Literature DB >> 21579304

Poly[1,4-bis-(ammonio-meth-yl)cyclo-hexane [di-μ-chlorido-dichloridoplumbate(II)]].

Matthew Kyle Rayner1, David Gordon Billing.   

Abstract

The title compound, {(C(8)H(20)N(2))[PbCl(4)]}(n), crystallizes as an layered inorganic-organic hybrid perovskite-type structure. Corner-sharing PbCl(6) octa-hedra extend parallel to the ac plane. Adjacent layers are staggered relative to one another, with diammonium cations separating these layers. The cations exhibit symmetry and inter-act with the inorganic sheets via N-H⋯Cl hydrogen bonding in the right-angled halogen sub-type of the terminal halide hydrogen-bonding motif.

Entities:  

Year:  2010        PMID: 21579304      PMCID: PMC2979563          DOI: 10.1107/S1600536810016818

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

Similar structures have been reported by Billing & Lemmerer (2006 ▶) and Dobrzycki & Woźniak (2009 ▶). Structure–properties relation experiments have been performed by Mitzi et al. (2001 ▶). For hydrogen-bonding nomenclature for inorganic–organic hybrids, see: Mitzi (1999 ▶). For the bromido- and iodidoplumbate(II) analogues of the title compound, see: Rayner & Billing (2010a ▶,b ▶).

Experimental

Crystal data

(C8H20N2)[PbCl4] M = 493.25 Orthorhombic, a = 7.7990 (2) Å b = 24.0666 (6) Å c = 7.9348 (2) Å V = 1489.33 (7) Å3 Z = 4 Mo Kα radiation μ = 12.02 mm−1 T = 173 K 0.54 × 0.41 × 0.04 mm

Data collection

Bruker APEXII CCD area-detector diffractometer Absorption correction: integration (XPREP; Bruker, 2005 ▶) T min = 0.032, T max = 0.685 13290 measured reflections 1850 independent reflections 1654 reflections with I > 2σ(I) R int = 0.049

Refinement

R[F 2 > 2σ(F 2)] = 0.031 wR(F 2) = 0.067 S = 1.16 1850 reflections 73 parameters H-atom parameters constrained Δρmax = 1.47 e Å−3 Δρmin = −3.53 e Å−3 Data collection: APEX2 (Bruker, 2005 ▶); cell refinement: SAINT (Bruker, 2005 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶) and DIAMOND (Brandenburg, 1999 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶) and PLATON (Spek, 2009 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810016818/wm2339sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810016818/wm2339Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
(C8H20N2)[PbCl4]F(000) = 928
Mr = 493.25Dx = 2.200 Mg m3
Orthorhombic, PnmaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2nCell parameters from 6650 reflections
a = 7.7990 (2) Åθ = 2.7–28.3°
b = 24.0666 (6) ŵ = 12.02 mm1
c = 7.9348 (2) ÅT = 173 K
V = 1489.33 (7) Å3Plate, colourless
Z = 40.54 × 0.41 × 0.04 mm
Bruker APEXII CCD area-detector diffractometer1850 independent reflections
Radiation source: fine-focus sealed tube1654 reflections with I > 2σ(I)
graphiteRint = 0.049
φ and ω scansθmax = 28.0°, θmin = 1.7°
Absorption correction: integration (XPREP; Bruker, 2005)h = −10→10
Tmin = 0.032, Tmax = 0.685k = −31→31
13290 measured reflectionsl = −10→10
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.031Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.067H-atom parameters constrained
S = 1.16w = 1/[σ2(Fo2) + (0.003P)2 + 19.9694P] where P = (Fo2 + 2Fc2)/3
1850 reflections(Δ/σ)max = 0.007
73 parametersΔρmax = 1.47 e Å3
0 restraintsΔρmin = −3.53 e Å3
Experimental. Numerical intergration absorption corrections based on indexed crystal faces were applied using the XPREP routine (Bruker, 2005)
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.
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.
xyzUiso*/Ueq
C10.5490 (8)0.6188 (2)0.9551 (8)0.0201 (12)
H1A0.61350.61590.84800.024*
H1B0.44290.64010.93260.024*
C20.5016 (8)0.5612 (2)1.0147 (8)0.0201 (12)
H20.42560.56541.11540.024*
C30.3984 (9)0.5318 (3)0.8783 (8)0.0256 (13)
H3A0.46830.52930.77440.031*
H3B0.29480.55400.85210.031*
C40.6555 (8)0.5265 (3)1.0676 (8)0.0239 (13)
H4A0.71500.54511.16230.029*
H4B0.73690.52380.97230.029*
N10.6553 (7)0.6496 (2)1.0812 (7)0.0213 (11)
H1C0.68160.68381.04000.032*
H1D0.75370.63031.10130.032*
H1E0.59540.65321.17890.032*
Cl10.05791 (19)0.63163 (6)1.02923 (19)0.0229 (3)
Cl2−0.1125 (3)0.75001.2974 (2)0.0194 (4)
Cl30.2609 (3)0.75000.6719 (3)0.0238 (4)
Pb10.08434 (4)0.75000.99093 (4)0.01374 (9)
U11U22U33U12U13U23
C10.019 (3)0.018 (3)0.023 (3)0.002 (2)−0.002 (2)0.001 (2)
C20.020 (3)0.021 (3)0.019 (3)0.000 (2)−0.003 (2)−0.001 (3)
C30.031 (4)0.020 (3)0.026 (3)−0.004 (3)−0.009 (3)0.000 (2)
C40.023 (3)0.021 (3)0.028 (3)−0.004 (3)−0.005 (3)−0.001 (3)
N10.023 (3)0.018 (2)0.023 (2)−0.003 (2)0.002 (2)−0.003 (2)
Cl10.0202 (7)0.0229 (7)0.0257 (7)0.0021 (5)0.0001 (6)−0.0037 (6)
Cl20.0170 (10)0.0221 (9)0.0192 (9)0.0000.0049 (7)0.000
Cl30.0222 (10)0.0297 (11)0.0197 (9)0.0000.0056 (8)0.000
Pb10.01269 (14)0.01657 (14)0.01196 (13)0.0000.00002 (12)0.000
C1—N11.495 (8)C4—H4B0.9900
C1—C21.512 (8)N1—H1C0.9100
C1—H1A0.9900N1—H1D0.9100
C1—H1B0.9900N1—H1E0.9100
C2—C31.523 (8)Cl1—Pb12.8723 (15)
C2—C41.521 (9)Cl2—Pb12.8759 (19)
C2—H21.0000Cl2—Pb1ii2.9002 (19)
C3—C4i1.525 (9)Cl3—Pb1iii2.834 (2)
C3—H3A0.9900Cl3—Pb12.882 (2)
C3—H3B0.9900Pb1—Cl3iv2.834 (2)
C4—C3i1.525 (9)Pb1—Cl1v2.8723 (15)
C4—H4A0.9900Pb1—Cl2vi2.900 (2)
N1—C1—C2112.4 (5)C1—N1—H1C109.5
N1—C1—H1A109.1C1—N1—H1D109.5
C2—C1—H1A109.1H1C—N1—H1D109.5
N1—C1—H1B109.1C1—N1—H1E109.5
C2—C1—H1B109.1H1C—N1—H1E109.5
H1A—C1—H1B107.9H1D—N1—H1E109.5
C1—C2—C3109.5 (5)Pb1—Cl2—Pb1ii157.64 (8)
C1—C2—C4113.4 (5)Pb1iii—Cl3—Pb1145.68 (9)
C3—C2—C4111.0 (5)Cl3iv—Pb1—Cl1v89.10 (3)
C1—C2—H2107.6Cl3iv—Pb1—Cl189.10 (3)
C3—C2—H2107.6Cl1v—Pb1—Cl1165.31 (6)
C4—C2—H2107.6Cl3iv—Pb1—Cl284.87 (6)
C2—C3—C4i111.8 (5)Cl1v—Pb1—Cl282.66 (3)
C2—C3—H3A109.2Cl1—Pb1—Cl282.66 (3)
C4i—C3—H3A109.2Cl3iv—Pb1—Cl391.42 (3)
C2—C3—H3B109.2Cl1v—Pb1—Cl397.31 (3)
C4i—C3—H3B109.2Cl1—Pb1—Cl397.31 (3)
H3A—C3—H3B107.9Cl2—Pb1—Cl3176.29 (6)
C2—C4—C3i111.4 (5)Cl3iv—Pb1—Cl2vi171.75 (6)
C2—C4—H4A109.3Cl1v—Pb1—Cl2vi89.84 (3)
C3i—C4—H4A109.3Cl1—Pb1—Cl2vi89.84 (3)
C2—C4—H4B109.3Cl2—Pb1—Cl2vi86.875 (17)
C3i—C4—H4B109.3Cl3—Pb1—Cl2vi96.83 (6)
H4A—C4—H4B108.0
N1—C1—C2—C3−178.3 (5)Pb1ii—Cl2—Pb1—Cl1v89.76 (3)
N1—C1—C2—C4−53.7 (7)Pb1ii—Cl2—Pb1—Cl1−89.76 (3)
C1—C2—C3—C4i−179.2 (5)Pb1ii—Cl2—Pb1—Cl2vi180.0
C4—C2—C3—C4i54.9 (8)Pb1iii—Cl3—Pb1—Cl3iv180.0
C1—C2—C4—C3i−178.3 (5)Pb1iii—Cl3—Pb1—Cl1v90.72 (3)
C3—C2—C4—C3i−54.6 (8)Pb1iii—Cl3—Pb1—Cl1−90.72 (3)
Pb1ii—Cl2—Pb1—Cl3iv0.0Pb1iii—Cl3—Pb1—Cl2vi0.0
D—H···AD—HH···AD···AD—H···A
N1—H1C···Cl3iii0.912.403.249 (5)156
N1—H1D···Cl1vii0.912.443.196 (6)141
N1—H1E···Cl1vi0.912.393.212 (5)150
N1—H1E···Cl2vi0.912.843.337 (5)115
Table 1

Selected bond lengths (Å)

Pb1—Cl3i2.834 (2)
Pb1—Cl1ii2.8723 (15)
Pb1—Cl2iii2.900 (2)

Symmetry codes: (i) ; (ii) ; (iii) .

Table 2

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H1C⋯Cl3iv0.912.403.249 (5)156
N1—H1D⋯Cl1v0.912.443.196 (6)141
N1—H1E⋯Cl1iii0.912.393.212 (5)150
N1—H1E⋯Cl2iii0.912.843.337 (5)115

Symmetry codes: (iii) ; (iv) ; (v) .

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Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2010-05-15

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