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In recent years, great technological advances have been achieved in the growth of hybrid organic–inorganic perovskites (HOIPs) and these have attracted extensive attention due to their optoelectronic properties, structural tunability and stability. We present here a new two-dimensional hybrid organic–inorganic perovskite, namely, poly[bis­(3-fluoro­cyclo­butyl­ammonium) [di-μ-iodido-di­iodido­plumbate(VI)]], {(C4H9FN)2[PbI4]}n, showing a two-dimensional reticular layer with the organic cations in the middle of the meshes. The calculated experimental band gap is 2.44 eV and the band gap is calculated as 2.20 eV theoretically, which further suggests the potential of this com­pound as a semiconductor.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229620015272/qf3046sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229620015272/qf3046Isup2.hkl
Contains datablock I

CCDC reference: 2034793

Computing details top

Data collection: CrysAlis PRO (Rigaku OD, 2018); cell refinement: CrysAlis PRO (Rigaku OD, 2018); data reduction: CrysAlis PRO (Rigaku OD, 2018); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Poly[bis(3-fluorocyclobutylammonium) [di-µ-iodido-diiodidoplumbate(VI)]] top
Crystal data top
(C4H9FN)2[PbI4]F(000) = 784
Mr = 895.03Dx = 2.991 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 13.6842 (5) ÅCell parameters from 6193 reflections
b = 8.5302 (3) Åθ = 2.5–30.5°
c = 8.9518 (3) ŵ = 14.70 mm1
β = 107.996 (4)°T = 293 K
V = 993.81 (6) Å3Block, yellow
Z = 20.16 × 0.16 × 0.15 mm
Data collection top
XtaLAB Synergy R, DW system, HyPix
diffractometer
Rint = 0.036
ω scansθmax = 30.8°, θmin = 2.9°
Absorption correction: multi-scan
(CrysAlis PRO; Rigaku OD, 2018)
h = 1817
Tmin = 0.110, Tmax = 0.119k = 1112
8813 measured reflectionsl = 1110
2537 independent reflections6193 standard reflections every 0 reflections
2191 reflections with I > 2σ(I) intensity decay: none
Refinement top
Refinement on F224 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.032H-atom parameters constrained
wR(F2) = 0.082 w = 1/[σ2(Fo2) + (0.0435P)2 + 2.3818P]
where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max = 0.001
2537 reflectionsΔρmax = 1.41 e Å3
79 parametersΔρmin = 1.63 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pb10.00000.50000.00000.03910 (10)
I10.04490 (4)0.30746 (5)0.32397 (4)0.05175 (13)
I30.23936 (4)0.57359 (6)0.08670 (5)0.06083 (15)
N10.2047 (5)0.5207 (8)0.6732 (8)0.0659 (17)
H1A0.14820.48620.60130.099*
H1B0.19560.51890.76730.099*
H1C0.21770.61840.65010.099*
F10.4838 (6)0.3014 (11)0.6462 (13)0.165 (4)
C10.2927 (7)0.4184 (11)0.6745 (11)0.078 (2)
H1D0.27670.30690.67910.117*
C20.3934 (9)0.4616 (16)0.7896 (12)0.101 (3)
H2A0.41720.38800.87580.151*
H2B0.39590.56830.82820.151*
C30.4441 (10)0.4411 (17)0.6632 (15)0.107 (3)
H3A0.48910.52880.65790.129*
C40.3406 (9)0.4540 (17)0.5475 (13)0.107 (3)
H4A0.32670.37520.46550.128*
H4B0.32480.55810.50290.128*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pb10.0509 (2)0.03570 (16)0.03248 (15)0.00137 (11)0.01549 (12)0.00018 (10)
I10.0702 (3)0.0445 (2)0.0418 (2)0.00003 (18)0.01929 (18)0.01497 (15)
I30.0558 (3)0.0680 (3)0.0569 (3)0.0057 (2)0.0148 (2)0.0059 (2)
N10.058 (4)0.074 (4)0.067 (4)0.005 (3)0.022 (3)0.010 (3)
F10.096 (5)0.137 (6)0.248 (9)0.047 (5)0.035 (5)0.035 (6)
C10.073 (5)0.078 (5)0.081 (5)0.001 (4)0.020 (4)0.005 (4)
C20.078 (7)0.154 (10)0.073 (6)0.021 (7)0.026 (5)0.006 (6)
C30.104 (7)0.110 (7)0.114 (7)0.005 (6)0.043 (6)0.017 (6)
C40.102 (7)0.147 (7)0.081 (5)0.029 (6)0.042 (5)0.004 (5)
Geometric parameters (Å, º) top
Pb1—I3i3.1865 (5)F1—C31.338 (14)
Pb1—I33.1865 (5)C1—C21.489 (14)
Pb1—I1ii3.2151 (4)C1—C41.509 (13)
Pb1—I1iii3.2151 (4)C1—H1D0.9800
Pb1—I13.2225 (3)C2—C31.509 (16)
Pb1—I1i3.2225 (3)C2—H2A0.9700
I1—Pb1iv3.2152 (4)C2—H2B0.9700
N1—C11.483 (11)C3—C41.477 (16)
N1—H1A0.8900C3—H3A0.9800
N1—H1B0.8900C4—H4A0.9700
N1—H1C0.8900C4—H4B0.9700
I3i—Pb1—I3180.0N1—C1—C4114.6 (9)
I3i—Pb1—I1ii93.302 (12)C2—C1—C486.9 (8)
I3—Pb1—I1ii86.698 (12)N1—C1—H1D112.4
I3i—Pb1—I1iii86.698 (12)C2—C1—H1D112.4
I3—Pb1—I1iii93.302 (12)C4—C1—H1D112.4
I1ii—Pb1—I1iii180.000 (16)C1—C2—C389.7 (8)
I3i—Pb1—I190.838 (12)C1—C2—H2A113.7
I3—Pb1—I189.162 (13)C3—C2—H2A113.7
I1ii—Pb1—I190.753 (5)C1—C2—H2B113.7
I1iii—Pb1—I189.247 (5)C3—C2—H2B113.7
I3i—Pb1—I1i89.163 (13)H2A—C2—H2B110.9
I3—Pb1—I1i90.837 (12)F1—C3—C4108.8 (11)
I1ii—Pb1—I1i89.246 (5)F1—C3—C2119.1 (13)
I1iii—Pb1—I1i90.754 (5)C4—C3—C287.3 (9)
I1—Pb1—I1i180.0F1—C3—H3A113.0
Pb1iv—I1—Pb1147.634 (15)C4—C3—H3A113.0
C1—N1—H1A109.5C2—C3—H3A113.0
C1—N1—H1B109.5C3—C4—C190.2 (9)
H1A—N1—H1B109.5C3—C4—H4A113.6
C1—N1—H1C109.5C1—C4—H4A113.6
H1A—N1—H1C109.5C3—C4—H4B113.6
H1B—N1—H1C109.5C1—C4—H4B113.6
N1—C1—C2115.8 (9)H4A—C4—H4B110.9
N1—C1—C2—C3133.9 (10)F1—C3—C4—C1101.7 (11)
C4—C1—C2—C318.0 (10)C2—C3—C4—C118.1 (10)
C1—C2—C3—F191.7 (13)N1—C1—C4—C3135.4 (9)
C1—C2—C3—C418.4 (10)C2—C1—C4—C318.4 (10)
Symmetry codes: (i) x, y+1, z; (ii) x, y+1/2, z1/2; (iii) x, y+1/2, z+1/2; (iv) x, y1/2, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2—H2B···F1v0.972.553.308 (13)135
N1—H1A···I10.892.883.693 (7)152
N1—H1B···I3vi0.892.773.612 (7)158
N1—H1C···I3vii0.892.723.609 (7)174
Symmetry codes: (v) x+1, y+1/2, z+3/2; (vi) x, y, z+1; (vii) x, y+3/2, z+1/2.
 

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