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In the context of personalized medicine, there is a growing interest in materials bearing at the same time diagnostic and therapy functions. This article reports a cheap and easily reproducible procedure to obtain materials with a high potential for these applications. Three new strontium iodide–fructose-based metal–organic frameworks with formulae [Sr(C6H12O6)2]I2, [Sr2(C6H12O6)3(H2O)3]I4·0.5H2O and [Sr(C6H12O6)(H2O)3I]I differing in stoichiometry, symmetry and crystal packing, were obtained and characterized by X-ray diffraction. Bulk quantum simulations show that both the ions and the sugar are crucial in determining the predicted nonlinear response; also, the relative arrangement of various functional groups in the unit cell plays a role in the computed optical properties. Small fragments of the three compounds were selected for in vacuo calculations, proving that the reduced dimensions of the particles have a great influence on the nonlinear optical response. Despite the similar chemical composition of the three compounds, second harmonic generation measurements and in crystal and in vacuo theoretical calculations agree that one of the compounds is a much more efficient second harmonic emitter than the other two, and is thus a suitable candidate for bio-sensor applications.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520619001951/um5025sup1.cif
Contains datablocks global, 1, 2, 3

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520619001951/um50251sup2.hkl
Contains datablock 1

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520619001951/um50252sup3.hkl
Contains datablock 2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520619001951/um50253sup4.hkl
Contains datablock 3

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520619001951/um5025sup5.pdf
Details on crystal data and data collections and refinements, relevant bond distances, list of hydrogen bonds, details of theoretical calculations, pictures of the asymmetric units and of the infinite MOF planes of compounds 1-3 with thermal ellipsoids, pictures of the fragments analyzed in the in vacuo calculations

CCDC references: 1854903; 1854904; 1854905

Computing details top

Data collection: CrysAlis PRO, Agilent Technologies, Version 1.171.37.35 (release 13-08-2014 CrysAlis171 .NET) (compiled Aug 13 2014,18:06:01) for (1), (2); CrysAlis PRO 1.171.38.41 (Rigaku OD, 2015) for (3). Cell refinement: CrysAlis PRO, Agilent Technologies, Version 1.171.37.35 (release 13-08-2014 CrysAlis171 .NET) (compiled Aug 13 2014,18:06:01) for (1), (2); CrysAlis PRO 1.171.38.41 (Rigaku OD, 2015) for (3). Data reduction: CrysAlis PRO, Agilent Technologies, Version 1.171.37.35 (release 13-08-2014 CrysAlis171 .NET) (compiled Aug 13 2014,18:06:01) for (1), (2); CrysAlis PRO 1.171.38.41 (Rigaku OD, 2015) for (3). Program(s) used to solve structure: SHELXS (Sheldrick, 2008) for (1), (3); ShelXT (Sheldrick, 2015) for (2). For all structures, program(s) used to refine structure: SHELXL (Sheldrick, 2015); molecular graphics: Olex2 (Dolomanov et al., 2009); software used to prepare material for publication: Olex2 (Dolomanov et al., 2009).

(1) top
Crystal data top
C12H24O12Sr·2(I)F(000) = 672
Mr = 701.73Dx = 2.307 Mg m3
Monoclinic, P21Cu Kα radiation, λ = 1.54184 Å
a = 7.8592 (4) ÅCell parameters from 3544 reflections
b = 12.9355 (5) Åθ = 4.4–63.6°
c = 9.9504 (3) ŵ = 28.24 mm1
β = 92.803 (4)°T = 293 K
V = 1010.37 (7) Å3Prismatic, colourless
Z = 20.06 × 0.03 × 0.02 mm
Data collection top
Xcalibur, Ruby, Gemini ultra
diffractometer
3344 independent reflections
Radiation source: sealed X-ray tube, Enhance Ultra (Cu) X-ray Source3018 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.044
Detector resolution: 10.2890 pixels mm-1θmax = 67.2°, θmin = 4.4°
ω scansh = 78
Absorption correction: gaussian
CrysAlisPro, Agilent Technologies, Version 1.171.37.35 (release 13-08-2014 CrysAlis171 .NET) (compiled Aug 13 2014,18:06:01) Numerical absorption correction based on gaussian integration over a multifaceted crystal model Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1515
Tmin = 0.774, Tmax = 0.881l = 1111
8924 measured reflections
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.037 w = 1/[σ2(Fo2) + (0.0479P)2 + 0.2566P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.092(Δ/σ)max = 0.050
S = 1.08Δρmax = 0.94 e Å3
3344 reflectionsΔρmin = 0.64 e Å3
255 parametersAbsolute structure: Flack x determined using 1184 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259).
15 restraintsAbsolute structure parameter: 0.032 (6)
Primary atom site location: structure-invariant direct methods
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
xyzUiso*/UeqOcc. (<1)
Sr11.13549 (14)0.59488 (8)0.33503 (10)0.0395 (3)
O10.5610 (11)0.5435 (8)0.0054 (8)0.049 (2)
O20.9190 (12)0.5724 (8)0.1241 (9)0.054 (2)
H20.888 (10)0.522 (4)0.072 (9)0.081*
O30.8097 (11)0.6242 (8)0.3616 (8)0.051 (2)
H30.765 (5)0.644 (12)0.433 (4)0.076*
O40.4598 (11)0.5408 (8)0.3567 (8)0.052 (2)
H40.36860.51380.33340.078*
O50.3446 (10)0.6217 (6)0.1236 (8)0.042 (2)
H50.28230.62430.05520.063*
O60.2152 (13)0.4396 (7)0.1761 (10)0.056 (2)
H60.16980.38260.17670.084*
O70.8552 (14)0.4647 (7)0.7844 (10)0.055 (2)
O81.0580 (17)0.5775 (7)0.5939 (9)0.068 (3)
H81.03 (2)0.622 (5)0.651 (4)0.102*
O91.1147 (17)0.4162 (7)0.4444 (10)0.070 (3)
H91.14 (3)0.360 (2)0.406 (8)0.106*
O100.8432 (12)0.2705 (7)0.5180 (8)0.054 (2)
H100.87990.26670.44250.081*
O110.8679 (11)0.2828 (7)0.7808 (7)0.0464 (19)
H110.78750.24620.80000.070*
C10.661 (2)0.6373 (12)0.0014 (13)0.056 (3)
H1A0.72510.63800.07960.067*
H1B0.58610.69690.00110.067*
C20.7824 (17)0.6441 (11)0.1230 (13)0.049 (3)
H2A0.83190.71370.12450.059*
C30.6841 (15)0.6314 (10)0.2519 (12)0.042 (3)
H3A0.61470.69330.26430.050*
C40.5706 (16)0.5392 (10)0.2465 (11)0.041 (3)
H4A0.64060.47650.25210.049*
C50.4568 (15)0.5362 (10)0.1156 (11)0.040 (3)
C60.3580 (18)0.4366 (10)0.0928 (14)0.048 (3)
H6A0.42960.37760.11630.058*
H6B0.31970.43050.00100.058*
C71.0313 (16)0.4780 (9)0.7987 (11)0.039 (3)
H7A1.05570.53960.85170.047*
H7B1.08070.41950.84740.047*
C81.113 (2)0.4877 (10)0.6680 (13)0.055 (4)
H8A1.23690.48980.68370.066*
C91.064 (2)0.3951 (11)0.5778 (13)0.052 (3)
H9A1.12700.33430.61200.062*
C100.878 (2)0.3711 (9)0.5725 (12)0.053 (4)
H10A0.81810.42270.51580.063*
C110.8055 (15)0.3734 (10)0.7137 (12)0.045 (3)
O12B0.552 (3)0.4694 (18)0.623 (2)0.080 (5)*0.589 (19)
H12B0.63270.49940.59150.120*0.589 (19)
C12B0.615 (3)0.378 (8)0.705 (9)0.078 (7)*0.589 (19)
H12A0.57040.31520.66480.094*0.589 (19)
H12C0.57400.38370.79510.094*0.589 (19)
O12A0.538 (4)0.370 (3)0.821 (3)0.080 (5)*0.411 (19)
H12D0.61100.35120.87790.120*0.411 (19)
C12A0.615 (4)0.382 (12)0.691 (13)0.078 (7)*0.411 (19)
H12E0.57380.32840.62950.094*0.411 (19)
H12F0.58530.44860.65260.094*0.411 (19)
I10.85919 (12)0.27773 (6)1.13263 (8)0.0541 (3)
I20.59121 (13)0.72785 (9)0.62268 (9)0.0641 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sr10.0416 (6)0.0382 (5)0.0392 (5)0.0028 (5)0.0080 (4)0.0036 (5)
O10.053 (6)0.059 (5)0.034 (4)0.004 (5)0.008 (4)0.010 (4)
O20.051 (6)0.067 (7)0.045 (5)0.003 (5)0.009 (4)0.005 (4)
O30.040 (5)0.074 (7)0.039 (4)0.002 (4)0.002 (4)0.013 (4)
O40.043 (5)0.074 (6)0.039 (4)0.012 (5)0.002 (4)0.003 (4)
O50.043 (5)0.043 (5)0.041 (4)0.009 (3)0.002 (3)0.001 (3)
O60.060 (6)0.048 (5)0.062 (5)0.008 (4)0.019 (5)0.003 (4)
O70.070 (7)0.045 (5)0.050 (5)0.004 (5)0.007 (5)0.011 (4)
O80.128 (10)0.036 (5)0.041 (4)0.002 (5)0.009 (5)0.001 (4)
O90.124 (10)0.042 (5)0.048 (5)0.002 (6)0.034 (6)0.004 (4)
O100.076 (6)0.045 (5)0.040 (4)0.007 (5)0.000 (4)0.008 (4)
O110.064 (6)0.041 (4)0.036 (4)0.011 (5)0.017 (3)0.001 (4)
C10.064 (9)0.064 (9)0.039 (7)0.001 (7)0.009 (6)0.005 (6)
C20.047 (8)0.049 (7)0.051 (7)0.002 (6)0.009 (6)0.004 (6)
C30.032 (6)0.047 (7)0.046 (6)0.009 (5)0.002 (5)0.007 (5)
C40.039 (7)0.045 (7)0.038 (6)0.007 (6)0.000 (5)0.005 (5)
C50.040 (7)0.046 (7)0.035 (6)0.014 (6)0.005 (5)0.001 (5)
C60.050 (8)0.044 (7)0.051 (7)0.002 (6)0.007 (6)0.004 (6)
C70.052 (8)0.035 (6)0.031 (5)0.007 (5)0.001 (5)0.004 (5)
C80.082 (11)0.045 (7)0.039 (6)0.010 (7)0.005 (6)0.003 (6)
C90.073 (10)0.045 (7)0.040 (6)0.005 (7)0.019 (6)0.008 (6)
C100.095 (12)0.033 (7)0.029 (6)0.020 (7)0.003 (6)0.006 (5)
C110.044 (8)0.049 (8)0.042 (6)0.003 (6)0.006 (5)0.005 (5)
I10.0655 (6)0.0534 (5)0.0433 (4)0.0060 (4)0.0009 (3)0.0034 (4)
I20.0695 (6)0.0771 (6)0.0462 (5)0.0039 (5)0.0074 (4)0.0090 (4)
Geometric parameters (Å, º) top
Sr1—O22.653 (9)O11—H110.8200
Sr1—O32.614 (9)O11—C111.424 (16)
Sr1—O4i2.642 (9)C1—H1A0.9700
Sr1—O5i2.754 (8)C1—H1B0.9700
Sr1—O6i2.650 (9)C1—C21.51 (2)
Sr1—O82.685 (9)C2—H2A0.9800
Sr1—O92.563 (9)C2—C31.538 (17)
Sr1—O10ii2.703 (9)C3—H3A0.9800
Sr1—O11ii2.690 (9)C3—C41.489 (19)
O1—C11.448 (18)C4—H4A0.9800
O1—C51.404 (14)C4—C51.544 (16)
O2—H20.854 (14)C5—C61.516 (19)
O2—C21.419 (17)C6—H6A0.9700
O3—H30.850 (13)C6—H6B0.9700
O3—C31.438 (15)C7—H7A0.9700
O4—Sr1iii2.642 (9)C7—H7B0.9700
O4—H40.8200C7—C81.483 (17)
O4—C41.433 (15)C8—H8A0.9800
O5—Sr1iii2.754 (8)C8—C91.53 (2)
O5—H50.8200C9—H9A0.9800
O5—C51.419 (14)C9—C101.50 (2)
O6—Sr1iii2.650 (9)C10—H10A0.9800
O6—H60.8200C10—C111.543 (17)
O6—C61.428 (17)C11—C12B1.49 (2)
O7—C71.395 (17)C11—C12A1.50 (3)
O7—C111.419 (16)O12B—H12B0.8200
O8—H80.857 (13)O12B—C12B1.50 (8)
O8—C81.431 (17)C12B—H12A0.9700
O9—H90.852 (13)C12B—H12C0.9700
O9—C91.430 (15)O12A—H12D0.8200
O10—Sr1iv2.703 (9)O12A—C12A1.46 (12)
O10—H100.8200C12A—H12E0.9700
O10—C101.431 (16)C12A—H12F0.9700
O11—Sr1iv2.690 (9)
O2—Sr1—O5i78.1 (3)C1—C2—H2A107.5
O2—Sr1—O8125.7 (4)C1—C2—C3109.9 (11)
O2—Sr1—O10ii122.7 (3)C3—C2—H2A107.5
O2—Sr1—O11ii76.6 (3)O3—C3—C2106.6 (9)
O3—Sr1—O260.1 (3)O3—C3—H3A108.9
O3—Sr1—O4i167.4 (3)O3—C3—C4111.3 (10)
O3—Sr1—O5i133.1 (3)C2—C3—H3A108.9
O3—Sr1—O6i115.6 (3)C4—C3—C2112.3 (10)
O3—Sr1—O869.3 (3)C4—C3—H3A108.9
O3—Sr1—O10ii81.9 (3)O4—C4—C3110.3 (10)
O3—Sr1—O11ii85.6 (3)O4—C4—H4A109.1
O4i—Sr1—O2127.9 (3)O4—C4—C5107.3 (9)
O4i—Sr1—O5i59.1 (3)C3—C4—H4A109.1
O4i—Sr1—O6i66.0 (3)C3—C4—C5111.8 (10)
O4i—Sr1—O899.4 (3)C5—C4—H4A109.1
O4i—Sr1—O10ii98.3 (3)O1—C5—O5112.3 (10)
O4i—Sr1—O11ii105.3 (3)O1—C5—C4108.7 (9)
O6i—Sr1—O266.8 (3)O1—C5—C6104.8 (10)
O6i—Sr1—O5i58.2 (3)O5—C5—C4105.6 (9)
O6i—Sr1—O8125.5 (3)O5—C5—C6110.9 (10)
O6i—Sr1—O10ii161.7 (3)C6—C5—C4114.8 (10)
O6i—Sr1—O11ii115.3 (3)O6—C6—C5107.5 (10)
O8—Sr1—O5i156.2 (3)O6—C6—H6A110.2
O8—Sr1—O10ii64.0 (3)O6—C6—H6B110.2
O8—Sr1—O11ii119.2 (3)C5—C6—H6A110.2
O9—Sr1—O2100.7 (4)C5—C6—H6B110.2
O9—Sr1—O390.3 (4)H6A—C6—H6B108.5
O9—Sr1—O4i78.9 (4)O7—C7—H7A109.0
O9—Sr1—O5i119.4 (3)O7—C7—H7B109.0
O9—Sr1—O6i65.9 (3)O7—C7—C8113.0 (10)
O9—Sr1—O859.7 (3)H7A—C7—H7B107.8
O9—Sr1—O10ii122.1 (3)C8—C7—H7A109.0
O9—Sr1—O11ii175.8 (4)C8—C7—H7B109.0
O10ii—Sr1—O5i106.5 (3)O8—C8—C7112.9 (12)
O11ii—Sr1—O5i63.4 (2)O8—C8—H8A109.4
O11ii—Sr1—O10ii58.1 (2)O8—C8—C9105.8 (11)
C5—O1—C1114.7 (10)C7—C8—H8A109.4
Sr1—O2—H2135 (3)C7—C8—C9110.0 (11)
C2—O2—Sr1113.0 (7)C9—C8—H8A109.4
C2—O2—H2107 (3)O9—C9—C8108.8 (11)
Sr1—O3—H3125 (3)O9—C9—H9A108.6
C3—O3—Sr1124.9 (6)O9—C9—C10108.7 (12)
C3—O3—H3108 (2)C8—C9—H9A108.6
Sr1iii—O4—H442.6C10—C9—C8113.4 (12)
C4—O4—Sr1iii124.1 (7)C10—C9—H9A108.6
C4—O4—H4109.5O10—C10—C9111.8 (11)
Sr1iii—O5—H5106.5O10—C10—H10A108.8
C5—O5—Sr1iii109.9 (6)O10—C10—C11106.8 (11)
C5—O5—H5109.5C9—C10—H10A108.8
Sr1iii—O6—H6124.2C9—C10—C11111.7 (11)
C6—O6—Sr1iii125.7 (8)C11—C10—H10A108.8
C6—O6—H6109.5O7—C11—O11111.9 (10)
C7—O7—C11113.6 (10)O7—C11—C10111.2 (11)
Sr1—O8—H8132 (3)O7—C11—C12B104 (4)
C8—O8—Sr1119.0 (8)O7—C11—C12A105 (6)
C8—O8—H8108 (3)O11—C11—C10106.0 (9)
Sr1—O9—H9124 (2)O11—C11—C12B113 (4)
C9—O9—Sr1126.3 (8)O11—C11—C12A117 (5)
C9—O9—H9110 (2)C12B—C11—C10111 (4)
Sr1iv—O10—H10115.4C12A—C11—C10106 (5)
C10—O10—Sr1iv123.6 (6)C12B—O12B—H12B109.5
C10—O10—H10109.5C11—C12B—O12B112 (5)
Sr1iv—O11—H1165.5C11—C12B—H12A109.2
C11—O11—Sr1iv123.2 (6)C11—C12B—H12C109.3
C11—O11—H11109.5O12B—C12B—H12A109.2
O1—C1—H1A109.5O12B—C12B—H12C109.3
O1—C1—H1B109.5H12A—C12B—H12C107.9
O1—C1—C2110.5 (11)C12A—O12A—H12D109.5
H1A—C1—H1B108.1C11—C12A—H12E110.1
C2—C1—H1A109.5C11—C12A—H12F110.0
C2—C1—H1B109.5O12A—C12A—C11108 (6)
O2—C2—C1114.6 (12)O12A—C12A—H12E110.1
O2—C2—H2A107.5O12A—C12A—H12F110.0
O2—C2—C3109.5 (10)H12E—C12A—H12F108.4
Symmetry codes: (i) x1, y, z; (ii) x2, y1/2, z1; (iii) x+1, y, z; (iv) x2, y+1/2, z1.
(2) top
Crystal data top
8(I)·2(C18H42O21Sr2)·(H2O)Dx = 2.225 Mg m3
Mr = 2572.73Cu Kα radiation, λ = 1.54184 Å
Orthorhombic, P212121Cell parameters from 12344 reflections
a = 12.3717 (2) Åθ = 3.6–62.3°
b = 17.4352 (3) ŵ = 29.80 mm1
c = 17.6607 (3) ÅT = 293 K
V = 3809.46 (11) Å3Prismatic, colourless
Z = 20.12 × 0.04 × 0.02 mm
F(000) = 2420
Data collection top
Xcalibur, Ruby, Gemini ultra
diffractometer
5862 independent reflections
Radiation source: sealed X-ray tube, Enhance Ultra (Cu) X-ray Source5441 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.047
Detector resolution: 10.2890 pixels mm-1θmax = 62.4°, θmin = 3.6°
ω scansh = 1314
Absorption correction: analytical
CrysAlisPro, Agilent Technologies, Version 1.171.37.35 (release 13-08-2014 CrysAlis171 .NET) (compiled Aug 13 2014,18:06:01) Analytical numeric absorption correction using a multifaceted crystal model based on expressions derived by R.C. Clark & J.S. Reid. (Clark, R. C. & Reid, J. S. (1995). Acta Cryst. A51, 887-897) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1318
Tmin = 0.204, Tmax = 0.575l = 1920
20551 measured reflections
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.032 w = 1/[σ2(Fo2) + (0.0463P)2 + 1.7828P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.083(Δ/σ)max = 0.001
S = 1.03Δρmax = 1.32 e Å3
5862 reflectionsΔρmin = 0.57 e Å3
413 parametersAbsolute structure: Flack x determined using 2174 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259).
17 restraintsAbsolute structure parameter: 0.024 (3)
Primary atom site location: dual
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
xyzUiso*/UeqOcc. (<1)
I10.40790 (6)0.04627 (4)0.31584 (4)0.04210 (19)
I20.94896 (6)0.78188 (4)0.15653 (4)0.0428 (2)
I31.17951 (7)0.79461 (5)0.39193 (4)0.0496 (2)
I41.40026 (8)0.48348 (5)0.46854 (5)0.0603 (2)
Sr10.60839 (7)0.20750 (5)0.34982 (5)0.0308 (2)
Sr20.89145 (8)0.57723 (5)0.35773 (6)0.0342 (2)
O10.3685 (6)0.2742 (4)0.0948 (4)0.044 (2)
O20.5442 (6)0.2616 (4)0.2136 (4)0.0410 (18)
H20.56140.30060.19060.062*
O30.4582 (6)0.1405 (4)0.2745 (4)0.0414 (19)
H30.44290.09600.28500.062*
O40.2382 (6)0.1527 (4)0.2344 (4)0.0370 (18)
H40.24200.15410.28070.056*
O50.2700 (6)0.1618 (4)0.0811 (4)0.0350 (17)
H50.31320.16170.04590.052*
O60.0948 (7)0.2300 (5)0.1334 (5)0.057 (2)
H60.03960.25580.13700.085*
O70.7667 (6)0.3525 (4)0.5510 (4)0.0367 (18)
O80.8360 (6)0.5029 (4)0.4869 (4)0.0406 (18)
H80.85870.50690.53030.061*
O90.7392 (6)0.4779 (4)0.3539 (4)0.0391 (17)
H90.70230.46680.31690.059*
O100.7522 (5)0.3161 (4)0.3477 (4)0.0342 (16)
H100.80440.32030.31930.051*
O110.6326 (5)0.2909 (4)0.4793 (4)0.0343 (16)
H110.60660.28650.52180.051*
O120.7725 (7)0.1796 (4)0.4429 (5)0.049 (2)
H120.81130.14160.44530.074*
O131.1655 (6)0.4466 (4)0.2148 (4)0.0401 (18)
O141.3308 (6)0.5591 (4)0.1688 (4)0.0433 (19)
H141.32450.52080.14230.065*
O151.2491 (6)0.6699 (4)0.2522 (5)0.044 (2)
H151.21590.69980.27950.066*
O161.0282 (6)0.6239 (4)0.2615 (5)0.042 (2)
H161.02360.66420.23780.063*
O171.0586 (6)0.4820 (4)0.3177 (4)0.0377 (17)
H171.08490.44120.33150.057*
O180.8870 (6)0.4969 (5)0.2240 (4)0.055 (2)
H180.83500.47460.20540.083*
O1W0.5025 (7)0.1301 (5)0.4486 (5)0.059 (2)
H1WA0.53920.09340.46730.089*
H1WB0.44580.10980.43010.089*
O2W0.4719 (7)0.3231 (5)0.3509 (5)0.056 (2)
H2WA0.43660.33850.38930.083*
H2WB0.45610.35090.31290.083*
O3W1.0347 (8)0.6143 (5)0.4528 (6)0.067 (3)
H3WA1.07760.58370.47530.101*
H3WB1.04920.65930.46830.101*
C10.4690 (10)0.2377 (7)0.0866 (7)0.046 (3)
H1A0.52120.27440.06750.055*
H1B0.46230.19690.04950.055*
C20.5108 (8)0.2040 (6)0.1608 (6)0.035 (2)
H2A0.57250.17060.14980.043*
C30.4236 (8)0.1568 (6)0.2003 (6)0.031 (2)
H3A0.41300.10860.17270.037*
C40.3165 (8)0.2006 (6)0.2034 (6)0.033 (2)
H4A0.32530.24540.23650.040*
C50.2832 (9)0.2286 (6)0.1236 (7)0.040 (3)
C60.1827 (9)0.2781 (7)0.1205 (8)0.052 (3)
H6A0.18600.31780.15890.063*
H6B0.17650.30240.07130.063*
C70.7053 (10)0.4235 (7)0.5547 (6)0.045 (3)
H7A0.72450.45070.60070.054*
H7B0.62890.41130.55730.054*
C80.7246 (9)0.4747 (6)0.4886 (6)0.035 (3)
H8A0.67460.51830.49060.042*
C90.7085 (8)0.4318 (6)0.4158 (6)0.030 (2)
H9A0.63160.41930.41080.036*
C100.7720 (8)0.3580 (6)0.4154 (6)0.030 (2)
H10A0.84920.37060.41750.036*
C110.7437 (8)0.3075 (6)0.4853 (6)0.031 (2)
C120.8095 (10)0.2360 (6)0.4963 (7)0.040 (3)
H12A0.88540.24690.48800.048*
H12B0.80070.21710.54750.048*
C131.2668 (9)0.4584 (6)0.2527 (7)0.040 (3)
H13A1.32040.42370.23190.048*
H13B1.25860.44670.30610.048*
C141.3063 (8)0.5406 (6)0.2440 (6)0.032 (2)
H14A1.37060.54830.27550.038*
C151.2183 (8)0.5942 (6)0.2696 (6)0.032 (2)
H15A1.20820.58920.32440.038*
C161.1127 (8)0.5774 (6)0.2296 (6)0.033 (2)
H16A1.12000.58890.17550.039*
C171.0800 (8)0.4931 (6)0.2400 (6)0.030 (2)
C180.9850 (10)0.4673 (7)0.1915 (7)0.049 (3)
H18A0.99350.48630.14030.059*
H18B0.98220.41180.18980.059*
O4W1.1648 (15)0.5560 (10)0.5611 (10)0.059 (5)*0.5
H4WA1.22170.54630.53590.088*0.5
H4WB1.17540.59540.58850.088*0.5
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.0459 (4)0.0289 (4)0.0515 (4)0.0030 (3)0.0009 (3)0.0008 (3)
I20.0523 (4)0.0352 (4)0.0410 (4)0.0012 (3)0.0004 (3)0.0020 (3)
I30.0425 (4)0.0585 (5)0.0479 (5)0.0086 (4)0.0054 (3)0.0139 (4)
I40.0557 (5)0.0606 (6)0.0647 (5)0.0006 (4)0.0040 (4)0.0061 (4)
Sr10.0256 (4)0.0294 (5)0.0375 (5)0.0015 (4)0.0001 (4)0.0022 (4)
Sr20.0265 (5)0.0322 (5)0.0437 (6)0.0017 (4)0.0033 (4)0.0045 (4)
O10.044 (5)0.037 (5)0.052 (5)0.008 (4)0.005 (4)0.013 (4)
O20.044 (4)0.036 (4)0.043 (4)0.017 (4)0.010 (4)0.007 (3)
O30.045 (5)0.036 (4)0.043 (5)0.009 (4)0.009 (4)0.010 (3)
O40.035 (4)0.043 (5)0.033 (4)0.007 (3)0.001 (3)0.002 (3)
O50.034 (4)0.027 (4)0.044 (4)0.000 (3)0.003 (3)0.000 (3)
O60.037 (4)0.045 (5)0.089 (7)0.007 (4)0.002 (5)0.003 (4)
O70.045 (5)0.032 (4)0.033 (4)0.003 (3)0.006 (3)0.001 (3)
O80.040 (4)0.040 (5)0.042 (4)0.018 (4)0.001 (3)0.001 (3)
O90.044 (4)0.037 (4)0.037 (4)0.008 (3)0.005 (3)0.002 (3)
O100.029 (4)0.035 (4)0.038 (4)0.006 (3)0.006 (3)0.004 (3)
O110.028 (4)0.040 (4)0.035 (4)0.003 (3)0.002 (3)0.000 (3)
O120.055 (5)0.026 (4)0.067 (6)0.008 (4)0.017 (4)0.005 (4)
O130.040 (4)0.030 (4)0.050 (5)0.001 (3)0.001 (4)0.001 (3)
O140.046 (5)0.035 (4)0.049 (5)0.007 (3)0.013 (4)0.007 (3)
O150.040 (4)0.039 (5)0.054 (5)0.006 (4)0.019 (4)0.008 (4)
O160.025 (4)0.031 (4)0.071 (6)0.003 (3)0.011 (4)0.015 (4)
O170.041 (4)0.026 (4)0.045 (4)0.001 (3)0.003 (3)0.007 (3)
O180.026 (4)0.084 (7)0.056 (5)0.008 (4)0.001 (4)0.007 (5)
O1W0.048 (5)0.067 (6)0.062 (6)0.013 (5)0.016 (4)0.003 (5)
O2W0.046 (5)0.060 (5)0.061 (6)0.014 (4)0.002 (5)0.007 (5)
O3W0.068 (7)0.054 (6)0.079 (7)0.000 (5)0.028 (5)0.004 (5)
C10.043 (7)0.050 (7)0.046 (7)0.016 (6)0.002 (5)0.006 (6)
C20.030 (5)0.026 (6)0.050 (7)0.004 (4)0.004 (5)0.001 (5)
C30.031 (6)0.029 (6)0.034 (6)0.001 (4)0.002 (4)0.002 (4)
C40.033 (6)0.026 (6)0.040 (6)0.005 (4)0.006 (5)0.001 (4)
C50.043 (7)0.026 (6)0.050 (7)0.003 (5)0.005 (5)0.003 (5)
C60.029 (6)0.050 (8)0.077 (9)0.013 (6)0.007 (6)0.011 (7)
C70.043 (7)0.055 (8)0.036 (7)0.006 (6)0.002 (5)0.009 (5)
C80.033 (6)0.024 (6)0.048 (7)0.001 (5)0.008 (5)0.006 (5)
C90.023 (5)0.034 (6)0.033 (6)0.005 (4)0.002 (4)0.003 (4)
C100.024 (5)0.031 (6)0.035 (6)0.005 (4)0.000 (4)0.005 (5)
C110.029 (5)0.030 (6)0.032 (6)0.014 (4)0.002 (4)0.002 (4)
C120.038 (6)0.038 (7)0.045 (7)0.002 (5)0.020 (5)0.005 (5)
C130.034 (6)0.033 (7)0.053 (7)0.007 (5)0.004 (5)0.002 (5)
C140.024 (5)0.030 (6)0.043 (6)0.001 (4)0.001 (4)0.004 (5)
C150.035 (6)0.029 (6)0.032 (6)0.005 (5)0.006 (5)0.002 (4)
C160.022 (5)0.034 (6)0.042 (6)0.003 (4)0.012 (5)0.005 (5)
C170.027 (5)0.028 (6)0.037 (6)0.000 (4)0.002 (4)0.003 (4)
C180.047 (7)0.051 (8)0.049 (7)0.010 (6)0.003 (6)0.007 (6)
Geometric parameters (Å, º) top
Sr1—O22.703 (7)O15—H150.8200
Sr1—O32.567 (7)O15—C151.408 (13)
Sr1—O102.599 (6)O16—H160.8200
Sr1—O112.726 (7)O16—C161.437 (12)
Sr1—O122.657 (8)O17—H170.8200
Sr1—O14i2.714 (7)O17—C171.412 (12)
Sr1—O15i2.605 (7)O18—H180.8200
Sr1—O1W2.565 (8)O18—C181.437 (14)
Sr1—O2W2.630 (8)O1W—H1WA0.8508
Sr1—C113.401 (10)O1W—H1WB0.8506
Sr2—O4ii2.636 (7)O2W—H2WA0.8501
Sr2—O5ii2.707 (7)O2W—H2WB0.8498
Sr2—O6ii2.674 (8)O3W—H3WA0.8507
Sr2—O82.712 (7)O3W—H3WB0.8508
Sr2—O92.560 (7)C1—H1A0.9700
Sr2—O162.532 (7)C1—H1B0.9700
Sr2—O172.745 (7)C1—C21.527 (16)
Sr2—O182.747 (8)C2—H2A0.9800
Sr2—O3W2.525 (9)C2—C31.525 (14)
O1—C11.404 (14)C3—H3A0.9800
O1—C51.416 (14)C3—C41.531 (14)
O2—H20.8200C4—H4A0.9800
O2—C21.433 (12)C4—C51.547 (15)
O3—H30.8200C5—C61.514 (15)
O3—C31.408 (12)C6—H6A0.9700
O4—Sr2iii2.636 (7)C6—H6B0.9700
O4—H40.8200C7—H7A0.9700
O4—C41.392 (12)C7—H7B0.9700
O5—Sr2iii2.707 (7)C7—C81.489 (16)
O5—H50.8200C8—H8A0.9800
O5—C51.394 (13)C8—C91.500 (14)
O6—Sr2iii2.674 (8)C9—H9A0.9800
O6—H60.8200C9—C101.508 (14)
O6—C61.392 (15)C10—H10A0.9800
O7—C71.453 (14)C10—C111.555 (14)
O7—C111.430 (12)C11—C121.501 (15)
O8—H80.8200C12—H12A0.9700
O8—C81.463 (13)C12—H12B0.9700
O9—H90.8200C13—H13A0.9700
O9—C91.409 (12)C13—H13B0.9700
O10—H100.8200C13—C141.522 (15)
O10—C101.422 (12)C14—H14A0.9800
O11—H110.8200C14—C151.504 (14)
O11—C111.410 (12)C15—H15A0.9800
O12—H120.8200C15—C161.514 (15)
O12—C121.438 (13)C16—H16A0.9800
O13—C131.437 (13)C16—C171.536 (14)
O13—C171.404 (12)C17—C181.522 (15)
O14—Sr1iv2.714 (7)C18—H18A0.9700
O14—H140.8200C18—H18B0.9700
O14—C141.399 (13)O4W—H4WA0.8500
O15—Sr1iv2.605 (7)O4W—H4WB0.8502
O2—Sr1—O11126.3 (2)Sr2—O18—H18126.9
O2—Sr1—O14i107.8 (2)C18—O18—Sr2120.6 (6)
O2—Sr1—C11126.3 (2)C18—O18—H18109.5
O3—Sr1—O259.0 (2)Sr1—O1W—H1WA112.8
O3—Sr1—O10145.1 (2)Sr1—O1W—H1WB112.3
O3—Sr1—O11139.2 (2)H1WA—O1W—H1WB106.0
O3—Sr1—O12142.2 (2)Sr1—O2W—H2WA125.3
O3—Sr1—O14i72.8 (2)Sr1—O2W—H2WB125.4
O3—Sr1—O15i91.0 (3)H2WA—O2W—H2WB109.3
O3—Sr1—O2W83.6 (3)Sr2—O3W—H3WA126.1
O3—Sr1—C11162.6 (3)Sr2—O3W—H3WB126.7
O10—Sr1—O286.2 (2)H3WA—O3W—H3WB107.2
O10—Sr1—O1163.1 (2)O1—C1—H1A109.1
O10—Sr1—O1267.6 (2)O1—C1—H1B109.1
O10—Sr1—O14i120.2 (2)O1—C1—C2112.7 (10)
O10—Sr1—O15i73.1 (2)H1A—C1—H1B107.8
O10—Sr1—O2W83.2 (2)C2—C1—H1A109.1
O10—Sr1—C1145.5 (2)C2—C1—H1B109.1
O11—Sr1—C1123.4 (2)O2—C2—C1112.7 (9)
O12—Sr1—O2147.0 (3)O2—C2—H2A108.8
O12—Sr1—O1159.7 (2)O2—C2—C3106.6 (9)
O12—Sr1—O14i71.9 (2)C1—C2—H2A108.8
O12—Sr1—C1144.2 (2)C3—C2—C1111.1 (8)
O14i—Sr1—O11125.4 (2)C3—C2—H2A108.8
O14i—Sr1—C11116.0 (2)O3—C3—C2108.6 (8)
O15i—Sr1—O270.8 (2)O3—C3—H3A109.3
O15i—Sr1—O11129.8 (2)O3—C3—C4109.3 (8)
O15i—Sr1—O1282.2 (3)C2—C3—H3A109.3
O15i—Sr1—O14i59.2 (2)C2—C3—C4111.1 (8)
O15i—Sr1—O2W129.2 (3)C4—C3—H3A109.3
O15i—Sr1—C11106.4 (3)O4—C4—C3108.5 (8)
O1W—Sr1—O2129.7 (3)O4—C4—H4A108.8
O1W—Sr1—O375.1 (3)O4—C4—C5111.2 (8)
O1W—Sr1—O10138.0 (3)C3—C4—H4A108.8
O1W—Sr1—O1176.5 (3)C3—C4—C5110.8 (9)
O1W—Sr1—O1282.7 (3)C5—C4—H4A108.8
O1W—Sr1—O14i73.9 (3)O1—C5—C4107.8 (9)
O1W—Sr1—O15i133.1 (3)O1—C5—C6106.2 (9)
O1W—Sr1—O2W94.0 (3)O5—C5—O1111.3 (9)
O1W—Sr1—C1192.5 (3)O5—C5—C4105.0 (8)
O2W—Sr1—O263.3 (3)O5—C5—C6111.1 (9)
O2W—Sr1—O1169.9 (2)C6—C5—C4115.5 (10)
O2W—Sr1—O12128.8 (3)O6—C6—C5107.0 (10)
O2W—Sr1—O14i155.4 (3)O6—C6—H6A110.3
O2W—Sr1—C1185.3 (3)O6—C6—H6B110.3
O4ii—Sr2—O5ii61.7 (2)C5—C6—H6A110.3
O4ii—Sr2—O6ii65.0 (3)C5—C6—H6B110.3
O4ii—Sr2—O8127.1 (2)H6A—C6—H6B108.6
O4ii—Sr2—O17127.0 (2)O7—C7—H7A109.0
O4ii—Sr2—O1873.2 (2)O7—C7—H7B109.0
O5ii—Sr2—O874.8 (2)O7—C7—C8113.1 (9)
O5ii—Sr2—O17171.1 (2)H7A—C7—H7B107.8
O5ii—Sr2—O18127.3 (2)C8—C7—H7A109.0
O6ii—Sr2—O5ii58.7 (2)C8—C7—H7B109.0
O6ii—Sr2—O8116.3 (3)O8—C8—C7111.6 (9)
O6ii—Sr2—O17124.7 (2)O8—C8—H8A109.6
O6ii—Sr2—O18124.1 (3)O8—C8—C9105.9 (8)
O8—Sr2—O1796.8 (2)C7—C8—H8A109.6
O8—Sr2—O18118.3 (2)C7—C8—C9110.6 (9)
O9—Sr2—O4ii82.8 (2)C9—C8—H8A109.6
O9—Sr2—O5ii80.6 (2)O9—C9—C8110.2 (8)
O9—Sr2—O6ii136.3 (3)O9—C9—H9A108.5
O9—Sr2—O860.8 (2)O9—C9—C10110.0 (8)
O9—Sr2—O1798.0 (2)C8—C9—H9A108.5
O9—Sr2—O1867.5 (2)C8—C9—C10111.1 (8)
O16—Sr2—O4ii80.3 (2)C10—C9—H9A108.5
O16—Sr2—O5ii125.8 (2)O10—C10—C9110.6 (8)
O16—Sr2—O6ii71.2 (3)O10—C10—H10A108.4
O16—Sr2—O8152.5 (2)O10—C10—C11109.8 (8)
O16—Sr2—O9133.7 (3)C9—C10—H10A108.4
O16—Sr2—O1761.2 (2)C9—C10—C11111.2 (8)
O16—Sr2—O1866.4 (3)C11—C10—H10A108.4
O17—Sr2—O1859.0 (2)O7—C11—Sr1161.9 (6)
O3W—Sr2—O4ii135.2 (3)O7—C11—C10106.8 (8)
O3W—Sr2—O5ii96.5 (3)O7—C11—C12104.0 (8)
O3W—Sr2—O6ii70.2 (3)O11—C11—Sr150.3 (4)
O3W—Sr2—O875.0 (3)O11—C11—O7111.6 (8)
O3W—Sr2—O9135.0 (3)O11—C11—C10106.1 (8)
O3W—Sr2—O1684.0 (3)O11—C11—C12111.5 (8)
O3W—Sr2—O1778.3 (3)C10—C11—Sr180.9 (5)
O3W—Sr2—O18135.7 (3)C12—C11—Sr186.1 (6)
C1—O1—C5116.3 (8)C12—C11—C10116.8 (9)
Sr1—O2—H2130.9O12—C12—C11108.1 (8)
C2—O2—Sr1114.8 (6)O12—C12—H12A110.1
C2—O2—H2109.5O12—C12—H12B110.1
Sr1—O3—H3118.7C11—C12—H12A110.1
C3—O3—Sr1127.6 (6)C11—C12—H12B110.1
C3—O3—H3109.5H12A—C12—H12B108.4
Sr2iii—O4—H4131.8O13—C13—H13A109.3
C4—O4—Sr2iii118.7 (6)O13—C13—H13B109.3
C4—O4—H4109.5O13—C13—C14111.6 (9)
Sr2iii—O5—H5141.4H13A—C13—H13B108.0
C5—O5—Sr2iii109.1 (6)C14—C13—H13A109.3
C5—O5—H5109.5C14—C13—H13B109.3
Sr2iii—O6—H6126.5O14—C14—C13112.5 (9)
C6—O6—Sr2iii124.1 (7)O14—C14—H14A109.4
C6—O6—H6109.5O14—C14—C15107.4 (8)
C11—O7—C7113.5 (8)C13—C14—H14A109.4
Sr2—O8—H8131.2C15—C14—C13108.8 (8)
C8—O8—Sr2114.6 (6)C15—C14—H14A109.4
C8—O8—H8109.5O15—C15—C14108.7 (8)
Sr2—O9—H9126.2O15—C15—H15A109.5
C9—O9—Sr2124.3 (6)O15—C15—C16108.2 (9)
C9—O9—H9109.5C14—C15—H15A109.5
Sr1—O10—H10127.7C14—C15—C16111.4 (9)
C10—O10—Sr1118.7 (5)C16—C15—H15A109.5
C10—O10—H10109.5O16—C16—C15109.6 (8)
Sr1—O11—H11132.4O16—C16—H16A109.6
C11—O11—Sr1106.3 (5)O16—C16—C17107.6 (8)
C11—O11—H11109.5C15—C16—H16A109.6
Sr1—O12—H12128.9C15—C16—C17110.8 (9)
C12—O12—Sr1121.6 (6)C17—C16—H16A109.6
C12—O12—H12109.5O13—C17—O17111.7 (8)
C17—O13—C13115.2 (8)O13—C17—C16108.5 (8)
Sr1iv—O14—H14137.2O13—C17—C18103.5 (8)
C14—O14—Sr1iv113.3 (6)O17—C17—C16107.3 (8)
C14—O14—H14109.5O17—C17—C18111.2 (8)
Sr1iv—O15—H15125.8C18—C17—C16114.8 (9)
C15—O15—Sr1iv124.7 (6)O18—C18—C17108.8 (9)
C15—O15—H15109.5O18—C18—H18A109.9
Sr2—O16—H16124.9O18—C18—H18B109.9
C16—O16—Sr2124.6 (6)C17—C18—H18A109.9
C16—O16—H16109.5C17—C18—H18B109.9
Sr2—O17—H17138.4H18A—C18—H18B108.3
C17—O17—Sr2108.0 (5)H4WA—O4W—H4WB109.5
C17—O17—H17109.5
Symmetry codes: (i) x+2, y1/2, z+1/2; (ii) x+1, y+1/2, z+1/2; (iii) x+1, y1/2, z+1/2; (iv) x+2, y+1/2, z+1/2.
(3) top
Crystal data top
C6H18IO9Sr·IDx = 2.364 Mg m3
Mr = 575.62Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, P212121Cell parameters from 3777 reflections
a = 9.1192 (3) Åθ = 3.5–24.1°
b = 13.0908 (5) ŵ = 7.18 mm1
c = 13.5504 (8) ÅT = 293 K
V = 1617.63 (13) Å3Prismatic, colourless
Z = 40.27 × 0.11 × 0.04 mm
F(000) = 1080
Data collection top
Xcalibur, Ruby, Gemini ultra
diffractometer
2757 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source2358 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.065
Detector resolution: 10.2890 pixels mm-1θmax = 24.7°, θmin = 3.4°
ω scansh = 1010
Absorption correction: gaussian
CrysAlisPro 1.171.38.41 (Rigaku Oxford Diffraction, 2015) Numerical absorption correction based on gaussian integration over a multifaceted crystal model Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1515
Tmin = 0.310, Tmax = 0.788l = 1515
12121 measured reflections
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.039 w = 1/[σ2(Fo2) + (0.0316P)2 + 1.0965P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.080(Δ/σ)max = 0.001
S = 1.04Δρmax = 1.22 e Å3
2757 reflectionsΔρmin = 1.20 e Å3
170 parametersAbsolute structure: Flack x determined using 852 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259).
17 restraintsAbsolute structure parameter: 0.028 (10)
Primary atom site location: structure-invariant direct methods
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
xyzUiso*/UeqOcc. (<1)
I10.26889 (9)0.33345 (7)0.43707 (7)0.0492 (3)
Sr030.30922 (10)0.32713 (8)0.71049 (9)0.0311 (3)
O10.1832 (7)0.0059 (5)0.8503 (6)0.0271 (18)
O20.4438 (8)0.1235 (5)0.8673 (6)0.034 (2)
H20.40670.16310.90750.050*
O30.6306 (7)0.0213 (5)0.8203 (7)0.034 (2)
H30.68150.07230.81240.051*
O40.4420 (8)0.1532 (5)0.7044 (7)0.035 (2)
H40.51400.13650.67190.053*
O50.2242 (7)0.1813 (5)0.8339 (6)0.0286 (18)
H50.16700.17790.88050.043*
O60.1459 (9)0.1702 (6)0.6422 (7)0.048 (2)
H60.08810.16870.59580.072*
O1W0.5009 (10)0.3419 (7)0.8541 (8)0.059 (3)
H1WA0.48340.36560.91130.089*
H1WB0.59020.32360.85050.089*
O2W0.1892 (12)0.4066 (7)0.8645 (9)0.079 (4)
H2WA0.14300.37390.90890.118*
H2WB0.18940.46950.88010.118*
C10.2650 (12)0.0053 (9)0.9403 (9)0.034 (3)
H1A0.22320.06040.97910.041*
H1B0.25780.05710.97860.041*
C20.4253 (10)0.0283 (7)0.9195 (10)0.027 (3)
H2A0.48050.03000.98150.033*
C30.4886 (10)0.0532 (8)0.8515 (9)0.026 (3)
H3A0.49630.11800.88730.032*
C40.3927 (11)0.0671 (7)0.7624 (9)0.025 (3)
H4A0.40000.00550.72170.030*
C50.2327 (10)0.0847 (7)0.7868 (9)0.024 (3)
C60.1272 (13)0.0800 (7)0.7017 (9)0.035 (3)
H6A0.14610.01950.66230.042*
H6B0.02730.07640.72610.042*
O3W0.078 (2)0.4012 (15)0.6331 (18)0.058 (7)*0.55 (3)
H3WA0.00750.36510.60540.087*0.55 (3)
H3WB0.05620.46670.62900.087*0.55 (3)
O3X0.041 (2)0.3700 (16)0.695 (2)0.051 (8)*0.45 (3)
H3XA0.00460.42700.71080.077*0.45 (3)
H3XB0.02920.33030.67260.077*0.45 (3)
I20.35571 (9)0.27304 (7)1.09764 (8)0.0495 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.0481 (5)0.0449 (5)0.0547 (6)0.0183 (4)0.0166 (4)0.0096 (5)
Sr030.0242 (5)0.0197 (5)0.0495 (8)0.0003 (4)0.0017 (5)0.0052 (6)
O10.027 (4)0.026 (4)0.029 (5)0.004 (3)0.004 (4)0.012 (3)
O20.035 (4)0.020 (4)0.046 (6)0.000 (3)0.007 (4)0.006 (4)
O30.022 (4)0.024 (4)0.055 (6)0.000 (3)0.000 (4)0.001 (4)
O40.028 (4)0.032 (4)0.046 (6)0.010 (3)0.015 (4)0.013 (4)
O50.033 (4)0.020 (3)0.032 (5)0.004 (3)0.009 (4)0.002 (3)
O60.048 (5)0.047 (5)0.049 (6)0.015 (5)0.020 (5)0.020 (5)
O1W0.055 (5)0.058 (7)0.063 (8)0.008 (5)0.008 (5)0.002 (6)
O2W0.098 (8)0.041 (5)0.098 (10)0.003 (6)0.050 (7)0.021 (6)
C10.040 (7)0.030 (6)0.033 (8)0.004 (5)0.019 (7)0.011 (6)
C20.022 (5)0.031 (6)0.029 (8)0.003 (4)0.001 (5)0.001 (6)
C30.024 (5)0.017 (5)0.037 (9)0.000 (4)0.003 (6)0.001 (5)
C40.027 (6)0.014 (5)0.034 (8)0.002 (4)0.012 (5)0.001 (5)
C50.019 (5)0.016 (5)0.038 (8)0.000 (4)0.005 (6)0.002 (5)
C60.036 (6)0.026 (6)0.043 (9)0.002 (5)0.005 (7)0.002 (6)
I20.0336 (4)0.0582 (5)0.0568 (7)0.0015 (4)0.0048 (4)0.0138 (5)
Geometric parameters (Å, º) top
I1—Sr033.7241 (16)O6—H60.8201
Sr03—O2i2.569 (7)O6—C61.440 (12)
Sr03—O3i2.634 (7)O1W—H1WA0.8501
Sr03—O42.581 (7)O1W—H1WB0.8500
Sr03—O52.654 (7)O2W—H2WA0.8498
Sr03—O62.701 (8)O2W—H2WB0.8501
Sr03—O1W2.623 (9)C1—H1A0.9700
Sr03—O2W2.576 (10)C1—H1B0.9700
Sr03—C53.410 (10)C1—C21.518 (14)
Sr03—O3W2.544 (18)C2—H2A0.9800
Sr03—O3X2.52 (2)C2—C31.522 (15)
O1—C11.437 (14)C3—H3A0.9800
O1—C51.417 (12)C3—C41.501 (16)
O2—Sr03ii2.569 (7)C4—H4A0.9800
O2—H20.8248C4—C51.514 (13)
O2—C21.443 (13)C5—C61.504 (16)
O3—Sr03ii2.634 (7)C6—H6A0.9700
O3—H30.8199C6—H6B0.9700
O3—C31.425 (12)O3W—H3WA0.8833
O4—H40.8201O3W—H3WB0.8832
O4—C41.446 (11)O3X—H3XA0.8790
O5—H50.8201O3X—H3XB0.8780
O5—C51.418 (11)
O2i—Sr03—I170.90 (19)Sr03—O4—H4128.9
O2i—Sr03—O3i60.6 (2)C4—O4—Sr03121.7 (5)
O2i—Sr03—O478.3 (2)C4—O4—H4109.5
O2i—Sr03—O5134.1 (2)Sr03—O5—H5135.2
O2i—Sr03—O6122.3 (3)C5—O5—Sr03110.0 (6)
O2i—Sr03—O1W72.6 (3)C5—O5—H5109.5
O2i—Sr03—O2W127.1 (3)Sr03—O6—H6129.4
O2i—Sr03—C5122.5 (2)C6—O6—Sr03119.8 (6)
O3i—Sr03—I180.89 (19)C6—O6—H6109.5
O3i—Sr03—O5148.8 (2)Sr03—O1W—H1WA125.3
O3i—Sr03—O6142.6 (2)Sr03—O1W—H1WB125.1
O3i—Sr03—C5171.4 (3)H1WA—O1W—H1WB109.6
O4—Sr03—I192.0 (2)Sr03—O2W—H2WA125.5
O4—Sr03—O3i138.5 (2)Sr03—O2W—H2WB126.2
O4—Sr03—O561.5 (2)H2WA—O2W—H2WB108.3
O4—Sr03—O665.0 (3)O1—C1—H1A109.4
O4—Sr03—O1W77.0 (3)O1—C1—H1B109.4
O4—Sr03—C544.3 (2)O1—C1—C2111.3 (10)
O5—Sr03—I1127.88 (16)H1A—C1—H1B108.0
O5—Sr03—O660.5 (2)C2—C1—H1A109.4
O5—Sr03—C523.0 (2)C2—C1—H1B109.4
O6—Sr03—I167.76 (18)O2—C2—C1112.0 (8)
O6—Sr03—C544.2 (2)O2—C2—H2A109.9
O1W—Sr03—I1143.4 (2)O2—C2—C3105.3 (9)
O1W—Sr03—O3i84.7 (3)C1—C2—H2A109.9
O1W—Sr03—O577.3 (3)C1—C2—C3109.8 (9)
O1W—Sr03—O6132.7 (3)C3—C2—H2A109.9
O1W—Sr03—C588.8 (3)O3—C3—C2108.6 (8)
O2W—Sr03—I1139.0 (3)O3—C3—H3A109.6
O2W—Sr03—O3i80.0 (3)O3—C3—C4109.0 (10)
O2W—Sr03—O4125.6 (3)C2—C3—H3A109.6
O2W—Sr03—O569.9 (3)C4—C3—C2110.5 (8)
O2W—Sr03—O6110.5 (3)C4—C3—H3A109.6
O2W—Sr03—O1W69.7 (4)O4—C4—C3110.5 (8)
O2W—Sr03—C592.5 (3)O4—C4—H4A108.3
C5—Sr03—I1107.6 (2)O4—C4—C5107.4 (8)
O3W—Sr03—I160.0 (5)C3—C4—H4A108.3
O3W—Sr03—O2i117.4 (6)C3—C4—C5113.8 (10)
O3W—Sr03—O3i74.9 (5)C5—C4—H4A108.3
O3W—Sr03—O4135.3 (5)O1—C5—Sr03157.9 (7)
O3W—Sr03—O5107.0 (5)O1—C5—O5111.0 (9)
O3W—Sr03—O672.1 (5)O1—C5—C4109.2 (8)
O3W—Sr03—O1W146.0 (5)O1—C5—C6103.4 (8)
O3W—Sr03—O2W80.1 (6)O5—C5—Sr0347.0 (5)
O3W—Sr03—C5108.1 (5)O5—C5—C4106.7 (8)
O3X—Sr03—I179.5 (6)O5—C5—C6110.3 (8)
O3X—Sr03—O2i139.6 (7)C4—C5—Sr0383.0 (5)
O3X—Sr03—O3i88.5 (5)C6—C5—Sr0386.3 (6)
O3X—Sr03—O4130.5 (5)C6—C5—C4116.3 (10)
O3X—Sr03—O585.9 (6)O6—C6—C5108.7 (9)
O3X—Sr03—O666.8 (5)O6—C6—H6A110.0
O3X—Sr03—O1W133.8 (6)O6—C6—H6B110.0
O3X—Sr03—O2W64.2 (6)C5—C6—H6A110.0
O3X—Sr03—C591.9 (6)C5—C6—H6B110.0
C5—O1—C1115.1 (8)H6A—C6—H6B108.3
Sr03ii—O2—H2118.2Sr03—O3W—H3WA125.2
C2—O2—Sr03ii121.4 (5)Sr03—O3W—H3WB125.8
C2—O2—H299.9H3WA—O3W—H3WB109.0
Sr03ii—O3—H3130.3Sr03—O3X—H3XA128.7
C3—O3—Sr03ii121.3 (5)Sr03—O3X—H3XB127.1
C3—O3—H3108.4H3XA—O3X—H3XB104.2
Symmetry codes: (i) x+1, y+1/2, z+3/2; (ii) x+1, y1/2, z+3/2.
 

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