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Acta Crystallographica Section E: Crystallographic Communications logoLink to Acta Crystallographica Section E: Crystallographic Communications
. 2026 Jun 26;82(Pt 7):888–892. doi: 10.1107/S2056989026006596

From an unusual organotin(IV) coordination compound to the first ionic organic–inorganic mixed-valent tin(IV)–tin(II) compound

Daniel Schwarte a, Swantje Warf a, Martin Reichelt a, Hans Reuter a,*
Editor: Y Ozawab
PMCID: PMC13330802  PMID: 42403995

The previously unknown 1:3 complex of iso­propyl­stannate(IV) iodide, iPrSnI3, and pyridine N-oxide, PyNO, partially decomposes upon prolonged storage in deutero­chloro­form, forming a novel mixed-valent organic–inorganic tin(IV) and tin(II) compound. Both compounds exhibit an ionic structure and contain an octa­hedral [iPrSnI2(pyNO)3] + ion, in which the three Lewis base mol­ecules are arranged in a facial configuration and the two iodine atoms are in a cis position, whilst charge balancing is ensured in the first compound by an isolated iodide ion and in the second by a tri­iodido­stannate(II) ion, [SnI3]−, which is linked via tetrel bonds to one-dimensional chains.

Keywords: tetrel bonds, mixed-valent, coordination compounds, crystal structure, tin

Abstract

In the search for complexes of the monoorganotin(IV) triiodides, RSnI3, with Lewis bases, LB, a 1:3 complex was was obtained for the first time in the case of iso­propyl­tin(IV) triiodide, iPrSnI3, and LB = pyridine-N-oxide, PyNO. The compound, di­iodido­(isoprop­yl)tris­(pyridine N-oxide)tin(III) iodide, [Sn(C3H7)I2(C5H5NO)3]I, has an ionic structure and consists of a previously unknown [iPrSn(pyNO)3]+ and an isolated I− ion. The novel cation exhibits a facial arrangement of the PyNO mol­ecules and a cis arrangement of the iodine atoms. In CDCl3, over the course of several weeks, this compound gives rise to a new, second compound, also of ionic structure, containing an tri­iodido­stannate(II) ion, [SnI3]−, and a solvent mol­ecule in addition to the already known cation, namely, di­iodido­(isoprop­yl)tris­(pyridine N-oxide)tin(IV) tri­iodido­stannate(II) deutero­chloro­form monosolvate, [Sn(C3H7)I2(C5H5NO)3][SnI3]·CDCl3. The anion exhibits a trigonal–pyramidal structure in order to achieve a stable electron octet at the divalent tin atom but is associated in the crystal via tetrel bonds into one-dimensional chains in which the tin atoms exhibit a 33-aaa coordination mode.

1. Introduction

The excellent coordination behaviour of organotin(IV) halides, R4–nSnHaln with Hal = Cl, Br, I, and n = 1, 2, 3 has been known for over 100 years (Krause & von Grosse, 1937 ▸). Nevertheless, it is surprising how little is still known today about the structures of complexes of monoorganotin(IV) trihalides, RSnHal3, particularly those containing the halogens bromine and iodine. In the case where Hal = I, only three crystal structures are described in the literature, all with R = ethyl and two Lewis base mol­ecules LB: EtSnI3(Ph2SO)2 (Jatsenko et al., 1985 ▸), EtSnI3(Ph3PO)2 (Tursina et al., 1986 ▸) and EtSnI3(HMPTA)2 (Aslanov et al., 1985 ▸). In all three compounds, the tin atoms are coordinated in a distorted octa­hedral arrangement, but with different stereochemistry: the first compound exhibits a mer–cis configuration, the second a mer–trans configuration and the third a fac–cis configuration with respect to the three iodine atoms and the two Lewis base mol­ecules. Thus, these complexes simultaneously represent all three possible arrangements of ligands in octa­hedral complexes of the composition RSnHal3LB2.

Here we report on our search for suitable complexes containing pyridine-N-oxide, PyNO, as a Lewis base. In the case of iso­propyl­tin(IV) triiodide, iPrSnI3, we were able to isolate a compound of composition iPrSnI3·3PyNO, 1, in which, for the first time, three Lewis base mol­ecules are incorporated. Moreover, this compound decomposed partially giving rise to single crystals of a mixed-valent tin(IV)-tin(II) compound of overall composition iPrSnI3·SnI2·3PyNO·CDCl3, 2.

2. Results and discussion

Single crystals of compound 1 were first synthesized on a Petri dish by adding iso­propyl­tin(IV) triiodide to an excess of pyridine-N-oxide using chloro­form as the solvent. As the elemental analysis carried out indicated a significantly higher C and H content than would be expected for a 1:2 complex a single crystal structure X-ray analysis was performed with a needle-like fragment of a larger yellow bloc, confirming the 1:3-composition according to its constitution of [iPrSnIVI2(pyNO)3]I. Based on this stoichiometry, the compound was then synthesized on a micro-scale and fully characterized by 1H and 13C NMR spectroscopy and elemental analysis.

During the spectroscopic characterization process, the NMR tube remained unemptied for several weeks due to bottlenecks in the waste disposal process. Thereafter, several crystals were found on the inner wall, their shape clearly differing from that of the crystals originally placed there. The subsequent X-ray structure analysis revealed the unexpected formation of the ionic organic-inorganic mixed-valent tin(IV)-tin(II) compound 2 with the constitution of [iPrSnIVI2(pyNO)3][SnIII3]·CDCl3.2.

Both compounds are ionic in nature and contain a previously unknown [RSnIVHal2(LB)3]+ ion with R = iPr, Hal = I, and LB = PyNO. In this cation (Fig. 1 ▸), the tin atom has a distorted octa­hedral coordination, with the three PyNO mol­ecules adopting a fac configuration and the iodine atoms being in a cis position relative to one another which results in the organic moiety being in a trans position to one of the three PyNO mol­ecules.

Figure 1.

Figure 1

Different representations of the asymmetric unit of 1 reflecting the main component of the disordered iodine atoms and one position of the disordered isopropyl group: (a) ball-and-stick model with atom and pyridine N-oxide (in circles) numbering. With the exception of the hydrogen atoms, which are shown as spheres of arbitrary radius, all other atoms are drawn as anisotropic displacement ellipsoids at the 60% probability level, (b) ball-and-stick model illustrating the stereochemical descriptors of the cation, and (c) space-filling model visualizing the shape of the cation; colour code and van der Waals radii used: Sn = bronze, 2.17 Å; I = violet, 1.98 Å; C = dark grey, 1.70 Å; H = white, 1.20 Å; O = red, 1.52 Å; N = light blue, 1.55 Å.

Some conformational flexibility of this cation is indicated in the case of the isopropyl group which is statistically disordered over two sets of sites with the same degree of occupancy as well as in a slight disorder (∼97:3) of the iodine atoms in 1, and in some different orientation of the PyNO mol­ecules in 1 and 2. Some characteristic structural features of the cation are summarised in Table 1 ▸. More remarkable, however, are the unusual long tin–carbon distances. In comparable but neutral compounds such as iPrSnCl3(LB)2, the tin–carbon bond lengths are also relatively long [2.169 (5)/2.171 (4) Å (Reuter et al., 1992 ▸), LB = DMF; 2.148 (6)–2.177 (3) Å (Kastner et al., 1999 ▸), LB = DMSO], but significantly shorter than in the present case [2.219 (5) Å, 1; 2.229 (6) Å, 2]. However, it appears that long tin–carbon bond lengths are a characteristic feature of monoorganotin(IV) iodine compounds as comparable or longer values are found in the complexes mer,cis-EtSnI3·2Ph2SO [d(Sn—C) = 2.22 (1) Å; Yatsenko et al., 1985 ▸], fac,cis-EtSnI3·2HMPTA [d(Sn—C) = 2.25 (3); Aslanov et al., 1985 ▸] and mer,trans-EtSnI3·2Ph3PO [d(Sn—C) = 2.25 (1) Å; Tursina et al., 1986 ▸] at room temperature.

Table 1. Selected atom distances and angles (Å, °) in the [iPrSnI2(pyNO)3] + ion of 1 and 2.

  1 2
d(Sn—C) 2.219 (5)a 2.229 (6)
d(Sn—I) 2.7886 (4) 2.8145 (5)
  2.8468 (4) 2.8206 (6)
d(Sn—O)trans 2.132 (3) 2.169 (3)
d(Sn—O)cis 2.181 (3) 2.185 (4)
  2.184 (3) 2.163 (4)
(C—Sn—O)trans 173.3 (1)/155.2 (3) 165.0 (2)°
(I—Sn—O)trans 166.9 (1) 169.4 (1)
  169.2 (1) 161.9 (1)

Note: (a) Refined value for both positions of the disordered isopropyl group.

The Sn—I bond lengths (main component of 1) ranging from 2.7886 (4) to 2.8468 (4) Å are, on average, shorter than those in the neutral RSnI3·2LB complexes mentioned above for which values between 2.821 (1) and 2.949 (3) Å are found at room temperature. Significantly shorter [2.634 (3); 2.715 (2) Å] Sn—I distances are found there only in the case of iodine atoms that are in a trans position relative to the organic moiety. This bond shortening is usually referred to as the trans strengthening (Jatsenko et al., 1985 ▸).

Pyridine N-oxide complexes of monoorganotin(IV) tri­halides have not yet been described in the literature. With regard to the Sn—O bond lengths, there is no consistent pattern in the two cations described here. In compound 1, the Sn—O bond in the trans position relative to the organic moiety is significantly shorter [2.131 (2) Å] than the two Sn—O bonds in the cis positions [2.181 (4), 2.182 (4) Å]. In compound 2, one Sn—O bond in the cis position is of similar [2.184 (4) Å] length to that in compound 1, but the second Sn—O bond in the cis position [2.161 (3) Å] is almost as long as the one in the trans position [2.165 (2) Å], with both being significantly longer than the cis bonds in compound 1.

The structural changes in the pyridine N-oxide mol­ecules resulting from their inter­action with the tin atoms are most pronounced in the N—O bond lengths, which are slightly longer than in the free mol­ecule [1.306 (2) Å, T = 173 K; Shishkin et al. 2013 ▸] whereby the bond elongation is all the more pronounced [1: d(N—O)trans = 1.352 (4) Å, d(N—O)cis = 1.347 (4)/1.249 (4) Å; 2: d(N—O)trans = 1.353 (6), d(N—O)cis = 1.247 (5)/1.352 (6) Å] the stronger the mol­ecule is bound to the tin atom. The associated Sn—O—N bond angles are 120.4 (2)–125.3 (2)° in 1 and 123.1 (3)–127.3 (3)° in 2.

In 1, the isolated iodine anions are arranged in layers perpendicular to the c axis (Fig. 2 ▸). The individual layers are separated by bilayers of cations in which the isopropyl groups face inwards and the pyridine N-oxide mol­ecules face outwards. In this arrangement, the inter­actions between the individual building units are limited to van der Waals contacts.

Figure 2.

Figure 2

Perspective view into the crystal structure of 1 looking down the b axis; cations are drawn as ball-and-stick models, the isolated iodine atoms as spheres of arbitrary radii, colours as shown in the previous illustration.

The three building units in the asymmetric unit of 2 are shown in Fig. 3 ▸a. Unlike in 1, there is no disorder in the cation. The [SnI3]− ion (Fig. 3 ▸b) has a pyramidal shape with three iodine atoms at the base and the tin atom at the apex. In this species, the tin atom achieves a stable octet of electrons via its spherical, non-bonding 5s electron pair and the six electrons in the 2e–2c bonds with the iodine atoms, in which its three orthogonal 5p orbitals are involved. Accordingly, the bond angles between the iodine atoms vary between 91.64 (2) and 94.53 (1)°. What is striking, however, are the varying tin–iodine distances, which range from 2.9196 (6) to 3.0481 (5) Å.

Figure 3.

Figure 3

(left) Ball-and-stick model of the asymmetric unit of 2 with numbering of selected atoms and numbers of the pyridine-N-oxide ligands, numbering of all other atoms according to the numbering scheme of 1, (right) ball-and-stick model of the trigonal–pyramidal [SnI3]− ion with atom numbering and bond lengths (Å) and bond angles (°), all atoms are drawn as thermal displacement ellipsoids at the 60% probability level.

The existence of the [SnIII3]− ion naturally raises the question of how it is formed. In most cases of incidentally discovered mixed-valent tin(II)–tin(IV) compounds, their formation is based on the partial oxidation of a tin(II) species to tetra­valent tin. In the present case, however, it is evidently a matter of the partial reduction of a tin(IV) species to divalent tin. It remains unclear to what extent the cleavage of the tin–carbon bond or the oxidation of iodide ions to elemental iodine play a role in this process, or whether both reactions are involved, as neither their reaction products nor a violet colour in the reaction solution were observed.

A look inside the crystal structure of 2 (Fig. 4 ▸) reveals that the cations are arranged in a similar way to those in the parent compound 1, namely through the inter­action of their isopropyl groups. The [SnI3]− ions (Fig. 5 ▸) are arranged in rows along the b-axis direction related to each other via the twofold screw axis giving rise to some additional, long-range Sn⋯I distances, expanding the original coordination numbers of the tin atoms from three, trigonal-pyramidal, to six in a distorted octa­hedral fashion. Even though long [3.3802 (5)–3.8473 (6) Å], the resulting tin–iodine distances are shorter than the sum (4.15 Å) of the van der Waals radii (Mantina et al., 2009 ▸) of tin (2.17 Å) and iodine (1.98 Å), leading to a considerable inter-penetration of their van der Waals spheres qu­anti­fied by high inter-penetration indices p (Echeverría & Alvarez, 2023 ▸).

Figure 4.

Figure 4

Perspective view into the crystal structure of 2 looking down the b axis, all components are drawn as ball-and-stick model using the previous colour code with the addition for Cl = green.

Figure 5.

Figure 5

Different representations of the tetrel bonds linking the [SnI3]− ion into linear chains in direction of the twofold rotation axis. (above) side-view on a chain as polyhedron model with resulting octa­hedra (left) and constituting trigonal-pyramids (right), all atoms are drawn as thermal displacement ellipsoids at the 60% probability level and the tetrel bonds as dashed sticks, (below, left) geometric parameters [Å,°] characterizing the tetrel bonds with asymmetry parameters Q (grey), and (below, right) space-filling model visualizing the inter-penetration of the van der Waals radii of tin and iodine as result of the tetrel bond formation, inter-penetration indices p (grey), colour code and van der Waals radii as previously.

Such additional weak inter­actions are typical of many tin(II) compounds and are always found on the opposite side to the strong, regular bonds via which the tin(II) atom achieves the electron octet. They belong to the tetrel bonds (Bauzá et al. 2019 ▸; Brammer et al. 2023 ▸) or more specifically to the stannic bonds (Reuter, 2025 ▸) and are usually explained by 3c–4e bonds between the empty orthogonal 5p orbitals of the tin(II) atom and the double-occupied p-orbitals of two trans-configurated electron-donor atoms X. Only rarely are the two donor atoms equidistant from the central tin atom and is the 3c–4e bond symmetric (s); an example of this can be found in one of the two tin atoms in tin diiodide, SnI2 (Howie et al. 1972 ▸). Much more frequently, the two donor atoms are at different distances from the tin atom, as shown here, making the 3c–4e bond asymmetrical (a). Qu­anti­tatively, the degree of asymmetry in such a trans-figured X—Sn⋯Y arrangement can be determined by the quotient Q = d(Sn⋯Y)long/d(Sn—X)short (Schröder et al., 2024 ▸). In the present case these values are 1.11, 1.21, and 1.32, indicating a strong asymmetry. Based on these observations, the extended coordination of the tin(II) atoms of the [SnI3]− ions should be described as 33-aaa coordination mode (Schröder et al., 2024 ▸), which is more precise than the term ‘distorted octa­hedral’.

3. Experimental

3.1. Synthesis and crystallization

iPrSnI3: under stirring, a solution of 6.75 g (25 mmol) of iso­propyl­tin(IV) trichloride, iPrSnCl3, in acetone (50 ml) was added to a solution of 11.25 g (75 mmol) of sodium iodide in acetone (120 ml). After stirring for 1 h, the solid formed was filtered off and the solution was evaporated down in a rotary evaporator. The remaining residue was distilled by fractional distillation (b.p.: 367–368 K/20 mbar, light yellow, oily liquid), yield: 8.71 g (16.1 mmol, 64%).

1H NMR (250 MHz, CDCl3): δ, nJ(119/117Sn—1H) (ppm, Hz) 1.21, 216.7/207.4 (d, –CH–, 1H); 2.70 (sep, –CH3, 6H); 13C NMR (250 MHz, CDCl3): δ, nJ(119/117Sn—13C) (ppm, Hz) 20.18, 387.3/370.2 (–CH3), 37.65, 500.3/478.0 (–CH–); analysis: calculated for C3H7I3Sn (542.51): C 6.64, H 1.30; found: C 6.69, H 1.35%.

iPrSnI3·3PyNO, 1: in a beaker, 0.54 g (1 mmol) of iso­propyl­tin(IV) triiodide, iPrSnI3, and 0.28 g (3 mmol) of pyridine N-oxide (Sigma-Aldrich) were dissolved in 20 ml of chloro­form. Upon slow evaporation of the solvent in air, the complex crystallized as yellow, translucent crystals, which were dried between two filter papers, yield: 0.47 g (0.57 mmol, 85%).

1H NMR (250 MHz, CDCl3): δ, nJ(119/117Sn—1H) (ppm, Hz) 1.21, 281.1/267.9 (d, CH, 1H); 2.70 (septet, CH3, 6H) 7.49–7.63 (multiplet, meta-, para-HpyNO, 9H), 8.52 (d, ortho-HpyNO, 6H); 13C NMR (250 MHz, CDCl3): δ, nJ(119/117Sn—13C) (ppm, Hz) 21.54, 46.2 (–CH3), 48.79 (–CH–), 126.39 (meta-CpyNO), 130.91 para-CpyNO), 140.66 (ortho-CpyNO); analysis: calculated for C18H22I3N3O3Sn2 (827.77): C 26.12, H 2.68, N 5.08; found: C 26.43, H 2.72, N 5.13%.

Single crystals of [iPrSnIVI2(pyNO)3][SnIII3] · CDCl3, 2, were obtained after the NMR tube had been left standing for some time.

3.2. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2 ▸. Hydrogen atoms were refined with calculated positions (–CH– = 1.00 Å, –CH3 = 0.98 Å, –CHpyNO = 0.95 Å, AFIX) and isotropic displacement parameters Uiso(H) = P × Ueq(C) with P = 1.2 for all hydrogen atoms without those of the methyl groups (P = 1.5).

Table 2. Experimental details.

  1 2
Crystal data
Chemical formula [Sn(C3H7)I2(C5H5NO)3]I [Sn(C3H7)I2(C5H5NO)3][SnI3]·CHCl3
M r 827.77 1319.63
Crystal system, space group Triclinic, PInline graphic Monoclinic, C2/c
Temperature (K) 100 200
a, b, c (Å) 8.5224 (3), 9.2972 (4), 16.9400 (8) 40.7321 (18), 8.5279 (4), 20.3457 (9)
α, β, γ (°) 81.649 (1), 75.958 (2), 71.025 (1) 90, 102.553 (2), 90
V (Å3) 1228.14 (9) 6898.3 (5)
Z 2 8
Radiation type Mo Kα Mo Kα
μ (mm−1) 4.83 6.18
Crystal size (mm) 0.33 × 0.18 × 0.12 0.28 × 0.19 × 0.11
 
Data collection
Diffractometer Bruker APEXII CCD Bruker APEXII CCD
Absorption correction Multi-scan (SADABS; Krause et al., 2015 ▸) Multi-scan (SADABS; Krause et al., 2015 ▸)
Tmin, Tmax 0.455, 0.693 0.453, 0.712
No. of measured, independent and observed [I > 2σ(I)] reflections 94618, 5925, 5243 146956, 8327, 6129
R int 0.088 0.091
(sin θ/λ)max (Å−1) 0.661 0.661
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.029, 0.069, 1.05 0.032, 0.078, 1.11
No. of reflections 5925 8327
No. of parameters 271 319
No. of restraints 8 0
H-atom treatment H-atom parameters constrained H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 1.43, −1.62 0.94, −1.51

Computer programs: APEX2 and SAINT (Bruker, 2009 ▸), SHELXS97 (Sheldrick 2008 ▸), SHELXL2014/7 (Sheldrick, 2015 ▸), DIAMOND (Brandenburg, 2006 ▸), Mercury (Macrae et al. (2020 ▸) and publCIF(Westrip, 2010 ▸).

Disorder of the isopropyl group in the crystal structure of 1 has been modeled via tin–carbon and carbon–carbon constrains (DFIX) and common anisotropic temperature factors while occupation factors were fixed to 0.5. In the case of the disordered iodine atoms in the cation of 1, the occupancy factors (0.967/0.033 for I1, 0.969/0.031 for I2) and positions were freely refined with the anisotropic displacement parameters of the main components.

Supplementary Material

Crystal structure: contains datablock(s) 1, 2. DOI: 10.1107/S2056989026006596/ox2024sup1.cif

e-82-00888-sup1.cif (7.1MB, cif)

Structure factors: contains datablock(s) 1. DOI: 10.1107/S2056989026006596/ox20241sup2.hkl

e-82-00888-1sup2.hkl (471.1KB, hkl)

Structure factors: contains datablock(s) 2. DOI: 10.1107/S2056989026006596/ox20242sup3.hkl

e-82-00888-2sup3.hkl (661.5KB, hkl)

CCDC references: 2564137, 2564136

Additional supporting information: crystallographic information; 3D view; checkCIF report

Acknowledgments

The Deutsche Forschungsgemeinschaft and the Government of Lower-Saxony are thanked for the funding of the diffractometer.

supplementary crystallographic information

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) iodide (1) . Crystal data

[Sn(C3H7)I2(C5H5NO)3]I Z = 2
Mr = 827.77 F(000) = 768
Triclinic, P1 Dx = 2.238 Mg m−3
a = 8.5224 (3) Å Mo Kα radiation, λ = 0.71073 Å
b = 9.2972 (4) Å Cell parameters from 9764 reflections
c = 16.9400 (8) Å θ = 2.3–28.6°
α = 81.649 (1)° µ = 4.83 mm−1
β = 75.958 (2)° T = 100 K
γ = 71.025 (1)° Needle, yellow
V = 1228.14 (9) Å3 0.33 × 0.18 × 0.12 mm

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) iodide (1) . Data collection

Bruker APEXII CCD diffractometer 5243 reflections with I > 2σ(I)
φ and ω scans Rint = 0.088
Absorption correction: multi-scan (SADABS; Krause et al., 2015) θmax = 28.0°, θmin = 2.9°
Tmin = 0.455, Tmax = 0.693 h = −11→11
94618 measured reflections k = −12→12
5925 independent reflections l = −22→22

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) iodide (1) . Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.029 w = 1/[σ2(Fo2) + (0.0184P)2 + 4.7037P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.069 (Δ/σ)max = 0.001
S = 1.05 Δρmax = 1.43 e Å−3
5925 reflections Δρmin = −1.62 e Å−3
271 parameters Extinction correction: SHELXL-2014/7 (Sheldrick, 2015), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
8 restraints Extinction coefficient: 0.00180 (15)
Primary atom site location: structure-invariant direct methods

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) iodide (1) . Special details

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.

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) iodide (1) . Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq Occ. (<1)
Sn1 0.33877 (3) 0.84757 (3) 0.82740 (2) 0.01992 (8)
C1 0.2579 (10) 0.9256 (8) 0.9528 (3) 0.0245 (13) 0.5
H1 0.1578 0.8907 0.9811 0.029* 0.5
C2 0.204 (3) 1.0955 (9) 0.9528 (13) 0.0331 (11) 0.5
H2A 0.3037 1.1317 0.9330 0.050* 0.5
H2B 0.1502 1.1258 1.0084 0.050* 0.5
H2C 0.1233 1.1405 0.9170 0.050* 0.5
C3 0.3958 (11) 0.8534 (13) 0.9993 (6) 0.0331 (11) 0.5
H3A 0.4120 0.7435 1.0086 0.050* 0.5
H3B 0.3643 0.8984 1.0519 0.050* 0.5
H3C 0.5016 0.8710 0.9680 0.050* 0.5
C4 0.3282 (11) 0.9541 (8) 0.9383 (4) 0.0245 (13) 0.5
H4 0.4350 0.9837 0.9253 0.029* 0.5
C5 0.191 (3) 1.1036 (11) 0.9448 (13) 0.0331 (11) 0.5
H5A 0.1941 1.1545 0.9909 0.050* 0.5
H5B 0.0804 1.0861 0.9535 0.050* 0.5
H5C 0.2083 1.1681 0.8944 0.050* 0.5
C6 0.3467 (13) 0.8439 (12) 1.0116 (5) 0.0331 (11) 0.5
H6A 0.4542 0.7622 0.9997 0.050* 0.5
H6B 0.2523 0.8002 1.0256 0.050* 0.5
H6C 0.3456 0.8972 1.0577 0.050* 0.5
I1A 0.00404 (4) 0.91616 (4) 0.81085 (2) 0.03333 (11) 0.9842 (9)
I1B 0.0218 (12) 0.820 (3) 0.8293 (12) 0.03333 (11) 0.0158 (9)
I2A 0.36423 (10) 0.53886 (4) 0.88418 (5) 0.03183 (15) 0.969 (3)
I2B 0.417 (3) 0.5249 (4) 0.8557 (14) 0.03183 (15) 0.031 (3)
O1 0.4447 (3) 0.7754 (3) 0.70685 (16) 0.0227 (6)
N1 0.3663 (4) 0.7237 (4) 0.66165 (19) 0.0191 (6)
C11 0.2460 (5) 0.8233 (4) 0.6254 (2) 0.0223 (8)
H11 0.2143 0.9294 0.6319 0.027*
C12 0.1693 (5) 0.7683 (5) 0.5784 (2) 0.0269 (9)
H12 0.0802 0.8363 0.5546 0.032*
C13 0.2217 (6) 0.6150 (5) 0.5661 (2) 0.0286 (9)
H13 0.1716 0.5773 0.5325 0.034*
C14 0.3489 (6) 0.5164 (5) 0.6034 (3) 0.0304 (9)
H14 0.3869 0.4105 0.5954 0.037*
C15 0.4186 (5) 0.5730 (4) 0.6516 (3) 0.0260 (8)
H15 0.5042 0.5062 0.6781 0.031*
O2 0.6099 (4) 0.8154 (3) 0.81148 (18) 0.0262 (6)
N2 0.7301 (4) 0.6804 (4) 0.7976 (2) 0.0242 (7)
C21 0.7980 (5) 0.6384 (5) 0.7211 (3) 0.0274 (9)
H21 0.7603 0.7032 0.6763 0.033*
C22 0.9229 (5) 0.5007 (5) 0.7080 (3) 0.0333 (10)
H22 0.9700 0.4691 0.6541 0.040*
C23 0.9797 (6) 0.4079 (5) 0.7741 (3) 0.0378 (11)
H23 1.0656 0.3128 0.7659 0.045*
C24 0.9097 (6) 0.4562 (5) 0.8511 (3) 0.0405 (11)
H24 0.9486 0.3953 0.8967 0.049*
C25 0.7832 (6) 0.5928 (5) 0.8624 (3) 0.0344 (10)
H25 0.7333 0.6255 0.9159 0.041*
O3 0.3312 (3) 1.0686 (3) 0.76145 (18) 0.0264 (6)
N3 0.4763 (4) 1.1026 (3) 0.72691 (19) 0.0201 (6)
C31 0.5590 (6) 1.0604 (5) 0.6523 (2) 0.0262 (8)
H31 0.5170 1.0054 0.6236 0.031*
C32 0.7064 (6) 1.0974 (5) 0.6174 (3) 0.0322 (10)
H32 0.7669 1.0660 0.5647 0.039*
C33 0.7661 (5) 1.1788 (5) 0.6581 (3) 0.0324 (10)
H33 0.8675 1.2043 0.6343 0.039*
C34 0.6742 (6) 1.2232 (5) 0.7351 (3) 0.0308 (9)
H34 0.7116 1.2809 0.7645 0.037*
C35 0.5307 (6) 1.1836 (5) 0.7680 (3) 0.0274 (9)
H35 0.4682 1.2135 0.8207 0.033*
I3 0.78826 (3) 0.77318 (3) 0.48262 (2) 0.02366 (8)

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) iodide (1) . Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Sn1 0.02376 (14) 0.01856 (13) 0.01909 (14) −0.00794 (10) −0.00818 (10) 0.00338 (10)
C1 0.028 (4) 0.024 (3) 0.025 (3) −0.013 (3) −0.005 (3) −0.002 (2)
C2 0.038 (3) 0.0302 (18) 0.021 (2) −0.0030 (18) 0.0023 (18) −0.0029 (15)
C3 0.038 (3) 0.0302 (18) 0.021 (2) −0.0030 (18) 0.0023 (18) −0.0029 (15)
C4 0.028 (4) 0.024 (3) 0.025 (3) −0.013 (3) −0.005 (3) −0.002 (2)
C5 0.038 (3) 0.0302 (18) 0.021 (2) −0.0030 (18) 0.0023 (18) −0.0029 (15)
C6 0.038 (3) 0.0302 (18) 0.021 (2) −0.0030 (18) 0.0023 (18) −0.0029 (15)
I1A 0.02310 (15) 0.0481 (2) 0.02945 (16) −0.01426 (13) −0.00183 (11) −0.00302 (14)
I1B 0.02310 (15) 0.0481 (2) 0.02945 (16) −0.01426 (13) −0.00183 (11) −0.00302 (14)
I2A 0.0489 (3) 0.01971 (14) 0.0267 (3) −0.01293 (14) −0.0071 (3) 0.00379 (13)
I2B 0.0489 (3) 0.01971 (14) 0.0267 (3) −0.01293 (14) −0.0071 (3) 0.00379 (13)
O1 0.0243 (14) 0.0293 (14) 0.0202 (13) −0.0146 (11) −0.0071 (11) −0.0001 (11)
N1 0.0203 (15) 0.0198 (15) 0.0188 (15) −0.0087 (12) −0.0050 (12) 0.0006 (12)
C11 0.027 (2) 0.0180 (18) 0.0206 (19) −0.0080 (15) −0.0042 (15) 0.0038 (14)
C12 0.028 (2) 0.031 (2) 0.023 (2) −0.0113 (17) −0.0086 (16) 0.0071 (16)
C13 0.037 (2) 0.036 (2) 0.020 (2) −0.0212 (19) −0.0068 (17) −0.0008 (17)
C14 0.039 (2) 0.022 (2) 0.032 (2) −0.0105 (18) −0.0077 (19) −0.0044 (17)
C15 0.027 (2) 0.0201 (19) 0.028 (2) −0.0023 (16) −0.0093 (17) 0.0002 (16)
O2 0.0270 (14) 0.0179 (13) 0.0367 (16) −0.0065 (11) −0.0143 (12) 0.0005 (11)
N2 0.0225 (16) 0.0177 (15) 0.0359 (19) −0.0063 (13) −0.0145 (14) 0.0019 (14)
C21 0.0217 (19) 0.028 (2) 0.035 (2) −0.0123 (16) −0.0064 (17) 0.0020 (17)
C22 0.023 (2) 0.033 (2) 0.047 (3) −0.0152 (18) −0.0028 (19) −0.007 (2)
C23 0.023 (2) 0.021 (2) 0.068 (3) −0.0055 (17) −0.011 (2) 0.000 (2)
C24 0.039 (3) 0.030 (2) 0.052 (3) −0.005 (2) −0.023 (2) 0.011 (2)
C25 0.038 (2) 0.028 (2) 0.038 (3) −0.0046 (19) −0.018 (2) 0.0033 (19)
O3 0.0206 (13) 0.0195 (13) 0.0354 (16) −0.0069 (11) −0.0037 (12) 0.0081 (12)
N3 0.0195 (15) 0.0138 (14) 0.0238 (16) −0.0038 (12) −0.0030 (13) 0.0030 (12)
C31 0.037 (2) 0.024 (2) 0.0208 (19) −0.0147 (17) −0.0071 (17) 0.0021 (15)
C32 0.038 (2) 0.024 (2) 0.028 (2) −0.0114 (18) 0.0057 (18) 0.0004 (17)
C33 0.024 (2) 0.024 (2) 0.044 (3) −0.0093 (17) 0.0008 (19) 0.0056 (18)
C34 0.032 (2) 0.029 (2) 0.037 (2) −0.0161 (18) −0.0102 (19) 0.0009 (18)
C35 0.035 (2) 0.024 (2) 0.025 (2) −0.0127 (17) −0.0036 (17) −0.0012 (16)
I3 0.02654 (14) 0.01875 (13) 0.02718 (14) −0.00621 (10) −0.00905 (10) −0.00196 (10)

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) iodide (1) . Geometric parameters (Å, º)

Sn1—O1 2.132 (3) C11—H11 0.9500
Sn1—O3 2.181 (3) C12—C13 1.379 (6)
Sn1—O2 2.184 (3) C12—H12 0.9500
Sn1—C4 2.219 (5) C13—C14 1.390 (6)
Sn1—C1 2.219 (5) C13—H13 0.9500
Sn1—I1B 2.7883 (10) C14—C15 1.364 (6)
Sn1—I1A 2.7886 (4) C14—H14 0.9500
Sn1—I2A 2.8468 (4) C15—H15 0.9500
Sn1—I2B 2.8476 (10) O2—N2 1.347 (4)
C1—C3 1.495 (5) N2—C21 1.342 (6)
C1—C2 1.496 (5) N2—C25 1.348 (5)
C1—H1 1.0000 C21—C22 1.380 (6)
C2—H2A 0.9800 C21—H21 0.9500
C2—H2B 0.9800 C22—C23 1.394 (7)
C2—H2C 0.9800 C22—H22 0.9500
C3—H3A 0.9800 C23—C24 1.371 (7)
C3—H3B 0.9800 C23—H23 0.9500
C3—H3C 0.9800 C24—C25 1.376 (6)
C4—C6 1.495 (5) C24—H24 0.9500
C4—C5 1.495 (5) C25—H25 0.9500
C4—H4 1.0000 O3—N3 1.349 (4)
C5—H5A 0.9800 N3—C31 1.334 (5)
C5—H5B 0.9800 N3—C35 1.343 (5)
C5—H5C 0.9800 C31—C32 1.381 (6)
C6—H6A 0.9800 C31—H31 0.9500
C6—H6B 0.9800 C32—C33 1.371 (7)
C6—H6C 0.9800 C32—H32 0.9500
I1A—I1B 0.88 (2) C33—C34 1.392 (6)
I2A—I2B 0.57 (3) C33—H33 0.9500
O1—N1 1.352 (4) C34—C35 1.358 (6)
N1—C11 1.345 (5) C34—H34 0.9500
N1—C15 1.348 (5) C35—H35 0.9500
C11—C12 1.381 (6)
O1—Sn1—O3 80.74 (11) C4—C6—H6B 109.5
O1—Sn1—O2 75.61 (11) H6A—C6—H6B 109.5
O3—Sn1—O2 84.77 (10) C4—C6—H6C 109.5
O1—Sn1—C4 155.2 (2) H6A—C6—H6C 109.5
O3—Sn1—C4 87.0 (2) H6B—C6—H6C 109.5
O2—Sn1—C4 81.9 (2) I1B—I1A—Sn1 80.9 (3)
O1—Sn1—C1 173.3 (2) I1A—I1B—Sn1 80.9 (3)
O3—Sn1—C1 97.6 (2) I2B—I2A—Sn1 84.3 (3)
O2—Sn1—C1 97.8 (2) I2A—I2B—Sn1 84.2 (3)
O1—Sn1—I1B 93.8 (4) N1—O1—Sn1 125.3 (2)
O3—Sn1—I1B 103.4 (5) C11—N1—C15 122.4 (3)
O2—Sn1—I1B 165.6 (5) C11—N1—O1 119.7 (3)
C4—Sn1—I1B 110.0 (5) C15—N1—O1 117.9 (3)
C1—Sn1—I1B 92.9 (4) N1—C11—C12 118.7 (4)
O1—Sn1—I1A 94.17 (7) N1—C11—H11 120.6
O3—Sn1—I1A 85.50 (7) C12—C11—H11 120.6
O2—Sn1—I1A 166.89 (8) C13—C12—C11 120.3 (4)
C4—Sn1—I1A 106.3 (2) C13—C12—H12 119.9
C1—Sn1—I1A 92.2 (2) C11—C12—H12 119.9
I1B—Sn1—I1A 18.2 (5) C12—C13—C14 119.1 (4)
O1—Sn1—I2A 88.79 (8) C12—C13—H13 120.4
O3—Sn1—I2A 169.37 (8) C14—C13—H13 120.4
O2—Sn1—I2A 94.43 (7) C15—C14—C13 119.4 (4)
C4—Sn1—I2A 103.4 (2) C15—C14—H14 120.3
C1—Sn1—I2A 93.0 (2) C13—C14—H14 120.3
I1B—Sn1—I2A 75.3 (5) N1—C15—C14 120.1 (4)
I1A—Sn1—I2A 93.510 (16) N1—C15—H15 120.0
O1—Sn1—I2B 78.3 (5) C14—C15—H15 120.0
O3—Sn1—I2B 158.8 (5) N2—O2—Sn1 123.5 (2)
O2—Sn1—I2B 87.1 (4) C21—N2—O2 120.4 (3)
C4—Sn1—I2B 111.2 (4) C21—N2—C25 121.8 (4)
C1—Sn1—I2B 102.8 (5) O2—N2—C25 117.8 (4)
I1B—Sn1—I2B 81.1 (6) N2—C21—C22 119.6 (4)
I1A—Sn1—I2B 99.0 (3) N2—C21—H21 120.2
I2A—Sn1—I2B 11.5 (5) C22—C21—H21 120.2
C3—C1—C2 111.0 (10) C21—C22—C23 119.7 (5)
C3—C1—Sn1 110.4 (5) C21—C22—H22 120.1
C2—C1—Sn1 112.2 (9) C23—C22—H22 120.1
C3—C1—H1 107.7 C24—C23—C22 118.9 (4)
C2—C1—H1 107.7 C24—C23—H23 120.5
Sn1—C1—H1 107.7 C22—C23—H23 120.5
C1—C2—H2A 109.5 C23—C24—C25 120.0 (4)
C1—C2—H2B 109.5 C23—C24—H24 120.0
H2A—C2—H2B 109.5 C25—C24—H24 120.0
C1—C2—H2C 109.5 N2—C25—C24 119.9 (5)
H2A—C2—H2C 109.5 N2—C25—H25 120.0
H2B—C2—H2C 109.5 C24—C25—H25 120.0
C1—C3—H3A 109.5 N3—O3—Sn1 120.4 (2)
C1—C3—H3B 109.5 C31—N3—C35 121.5 (3)
H3A—C3—H3B 109.5 C31—N3—O3 119.9 (3)
C1—C3—H3C 109.5 C35—N3—O3 118.5 (3)
H3A—C3—H3C 109.5 N3—C31—C32 119.3 (4)
H3B—C3—H3C 109.5 N3—C31—H31 120.4
C6—C4—C5 120.2 (11) C32—C31—H31 120.4
C6—C4—Sn1 113.6 (6) C33—C32—C31 120.6 (4)
C5—C4—Sn1 109.9 (8) C33—C32—H32 119.7
C6—C4—H4 103.7 C31—C32—H32 119.7
C5—C4—H4 103.7 C32—C33—C34 118.2 (4)
Sn1—C4—H4 103.7 C32—C33—H33 120.9
C4—C5—H5A 109.5 C34—C33—H33 120.9
C4—C5—H5B 109.5 C35—C34—C33 119.6 (4)
H5A—C5—H5B 109.5 C35—C34—H34 120.2
C4—C5—H5C 109.5 C33—C34—H34 120.2
H5A—C5—H5C 109.5 N3—C35—C34 120.7 (4)
H5B—C5—H5C 109.5 N3—C35—H35 119.7
C4—C6—H6A 109.5 C34—C35—H35 119.7

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) triiodidostannate(II) deuterochloroform monosolvate (2) . Crystal data

[Sn(C3H7)I2(C5H5NO)3][SnI3]·CHCl3 F(000) = 4784
Mr = 1319.63 Dx = 2.541 Mg m−3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
a = 40.7321 (18) Å Cell parameters from 9880 reflections
b = 8.5279 (4) Å θ = 2.6–26.1°
c = 20.3457 (9) Å µ = 6.18 mm−1
β = 102.553 (2)° T = 200 K
V = 6898.3 (5) Å3 Plate, yellow
Z = 8 0.28 × 0.19 × 0.11 mm

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) triiodidostannate(II) deuterochloroform monosolvate (2) . Data collection

Bruker APEXII CCD diffractometer 6129 reflections with I > 2σ(I)
φ and ω scans Rint = 0.091
Absorption correction: multi-scan (SADABS; Krause et al., 2015) θmax = 28.0°, θmin = 2.4°
Tmin = 0.453, Tmax = 0.712 h = −53→53
146956 measured reflections k = −11→11
8327 independent reflections l = −26→26

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) triiodidostannate(II) deuterochloroform monosolvate (2) . Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.032 w = 1/[σ2(Fo2) + (0.0189P)2 + 43.8049P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.078 (Δ/σ)max = 0.001
S = 1.11 Δρmax = 0.94 e Å−3
8327 reflections Δρmin = −1.51 e Å−3
319 parameters Extinction correction: SHELXL-2014/7 (Sheldrick 2015), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraints Extinction coefficient: 0.000136 (8)
Primary atom site location: structure-invariant direct methods

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) triiodidostannate(II) deuterochloroform monosolvate (2) . Special details

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.

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) triiodidostannate(II) deuterochloroform monosolvate (2) . Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
Sn1 0.07997 (2) 0.30880 (5) 0.45557 (2) 0.04285 (11)
C1 0.02477 (16) 0.3347 (12) 0.4161 (3) 0.077 (2)
H1 0.0205 0.4497 0.4186 0.093*
C2 0.0146 (2) 0.2971 (14) 0.3464 (4) 0.112 (4)
H2A 0.0195 0.1865 0.3395 0.134*
H2B 0.0268 0.3632 0.3204 0.134*
H2C −0.0097 0.3157 0.3312 0.134*
C3 0.00585 (17) 0.2631 (15) 0.4621 (4) 0.118 (4)
H3A −0.0180 0.2567 0.4398 0.176*
H3B 0.0084 0.3274 0.5028 0.176*
H3C 0.0146 0.1575 0.4743 0.176*
I12 0.10079 (2) 0.26591 (7) 0.33365 (2) 0.06953 (15)
I11 0.08419 (2) −0.00522 (5) 0.50013 (2) 0.05628 (12)
O1 0.13196 (8) 0.3397 (4) 0.50774 (17) 0.0403 (8)
N1 0.15855 (10) 0.2490 (6) 0.5026 (2) 0.0396 (10)
C11 0.17589 (13) 0.2835 (8) 0.4550 (3) 0.0486 (14)
H11 0.1688 0.3668 0.4241 0.058*
C12 0.20410 (14) 0.1962 (8) 0.4517 (3) 0.0579 (17)
H12 0.2159 0.2158 0.4172 0.069*
C13 0.21485 (13) 0.0818 (8) 0.4982 (3) 0.0545 (16)
H13 0.2345 0.0229 0.4967 0.065*
C14 0.19708 (13) 0.0516 (8) 0.5478 (3) 0.0493 (14)
H14 0.2043 −0.0278 0.5805 0.059*
C15 0.16877 (12) 0.1388 (7) 0.5486 (2) 0.0423 (13)
H15 0.1564 0.1201 0.5824 0.051*
O2 0.08545 (9) 0.5609 (5) 0.45361 (19) 0.0492 (10)
N2 0.10945 (12) 0.6393 (6) 0.4303 (2) 0.0472 (12)
C21 0.10139 (18) 0.7087 (9) 0.3698 (3) 0.0632 (19)
H21 0.0794 0.6961 0.3426 0.076*
C22 0.1243 (2) 0.7966 (9) 0.3471 (3) 0.077 (2)
H22 0.1183 0.8448 0.3041 0.092*
C23 0.1561 (2) 0.8166 (9) 0.3859 (4) 0.074 (2)
H23 0.1723 0.8772 0.3700 0.089*
C24 0.16394 (17) 0.7461 (8) 0.4488 (3) 0.0599 (17)
H24 0.1858 0.7577 0.4767 0.072*
C25 0.13996 (14) 0.6597 (7) 0.4702 (3) 0.0486 (14)
H25 0.1450 0.6138 0.5138 0.058*
O3 0.07154 (8) 0.3721 (5) 0.55466 (17) 0.0473 (10)
N3 0.09476 (10) 0.4454 (6) 0.6019 (2) 0.0392 (10)
C31 0.11610 (12) 0.3596 (8) 0.6463 (2) 0.0434 (13)
H31 0.1153 0.2485 0.6436 0.052*
C32 0.13918 (13) 0.4318 (8) 0.6960 (3) 0.0496 (15)
H32 0.1544 0.3707 0.7280 0.060*
C33 0.14039 (14) 0.5927 (8) 0.6997 (3) 0.0517 (15)
H33 0.1565 0.6440 0.7337 0.062*
C34 0.11792 (15) 0.6778 (8) 0.6534 (3) 0.0496 (14)
H34 0.1184 0.7891 0.6552 0.060*
C35 0.09471 (14) 0.6026 (8) 0.6043 (3) 0.0473 (14)
H35 0.0789 0.6612 0.5725 0.057*
Sn2 0.24796 (2) 0.79515 (5) 0.25634 (2) 0.04113 (10)
I21 0.21911 (2) 0.55232 (5) 0.33816 (2) 0.04399 (10)
I22 0.18709 (2) 1.00095 (5) 0.23342 (2) 0.04525 (10)
I23 0.27972 (2) 0.97219 (6) 0.37615 (2) 0.05848 (13)
C4 0.03371 (16) 0.1989 (9) 0.6593 (4) 0.0677 (19)
H4 0.0430 0.2117 0.6180 0.081*
Cl1 −0.00929 (5) 0.1675 (3) 0.63373 (14) 0.1039 (8)
Cl2 0.04250 (5) 0.3705 (3) 0.70730 (10) 0.0815 (6)
Cl3 0.05415 (5) 0.0359 (3) 0.70536 (12) 0.0887 (6)

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) triiodidostannate(II) deuterochloroform monosolvate (2) . Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Sn1 0.02725 (17) 0.0714 (3) 0.02831 (18) 0.00606 (17) 0.00268 (13) −0.00730 (17)
C1 0.040 (3) 0.129 (7) 0.055 (4) 0.005 (4) −0.007 (3) −0.014 (4)
C2 0.062 (5) 0.165 (10) 0.092 (6) −0.008 (6) −0.017 (5) 0.028 (7)
C3 0.026 (3) 0.233 (13) 0.089 (6) 0.009 (5) 0.000 (4) −0.018 (7)
I12 0.0773 (3) 0.1009 (4) 0.0335 (2) 0.0170 (3) 0.0188 (2) −0.0052 (2)
I11 0.0451 (2) 0.0678 (3) 0.0562 (2) −0.00668 (19) 0.01153 (18) −0.0076 (2)
O1 0.0242 (17) 0.057 (2) 0.0388 (19) 0.0067 (16) 0.0060 (14) −0.0019 (17)
N1 0.023 (2) 0.061 (3) 0.034 (2) 0.0021 (19) 0.0050 (17) 0.002 (2)
C11 0.037 (3) 0.071 (4) 0.041 (3) 0.005 (3) 0.016 (2) 0.010 (3)
C12 0.034 (3) 0.088 (5) 0.057 (4) 0.009 (3) 0.022 (3) 0.017 (3)
C13 0.028 (3) 0.081 (5) 0.056 (4) 0.014 (3) 0.013 (3) 0.008 (3)
C14 0.031 (3) 0.073 (4) 0.041 (3) 0.007 (3) 0.002 (2) 0.008 (3)
C15 0.025 (2) 0.072 (4) 0.030 (3) −0.001 (2) 0.004 (2) 0.005 (3)
O2 0.036 (2) 0.070 (3) 0.043 (2) 0.0123 (19) 0.0114 (17) −0.001 (2)
N2 0.051 (3) 0.062 (3) 0.031 (2) 0.017 (2) 0.012 (2) 0.006 (2)
C21 0.074 (4) 0.083 (5) 0.032 (3) 0.029 (4) 0.009 (3) 0.006 (3)
C22 0.116 (7) 0.082 (5) 0.040 (4) 0.029 (5) 0.034 (4) 0.019 (4)
C23 0.084 (5) 0.080 (5) 0.072 (5) 0.016 (4) 0.050 (4) 0.008 (4)
C24 0.057 (4) 0.065 (4) 0.063 (4) 0.010 (3) 0.026 (3) 0.005 (3)
C25 0.046 (3) 0.063 (4) 0.039 (3) 0.010 (3) 0.013 (3) 0.004 (3)
O3 0.0303 (18) 0.081 (3) 0.0298 (18) −0.0082 (19) 0.0046 (15) −0.0142 (18)
N3 0.026 (2) 0.064 (3) 0.028 (2) −0.001 (2) 0.0044 (17) −0.005 (2)
C31 0.032 (3) 0.066 (4) 0.033 (3) 0.000 (3) 0.009 (2) −0.003 (3)
C32 0.030 (3) 0.082 (5) 0.034 (3) −0.006 (3) 0.002 (2) 0.001 (3)
C33 0.041 (3) 0.078 (5) 0.037 (3) −0.012 (3) 0.010 (2) −0.011 (3)
C34 0.051 (3) 0.061 (4) 0.038 (3) −0.006 (3) 0.011 (3) −0.007 (3)
C35 0.037 (3) 0.069 (4) 0.038 (3) 0.005 (3) 0.011 (2) −0.004 (3)
Sn2 0.03211 (18) 0.0585 (2) 0.03364 (19) 0.00321 (17) 0.00892 (14) 0.00114 (17)
I21 0.03067 (17) 0.0658 (3) 0.03681 (18) 0.00703 (16) 0.01019 (14) 0.01054 (17)
I22 0.03276 (18) 0.0618 (2) 0.04178 (19) 0.00575 (16) 0.00928 (14) 0.00537 (17)
I23 0.0412 (2) 0.0936 (3) 0.0390 (2) −0.0066 (2) 0.00527 (16) −0.0089 (2)
C4 0.049 (4) 0.081 (5) 0.074 (5) −0.003 (3) 0.014 (3) 0.002 (4)
Cl1 0.0492 (10) 0.1056 (17) 0.150 (2) −0.0147 (11) 0.0054 (12) 0.0017 (16)
Cl2 0.0779 (13) 0.0957 (15) 0.0771 (12) −0.0138 (11) 0.0305 (10) −0.0118 (11)
Cl3 0.0740 (13) 0.0922 (15) 0.0928 (15) 0.0099 (11) 0.0026 (11) 0.0101 (12)

Diiodido(isopropyl)tris(pyridine N-oxide)tin(IV) triiodidostannate(II) deuterochloroform monosolvate (2) . Geometric parameters (Å, º)

Sn1—O2 2.163 (4) C24—C25 1.368 (9)
Sn1—O1 2.169 (3) O3—N3 1.347 (5)
Sn1—O3 2.185 (3) N3—C31 1.329 (7)
Sn1—C1 2.228 (6) N3—C35 1.341 (8)
Sn1—I12 2.8144 (5) C31—C32 1.368 (7)
Sn1—I11 2.8206 (6) C32—C33 1.375 (9)
C1—C2 1.426 (11) C33—C34 1.370 (8)
C1—C3 1.467 (12) C34—C35 1.376 (8)
O1—N1 1.354 (5) Sn2—I23 2.9196 (6)
N1—C15 1.328 (7) Sn2—I22 2.9903 (5)
N1—C11 1.349 (6) Sn2—I21 3.0481 (5)
C11—C12 1.383 (8) Sn2—I21i 3.3802 (5)
C12—C13 1.364 (9) Sn2—I22ii 3.6188 (5)
C13—C14 1.387 (8) Sn2—I23ii 3.8473 (6)
C14—C15 1.376 (8) I21—Sn2ii 3.3802 (5)
O2—N2 1.353 (6) I22—Sn2i 3.6188 (5)
N2—C25 1.340 (7) I23—Sn2i 3.8473 (6)
N2—C21 1.341 (7) C4—Cl1 1.736 (7)
C21—C22 1.353 (11) C4—Cl2 1.753 (8)
C22—C23 1.372 (11) C4—Cl3 1.779 (8)
C23—C24 1.387 (10)
O2—Sn1—O1 78.14 (14) C22—C23—C24 118.4 (7)
O2—Sn1—O3 78.98 (15) C25—C24—C23 119.3 (7)
O1—Sn1—O3 81.42 (12) N2—C25—C24 120.6 (6)
O2—Sn1—C1 89.7 (3) N3—O3—Sn1 123.1 (3)
O1—Sn1—C1 165.0 (2) C31—N3—C35 122.1 (5)
O3—Sn1—C1 87.7 (2) C31—N3—O3 119.0 (5)
O2—Sn1—I12 93.49 (10) C35—N3—O3 118.9 (4)
O1—Sn1—I12 89.88 (9) N3—C31—C32 119.9 (6)
O3—Sn1—I12 169.47 (10) C31—C32—C33 120.0 (6)
C1—Sn1—I12 99.74 (18) C34—C33—C32 118.7 (5)
O2—Sn1—I11 161.88 (10) C33—C34—C35 120.2 (6)
O1—Sn1—I11 88.47 (10) N3—C35—C34 119.1 (6)
O3—Sn1—I11 87.07 (12) I23—Sn2—I22 91.639 (16)
C1—Sn1—I11 101.3 (3) I23—Sn2—I21 92.798 (16)
I12—Sn1—I11 98.680 (19) I22—Sn2—I21 94.528 (14)
C2—C1—C3 117.4 (8) I23—Sn2—I21i 88.901 (15)
C2—C1—Sn1 113.0 (6) I22—Sn2—I21i 87.046 (14)
C3—C1—Sn1 111.0 (5) I21—Sn2—I21i 177.647 (18)
N1—O1—Sn1 127.3 (3) I23—Sn2—I22ii 97.168 (15)
C15—N1—C11 121.8 (5) I22—Sn2—I22ii 170.674 (17)
C15—N1—O1 118.9 (4) I21—Sn2—I22ii 82.027 (13)
C11—N1—O1 118.9 (4) I21i—Sn2—I22ii 96.151 (12)
N1—C11—C12 119.2 (5) I23—Sn2—I23ii 164.661 (19)
C13—C12—C11 119.8 (5) I22—Sn2—I23ii 101.773 (14)
C12—C13—C14 119.9 (5) I21—Sn2—I23ii 78.886 (13)
C15—C14—C13 118.7 (5) I21i—Sn2—I23ii 99.090 (12)
N1—C15—C14 120.6 (5) I22ii—Sn2—I23ii 69.102 (11)
N2—O2—Sn1 125.7 (3) Sn2—I21—Sn2ii 83.248 (9)
C25—N2—C21 120.6 (6) Sn2—I22—Sn2i 80.039 (9)
C25—N2—O2 119.9 (4) Sn2—I23—Sn2i 77.057 (10)
C21—N2—O2 119.2 (5) Cl1—C4—Cl2 111.5 (4)
N2—C21—C22 120.5 (7) Cl1—C4—Cl3 111.3 (4)
C21—C22—C23 120.5 (6) Cl2—C4—Cl3 110.1 (4)

Symmetry codes: (i) −x+1/2, y+1/2, −z+1/2; (ii) −x+1/2, y−1/2, −z+1/2.

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) 1, 2. DOI: 10.1107/S2056989026006596/ox2024sup1.cif

e-82-00888-sup1.cif (7.1MB, cif)

Structure factors: contains datablock(s) 1. DOI: 10.1107/S2056989026006596/ox20241sup2.hkl

e-82-00888-1sup2.hkl (471.1KB, hkl)

Structure factors: contains datablock(s) 2. DOI: 10.1107/S2056989026006596/ox20242sup3.hkl

e-82-00888-2sup3.hkl (661.5KB, hkl)

CCDC references: 2564137, 2564136

Additional supporting information: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Crystallographic Communications are provided here courtesy of International Union of Crystallography

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