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ISSN: 2056-9890

Syntheses and structures of bis­(2-amino­py­rimi­dine-κN1)di­chlorido­zinc(II) (ortho­rhom­bic polymorph) and bis­(2-am­ino­py­rimi­dine-κN1)di­iodido­zinc(II)

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aInstitut für Anorganische Chemie, Universität Kiel, Max-Eyth.-Str. 2, 24118 Kiel, Germany, and bSuman Ramesh Tulsiani Technical Campus - Faculty of Engineering. Kamshet, Pune, India
*Correspondence e-mail: [email protected]

Edited by W. T. A. Harrison, University of Aberdeen, United Kingdom (Received 5 February 2026; accepted 19 February 2026; online 24 February 2026)

The title compounds, [ZnCl2(C4H5N3)2] (1) and [ZnI2(C4H5N3)2] (2) (C4H5N3 = 2-amino­pyrimidine), were prepared from a solvent mixture of tri­chloro­methane and methanol and structurally characterized. The asymmetric unit of 1 consists of one ZnII cation that is situated on a twofold rotation axis and one chloride anion as well as one 2-amino­pyrimidine ligand in general positions. The asymmetric unit of 2 is built up of one ZnII cation, two iodide anions and two 2-amino­pyrimidine ligands, all of them located in general positions. In both compounds, the metal cations are tetra­hedrally coordinated by two halide anions and two 2-amino­pyrimidine ligands. In compound 1, the discrete complexes are linked by N—H⋯Cl hydrogen bonds into layers that are further connected by weak C—H⋯Cl inter­actions. In compound 2, the complexes are connected via N—H⋯I hydrogen bonds into layers that are further linked by a number of N—H⋯I and C—H⋯I hydrogen bonds. Compound 1 represents a second polymorphic modification of ZnCl2(C4H5N3)2 that crystallizes in the ortho­rhom­bic non-centrosymmetric space group Pba2, whereas the known form crystallizes in the monoclinic, centrosymmetric space group C2/c [Lin & Zeng (2007View full citation). Acta Cryst. E63, m1597].

1. Chemical context

Investigations on the synthesis and crystal structures of new coordination compounds is still a major field in inorganic chemistry. Our inter­est is focused on coordination compounds based on transition-metal halides and N-donor coligands. In the beginning, we concentrated on compounds based on univalent cations such as CuI because they show a versatile structural behavior that can be traced back to the fact that the metal cations are frequently linked by bridging halide anions (Kromp & Sheldrick, 1999View full citation; Peng et al., 2010View full citation; Näther et al., 2001View full citation, 2002View full citation). Moreover, multiple compounds with a different ratio between the metal halide and the coligand are often observed (Näther & Jess, 2002View full citation; Näther et al., 2003View full citation). In further work, we investigated coordination compounds with twofold positively charged metal cations such as ZnII or CdII, but compared to the copper(I) halides these show a limited structural variability (Bhosekar et al., 2006View full citation; Neumann et al., 2018aView full citation,bView full citation). Such compounds, however, are of inter­est because of their luminescence properties (Zeng et al., 2010View full citation; Neumann et al., 2018aView full citation,bView full citation; Jess et al., 2020View full citation; Kokina et al., 2020View full citation).

In the course of our systematic investigations, we became inter­ested in 2-amino­pyrimidine (C4H5N3) as coligand. On the one hand, the coordination of a metal cation might be more difficult, because of steric inter­ference from the neighbouring amino group, but on the other strong hydrogen bonding can be expected.

In this context it is noted that two compounds with the composition ZnCl2(C4H5N3)2 (CSD refcode YIDPAD; Lin & Zeng, 2007View full citation) and ZnBr2(C4H5N3)2 (LOBPOI; Qu et al., 2008View full citation) are already reported in the CSD (Version 5.43, 2025; Groom et al., 2016View full citation), as found using a CONQUEST (Bruno et al., 2002View full citation) search. Both of them consist of discrete neutral complexes that are linked by inter­molecular hydrogen bonds. In the course of our investigations, we obtained crystals of the missing compound with ZnI2, and with ZnCl2 we obtained crystals of a second polymorph of ZnCl2(C4H5N3)2 (Lin & Zeng, 2007View full citation).

[Scheme 1]

2. Structural commentary

ZnCl2(C4H5N3)2 (1) represents a second polymorphic modification of the form that is already reported in the literature (Lin & Zeng, 2007View full citation). In contrast to the reported form that crystallizes in the centrosymmetric monoclinic space group C2/c, compound 1 crystallizes in the non-centrosymmetric ortho­rhom­bic space group Pba2. The asymmetric unit of 1 consists of one ZnII cation located on a twofold rotation axis and one chloride anion and one 2-amino­pyrimidine ligand in general positions (Fig. 1[link]). In the crystal structure, the ZnII cations are fourfold coordinated by two symmetry-related halide anions and two symmetry-related 2-amino­pyrimidine ligands (Fig. 1[link]). Bond lengths and angles show that the tetra­hedra are only slightly distorted (Table 1[link]). The overall geometry is very similar to the form reported in the literature (Lin & Zeng, 2007View full citation). Compound 1 was crystallized from the mixed solvents of methanol and tri­chloro­methane (see Synthesis and crystallization) whereas the form reported by Lin & Zeng was crystallized from an ethanol solution.

Table 1
Selected geometric parameters (Å, °) for 1[link]

Zn1—N1 2.028 (3) Zn1—Cl1 2.2613 (10)
       
N1i—Zn1—N1 111.5 (2) N1—Zn1—Cl1 111.64 (9)
N1—Zn1—Cl1i 105.22 (9) Cl1i—Zn1—Cl1 111.79 (6)
Symmetry code: (i) Mathematical equation.
[Figure 1]
Figure 1
The mol­ecular structure of 1 with displacement ellipsoids drawn at the 50% probability level and intra­molecular N—H⋯Cl hydrogen bonding shown as dashed lines. Symmetry code: (i) −x + 1, −y + 1, z.

The iodide compound ZnI2(C4H5N3)2 (2) is not isotypic to any of the zinc(II) halide compounds known in the literature and also not to 1. Its asymmetric unit is built up of one ZnII cation as well as two crystallographically independent iodide anions and 2-amino­pyrimidine ligands that are located in general positions (Fig. 2[link]). As in 1, the ZnII cations are fourfold coordinated by two iodide anions and two 2-amino­pyrimidine ligands within slightly distorted tetra­hedra (Fig. 2[link] and Table 2[link]).

Table 2
Selected geometric parameters (Å, °) for 2[link]

Zn1—N11 2.040 (3) Zn1—I2 2.5686 (6)
Zn1—N1 2.052 (4) Zn1—I1 2.5948 (6)
       
N11—Zn1—N1 103.25 (14) N11—Zn1—I1 109.47 (10)
N11—Zn1—I2 110.46 (10) N1—Zn1—I1 114.82 (10)
N1—Zn1—I2 107.01 (10) I2—Zn1—I1 111.50 (2)
[Figure 2]
Figure 2
The mol­ecular structure of 2 with displacement ellipsoids drawn at the 50% probability level and the intra­molecular N—H⋯I hydrogen bonding shown as a dashed line.

3. Supra­molecular features

In the extended structure of 1, the discrete complexes are linked via N—H⋯Cl hydrogen bonds between the amino H atom and the chloride anions (Fig. 3[link]). One of these H atoms acts as donor for an intra­molecular, the second for an inter­molecular hydrogen bond. The H⋯Cl distances are relatively short and the N—H⋯Cl angles close to linear indicate strong hydrogen bonding (Table 3[link]). In this way, layers are formed,that lie parallel to the ab plane with the hydrogen bonds pointed in the direction of the crystallographic b axis (Fig. 3[link]). These layers are further linked by C—H⋯Cl hydrogen bonds between one of the H atoms of the six-membered rings and the chloride anions (Fig. 4[link] and Table 3[link]). From Fig. 4[link] it may be seen that all the pyrimidine rings point in the crystallographic c-axis direction, clearly proving the non-centrosymmetry of this structure (Fig. 4[link]).

Table 3
Hydrogen-bond geometry (Å, °) for 1[link]

D—H⋯A D—H H⋯A DA D—H⋯A
N3—H3A⋯Cl1ii 0.91 (2) 2.52 (3) 3.431 (4) 177 (5)
N3—H3B⋯Cl1 0.92 (2) 2.43 (3) 3.311 (4) 162 (4)
C2—H2⋯Cl1iii 0.94 2.92 3.772 (5) 152
Symmetry codes: (ii) Mathematical equation; (iii) Mathematical equation.
[Figure 3]
Figure 3
Crystal structure of 1 with a view onto the layers formed by inter­molecular N—H⋯Cl hydrogen bonds (shown as dashed lines).
[Figure 4]
Figure 4
Crystal structure of 1 with a view along the a-axis direction showing the non-centrosymmetry of this structure. Inter­molecular hydrogen bonds are shown as dashed lines.

The structure of 1 is completely different from that of the other polymorph already reported in the literature. In this modification, each complex is linked to neighbouring complexes by centrosymmetric pairs of N—H⋯N hydrogen bonds (Fig. 5[link]). The second N—H H atom is only involved in intra­molecular N—H⋯Cl hydrogen bonding but in contrast to the form presented here, the N—H⋯N and N—H⋯Cl angles are far from linear, surprisingly indicating weaker inter­actions. Finally, in contrast to the title polymorph, in the known form the complexes are linked into chains that propagate in the c-axis direction (Fig. 5[link]).

[Figure 5]
Figure 5
Crystal structure of the second polymorph of 1 already reported in the literature (Lin & Zeng, 2007View full citation) with inter­molecular N—H⋯N and N—H⋯Cl hydrogen bonds shown as dashed lines.

In the iodide compound 2, the discrete complexes are linked by inter­molecular N—H⋯I hydrogen bonds into layers that in this compound are parallel to the bc plane (Fig. 6[link]). As in compound 1, one amine H atom is involved in an intra­molecular hydrogen bond, whereas the second H atom shows inter­molecular hydrogen bonding. Bond lengths and angles also indicate a significant inter­action (Table 4[link]). These layers are further linked by pairs of C—H⋯I inter­actions between the iodide anions and the H atoms of the pyrimidine rings (Fig. 7[link]).

Table 4
Hydrogen-bond geometry (Å, °) for 2[link]

D—H⋯A D—H H⋯A DA D—H⋯A
N3—H3A⋯I1 0.88 (2) 2.96 (3) 3.742 (4) 150 (4)
N3—H3B⋯I1i 0.89 (2) 3.03 (2) 3.922 (4) 173 (5)
C2—H2⋯I2ii 0.94 3.31 3.982 (5) 130
C4—H4⋯N11 0.94 2.67 3.275 (6) 123
N13—H13A⋯I1 0.90 2.84 3.738 (4) 173
N13—H13B⋯I2iii 0.90 2.81 3.693 (4) 169
C13—H13⋯I2iv 0.94 3.10 4.001 (5) 162
C14—H14⋯I2 0.94 3.14 3.815 (5) 130
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation.
[Figure 6]
Figure 6
Crystal structure of 2 along the b-axis direction with a view onto the layers and inter­molecular N—H⋯I hydrogen bonds shown as dashed lines.
[Figure 7]
Figure 7
Crystal structure of 2 with a view along the a-axis direction and inter­molecular hydrogen bonds shown as dashed lines.

4. Database survey

A search in the CSD (Version 5.43, 2025; Groom et al., 2016View full citation) using CONQUEST (Bruno et al., 2002View full citation) revealed that two Zn halide coordination compounds with the composition ZnCl2(C4H5N3)2 (Lin & Zeng, 2007View full citation) and ZnBr2(C4H5N3)2 (Qu et al., 2008View full citation) are already reported (see above). There are additional Zn compounds with different anions that are related to the title compounds, including (Zn(NCS)2(C4H5N3)2 (Jin et al., 2010View full citation), (Zn(NO3)2(C4H5N3)2(H2O) (Gao & Ng, 2010View full citation) and (Zn(C11H5O2F3)2(C4H5N3)2 (Perdih, 2016View full citation) that also consists of discrete complexes. There is also a compound with mixed hydroxide nitrate anions that forms a polymeric structure (Kang et al., 2011View full citation).

Finally, it is noted that some compounds are reported in which the 2-amino­pyrimidine ligands are protonated, but none of them contain zinc(II) as cation. These include, for example, 2-amino-1,3-di­hydro­pyrimidiniumtetra­bromo­copper(II) (Pon et al., 1997View full citation), 2-amino­pyrimidiniumtetra­bromo­cobalt(II) mono­hydrate (Masaki et al., 2002View full citation), 2-amino-1,3-di­hydro­pyrimidin­ium­tetra­aqua­dibromo­manganese(II) dibromide (Lee et al., 2003View full citation) and 2-amino-1,3-di­hydro­pyrimidiniumtetra­aqua­di­bromo­nickel(II) dibromide (Masaki et al., 2002View full citation). In three additional compounds, the 2-amino­pyridine ligand is also protonated and act as counter-cation for Mo and W cluster compounds (Chen et al., 2015View full citation; Xiao et al., 2018View full citation).

5. Synthesis and crystallization

Zinc chloride and zinc iodide as well as 2-amino­pyrimidine were purchased from Sigma-Aldrich.

To prepare 1, 0.500 mmol (68.1 mg) of zinc chloride and 1.00 mmol (95.1 mg) of 2-amino­pyrimidine were reacted in a solvent mixture of 1 ml of tri­chloro­methane and 1 ml of methanol. Within 3 d, crystals suitable for single crystal X-ray diffraction were obtained in the form of colorless blocks.

Compound 2 was prepared by reacting 0.500 mmol (159.6 mg) of zinc iodide and 1.00 mmol (95.1 mg) of 2-amino­pyrimidine in a solvent mixture of 3 ml of tri­chloro­methane and 3 ml of methanol. Within 3 d, colorless blocks suitable for single crystal X-ray diffraction were obtained.

6. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 5[link]. The C—H hydrogen atoms were positioned with idealized geometry and were refined as riding atoms with Uiso(H) = 1.2Ueq(C). The N—H H atoms were located in difference maps and were refined isotropically with restraints (DFIX).

Table 5
Experimental details

  1 2
Crystal data
Chemical formula [ZnCl2(C4H5N3)2] [ZnI2(C4H5N3)2]
Mr 326.49 509.39
Crystal system, space group Orthorhombic, Pba2 Monoclinic, P21/n
Temperature (K) 220 220
a, b, c (Å) 7.6628 (7), 12.0590 (8), 6.8735 (4) 9.5469 (6), 15.3764 (13), 10.1518 (6)
α, β, γ (°) 90, 90, 90 90, 95.884 (7), 90
V3) 635.15 (8) 1482.40 (18)
Z 2 4
Radiation type Mo Kα Mo Kα
μ (mm−1) 2.34 5.81
Crystal size (mm) 0.18 × 0.16 × 0.14 0.16 × 0.10 × 0.06
 
Data collection
Diffractometer Stoe IPDS1 Stoe IPDS1
Absorption correction Numerical (X-RED and X-SHAPE; Stoe, 2008View full citation) Numerical (X-RED and X-SHAPE; Stoe, 2008View full citation)
Tmin, Tmax 0.636, 0.842 0.296, 0.471
No. of measured, independent and observed [I > 2σ(I)] reflections 5690, 1490, 1251 14800, 3491, 2946
Rint 0.045 0.091
(sin θ/λ)max−1) 0.660 0.661
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.032, 0.080, 1.00 0.036, 0.094, 1.03
No. of reflections 1490 3491
No. of parameters 87 163
No. of restraints 3 2
H-atom treatment H atoms treated by a mixture of independent and constrained refinement H atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å−3) 0.49, −0.43 1.17, −1.28
Absolute structure Flack x determined using 505 quotients [(I+)−(I)]/[(I+)+(I)] (Parsons et al., 2013View full citation)
Absolute structure parameter 0.007 (13)
Computer programs: X-AREA (Stoe, 2008View full citation), SHELXT (Sheldrick, 2015aView full citation), SHELXL (Sheldrick, 2015bView full citation), DIAMOND (Brandenburg, 1999View full citation) and XP in SHELXTL-PC (Sheldrick, 2008View full citation) and publCIF (Westrip, 2010View full citation).

Supporting information


Computing details top

Bis(2-aminopyrimidine-κN1)dichloridozinc(II) (1) top
Crystal data top
[ZnCl2(C4H5N3)2]Dx = 1.707 Mg m3
Mr = 326.49Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pba2Cell parameters from 6615 reflections
a = 7.6628 (7) Åθ = 3.0–28.0°
b = 12.0590 (8) ŵ = 2.34 mm1
c = 6.8735 (4) ÅT = 220 K
V = 635.15 (8) Å3Block, colorless
Z = 20.18 × 0.16 × 0.14 mm
F(000) = 328
Data collection top
Stoe IPDS-1
diffractometer
1251 reflections with I > 2σ(I)
Phi scansRint = 0.045
Absorption correction: numerical
(X-Red and X-Shape; Stoe, 2008)
θmax = 28.0°, θmin = 3.2°
Tmin = 0.636, Tmax = 0.842h = 1010
5690 measured reflectionsk = 1515
1490 independent reflectionsl = 89
Refinement top
Refinement on F2H atoms treated by a mixture of independent and constrained refinement
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0537P)2]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.032(Δ/σ)max < 0.001
wR(F2) = 0.080Δρmax = 0.49 e Å3
S = 1.00Δρmin = 0.43 e Å3
1490 reflectionsExtinction correction: SHELXL-2016/6 (Sheldrick 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
87 parametersExtinction coefficient: 0.038 (7)
3 restraintsAbsolute structure: Flack x determined using 505 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
Primary atom site location: dualAbsolute structure parameter: 0.007 (13)
Hydrogen site location: mixed
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
Zn10.5000000.5000000.88265 (9)0.0219 (2)
Cl10.74418 (15)0.50555 (6)1.06713 (13)0.0302 (3)
N10.4752 (4)0.6381 (3)0.7166 (5)0.0222 (7)
N20.4748 (6)0.8362 (4)0.6738 (8)0.0446 (12)
N30.5753 (6)0.7516 (3)0.9660 (7)0.0349 (9)
H3A0.623 (6)0.819 (3)0.998 (8)0.035 (12)*
H3B0.634 (5)0.692 (3)1.018 (7)0.029 (12)*
C10.5104 (5)0.7413 (4)0.7842 (6)0.0232 (8)
C20.4046 (7)0.8250 (4)0.4924 (8)0.0388 (11)
H20.3781920.8880200.4173730.047*
C30.3723 (6)0.7190 (4)0.4194 (6)0.0372 (11)
H30.3283920.7092060.2928740.045*
C40.4057 (6)0.6306 (3)0.5345 (7)0.0304 (9)
H40.3793380.5596490.4860910.036*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Zn10.0307 (3)0.0128 (3)0.0223 (3)0.0020 (2)0.0000.000
Cl10.0370 (6)0.0213 (5)0.0322 (6)0.0024 (4)0.0098 (4)0.0014 (5)
N10.0293 (18)0.0158 (14)0.0215 (17)0.0022 (11)0.0010 (13)0.0017 (13)
N20.058 (3)0.029 (2)0.047 (3)0.0026 (17)0.004 (2)0.008 (2)
N30.058 (2)0.0152 (14)0.032 (2)0.0020 (19)0.011 (2)0.0034 (14)
C10.0279 (19)0.0170 (18)0.025 (2)0.0020 (15)0.0059 (17)0.0000 (16)
C20.055 (3)0.030 (2)0.031 (2)0.008 (2)0.002 (2)0.0150 (19)
C30.046 (2)0.042 (2)0.024 (3)0.005 (2)0.0037 (18)0.0048 (18)
C40.035 (2)0.030 (2)0.026 (2)0.0036 (16)0.0062 (18)0.0002 (16)
Geometric parameters (Å, º) top
Zn1—N1i2.028 (3)N3—C11.351 (6)
Zn1—N12.028 (3)N3—H3A0.91 (2)
Zn1—Cl1i2.2612 (10)N3—H3B0.92 (2)
Zn1—Cl12.2613 (10)C2—C31.396 (7)
N1—C11.355 (6)C2—H20.9400
N1—C41.363 (6)C3—C41.352 (6)
N2—C21.365 (7)C3—H30.9400
N2—C11.401 (6)C4—H40.9400
N1i—Zn1—N1111.5 (2)N3—C1—N1118.4 (4)
N1i—Zn1—Cl1i111.64 (9)N3—C1—N2119.8 (4)
N1—Zn1—Cl1i105.22 (9)N1—C1—N2121.7 (4)
N1i—Zn1—Cl1105.22 (9)N2—C2—C3119.3 (4)
N1—Zn1—Cl1111.64 (9)N2—C2—H2120.4
Cl1i—Zn1—Cl1111.79 (6)C3—C2—H2120.4
C1—N1—C4117.0 (3)C4—C3—C2118.6 (4)
C1—N1—Zn1122.8 (3)C4—C3—H3120.7
C4—N1—Zn1119.9 (3)C2—C3—H3120.7
C2—N2—C1119.4 (4)C3—C4—N1124.0 (4)
C1—N3—H3A117 (3)C3—C4—H4118.0
C1—N3—H3B118 (3)N1—C4—H4118.0
H3A—N3—H3B114 (4)
Symmetry code: (i) x+1, y+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N3—H3A···Cl1ii0.91 (2)2.52 (3)3.431 (4)177 (5)
N3—H3B···Cl10.92 (2)2.43 (3)3.311 (4)162 (4)
C2—H2···Cl1iii0.942.923.772 (5)152
Symmetry codes: (ii) x+3/2, y+1/2, z; (iii) x1/2, y+3/2, z1.
Bis(2-aminopyrimidine-κN1)diiodidozinc(II) (2) top
Crystal data top
[ZnI2(C4H5N3)2]F(000) = 944
Mr = 509.39Dx = 2.282 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 9.5469 (6) ÅCell parameters from 8000 reflections
b = 15.3764 (13) Åθ = 10.4–25.7°
c = 10.1518 (6) ŵ = 5.81 mm1
β = 95.884 (7)°T = 220 K
V = 1482.40 (18) Å3Block, colorless
Z = 40.16 × 0.10 × 0.06 mm
Data collection top
Stoe IPDS-1
diffractometer
2946 reflections with I > 2σ(I)
Phi scansRint = 0.091
Absorption correction: numerical
(X-Red and X-Shape; Stoe, 2008)
θmax = 28.0°, θmin = 2.4°
Tmin = 0.296, Tmax = 0.471h = 1212
14800 measured reflectionsk = 2020
3491 independent reflectionsl = 1313
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)] = 0.036 w = 1/[σ2(Fo2) + (0.0549P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.094(Δ/σ)max = 0.001
S = 1.03Δρmax = 1.17 e Å3
3491 reflectionsΔρmin = 1.28 e Å3
163 parametersExtinction correction: SHELXL-2016/6 (Sheldrick 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
2 restraintsExtinction coefficient: 0.0054 (4)
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*/Ueq
Zn10.75540 (4)0.82087 (3)0.75052 (5)0.02767 (14)
I10.86634 (3)0.67008 (2)0.71225 (3)0.03788 (12)
I20.83722 (3)0.93595 (2)0.59175 (3)0.03509 (12)
N10.7972 (4)0.8692 (2)0.9389 (3)0.0299 (7)
N20.9550 (5)0.9284 (3)1.1144 (5)0.0474 (10)
N31.0345 (4)0.8344 (3)0.9503 (5)0.0391 (9)
H3A1.031 (5)0.792 (2)0.892 (4)0.033 (13)*
H3B1.113 (4)0.837 (4)1.006 (5)0.049 (16)*
C10.9279 (4)0.8763 (3)1.0011 (4)0.0293 (8)
C20.8455 (5)0.9696 (3)1.1649 (5)0.0407 (10)
H20.8618541.0047691.2406750.049*
C30.7096 (5)0.9592 (4)1.1032 (6)0.0460 (11)
H30.6325640.9858921.1376340.055*
C40.6905 (5)0.9095 (3)0.9917 (5)0.0403 (10)
H40.5987360.9028990.9496210.048*
N110.5413 (3)0.8105 (2)0.7281 (4)0.0286 (7)
N120.3223 (4)0.7503 (3)0.7851 (5)0.0480 (10)
N130.5463 (4)0.7037 (3)0.8897 (4)0.0405 (9)
H13A0.6271170.6938060.8536570.061*
H13B0.4931260.6647560.9282670.061*
C110.4698 (4)0.7547 (3)0.8001 (4)0.0296 (8)
C120.2495 (4)0.8033 (3)0.6940 (5)0.0370 (10)
H120.1506380.8010760.6817570.044*
C130.3224 (5)0.8608 (3)0.6193 (5)0.0397 (10)
H130.2736870.8980930.5570580.048*
C140.4642 (5)0.8618 (3)0.6384 (5)0.0371 (9)
H140.5126750.8999890.5868820.044*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Zn10.0211 (2)0.0315 (2)0.0306 (3)0.00168 (16)0.00331 (19)0.00062 (17)
I10.02970 (17)0.03171 (17)0.0529 (2)0.00108 (10)0.00748 (13)0.00385 (11)
I20.03910 (19)0.02980 (17)0.03796 (19)0.00264 (10)0.01170 (13)0.00272 (10)
N10.0257 (16)0.0353 (18)0.0290 (18)0.0031 (13)0.0035 (14)0.0019 (13)
N20.048 (2)0.045 (2)0.049 (3)0.0071 (18)0.003 (2)0.0010 (18)
N30.0285 (19)0.046 (2)0.042 (2)0.0032 (15)0.0006 (17)0.0062 (17)
C10.0274 (19)0.0267 (19)0.033 (2)0.0041 (14)0.0008 (16)0.0029 (15)
C20.049 (3)0.036 (2)0.037 (2)0.0031 (19)0.006 (2)0.0065 (19)
C30.042 (3)0.049 (3)0.048 (3)0.003 (2)0.009 (2)0.013 (2)
C40.027 (2)0.049 (3)0.045 (3)0.0028 (18)0.0058 (19)0.012 (2)
N110.0200 (15)0.0340 (17)0.0314 (19)0.0005 (12)0.0000 (14)0.0044 (13)
N120.034 (2)0.055 (3)0.055 (3)0.0010 (17)0.0069 (19)0.000 (2)
N130.0268 (18)0.050 (2)0.044 (2)0.0027 (15)0.0034 (16)0.0186 (18)
C110.0246 (19)0.034 (2)0.031 (2)0.0015 (14)0.0058 (16)0.0016 (15)
C120.0203 (19)0.052 (3)0.038 (3)0.0063 (17)0.0002 (17)0.004 (2)
C130.034 (2)0.043 (3)0.040 (3)0.0090 (18)0.0064 (19)0.0030 (19)
C140.034 (2)0.034 (2)0.043 (3)0.0013 (17)0.0001 (19)0.0050 (18)
Geometric parameters (Å, º) top
Zn1—N112.040 (3)C3—H30.9400
Zn1—N12.052 (4)C4—H40.9400
Zn1—I22.5686 (6)N11—C111.356 (5)
Zn1—I12.5948 (6)N11—C141.361 (6)
N1—C11.344 (5)N12—C121.368 (6)
N1—C41.349 (6)N12—C111.403 (6)
N2—C21.367 (7)N13—C111.356 (6)
N2—C11.403 (6)N13—H13A0.9000
N3—C11.351 (6)N13—H13B0.9001
N3—H3A0.876 (19)C12—C131.396 (7)
N3—H3B0.89 (2)C12—H120.9400
C2—C31.391 (7)C13—C141.348 (6)
C2—H20.9400C13—H130.9400
C3—C41.363 (7)C14—H140.9400
N11—Zn1—N1103.25 (14)N1—C4—C3123.1 (4)
N11—Zn1—I2110.46 (10)N1—C4—H4118.5
N1—Zn1—I2107.01 (10)C3—C4—H4118.5
N11—Zn1—I1109.47 (10)C11—N11—C14117.3 (4)
N1—Zn1—I1114.82 (10)C11—N11—Zn1122.9 (3)
I2—Zn1—I1111.50 (2)C14—N11—Zn1119.8 (3)
C1—N1—C4118.6 (4)C12—N12—C11118.6 (4)
C1—N1—Zn1123.4 (3)C11—N13—H13A104.5
C4—N1—Zn1117.0 (3)C11—N13—H13B112.8
C2—N2—C1119.2 (4)H13A—N13—H13B127.6
C1—N3—H3A129 (4)N11—C11—N13117.5 (4)
C1—N3—H3B111 (4)N11—C11—N12121.8 (4)
H3A—N3—H3B115 (5)N13—C11—N12120.7 (4)
N1—C1—N3118.8 (4)N12—C12—C13119.9 (4)
N1—C1—N2121.0 (4)N12—C12—H12120.1
N3—C1—N2120.2 (4)C13—C12—H12120.1
N2—C2—C3119.5 (4)C14—C13—C12118.5 (4)
N2—C2—H2120.3C14—C13—H13120.7
C3—C2—H2120.3C12—C13—H13120.7
C4—C3—C2118.5 (5)C13—C14—N11123.8 (4)
C4—C3—H3120.7C13—C14—H14118.1
C2—C3—H3120.7N11—C14—H14118.1
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N3—H3A···I10.88 (2)2.96 (3)3.742 (4)150 (4)
N3—H3B···I1i0.89 (2)3.03 (2)3.922 (4)173 (5)
C2—H2···I2ii0.943.313.982 (5)130
C4—H4···N110.942.673.275 (6)123
N13—H13A···I10.902.843.738 (4)173
N13—H13B···I2iii0.902.813.693 (4)169
C13—H13···I2iv0.943.104.001 (5)162
C14—H14···I20.943.143.815 (5)130
Symmetry codes: (i) x+1/2, y+3/2, z+1/2; (ii) x+2, y+2, z+2; (iii) x1/2, y+3/2, z+1/2; (iv) x+1, y+2, z+1.
 

Acknowledgements

Financial support by the State of Schleswig-Holstein is gratefully acknowledged.

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