research communications
H-imidazol-3-ium] hexachloridostannate(IV)
optical property and Hirshfeld surface analysis of bis[1-(prop-2-en-1-yl)-1aChemistry Department, College of Science, IMSIU (Imam Mohammad Ibn Saud Islamic University), Riyadh 11623, Kingdom of Saudi Arabia
*Correspondence e-mail: hhferjani@imamu.edu.sa
A new 0D organic–inorganic hybrid material bis[1-(prop-2-en-1-yl)-1H-imidazol-3-ium] hexachloridostannate(IV), (C6H9N2)2[SnCl6], has been prepared and characterized by single-crystal X-ray diffraction, Hirshfeld surface analysis and UV–visible spectroscopy. The structure consists of isolated [SnCl6]2− octahedral anions separated by layers of organic 1-(prop-2-en-1-yl)-1H-imidazol-3-ium cations. The 1-(prop-2-en-1-yl) fragment in the organic cation exhibits disorder over two sets of atomic sites having occupancies of 0.512 (9) and 0.488 (9). The crystal packing of the title compound is established by intermolecular N/C–H⋯Cl hydrogen bond and π– π stacking interactions. Hirshfeld surface analysis employing three-dimensional molecular surface contours and two-dimensional fingerprint plots has been used to analyse the intermolecular interactions present in the structure. The optical properties of the crystal were studied using UV–visible absorption spectroscopy, showing one intense band at 208 nm, which is attributed to π–π* transitions in the cations.
Keywords: chloridostannate(IV); 1-(prop-2-en-1-yl)-1H-imidazole; Hirshfeld surface; fingerprint plots; optical absorption.; crystal structure.
CCDC reference: 2021940
1. Chemical context
Tin(IV) halide organic–inorganic hybrid compounds are significant materials because of their interesting structural topologies and their wide range of optical applications such as luminescence, non-linear activity and semiconductivity (Hajji et al., 2016, 2019; BelhajSalah et al., 2018). As part of a continuing search of new organic–inorganic hybrid compounds such as Bi2Cl104− (Ferjani & Boughzala, 2018; Ferjani et al., 2020) and Hg2Cl6 (Garci et al., 2019), the synthesis and characterization of a new hybrid material, bis[1-(prop-2-en-1-yl)-1H-imidazol-3-ium] hexachloridostannate(IV), (C6H9N2)2[SnCl6] is reported.
Imidazole was chosen as the organic cation because the resulting complexes show interesting structural, chemical and physical properties significant for et al., 2019; Babar et al., 2019; Ishak et al., 2019). The Hirshfeld surface analysis was performed to completely characterize the intermolecular interactions and explain the crystalline architecture. Moreover, the UV–visible spectrum was also investigated.
magnetism, ferroelectricity, and conductivity (Tritt-Goc2. Structural commentary
The 6H9N2)2[SnCl6] contains one (C6H9N2)+ cation and one half of an [SnCl6]2− anion (Fig. 1). The SnIV atom is located on a special position of 21/n (crystallographic center of inversion) and is coordinated by six chlorine atoms in an octahedral geometry. The hexachlorostannate(IV) octahedron is nearly perfect with Sn—Cl bond lengths ranging from 2.4136 (6) to 2.4363 (6) Å and Cl—Sn—Cl bond angles between 88.44 (3) and 180°. These bond lengths and angles are in good agreement with those observed in similar compounds based on hexachlorostannate(IV) (van Megen et al., 2013; Zhou et al., 2012; Rademeyer et al., 2007). The organic (C6H9N2)+ cations are related to each other by 21/n symmetry elements. The overall negative charges in the structure are counter-balanced by the protonated 1-(prop-2-en-1-yl)-1H-imidazol-3-ium cations (Fig. 1). As usual, this aromatic amine is protonated at the N1 atom. The C=C and ring C—N bond lengths vary from 1.253 (8) to 1.307 (5), and 1.265 (6) to 1.349 (5) Å, respectively, which agree well with those in homologous materials involving 1-(prop-2-en-1-yl)-1H-imidazole (Ferjani, 2020; Parshina et al., 2019). The can be described as an organization of organic–inorganic layers, which propagate along the a axis at y = 0 and y = 1/2 (Fig. 2). These layers are formed by [SnCl6]2− octahedra and (C6H9N2)+ organic cations.
of (C3. Supramolecular features
The cohesion and stabilization of the title structure is ensured by N—H⋯Cl and C—H⋯Cl hydrogen bonds between the NH+ unit of 1H-imidazol-3-ium as the donor group and the chlorine atoms of the [SnCl6]2− octahedron as acceptor with H⋯Cl lengths ranging between 2.67 and 2.98 Å (Fig. 2 and Table 1). Additional stabilization is provided by weak π–π stacking interactions between 1H-imidazol-3-ium rings with a centroid-to-centroid distance of 3.996 (2) Å (Fig. 3).
4. Hirshfeld surface analysis
The Hirshfeld surface analysis (Spackman & Jayatilaka, 2009) was performed and the associated 2D fingerprint plots (McKinnon et al., 2007) generated using Crystal Explorer 17 (Turner et al., 2017). The Hirshfeld surface was calculated using a standard (high) surface resolution with the three-dimensional (3D) dnorm surface plotted over a fixed colour scale mapped over the range −0.208 (red) to 1.180 (blue) a.u. The dnorm mapping indicates that strong hydrogen-bonding interactions, such as N—H⋯Cl hydrogen bonding between chlorine atoms and imidazolium groups and C—H⋯Cl hydrogen bonding between chlorine atoms and the hydrogen atoms of the 1-(prop-2-en-1-yl) groups, appear to be the primary interactions in the structure, seen as a bright-red area in the Hirshfeld surface (Fig. 4).
A shape-index map of the title compound was calculated in the range −0.995 to 0.996 a.u. (Fig. 4). The convex blue regions on the shape-index symbolize hydrogen-donor groups and the concave red regions symbolize hydrogen-acceptor groups. π–π interactions are generally indicated by adjacent red and blue triangles on the shape-index map of the Hirshfeld surface.
A curvedness map of the title compound was generated in the range −3.411 to 0.368 a.u. (Fig. 4). The large flat region of green around the rings delineated by a blue outline on the Hirshfeld surface plotted over curvedness refer to the π–π stacking interactions.
The overall 2D fingerprint plot for all contacts are shown in Fig. 5, together with their relative contributions to the Hirshfeld surface. The 2D fingerprint plots show that the dominant intermolecular H⋯Cl (N/C-H⋯Cl) and H⋯H interactions contribute 59.8% and 25.6%, respectively, to the overall crystal packing. The fingerprint plot of H⋯Cl contacts, which represent the largest contribution to the Hirshfeld surfaces (59.8%), shows two large spikes highly concentrated at the edges, having almost the same de + di = 2.7 Å (Fig. 5). The H⋯H interactions appear as the next largest region of the fingerprint plot (25.6%), and have a distinct pattern with a minimum value of de = di = 1 Å (Fig. 5). Apart from these above, C⋯Cl, C⋯H, Cl⋯Cl, Cl⋯N, N⋯H, C⋯C, and C⋯N interactions were observed, which are summarized in Fig. 5.
5. Database survey
In the Cambridge Structural Database (Version 5.40, November 2019; Groom et al., 2016), eight structures of transition-metal coordination compounds with the 1-allylimidazole ligand are reported. The environment for the central ion in the [ML6]2+ ion is provided by the nitrogen atoms of six imidazole rings (Kurdziel & Glowiak, 2000; Kurdziel & Glowiak, 1998) or by other ligands with the imidazole rings (Glowiak & Kurdziel, 2000; Curtis et al. 2008; Kurdziel & Glowiak, 1998; Li & Liu, 2010). However, there is no structure reported of a post-transition-metal complex with 1-allylimidazole as ligand. One bismuth complex with 1-allylimidazole (C6H9N2)4[Bi4I16]·2H2O has been recently determined by Ferjani (2020), but is not yet available in the CSD. This and the title structure have the same monoclinic crystallographic P21/n symmetry. However, one has two cations in the and the other has only one. The half anionic cluster in the sits on a crystallographic inversion center.
6. UV–visible spectroscopy
Optical absorption (OA) of the title compound was measured at ambient temperature in water. The experimental UV–visible . It shows one intense absorption band at 208 nm. According to a similar compound studied previously (Maalaoui et al., 2012; Lassoued et al., 2017; Hermi et al., 2020; Mathlouthi et al., 2017), we assign this band to π–π* transitions within the (C6H9N2)+ organic cations.
of the title compound is shown in Fig. 67. Synthesis and crystallization
The title compound was prepared by dissolving 0.34 g (1 mmol) of 1-allylimidazole [1-(prop-2-en-1-yl)-1H-imidazole] and 0.3 g (2 mmol) of tin(II) chloride in 10 ml of concentrated (37%) hydrochloric acid. The mixture was stirred with heating and then kept at room temperature. Three days later, colourless single crystals suitable for structural determination were obtained.
8. Refinement
Crystal data, data collection and structure . The disordered 1-(prop-2-en-1-yl) fragment in the organic cation was refined by splitting atoms C4 and C5 over two positions (C4A, C4B) and (C5A, C5B) with occupancy factors of 0.512 (9) and 0.488 (9). Geometrical restraints (SADI) on bond lengths were applied. H atoms were located in difference-Fourier maps but introduced in calculated positions and treated as riding on their parent atoms, with C—H = 0.93 and 0.97 Å, N—H = 0.86 Å with Uiso(H) = 1.2Ueq(C, N).
details are summarized in Table 2
|
Supporting information
CCDC reference: 2021940
https://doi.org/10.1107/S2056989020012177/vm2239sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2056989020012177/vm2239Isup3.hkl
Data collection: X-AREA (Stoe & Cie, 2002); cell
X-AREA (Stoe & Cie, 2002); data reduction: X-RED32 (Stoe & Cie, 2002); program(s) used to solve structure: SHELXT (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2014/7 (Sheldrick, 2015b); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).(C6H8N2)2[SnCl6] | F(000) = 536 |
Mr = 547.68 | Dx = 1.745 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
a = 9.3953 (5) Å | Cell parameters from 19596 reflections |
b = 11.7817 (6) Å | θ = 2.3–34.4° |
c = 9.8243 (5) Å | µ = 2.00 mm−1 |
β = 106.547 (4)° | T = 298 K |
V = 1042.44 (10) Å3 | Prism, colorless |
Z = 2 | 0.71 × 0.66 × 0.42 mm |
Stoe IPDS2 diffractometer | 4294 independent reflections |
Radiation source: sealed X-ray tube, 12 x 0.4 mm long-fine focus | 3326 reflections with I > 2σ(I) |
Detector resolution: 6.67 pixels mm-1 | Rint = 0.035 |
rotation method scans | θmax = 34.2°, θmin = 2.7° |
Absorption correction: integration (X-RED32; Stoe & Cie, 2002) | h = −11→14 |
Tmin = 0.311, Tmax = 0.358 | k = −17→18 |
12972 measured reflections | l = −15→15 |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-atom parameters constrained |
R[F2 > 2σ(F2)] = 0.039 | w = 1/[σ2(Fo2) + (0.0288P)2 + 0.5447P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.086 | (Δ/σ)max < 0.001 |
S = 1.14 | Δρmax = 0.65 e Å−3 |
4294 reflections | Δρmin = −0.93 e Å−3 |
126 parameters | Extinction correction: SHELXL-2014/7 (Sheldrick 2014, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
5 restraints | Extinction coefficient: 0.0276 (10) |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Sn1 | 1.0000 | 0.5000 | 0.5000 | 0.03804 (7) | |
Cl2 | 0.87600 (8) | 0.32725 (6) | 0.39099 (8) | 0.05747 (17) | |
Cl3 | 1.12514 (8) | 0.39362 (6) | 0.70986 (7) | 0.05588 (17) | |
Cl1 | 0.79125 (8) | 0.53542 (7) | 0.59310 (8) | 0.06053 (18) | |
N2 | 0.3752 (3) | 0.5613 (2) | 0.1386 (4) | 0.0803 (9) | |
N1 | 0.5438 (4) | 0.4614 (4) | 0.2679 (4) | 0.0884 (10) | |
H1A | 0.6204 | 0.4413 | 0.3351 | 0.106* | |
C2 | 0.4639 (4) | 0.3926 (3) | 0.1674 (5) | 0.0778 (10) | |
H2 | 0.4800 | 0.3156 | 0.1572 | 0.093* | |
C3 | 0.3583 (4) | 0.4548 (3) | 0.0861 (4) | 0.0718 (9) | |
H3 | 0.2849 | 0.4301 | 0.0065 | 0.086* | |
C1 | 0.4905 (5) | 0.5607 (4) | 0.2501 (5) | 0.0895 (13) | |
H1 | 0.5276 | 0.6231 | 0.3073 | 0.107* | |
C6 | 0.0239 (5) | 0.6629 (5) | −0.0277 (6) | 0.1064 (17) | |
H6A | 0.0288 | 0.6570 | −0.1207 | 0.128* | 0.512 (9) |
H6B | −0.0676 | 0.6696 | −0.0097 | 0.128* | 0.512 (9) |
C5A | 0.1409 (7) | 0.6617 (7) | 0.0733 (9) | 0.0645 (19) | 0.488 (9) |
H5A | 0.1396 | 0.6674 | 0.1674 | 0.077* | 0.488 (9) |
C4A | 0.2828 (8) | 0.6505 (7) | 0.0334 (13) | 0.085 (3) | 0.512 (9) |
H4A1 | 0.3346 | 0.7226 | 0.0435 | 0.102* | 0.512 (9) |
H4A2 | 0.2635 | 0.6247 | −0.0639 | 0.102* | 0.512 (9) |
C4B | 0.2765 (9) | 0.6630 (6) | 0.1398 (10) | 0.073 (2) | 0.488 (9) |
H4B1 | 0.2290 | 0.6558 | 0.2150 | 0.087* | 0.488 (9) |
H4B2 | 0.3340 | 0.7326 | 0.1543 | 0.087* | 0.488 (9) |
C5B | 0.1662 (11) | 0.6638 (8) | 0.0018 (11) | 0.086 (3) | 0.512 (9) |
H5B | 0.2039 | 0.6651 | −0.0761 | 0.103* | 0.512 (9) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Sn1 | 0.04007 (11) | 0.03416 (10) | 0.03755 (11) | 0.00060 (9) | 0.00730 (7) | 0.00264 (8) |
Cl2 | 0.0611 (4) | 0.0399 (3) | 0.0626 (4) | −0.0058 (3) | 0.0033 (3) | −0.0064 (3) |
Cl3 | 0.0597 (4) | 0.0527 (3) | 0.0467 (3) | 0.0001 (3) | 0.0015 (3) | 0.0136 (3) |
Cl1 | 0.0553 (4) | 0.0704 (4) | 0.0611 (4) | 0.0057 (3) | 0.0250 (3) | −0.0003 (3) |
N2 | 0.0484 (14) | 0.0470 (14) | 0.140 (3) | −0.0018 (11) | 0.0178 (16) | 0.0098 (16) |
N1 | 0.0568 (17) | 0.107 (3) | 0.090 (2) | −0.0018 (19) | 0.0023 (15) | 0.016 (2) |
C2 | 0.071 (2) | 0.0554 (19) | 0.111 (3) | 0.0096 (17) | 0.033 (2) | 0.005 (2) |
C3 | 0.069 (2) | 0.067 (2) | 0.071 (2) | −0.0158 (17) | 0.0064 (16) | −0.0003 (17) |
C1 | 0.066 (2) | 0.086 (3) | 0.117 (3) | −0.024 (2) | 0.027 (2) | −0.038 (3) |
C6 | 0.078 (3) | 0.124 (4) | 0.107 (3) | −0.015 (3) | 0.009 (2) | 0.037 (3) |
C5A | 0.064 (4) | 0.076 (4) | 0.059 (4) | 0.012 (3) | 0.028 (3) | 0.014 (3) |
C4A | 0.068 (4) | 0.068 (4) | 0.127 (9) | 0.020 (3) | 0.042 (5) | 0.045 (5) |
C4B | 0.075 (5) | 0.052 (4) | 0.081 (6) | 0.000 (3) | 0.005 (4) | 0.002 (3) |
C5B | 0.099 (7) | 0.078 (5) | 0.072 (5) | 0.010 (5) | 0.010 (5) | 0.023 (4) |
Sn1—Cl3 | 2.4131 (6) | C3—H3 | 0.9300 |
Sn1—Cl3i | 2.4131 (6) | C1—H1 | 0.9300 |
Sn1—Cl1i | 2.4247 (7) | C6—C5A | 1.253 (8) |
Sn1—Cl1 | 2.4247 (7) | C6—C5B | 1.285 (10) |
Sn1—Cl2 | 2.4363 (6) | C6—H6A | 0.9300 |
Sn1—Cl2i | 2.4363 (6) | C6—H6B | 0.9300 |
N2—C1 | 1.303 (5) | C5A—C4A | 1.499 (9) |
N2—C3 | 1.349 (5) | C5A—H5A | 0.9300 |
N2—C4B | 1.517 (8) | C4A—H4A1 | 0.9700 |
N2—C4A | 1.554 (8) | C4A—H4A2 | 0.9700 |
N1—C1 | 1.265 (6) | C4B—C5B | 1.453 (9) |
N1—C2 | 1.331 (5) | C4B—H4B1 | 0.9700 |
N1—H1A | 0.8600 | C4B—H4B2 | 0.9700 |
C2—C3 | 1.307 (5) | C5B—H5B | 0.9300 |
C2—H2 | 0.9300 | ||
Cl3—Sn1—Cl3i | 180.0 | C2—C3—H3 | 126.2 |
Cl3—Sn1—Cl1i | 89.04 (3) | N2—C3—H3 | 126.2 |
Cl3i—Sn1—Cl1i | 90.96 (3) | N1—C1—N2 | 108.8 (4) |
Cl3—Sn1—Cl1 | 90.96 (3) | N1—C1—H1 | 125.6 |
Cl3i—Sn1—Cl1 | 89.04 (3) | N2—C1—H1 | 125.6 |
Cl1i—Sn1—Cl1 | 180.0 | C5A—C6—H6A | 120.0 |
Cl3—Sn1—Cl2 | 89.85 (2) | C5A—C6—H6B | 120.0 |
Cl3i—Sn1—Cl2 | 90.15 (2) | H6A—C6—H6B | 120.0 |
Cl1i—Sn1—Cl2 | 91.56 (3) | C6—C5A—C4A | 116.0 (7) |
Cl1—Sn1—Cl2 | 88.44 (3) | C6—C5A—H5A | 122.0 |
Cl3—Sn1—Cl2i | 90.15 (2) | C4A—C5A—H5A | 122.0 |
Cl3i—Sn1—Cl2i | 89.85 (2) | C5A—C4A—N2 | 104.8 (6) |
Cl1i—Sn1—Cl2i | 88.44 (3) | C5A—C4A—H4A1 | 110.8 |
Cl1—Sn1—Cl2i | 91.56 (3) | N2—C4A—H4A1 | 110.8 |
Cl2—Sn1—Cl2i | 180.0 | C5A—C4A—H4A2 | 110.8 |
C1—N2—C3 | 107.2 (3) | N2—C4A—H4A2 | 110.8 |
C1—N2—C4B | 111.2 (4) | H4A1—C4A—H4A2 | 108.9 |
C3—N2—C4B | 137.0 (4) | C5B—C4B—N2 | 105.8 (7) |
C1—N2—C4A | 137.4 (5) | C5B—C4B—H4B1 | 110.6 |
C3—N2—C4A | 113.1 (6) | N2—C4B—H4B1 | 110.6 |
C1—N1—C2 | 110.1 (3) | C5B—C4B—H4B2 | 110.6 |
C1—N1—H1A | 124.9 | N2—C4B—H4B2 | 110.6 |
C2—N1—H1A | 124.9 | H4B1—C4B—H4B2 | 108.7 |
C3—C2—N1 | 106.3 (3) | C6—C5B—C4B | 129.0 (10) |
C3—C2—H2 | 126.8 | C6—C5B—H5B | 115.5 |
N1—C2—H2 | 126.8 | C4B—C5B—H5B | 115.5 |
C2—C3—N2 | 107.6 (3) | ||
C1—N1—C2—C3 | 0.2 (5) | C4A—N2—C1—N1 | −160.5 (6) |
N1—C2—C3—N2 | −0.1 (5) | C6—C5A—C4A—N2 | −135.5 (8) |
C1—N2—C3—C2 | 0.0 (5) | C1—N2—C4A—C5A | −106.0 (7) |
C4B—N2—C3—C2 | −152.5 (7) | C3—N2—C4A—C5A | 94.2 (8) |
C4A—N2—C3—C2 | 165.9 (4) | C1—N2—C4B—C5B | 171.4 (6) |
C2—N1—C1—N2 | −0.1 (5) | C3—N2—C4B—C5B | −36.7 (11) |
C3—N2—C1—N1 | 0.1 (5) | N2—C4B—C5B—C6 | 124.1 (9) |
C4B—N2—C1—N1 | 160.4 (5) |
Symmetry code: (i) −x+2, −y+1, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···Cl2 | 0.86 | 2.67 | 3.399 (4) | 144 |
N1—H1A···Cl1 | 0.86 | 2.81 | 3.485 (4) | 136 |
C2—H2···Cl3ii | 0.93 | 2.79 | 3.672 (4) | 158 |
C3—H3···Cl3iii | 0.93 | 2.90 | 3.790 (4) | 160 |
C4A—H4A1···Cl2iv | 0.97 | 2.89 | 3.716 (9) | 144 |
C4A—H4A1···Cl1v | 0.97 | 2.94 | 3.743 (10) | 141 |
C4B—H4B1···Cl1vi | 0.97 | 2.98 | 3.702 (10) | 133 |
C4B—H4B2···Cl1v | 0.97 | 2.80 | 3.590 (7) | 139 |
C5B—H5B···Cl2vii | 0.93 | 2.97 | 3.766 (11) | 145 |
Symmetry codes: (ii) x−1/2, −y+1/2, z−1/2; (iii) x−1, y, z−1; (iv) −x+3/2, y+1/2, −z+1/2; (v) x−1/2, −y+3/2, z−1/2; (vi) −x+1, −y+1, −z+1; (vii) −x+1, −y+1, −z. |
Acknowledgements
Dr Necmi Dege of the Department of Physics, Ondokuz Mayıs University (Samsun, Turkey), is thanked for performing the SCXRD and UV–visible measurements related to this work.
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