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The judicious selection of suitable ligands is vitally important in the construction of novel metal–organic frameworks (MOFs) with fascinating structures and inter­esting properties. Recently, imid­azole-containing multidentate ligands have received much attention. Two new CdII coordination frameworks, namely, poly[tris­{μ-1,4-bis­[(1H-imid­azol-1-yl)meth­yl]benzene-κ2N3:N3′}tetra­kis­(nitrato-κ2O,O′)dicadmium], [Cd2(NO3)4(C14H14N4)3]n, (I), and poly[[bis­{μ3-1,3,5-tris­[(1H-imid­azol-1-yl)meth­yl]benzene-κ3N3:N3′:N3′′}cadmium] hexa­fluoro­silicate], {[Cd(C18H18N6)2](SiF6)}n, (II), have been synthesized and characterized by elemental analysis, IR spectroscopy and single-crystal X-ray diffraction. In polymer (I), the 1,4-bis­[(1H-imid­azol-1-yl)meth­yl]benzene ligand bridges Cd2+ ions with a distorted seven-coordinated penta­gonal bipyramidal geometry, forming a one-dimensional ladder chain, and the nitrate anions coordinate to the Cd2+ ions in a terminal bidentate fashion. In the crystal, adjacent chains are further connected by C—H...O hydrogen bonds to generate a two-dimensional (2D) supra­molecular structure. Polymer (II) exhibits a 2D layered structure in which 1,3,5-tris­[(1H-imid­azol-1-yl)meth­yl] benzene ligands join Cd2+ centres having a six-coordinated octa­hedral structure. The layers are connected by hexa­fluoro­silicate anions via C—H...F hydrogen-bond inter­actions, giving rise to a three-dimensional supra­molecular network structure in the solid state. In addition, powder X-ray diffraction (PXRD) patterns were recorded, thermogravimetric analyses (TGA) carried out and fluorescence properties investigated.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229620002594/ep3002sup1.cif
Contains datablocks I, II, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229620002594/ep3002Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229620002594/ep3002IIsup3.hkl
Contains datablock p

CCDC references: 1986082; 1986081

Computing details top

For both structures, data collection: CrystalClear (Rigaku, 2007); cell refinement: CrystalClear (Rigaku, 2007); data reduction: CrystalClear (Rigaku, 2007); program(s) used to solve structure: SHELXT2014 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015b); molecular graphics: XP in SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Poly[tris{µ-1,4-bis[(1H-imidazol-1-yl)methyl]benzene-κ2N3:N3'}tetrakis(nitrato-κ2O,O')dicadmium] (I) top
Crystal data top
[Cd2(NO3)4(C14H14N4)3]Z = 1
Mr = 1187.72F(000) = 598
Triclinic, P1Dx = 1.647 Mg m3
a = 9.9336 (8) ÅMo Kα radiation, λ = 0.71073 Å
b = 10.3115 (10) ÅCell parameters from 3703 reflections
c = 12.1571 (11) Åθ = 3.9–28.5°
α = 98.729 (8)°µ = 0.97 mm1
β = 101.515 (7)°T = 293 K
γ = 94.942 (7)°Block, colourless
V = 1197.31 (19) Å30.25 × 0.22 × 0.15 mm
Data collection top
Rigaku Mercury CCD
diffractometer
5498 independent reflections
Radiation source: fine-focus sealed tube4527 reflections with I > 2σ(I)
Detector resolution: 28.5714 pixels mm-1Rint = 0.028
Graphite Monochromator scansθmax = 29.5°, θmin = 3.5°
Absorption correction: multi-scan
(REQAB; Jacobson, 1998)
h = 912
Tmin = 0.780, Tmax = 1.000k = 1213
10076 measured reflectionsl = 1616
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.034H-atom parameters constrained
wR(F2) = 0.076 w = 1/[σ2(Fo2) + (0.0289P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.001
5498 reflectionsΔρmax = 0.36 e Å3
325 parametersΔρmin = 0.53 e Å3
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*/Ueq
Cd10.02489 (2)0.75236 (2)0.24022 (2)0.04331 (8)
O10.0036 (3)0.9793 (2)0.34675 (18)0.0688 (6)
O20.2029 (3)0.9436 (2)0.3217 (2)0.0803 (7)
O30.2210 (2)0.6904 (2)0.16238 (19)0.0686 (6)
O40.0572 (3)0.5348 (2)0.14411 (19)0.0712 (6)
O50.1688 (3)1.1387 (2)0.39597 (19)0.0864 (8)
O60.2441 (3)0.4946 (2)0.0862 (2)0.1019 (9)
N10.0954 (2)0.6770 (2)0.40504 (18)0.0460 (5)
N20.1389 (2)0.6716 (2)0.58797 (17)0.0437 (5)
N30.0487 (2)0.8305 (2)0.07670 (17)0.0431 (5)
N40.1947 (2)0.9195 (2)0.04090 (17)0.0444 (5)
N50.2041 (2)0.7059 (2)0.24472 (18)0.0447 (5)
N60.3986 (2)0.71194 (18)0.30249 (17)0.0408 (5)
C10.0923 (3)0.7403 (3)0.5072 (2)0.0464 (6)
H1A0.06130.82260.52100.056*
C20.1461 (3)0.5617 (3)0.4237 (2)0.0496 (7)
H2A0.15940.49550.36720.060*
C30.1738 (3)0.5581 (3)0.5351 (2)0.0514 (7)
H3A0.21010.49060.56980.062*
C40.1558 (3)0.7153 (3)0.7105 (2)0.0547 (7)
H4A0.14040.63920.74640.066*
H4B0.08690.77350.72390.066*
C50.2975 (3)0.7869 (2)0.7641 (2)0.0453 (6)
C60.3866 (3)0.7384 (3)0.8453 (2)0.0624 (8)
H6A0.35920.65930.86720.075*
C70.5158 (3)0.8050 (3)0.8949 (3)0.0649 (9)
H7A0.57350.77080.95070.078*
C80.5615 (3)0.9209 (2)0.8638 (2)0.0438 (6)
C90.4722 (3)0.9679 (3)0.7816 (2)0.0596 (8)
H9A0.50011.04580.75820.072*
C100.3429 (3)0.9025 (3)0.7333 (3)0.0639 (8)
H10A0.28460.93740.67830.077*
C110.6980 (3)0.9999 (3)0.9186 (2)0.0542 (7)
H11A0.72841.04890.86410.065*
H11B0.68631.06350.98250.065*
C120.1409 (3)0.9133 (3)0.0667 (2)0.0465 (6)
H12A0.16590.96260.12840.056*
C130.1325 (3)0.8338 (3)0.1053 (2)0.0582 (8)
H13A0.14870.81620.18440.070*
C140.0435 (3)0.7796 (3)0.0327 (2)0.0501 (7)
H14A0.01300.71710.05350.060*
C150.2613 (3)0.7414 (2)0.3318 (2)0.0411 (6)
H15A0.21250.78160.40410.049*
C160.3107 (3)0.6514 (2)0.1561 (2)0.0488 (7)
H16A0.30190.61770.08280.059*
C170.4310 (3)0.6537 (2)0.1911 (2)0.0500 (7)
H17A0.51900.62180.14760.060*
C180.4922 (3)0.7248 (3)0.3822 (2)0.0517 (7)
H18A0.58460.73160.34060.062*
H18B0.46120.80510.43790.062*
C190.4963 (3)0.6073 (2)0.4432 (2)0.0426 (6)
C200.5375 (3)0.4812 (2)0.3833 (2)0.0463 (6)
H20A0.56290.46750.30410.056*
C210.4585 (3)0.6256 (2)0.5603 (2)0.0473 (7)
H21A0.43010.71030.60180.057*
N70.1256 (3)1.0219 (2)0.35643 (18)0.0568 (6)
N80.1749 (3)0.5723 (3)0.1292 (2)0.0596 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cd10.03512 (13)0.05554 (14)0.04043 (12)0.00531 (9)0.00949 (9)0.01026 (8)
O10.0626 (17)0.0659 (13)0.0714 (15)0.0001 (11)0.0104 (13)0.0012 (10)
O20.0732 (19)0.0791 (15)0.0903 (17)0.0066 (13)0.0281 (15)0.0072 (12)
O30.0515 (15)0.0641 (13)0.0860 (16)0.0066 (11)0.0150 (12)0.0004 (11)
O40.0600 (16)0.0713 (13)0.0774 (16)0.0004 (11)0.0267 (13)0.0135 (11)
O50.107 (2)0.0666 (14)0.0734 (16)0.0245 (13)0.0262 (15)0.0148 (11)
O60.072 (2)0.0993 (18)0.124 (2)0.0131 (14)0.0396 (17)0.0393 (16)
N10.0432 (15)0.0518 (13)0.0423 (13)0.0090 (10)0.0041 (10)0.0105 (10)
N20.0354 (13)0.0511 (13)0.0420 (12)0.0024 (10)0.0007 (10)0.0119 (10)
N30.0399 (14)0.0489 (12)0.0403 (12)0.0015 (10)0.0098 (10)0.0076 (9)
N40.0427 (14)0.0453 (12)0.0410 (13)0.0030 (10)0.0022 (10)0.0087 (9)
N50.0384 (14)0.0565 (13)0.0415 (12)0.0023 (10)0.0120 (10)0.0129 (10)
N60.0382 (13)0.0471 (12)0.0423 (12)0.0048 (9)0.0137 (10)0.0174 (9)
C10.0438 (17)0.0511 (15)0.0419 (15)0.0108 (12)0.0013 (12)0.0087 (11)
C20.0388 (17)0.0502 (16)0.0592 (18)0.0108 (12)0.0095 (14)0.0059 (12)
C30.0391 (17)0.0511 (17)0.0654 (19)0.0109 (13)0.0048 (14)0.0203 (14)
C40.0432 (18)0.0751 (19)0.0444 (16)0.0004 (14)0.0054 (13)0.0155 (13)
C50.0435 (17)0.0547 (15)0.0352 (14)0.0022 (12)0.0032 (12)0.0098 (11)
C60.057 (2)0.0630 (18)0.0610 (19)0.0112 (15)0.0100 (15)0.0313 (14)
C70.057 (2)0.0687 (19)0.0613 (19)0.0073 (15)0.0166 (16)0.0345 (15)
C80.0439 (17)0.0457 (14)0.0399 (14)0.0026 (12)0.0024 (12)0.0120 (11)
C90.061 (2)0.0542 (16)0.0596 (19)0.0010 (14)0.0079 (15)0.0297 (14)
C100.058 (2)0.0698 (19)0.0604 (19)0.0052 (16)0.0074 (16)0.0296 (15)
C110.0500 (19)0.0485 (15)0.0598 (18)0.0003 (13)0.0024 (14)0.0178 (13)
C120.0465 (18)0.0509 (15)0.0405 (15)0.0065 (12)0.0069 (13)0.0063 (11)
C130.071 (2)0.0645 (18)0.0382 (16)0.0038 (16)0.0151 (15)0.0057 (13)
C140.054 (2)0.0557 (16)0.0442 (16)0.0096 (13)0.0182 (14)0.0089 (12)
C150.0361 (16)0.0514 (15)0.0366 (14)0.0009 (11)0.0077 (11)0.0124 (11)
C160.0495 (19)0.0576 (16)0.0383 (15)0.0019 (13)0.0109 (13)0.0080 (12)
C170.0387 (17)0.0629 (17)0.0451 (16)0.0047 (13)0.0023 (13)0.0146 (12)
C180.0497 (19)0.0575 (16)0.0601 (18)0.0158 (13)0.0273 (15)0.0225 (13)
C190.0349 (16)0.0511 (15)0.0497 (16)0.0069 (11)0.0212 (12)0.0162 (12)
C200.0442 (18)0.0573 (16)0.0410 (14)0.0033 (12)0.0172 (13)0.0102 (12)
C210.0452 (18)0.0476 (15)0.0507 (16)0.0013 (12)0.0189 (13)0.0062 (12)
N70.075 (2)0.0567 (16)0.0356 (13)0.0016 (14)0.0134 (13)0.0029 (10)
N80.0469 (17)0.0759 (18)0.0505 (15)0.0119 (14)0.0104 (13)0.0089 (12)
Geometric parameters (Å, º) top
Cd1—N12.261 (2)C4—H4A0.9700
Cd1—N32.268 (2)C4—H4B0.9700
Cd1—N52.297 (2)C5—C61.373 (4)
Cd1—O32.422 (2)C5—C101.369 (4)
Cd1—O42.446 (2)C6—C71.378 (4)
Cd1—O22.471 (2)C6—H6A0.9300
Cd1—O12.544 (2)C7—C81.374 (3)
O1—N71.230 (3)C7—H7A0.9300
O2—N71.245 (3)C8—C91.374 (3)
O3—N81.240 (3)C8—C111.493 (4)
O4—N81.256 (3)C9—C101.371 (4)
O5—N71.232 (3)C9—H9A0.9300
O6—N81.224 (3)C10—H10A0.9300
N1—C11.320 (3)C11—N4ii1.460 (3)
N1—C21.363 (3)C11—H11A0.9700
N2—C11.329 (3)C11—H11B0.9700
N2—C31.354 (3)C12—H12A0.9300
N2—C41.461 (3)C13—C141.340 (4)
N3—C121.305 (3)C13—H13A0.9300
N3—C141.366 (3)C14—H14A0.9300
N4—C121.324 (3)C15—H15A0.9300
N4—C131.361 (3)C16—C171.347 (4)
N4—C11i1.460 (3)C16—H16A0.9300
N5—C151.318 (3)C17—H17A0.9300
N5—C161.363 (3)C18—C191.515 (3)
N6—C151.334 (3)C18—H18A0.9700
N6—C171.357 (3)C18—H18B0.9700
N6—C181.471 (3)C19—C211.377 (3)
C1—H1A0.9300C19—C201.376 (3)
C2—C31.334 (4)C20—C21iii1.385 (3)
C2—H2A0.9300C20—H20A0.9300
C3—H3A0.9300C21—C20iii1.385 (3)
C4—C51.503 (4)C21—H21A0.9300
N1—Cd1—N3178.82 (7)C5—C6—C7121.0 (3)
N1—Cd1—N591.99 (8)C5—C6—H6A119.5
N3—Cd1—N587.24 (8)C7—C6—H6A119.5
N1—Cd1—O394.51 (8)C8—C7—C6121.5 (3)
N3—Cd1—O386.61 (8)C8—C7—H7A119.2
N5—Cd1—O3148.37 (8)C6—C7—H7A119.2
N1—Cd1—O486.24 (8)C9—C8—C7117.1 (3)
N3—Cd1—O494.75 (8)C9—C8—C11119.3 (2)
N5—Cd1—O497.63 (8)C7—C8—C11123.5 (2)
O3—Cd1—O452.11 (7)C10—C9—C8121.4 (3)
N1—Cd1—O286.29 (8)C10—C9—H9A119.3
N3—Cd1—O293.60 (8)C8—C9—H9A119.3
N5—Cd1—O2134.34 (8)C5—C10—C9121.4 (3)
O3—Cd1—O277.04 (8)C5—C10—H10A119.3
O4—Cd1—O2127.67 (8)C9—C10—H10A119.3
N1—Cd1—O191.81 (7)N4ii—C11—C8113.4 (2)
N3—Cd1—O187.23 (7)N4ii—C11—H11A108.9
N5—Cd1—O184.64 (8)C8—C11—H11A108.9
O3—Cd1—O1125.96 (8)N4ii—C11—H11B108.9
O4—Cd1—O1177.05 (8)C8—C11—H11B108.9
O2—Cd1—O149.90 (8)H11A—C11—H11B107.7
N7—O1—Cd194.61 (17)N3—C12—N4112.7 (2)
N7—O2—Cd197.78 (19)N3—C12—H12A123.6
N8—O3—Cd195.77 (17)N4—C12—H12A123.6
N8—O4—Cd194.20 (16)C14—C13—N4106.8 (2)
C1—N1—C2104.9 (2)C14—C13—H13A126.6
C1—N1—Cd1124.85 (17)N4—C13—H13A126.6
C2—N1—Cd1130.24 (18)C13—C14—N3109.5 (3)
C1—N2—C3106.9 (2)C13—C14—H14A125.3
C1—N2—C4125.8 (2)N3—C14—H14A125.3
C3—N2—C4127.3 (2)N5—C15—N6111.1 (2)
C12—N3—C14104.8 (2)N5—C15—H15A124.5
C12—N3—Cd1122.92 (17)N6—C15—H15A124.5
C14—N3—Cd1129.68 (18)C17—C16—N5109.5 (2)
C12—N4—C13106.2 (2)C17—C16—H16A125.3
C12—N4—C11i126.5 (2)N5—C16—H16A125.3
C13—N4—C11i127.3 (2)C16—C17—N6106.5 (3)
C15—N5—C16105.7 (2)C16—C17—H17A126.8
C15—N5—Cd1126.16 (18)N6—C17—H17A126.8
C16—N5—Cd1127.74 (17)N6—C18—C19111.3 (2)
C15—N6—C17107.3 (2)N6—C18—H18A109.4
C15—N6—C18124.9 (2)C19—C18—H18A109.4
C17—N6—C18127.3 (2)N6—C18—H18B109.4
N1—C1—N2111.5 (2)C19—C18—H18B109.4
N1—C1—H1A124.3H18A—C18—H18B108.0
N2—C1—H1A124.3C21—C19—C20118.9 (2)
C3—C2—N1109.8 (2)C21—C19—C18120.2 (2)
C3—C2—H2A125.1C20—C19—C18120.9 (2)
N1—C2—H2A125.1C19—C20—C21iii120.6 (2)
C2—C3—N2106.9 (2)C19—C20—H20A119.7
C2—C3—H3A126.5C21iii—C20—H20A119.7
N2—C3—H3A126.5C19—C21—C20iii120.6 (2)
N2—C4—C5112.0 (2)C19—C21—H21A119.7
N2—C4—H4A109.2C20iii—C21—H21A119.7
C5—C4—H4A109.2O1—N7—O5121.1 (3)
N2—C4—H4B109.2O1—N7—O2117.5 (2)
C5—C4—H4B109.2O5—N7—O2121.3 (3)
H4A—C4—H4B107.9O6—N8—O3120.7 (3)
C6—C5—C10117.6 (3)O6—N8—O4121.4 (3)
C6—C5—C4121.2 (2)O3—N8—O4117.9 (2)
C10—C5—C4121.2 (2)
C2—N1—C1—N20.5 (3)C11i—N4—C13—C14178.5 (3)
Cd1—N1—C1—N2179.41 (17)N4—C13—C14—N30.1 (3)
C3—N2—C1—N10.1 (3)C12—N3—C14—C130.2 (3)
C4—N2—C1—N1176.8 (2)Cd1—N3—C14—C13162.0 (2)
C1—N1—C2—C30.7 (3)C16—N5—C15—N60.0 (3)
Cd1—N1—C2—C3179.56 (19)Cd1—N5—C15—N6172.91 (14)
N1—C2—C3—N20.7 (3)C17—N6—C15—N50.5 (3)
C1—N2—C3—C20.4 (3)C18—N6—C15—N5172.9 (2)
C4—N2—C3—C2177.2 (3)C15—N5—C16—C170.4 (3)
C1—N2—C4—C590.5 (3)Cd1—N5—C16—C17173.21 (16)
C3—N2—C4—C585.8 (3)N5—C16—C17—N60.7 (3)
N2—C4—C5—C6117.2 (3)C15—N6—C17—C160.7 (3)
N2—C4—C5—C1062.4 (4)C18—N6—C17—C16172.9 (2)
C10—C5—C6—C71.0 (5)C15—N6—C18—C1981.2 (3)
C4—C5—C6—C7179.4 (3)C17—N6—C18—C1989.7 (3)
C5—C6—C7—C81.2 (5)N6—C18—C19—C21120.7 (3)
C6—C7—C8—C90.4 (5)N6—C18—C19—C2059.3 (3)
C6—C7—C8—C11177.1 (3)C21—C19—C20—C21iii0.3 (4)
C7—C8—C9—C100.4 (5)C18—C19—C20—C21iii179.7 (2)
C11—C8—C9—C10176.4 (3)C20—C19—C21—C20iii0.3 (4)
C6—C5—C10—C90.2 (5)C18—C19—C21—C20iii179.7 (2)
C4—C5—C10—C9179.8 (3)Cd1—O1—N7—O5173.5 (2)
C8—C9—C10—C50.6 (5)Cd1—O1—N7—O24.4 (3)
C9—C8—C11—N4ii152.1 (3)Cd1—O2—N7—O14.6 (3)
C7—C8—C11—N4ii31.3 (4)Cd1—O2—N7—O5173.4 (2)
C14—N3—C12—N40.1 (3)Cd1—O3—N8—O6176.5 (2)
Cd1—N3—C12—N4163.57 (17)Cd1—O3—N8—O41.5 (3)
C13—N4—C12—N30.1 (3)Cd1—O4—N8—O6176.5 (3)
C11i—N4—C12—N3178.6 (2)Cd1—O4—N8—O31.5 (3)
C12—N4—C13—C140.0 (3)
Symmetry codes: (i) x1, y, z1; (ii) x+1, y, z+1; (iii) x1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C15—H15A···O5iv0.932.383.267 (3)159
C16—H16A···O6v0.932.403.314 (4)168
C17—H17A···O6vi0.932.513.398 (4)160
Symmetry codes: (iv) x, y+2, z+1; (v) x, y+1, z; (vi) x1, y, z.
Poly[[bis{µ3-1,3,5-tris[(1H-imidazol-1-yl)methyl]benzene-κ3N3:N3':N3''}cadmium] hexafluorosilicate] (II) top
Crystal data top
[Cd(C18H18N6)2](SiF6)Dx = 1.521 Mg m3
Mr = 891.26Mo Kα radiation, λ = 0.71073 Å
Trigonal, P3Cell parameters from 3551 reflections
a = 9.5898 (2) Åθ = 4.1–29.1°
c = 12.2158 (3) ŵ = 0.67 mm1
V = 972.91 (5) Å3T = 293 K
Z = 1Block, colourless
F(000) = 4520.25 × 0.20 × 0.16 mm
Data collection top
Rigaku Mercury CCD
diffractometer
1623 independent reflections
Radiation source: fine-focus sealed tube1453 reflections with I > 2σ(I)
Detector resolution: 28.5714 pixels mm-1Rint = 0.022
Graphite Monochromator scansθmax = 29.3°, θmin = 4.1°
Absorption correction: multi-scan
(REQAB; Jacobson, 1998)
h = 1312
Tmin = 0.882, Tmax = 1.000k = 1212
8201 measured reflectionsl = 1516
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.027H-atom parameters constrained
wR(F2) = 0.066 w = 1/[σ2(Fo2) + (0.0287P)2 + 0.3052P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
1623 reflectionsΔρmax = 0.26 e Å3
86 parametersΔρmin = 0.35 e Å3
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*/Ueq
Cd11.00000.00000.50000.04031 (11)
Si10.00000.00000.00000.0305 (2)
F10.15248 (12)0.01996 (13)0.07938 (8)0.0457 (3)
N21.03296 (17)0.36519 (17)0.74645 (11)0.0389 (3)
C50.8255 (2)0.3663 (2)0.86320 (13)0.0378 (4)
N11.03700 (19)0.22129 (19)0.60726 (11)0.0446 (3)
C40.9968 (2)0.3999 (2)0.85695 (15)0.0437 (4)
H4A1.07020.51190.87480.052*
H4B1.01240.33360.91000.052*
C21.0838 (3)0.3742 (2)0.57260 (16)0.0533 (5)
H2A1.11350.41130.50130.064*
C60.6985 (2)0.2079 (2)0.86363 (14)0.0395 (4)
H6A0.72020.12360.86420.047*
C11.0070 (2)0.2215 (2)0.71248 (13)0.0433 (4)
H1A0.97180.13220.75780.052*
C31.0806 (2)0.4629 (2)0.65679 (18)0.0536 (5)
H3A1.10590.57000.65430.064*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cd10.04950 (14)0.04950 (14)0.02193 (14)0.02475 (7)0.0000.000
Si10.0354 (3)0.0354 (3)0.0208 (4)0.01768 (16)0.0000.000
F10.0468 (6)0.0531 (6)0.0391 (5)0.0264 (5)0.0117 (4)0.0019 (4)
N20.0355 (7)0.0412 (7)0.0392 (7)0.0186 (6)0.0046 (6)0.0062 (6)
C50.0394 (9)0.0442 (9)0.0310 (7)0.0216 (7)0.0062 (6)0.0088 (7)
N10.0571 (9)0.0504 (9)0.0300 (7)0.0298 (8)0.0006 (6)0.0006 (6)
C40.0411 (9)0.0499 (10)0.0412 (9)0.0237 (8)0.0116 (7)0.0170 (8)
C20.0623 (12)0.0536 (11)0.0424 (10)0.0278 (10)0.0094 (9)0.0117 (8)
C60.0458 (9)0.0404 (9)0.0365 (8)0.0247 (8)0.0079 (7)0.0022 (7)
C10.0592 (11)0.0447 (9)0.0308 (8)0.0297 (9)0.0025 (7)0.0003 (7)
C30.0536 (11)0.0403 (10)0.0623 (12)0.0200 (9)0.0097 (9)0.0076 (9)
Geometric parameters (Å, º) top
Cd1—N1i2.3650 (15)N2—C41.472 (2)
Cd1—N1ii2.3650 (15)C5—C6xi1.380 (2)
Cd1—N1iii2.3650 (15)C5—C61.394 (2)
Cd1—N12.3650 (15)C5—C41.510 (2)
Cd1—N1iv2.3651 (15)N1—C11.317 (2)
Cd1—N1v2.3651 (15)N1—C21.368 (2)
Si1—F11.6838 (9)C4—H4A0.9700
Si1—F1vi1.6838 (9)C4—H4B0.9700
Si1—F1vii1.6838 (9)C2—C31.345 (3)
Si1—F1viii1.6838 (9)C2—H2A0.9300
Si1—F1ix1.6838 (9)C6—C5xii1.380 (2)
Si1—F1x1.6838 (9)C6—H6A0.9300
N2—C11.338 (2)C1—H1A0.9300
N2—C31.363 (2)C3—H3A0.9300
N1i—Cd1—N1ii92.27 (5)F1ix—Si1—F1x180.00 (13)
N1i—Cd1—N1iii87.73 (5)C1—N2—C3106.54 (15)
N1ii—Cd1—N1iii180.0C1—N2—C4124.97 (15)
N1i—Cd1—N1180.00 (7)C3—N2—C4128.12 (16)
N1ii—Cd1—N187.73 (5)C6xi—C5—C6119.22 (17)
N1iii—Cd1—N192.27 (5)C6xi—C5—C4120.90 (16)
N1i—Cd1—N1iv92.27 (5)C6—C5—C4119.81 (15)
N1ii—Cd1—N1iv92.27 (5)C1—N1—C2104.80 (15)
N1iii—Cd1—N1iv87.73 (5)C1—N1—Cd1127.37 (12)
N1—Cd1—N1iv87.73 (5)C2—N1—Cd1127.70 (12)
N1i—Cd1—N1v87.73 (5)N2—C4—C5110.62 (13)
N1ii—Cd1—N1v87.73 (5)N2—C4—H4A109.5
N1iii—Cd1—N1v92.27 (5)C5—C4—H4A109.5
N1—Cd1—N1v92.27 (5)N2—C4—H4B109.5
N1iv—Cd1—N1v180.00 (6)C5—C4—H4B109.5
F1—Si1—F1vi180.0H4A—C4—H4B108.1
F1—Si1—F1vii89.86 (5)C3—C2—N1110.01 (17)
F1vi—Si1—F1vii90.14 (5)C3—C2—H2A125.0
F1—Si1—F1viii90.14 (5)N1—C2—H2A125.0
F1vi—Si1—F1viii89.86 (5)C5xii—C6—C5120.77 (17)
F1vii—Si1—F1viii180.00 (8)C5xii—C6—H6A119.6
F1—Si1—F1ix89.86 (5)C5—C6—H6A119.6
F1vi—Si1—F1ix90.14 (5)N1—C1—N2112.07 (16)
F1vii—Si1—F1ix90.14 (5)N1—C1—H1A124.0
F1viii—Si1—F1ix89.86 (5)N2—C1—H1A124.0
F1—Si1—F1x90.14 (5)C2—C3—N2106.58 (17)
F1vi—Si1—F1x89.86 (5)C2—C3—H3A126.7
F1vii—Si1—F1x89.86 (5)N2—C3—H3A126.7
F1viii—Si1—F1x90.14 (5)
C1—N2—C4—C587.9 (2)C2—N1—C1—N20.4 (2)
C3—N2—C4—C584.1 (2)Cd1—N1—C1—N2176.52 (11)
C6xi—C5—C4—N2104.42 (18)C3—N2—C1—N10.9 (2)
C6—C5—C4—N272.7 (2)C4—N2—C1—N1174.37 (15)
C1—N1—C2—C30.2 (2)N1—C2—C3—N20.8 (2)
Cd1—N1—C2—C3175.85 (14)C1—N2—C3—C21.0 (2)
C6xi—C5—C6—C5xii0.8 (3)C4—N2—C3—C2174.19 (17)
C4—C5—C6—C5xii176.40 (11)
Symmetry codes: (i) x+2, y, z+1; (ii) y+1, x+y+1, z+1; (iii) y+1, xy1, z; (iv) xy, x1, z+1; (v) x+y+2, x+1, z; (vi) x, y, z; (vii) y, x+y, z; (viii) y, xy, z; (ix) xy, x, z; (x) x+y, x, z; (xi) y+1, xy, z; (xii) x+y+1, x+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C4—H4B···F1xiii0.972.523.319 (2)139
C1—H1A···F1xiv0.932.403.259 (2)153
C1—H1A···F1xiii0.932.463.0247 (19)119
Symmetry codes: (xiii) xy+1, x, z+1; (xiv) x+1, y, z+1.
 

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