAlis PRO 1.171.39.46 (Rigaku OD, 2018) for (I).

(I) top
Crystal data top
B1Fe2.654Mg0.346O5F(000) = 505
Mr = 247.4Dx = 4.716 Mg m3
Orthorhombic, PbamMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P -2xab;-2yab;-2zCell parameters from 1018 reflections
a = 9.3166 (9) Åθ = 4.0–32.1°
b = 12.2751 (11) ŵ = 10.86 mm1
c = 3.0518 (3) ÅT = 100 K
V = 349.01 (6) Å3Prism, black
Z = 40.4 × 0.1 × 0.1 mm
Data collection top
Xcalibur, Eos
diffractometer
633 independent reflections
Radiation source: X-ray tube547 reflections with I > 3σ(I)
Graphite monochromatorRint = 0.038
Detector resolution: 16.2096 pixels mm-1θmax = 32.4°, θmin = 2.7°
ω scansh = 138
Absorption correction: multi-scan
CrysAlisPro 1.171.39.46 (Rigaku Oxford Diffraction, 2018) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1714
Tmin = 0.765, Tmax = 1l = 42
1752 measured reflections
Refinement top
Refinement on F4 constraints
R[F2 > 2σ(F2)] = 0.057Weighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
wR(F2) = 0.069(Δ/σ)max = 0.020
S = 2.48Δρmax = 1.84 e Å3
633 reflectionsΔρmin = 1.65 e Å3
34 parametersExtinction correction: B-C type 1 Gaussian isotropic (Becker & Coppens, 1974)
0 restraintsExtinction coefficient: 930 (130)
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Fe10000.0011 (4)*0.76
Mg1'0000.0011 (4)*0.24
Fe20.500.50.0168 (5)
Fe30.00119 (12)0.27600 (12)00.0106 (4)*0.77
Mg3'0.00119 (12)0.27600 (12)00.0106 (4)*0.25
Fe40.74311 (10)0.39731 (8)0.50.0036 (3)
O10.8465 (6)0.0439 (4)0.50.0059 (10)*
O20.3871 (6)0.0777 (4)00.0067 (10)*
O30.6233 (6)0.1410 (4)0.50.0057 (10)*
O40.1122 (5)0.1410 (4)00.0026 (9)*
O50.3460 (5)0.2622 (4)0.50.0042 (9)*
B10.2714 (8)0.3606 (6)0.50.0014 (13)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Fe40.0041 (5)0.0037 (5)0.0028 (5)0.0008 (4)00
Fe20.0174 (9)0.0146 (9)0.0184 (9)0.0007 (7)00
Geometric parameters (Å, º) top
Fe1—O12.077 (5)Fe4—O32.075 (5)
Fe1—O1i2.077 (5)Fe4—O4iii2.076 (4)
Fe1—O4ii2.084 (4)Fe4—O4i2.076 (4)
Fe1—O42.084 (4)Fe4—O52.091 (5)
Fe1—O4iii2.084 (4)Fe2—O22.022 (5)
Fe1—O4i2.084 (4)Fe2—O2v2.022 (5)
Mg1'—O12.077 (5)Fe3—O21.950 (5)
Mg1'—O1i2.077 (5)Fe3—O4vi2.091 (5)
Mg1'—O4ii2.084 (4)Mg3'—O21.950 (5)
Mg1'—O42.084 (4)Mg3'—O4vi2.091 (5)
Mg1'—O4iii2.084 (4)B1—O1vii1.381 (9)
Mg1'—O4i2.084 (4)B1—O31.393 (9)
Fe4—O21.985 (3)B1—O5vi1.365 (9)
Fe4—O2iv1.985 (3)
O1—Fe1—O1i180.0 (5)O4ii—Mg1'—O4i180.0 (5)
O1—Fe1—O4ii95.86 (17)O4—Mg1'—O4iii180.0 (5)
O1—Fe1—O495.86 (17)O4—Mg1'—O4i85.88 (15)
O1—Fe1—O4iii84.14 (17)O4iii—Mg1'—O4i94.12 (15)
O1—Fe1—O4i84.14 (17)O2—Fe4—O2iv100.49 (16)
O1i—Fe1—O4ii84.14 (17)O2—Fe4—O397.27 (16)
O1i—Fe1—O484.14 (17)O2—Fe4—O4iii82.42 (15)
O1i—Fe1—O4iii95.86 (17)O2—Fe4—O4i176.92 (16)
O1i—Fe1—O4i95.86 (17)O2—Fe4—O585.25 (16)
O4ii—Fe1—O494.12 (15)O2iv—Fe4—O397.27 (16)
O4ii—Fe1—O4iii85.88 (15)O2iv—Fe4—O4iii176.92 (16)
O4ii—Fe1—O4i180.0 (5)O2iv—Fe4—O4i82.42 (15)
O4—Fe1—O4iii180.0 (5)O2iv—Fe4—O585.25 (16)
O4—Fe1—O4i85.88 (15)O3—Fe4—O4iii83.28 (17)
O4iii—Fe1—O4i94.12 (15)O3—Fe4—O4i83.28 (17)
O1—Mg1'—O1i180.0 (5)O3—Fe4—O5176.0 (2)
O1—Mg1'—O4ii95.86 (17)O4iii—Fe4—O4i94.64 (16)
O1—Mg1'—O495.86 (17)O4iii—Fe4—O594.03 (18)
O1—Mg1'—O4iii84.14 (17)O4i—Fe4—O594.03 (18)
O1—Mg1'—O4i84.14 (17)O2—Fe2—O2v180.0 (5)
O1i—Mg1'—O4ii84.14 (17)O2—Fe3—O4vi179.0 (2)
O1i—Mg1'—O484.14 (17)O2—Mg3'—O4vi179.0 (2)
O1i—Mg1'—O4iii95.86 (17)O1vii—B1—O3119.1 (6)
O1i—Mg1'—O4i95.86 (17)O1vii—B1—O5vi121.6 (6)
O4ii—Mg1'—O494.12 (15)O3—B1—O5vi119.3 (6)
O4ii—Mg1'—O4iii85.88 (15)
Symmetry codes: (i) x, y, z; (ii) x, y, z1; (iii) x, y, z1; (iv) x, y, z+1; (v) x1, y, z; (vi) x1/2, y+1/2, z; (vii) x1/2, y+1/2, z.
(II) top
Crystal data top
BFe2.796Mg0.181O5Sn0.017F(000) = 245
Mr = 253.4Dx = 4.75 Mg m3
Monoclinic, P2/mMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yCell parameters from 1449 reflections
a = 10.638 (3) Åθ = 1.9–29.2°
b = 3.063 (2) ŵ = 11.36 mm1
c = 5.445 (5) ÅT = 293 K
β = 93.38 (4)°Tablet, black
V = 177.1 (2) Å30.06 × 0.03 × 0.01 mm
Z = 2
Data collection top
Bruker CCD
diffractometer
218 reflections with I > 3σ(I)
Radiation source: X-ray tubeRint = 0.081
Graphite monochromatorθmax = 29.2°, θmin = 1.9°
Absorption correction: multi-scan
(Krause et al., 2015)
h = 1414
Tmin = 0.800, Tmax = 0.860k = 44
1449 measured reflectionsl = 77
346 independent reflections
Refinement top
Refinement on F3 restraints
R[F2 > 2σ(F2)] = 0.06325 constraints
wR(F2) = 0.065Weighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
S = 1.74(Δ/σ)max = 0.046
346 reflectionsΔρmax = 1.28 e Å3
51 parametersΔρmin = 1.14 e Å3
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Fe10000.019 (2)0.97 (2)
Sn1'0000.019 (2)0.03 (2)
Fe200.50.50.030 (4)0.6 (2)
Mg2'00.50.50.030 (4)0.4 (2)
Fe30.5000.024 (2)
Fe40.500.50.021 (2)
Fe50.2726 (4)0.50.2210 (6)0.0202 (17)
O10.6908 (16)10.499 (2)0.019 (4)
O20.4659 (14)0.50.242 (3)0.019 (4)
O30.6969 (16)10.059 (2)0.019 (4)
O40.8872 (13)10.291 (3)0.019 (4)
O50.0922 (17)0.50.183 (3)0.019 (4)
B10.7586 (14)10.295 (2)0.018 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Fe10.037 (5)0.015 (3)0.003 (3)00.001 (2)0
Sn1'0.037 (5)0.015 (3)0.003 (3)00.001 (2)0
Fe20.045 (7)0.026 (6)0.019 (5)00.005 (3)0
Mg2'0.045 (7)0.026 (6)0.019 (5)00.005 (3)0
Fe30.042 (4)0.010 (3)0.020 (3)00.004 (3)0
Fe40.024 (4)0.024 (3)0.015 (3)00.000 (2)0
Fe50.038 (3)0.016 (2)0.007 (3)00.0010 (18)0
O10.031 (7)0.018 (6)0.006 (6)00.001 (3)0
O20.031 (7)0.018 (6)0.006 (6)00.001 (3)0
O30.031 (7)0.018 (6)0.006 (6)00.001 (3)0
O40.031 (7)0.018 (6)0.006 (6)00.001 (3)0
O50.031 (7)0.018 (6)0.006 (6)00.001 (3)0
B10.022 (11)0.016 (9)0.013 (8)00.008 (6)0
Geometric parameters (Å, º) top
Fe1—O4i2.042 (16)Fe3—O3xii2.101 (17)
Fe1—O4ii2.042 (16)Fe4—O1vi2.030 (17)
Fe1—O5iii2.046 (11)Fe4—O1xii2.030 (17)
Fe1—O52.046 (11)Fe4—O2iii2.096 (10)
Fe1—O5iv2.046 (11)Fe4—O22.096 (10)
Fe1—O5v2.046 (11)Fe4—O2xiii2.096 (10)
Fe2—O4vi2.219 (11)Fe4—O2xiv2.096 (10)
Fe2—O4vii2.219 (11)Fe5—O1vi2.180 (10)
Fe2—O4ii2.219 (11)Fe5—O1vii2.180 (10)
Fe2—O4viii2.219 (11)Fe5—O22.054 (16)
Fe2—O52.035 (16)Fe5—O3i2.199 (10)
Fe2—O5ix2.035 (16)Fe5—O3xv2.199 (10)
Fe3—O2iii2.066 (10)Fe5—O51.918 (18)
Fe3—O22.066 (10)B1—O11.36 (2)
Fe3—O2x2.066 (10)B1—O31.408 (18)
Fe3—O2xi2.066 (10)B1—O41.37 (2)
Fe3—O3i2.101 (17)
O4i—Fe1—O4ii180.0 (5)O2x—Fe3—O2xi95.7 (4)
O4i—Fe1—O5iii95.2 (5)O2x—Fe3—O3i96.5 (5)
O4i—Fe1—O595.2 (5)O2x—Fe3—O3xii83.5 (5)
O4i—Fe1—O5iv84.8 (5)O2xi—Fe3—O3i96.5 (5)
O4i—Fe1—O5v84.8 (5)O2xi—Fe3—O3xii83.5 (5)
O4ii—Fe1—O5iii84.8 (5)O3i—Fe3—O3xii180.0 (5)
O4ii—Fe1—O584.8 (5)O1vi—Fe4—O1xii180.0 (5)
O4ii—Fe1—O5iv95.2 (5)O1vi—Fe4—O2iii82.4 (5)
O4ii—Fe1—O5v95.2 (5)O1vi—Fe4—O282.4 (5)
O5iii—Fe1—O596.9 (5)O1vi—Fe4—O2xiii97.6 (5)
O5iii—Fe1—O5iv83.1 (5)O1vi—Fe4—O2xiv97.6 (5)
O5iii—Fe1—O5v180.0 (5)O1xii—Fe4—O2iii97.6 (5)
O5—Fe1—O5iv180.0 (5)O1xii—Fe4—O297.6 (5)
O5—Fe1—O5v83.1 (5)O1xii—Fe4—O2xiii82.4 (5)
O5iv—Fe1—O5v96.9 (5)O1xii—Fe4—O2xiv82.4 (5)
O4vi—Fe2—O4vii87.3 (4)O2iii—Fe4—O293.9 (4)
O4vi—Fe2—O4ii92.7 (4)O2iii—Fe4—O2xiii86.1 (4)
O4vi—Fe2—O4viii180.0 (5)O2iii—Fe4—O2xiv180.0 (5)
O4vi—Fe2—O599.4 (5)O2—Fe4—O2xiii180.0 (5)
O4vi—Fe2—O5ix80.6 (5)O2—Fe4—O2xiv86.1 (4)
O4vii—Fe2—O4ii180.0 (5)O2xiii—Fe4—O2xiv93.9 (4)
O4vii—Fe2—O4viii92.7 (4)O1vi—Fe5—O1vii89.3 (4)
O4vii—Fe2—O599.4 (5)O1vi—Fe5—O279.9 (5)
O4vii—Fe2—O5ix80.6 (5)O1vi—Fe5—O3i88.2 (4)
O4ii—Fe2—O4viii87.3 (4)O1vi—Fe5—O3xv161.2 (6)
O4ii—Fe2—O580.6 (5)O1vi—Fe5—O5102.2 (5)
O4ii—Fe2—O5ix99.4 (5)O1vii—Fe5—O279.9 (5)
O4viii—Fe2—O580.6 (5)O1vii—Fe5—O3i161.2 (6)
O4viii—Fe2—O5ix99.4 (5)O1vii—Fe5—O3xv88.2 (4)
O5—Fe2—O5ix180.0 (5)O1vii—Fe5—O5102.2 (5)
O2iii—Fe3—O295.7 (4)O2—Fe5—O3i81.4 (5)
O2iii—Fe3—O2x84.3 (4)O2—Fe5—O3xv81.4 (5)
O2iii—Fe3—O2xi180.0 (5)O2—Fe5—O5177.0 (6)
O2iii—Fe3—O3i83.5 (5)O3i—Fe5—O3xv88.3 (4)
O2iii—Fe3—O3xii96.5 (5)O3i—Fe5—O596.5 (5)
O2—Fe3—O2x180.0 (5)O3xv—Fe5—O596.5 (5)
O2—Fe3—O2xi84.3 (4)O1—B1—O3120.3 (14)
O2—Fe3—O3i83.5 (5)O1—B1—O4126.4 (13)
O2—Fe3—O3xii96.5 (5)O3—B1—O4113.3 (13)
Symmetry codes: (i) x+1, y+1, z; (ii) x1, y+1, z; (iii) x, y1, z; (iv) x, y1, z; (v) x, y, z; (vi) x+1, y+1, z+1; (vii) x+1, y+2, z+1; (viii) x1, y+2, z; (ix) x, y, z+1; (x) x+1, y1, z; (xi) x+1, y, z; (xii) x, y+1, z; (xiii) x+1, y1, z+1; (xiv) x+1, y, z+1; (xv) x+1, y+2, z.
 

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