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
CCDC reference: 2034793
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)]]
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Crystal data top
(C4H9FN)2[PbI4] | F(000) = 784 |
Mr = 895.03 | Dx = 2.991 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 13.6842 (5) Å | Cell parameters from 6193 reflections |
b = 8.5302 (3) Å | θ = 2.5–30.5° |
c = 8.9518 (3) Å | µ = 14.70 mm−1 |
β = 107.996 (4)° | T = 293 K |
V = 993.81 (6) Å3 | Block, yellow |
Z = 2 | 0.16 × 0.16 × 0.15 mm |
Data collection top
XtaLAB Synergy R, DW system, HyPix diffractometer | Rint = 0.036 |
ω scans | θmax = 30.8°, θmin = 2.9° |
Absorption correction: multi-scan (CrysAlis PRO; Rigaku OD, 2018) | h = −18→17 |
Tmin = 0.110, Tmax = 0.119 | k = −11→12 |
8813 measured reflections | l = −11→10 |
2537 independent reflections | 6193 standard reflections every 0 reflections |
2191 reflections with I > 2σ(I) | intensity decay: none |
Refinement top
Refinement on F2 | 24 restraints |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.032 | H-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 reflections | Δρmax = 1.41 e Å−3 |
79 parameters | Δρmin = −1.63 e Å−3 |
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 | x | y | z | Uiso*/Ueq | |
Pb1 | 0.0000 | 0.5000 | 0.0000 | 0.03910 (10) | |
I1 | 0.04490 (4) | 0.30746 (5) | 0.32397 (4) | 0.05175 (13) | |
I3 | 0.23936 (4) | 0.57359 (6) | 0.08670 (5) | 0.06083 (15) | |
N1 | 0.2047 (5) | 0.5207 (8) | 0.6732 (8) | 0.0659 (17) | |
H1A | 0.1482 | 0.4862 | 0.6013 | 0.099* | |
H1B | 0.1956 | 0.5189 | 0.7673 | 0.099* | |
H1C | 0.2177 | 0.6184 | 0.6501 | 0.099* | |
F1 | 0.4838 (6) | 0.3014 (11) | 0.6462 (13) | 0.165 (4) | |
C1 | 0.2927 (7) | 0.4184 (11) | 0.6745 (11) | 0.078 (2) | |
H1D | 0.2767 | 0.3069 | 0.6791 | 0.117* | |
C2 | 0.3934 (9) | 0.4616 (16) | 0.7896 (12) | 0.101 (3) | |
H2A | 0.4172 | 0.3880 | 0.8758 | 0.151* | |
H2B | 0.3959 | 0.5683 | 0.8282 | 0.151* | |
C3 | 0.4441 (10) | 0.4411 (17) | 0.6632 (15) | 0.107 (3) | |
H3A | 0.4891 | 0.5288 | 0.6579 | 0.129* | |
C4 | 0.3406 (9) | 0.4540 (17) | 0.5475 (13) | 0.107 (3) | |
H4A | 0.3267 | 0.3752 | 0.4655 | 0.128* | |
H4B | 0.3248 | 0.5581 | 0.5029 | 0.128* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Pb1 | 0.0509 (2) | 0.03570 (16) | 0.03248 (15) | −0.00137 (11) | 0.01549 (12) | 0.00018 (10) |
I1 | 0.0702 (3) | 0.0445 (2) | 0.0418 (2) | 0.00003 (18) | 0.01929 (18) | 0.01497 (15) |
I3 | 0.0558 (3) | 0.0680 (3) | 0.0569 (3) | −0.0057 (2) | 0.0148 (2) | −0.0059 (2) |
N1 | 0.058 (4) | 0.074 (4) | 0.067 (4) | 0.005 (3) | 0.022 (3) | −0.010 (3) |
F1 | 0.096 (5) | 0.137 (6) | 0.248 (9) | 0.047 (5) | 0.035 (5) | −0.035 (6) |
C1 | 0.073 (5) | 0.078 (5) | 0.081 (5) | −0.001 (4) | 0.020 (4) | −0.005 (4) |
C2 | 0.078 (7) | 0.154 (10) | 0.073 (6) | −0.021 (7) | 0.026 (5) | −0.006 (6) |
C3 | 0.104 (7) | 0.110 (7) | 0.114 (7) | −0.005 (6) | 0.043 (6) | −0.017 (6) |
C4 | 0.102 (7) | 0.147 (7) | 0.081 (5) | 0.029 (6) | 0.042 (5) | 0.004 (5) |
Geometric parameters (Å, º) top
Pb1—I3i | 3.1865 (5) | F1—C3 | 1.338 (14) |
Pb1—I3 | 3.1865 (5) | C1—C2 | 1.489 (14) |
Pb1—I1ii | 3.2151 (4) | C1—C4 | 1.509 (13) |
Pb1—I1iii | 3.2151 (4) | C1—H1D | 0.9800 |
Pb1—I1 | 3.2225 (3) | C2—C3 | 1.509 (16) |
Pb1—I1i | 3.2225 (3) | C2—H2A | 0.9700 |
I1—Pb1iv | 3.2152 (4) | C2—H2B | 0.9700 |
N1—C1 | 1.483 (11) | C3—C4 | 1.477 (16) |
N1—H1A | 0.8900 | C3—H3A | 0.9800 |
N1—H1B | 0.8900 | C4—H4A | 0.9700 |
N1—H1C | 0.8900 | C4—H4B | 0.9700 |
| | | |
I3i—Pb1—I3 | 180.0 | N1—C1—C4 | 114.6 (9) |
I3i—Pb1—I1ii | 93.302 (12) | C2—C1—C4 | 86.9 (8) |
I3—Pb1—I1ii | 86.698 (12) | N1—C1—H1D | 112.4 |
I3i—Pb1—I1iii | 86.698 (12) | C2—C1—H1D | 112.4 |
I3—Pb1—I1iii | 93.302 (12) | C4—C1—H1D | 112.4 |
I1ii—Pb1—I1iii | 180.000 (16) | C1—C2—C3 | 89.7 (8) |
I3i—Pb1—I1 | 90.838 (12) | C1—C2—H2A | 113.7 |
I3—Pb1—I1 | 89.162 (13) | C3—C2—H2A | 113.7 |
I1ii—Pb1—I1 | 90.753 (5) | C1—C2—H2B | 113.7 |
I1iii—Pb1—I1 | 89.247 (5) | C3—C2—H2B | 113.7 |
I3i—Pb1—I1i | 89.163 (13) | H2A—C2—H2B | 110.9 |
I3—Pb1—I1i | 90.837 (12) | F1—C3—C4 | 108.8 (11) |
I1ii—Pb1—I1i | 89.246 (5) | F1—C3—C2 | 119.1 (13) |
I1iii—Pb1—I1i | 90.754 (5) | C4—C3—C2 | 87.3 (9) |
I1—Pb1—I1i | 180.0 | F1—C3—H3A | 113.0 |
Pb1iv—I1—Pb1 | 147.634 (15) | C4—C3—H3A | 113.0 |
C1—N1—H1A | 109.5 | C2—C3—H3A | 113.0 |
C1—N1—H1B | 109.5 | C3—C4—C1 | 90.2 (9) |
H1A—N1—H1B | 109.5 | C3—C4—H4A | 113.6 |
C1—N1—H1C | 109.5 | C1—C4—H4A | 113.6 |
H1A—N1—H1C | 109.5 | C3—C4—H4B | 113.6 |
H1B—N1—H1C | 109.5 | C1—C4—H4B | 113.6 |
N1—C1—C2 | 115.8 (9) | H4A—C4—H4B | 110.9 |
| | | |
N1—C1—C2—C3 | −133.9 (10) | F1—C3—C4—C1 | 101.7 (11) |
C4—C1—C2—C3 | −18.0 (10) | C2—C3—C4—C1 | −18.1 (10) |
C1—C2—C3—F1 | −91.7 (13) | N1—C1—C4—C3 | 135.4 (9) |
C1—C2—C3—C4 | 18.4 (10) | C2—C1—C4—C3 | 18.4 (10) |
Symmetry codes: (i) −x, −y+1, −z; (ii) x, −y+1/2, z−1/2; (iii) −x, y+1/2, −z+1/2; (iv) −x, y−1/2, −z+1/2. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
C2—H2B···F1v | 0.97 | 2.55 | 3.308 (13) | 135 |
N1—H1A···I1 | 0.89 | 2.88 | 3.693 (7) | 152 |
N1—H1B···I3vi | 0.89 | 2.77 | 3.612 (7) | 158 |
N1—H1C···I3vii | 0.89 | 2.72 | 3.609 (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. |