Crystal structures of isotypic poly[bis(benzimidazolium) [tetra-μ-iodido-stannate(II)]] and poly[bis(5,6-difluorobenzimidazolium) [tetra-μ-iodido-stannate(II)]]
Abstract:The isostructural title compounds, {(C7H7N2)2[SnI4]}n, (1), and {(C7H5F2N2)2[SnI4]}n, (2), show a layered perovskite-type structure composed of anionic {[SnI4]2−}nsheets parallel to (100), which are decorated on both sides with templating benzimidazolium or 5,6-difluorobenzimidazolium cations, respectively. These planar organic heterocycles mainly form N—H...I hydrogen bonds to the terminal I atoms of the corner-sharing [SnI6] octahedra (point group symmetry 2) from the inorganic layer, but not to the bridging… Show more
“…The 1D "perovskitoids" 44 (which refers to exclusively facesharing ABX 3 compounds) (hep)PbBr 3 and (hex)PbBr 3 belong to the common CsNiBr 3 structure-type, 45 with face-sharing polymeric [PbBr 3 ]chains ( Figure 2). [46][47][48][49][50][51][52][53][54] Usually, a bulky cationic template, which is capable of separating the inorganic sections far apart, will lead to the formation of such low dimensional structure type. 44,55 (hep)PbBr 3 and (hex)PbBr 3 crystallize in non-centrosymmetric monoclinic space groups Cc and P2 1 , respectively.…”
Hybrid organic-inorganic halide perovskites are under intense investigations because of their astounding physical properties and promises for optoelectronics. Lead bromide and chloride perovskites exhibit intrinsic white-light emission believed to arise from self-trapped excitons (STEs). Here, we report a series of new structurally diverse hybrid lead bromide perovskites that have broad-band emission at room temperature. They feature Pb/Br structures which vary from 1D face-sharing structures to 3D corner- and edge-sharing structures. Through single-crystal X-ray diffraction and low-frequency Raman spectroscopy, we have identified the local distortion level of the octahedral environments of Pb within the structures. The band gaps of these compounds range from 2.92 to 3.50 eV, following the trend of "corner-sharing < edge-sharing < face-sharing". Density functional theory calculations suggest that the electronic structure is highly dependent on the connectivity mode of the PbBr octahedra, where the edge- and corner-sharing 1D structure of (2,6-dmpz)PbBr exhibits more disperse bands and smaller band gap (2.49 eV) than the face-sharing 1D structure of (hep)PbBr (3.10 eV). Using photoemission spectroscopy, we measured the energies of the valence band of these compounds and found them to remain almost constant, while the energy of conduction bands varies. Temperature-dependent PL measurements reveal that the 2D and 3D compounds have narrower PL emission at low temperature (∼5 K), whereas the 1D compounds have both free exciton emission and STE emission. The 1D compound (2,6-dmpz)PbBr has the highest photoluminescence quantum yield of 12%, owing to its unique structure that allows efficient charge carrier relaxation and light emission.
“…The 1D "perovskitoids" 44 (which refers to exclusively facesharing ABX 3 compounds) (hep)PbBr 3 and (hex)PbBr 3 belong to the common CsNiBr 3 structure-type, 45 with face-sharing polymeric [PbBr 3 ]chains ( Figure 2). [46][47][48][49][50][51][52][53][54] Usually, a bulky cationic template, which is capable of separating the inorganic sections far apart, will lead to the formation of such low dimensional structure type. 44,55 (hep)PbBr 3 and (hex)PbBr 3 crystallize in non-centrosymmetric monoclinic space groups Cc and P2 1 , respectively.…”
Hybrid organic-inorganic halide perovskites are under intense investigations because of their astounding physical properties and promises for optoelectronics. Lead bromide and chloride perovskites exhibit intrinsic white-light emission believed to arise from self-trapped excitons (STEs). Here, we report a series of new structurally diverse hybrid lead bromide perovskites that have broad-band emission at room temperature. They feature Pb/Br structures which vary from 1D face-sharing structures to 3D corner- and edge-sharing structures. Through single-crystal X-ray diffraction and low-frequency Raman spectroscopy, we have identified the local distortion level of the octahedral environments of Pb within the structures. The band gaps of these compounds range from 2.92 to 3.50 eV, following the trend of "corner-sharing < edge-sharing < face-sharing". Density functional theory calculations suggest that the electronic structure is highly dependent on the connectivity mode of the PbBr octahedra, where the edge- and corner-sharing 1D structure of (2,6-dmpz)PbBr exhibits more disperse bands and smaller band gap (2.49 eV) than the face-sharing 1D structure of (hep)PbBr (3.10 eV). Using photoemission spectroscopy, we measured the energies of the valence band of these compounds and found them to remain almost constant, while the energy of conduction bands varies. Temperature-dependent PL measurements reveal that the 2D and 3D compounds have narrower PL emission at low temperature (∼5 K), whereas the 1D compounds have both free exciton emission and STE emission. The 1D compound (2,6-dmpz)PbBr has the highest photoluminescence quantum yield of 12%, owing to its unique structure that allows efficient charge carrier relaxation and light emission.
“…What effectively determines this crystallographic cut is the size and shape of the spacer cation. Cations employed for this purpose to date include, but not limited to, ammonium, 1,6,[12][13][14][15] amidinium, [16][17] imidazolium 18 and phosphonium 19 ions. Among the <100> perovskites, the Ruddlesden-Popper (RP) perovskites, [20][21] are by far the most common structural type with less common types being the Dion-Jacobson (DJ), [22][23] and Aurivillius (AV) [24][25][26] phases both of which finding paradigms only in oxide perovskite families.…”
We present the new
homologous series (C(NH2)3)(CH3NH3)
n
Pb
n
I3n+1 (n = 1, 2, 3)
of layered 2D perovskites. Structural characterization
by single-crystal X-ray diffraction reveals that these compounds adopt
an unprecedented structure type, which is stabilized by the alternating
ordering of the guanidinium and methylammonium cations in the interlayer
space (ACI). Compared to the more common Ruddlesden–Popper
(RP) 2D perovskites, the ACI perovskites have a different stacking
motif and adopt a higher crystal symmetry. The higher symmetry of
the ACI perovskites is expressed in their physical properties, which
show a characteristic decrease of the bandgap with respect to their
RP perovskite counterparts with the same perovskite layer thickness
(n). The compounds show a monotonic decrease in the
optical gap as n increases: E
g = 2.27 eV for n = 1 to E
g = 1.99 eV for n = 2 and E
g = 1.73 eV for n = 3, which show slightly
narrower gaps compared to the corresponding RP perovskites. First-principles
theoretical electronic structure calculations confirm the experimental
optical gap trends suggesting that the ACI perovskites are direct
bandgap semiconductors with wide valence and conduction bandwidths.
To assess the potential of the ACI perovskites toward solar cell applications,
we studied the (C(NH2)3)(CH3NH3)3Pb3I10 (n = 3) compound. Compact thin films from the (C(NH2)3)(CH3NH3)3Pb3I10 compound with excellent surface coverage can be obtained
from the antisolvent dripping method. Planar photovoltaic devices
from optimized ACI perovskite films yield a power-conversion-efficiency
of 7.26% with a high open-circuit voltage of ∼1 V and a striking
fill factor of ∼80%.
“…Representations of the crystal structures of the two‐dimensional perovskites Bn 2 SnI 4 and BdiSnI 4 are shown in Figure . Single crystals/powders were obtained by reacting tin iodide with the corresponding organic salt in concentrated hydroiodic acid as reported previously . It is worth mentioning, that structural analogues with Pb could be obtained in a similar way using PbI 2 .…”
Section: Selection Of Lead‐free Perovskites Reported In Literaturementioning
Organic‐inorganic hybrid perovskites have attracted great attention over the last few years as potential light‐harvesting materials for efficient and cost‐effective solar cells. However, the use of lead iodide in state‐of‐the‐art perovskite devices may demonstrate an obstacle for future commercialization due to toxicity of lead. Herein we report on the synthesis and characterization of low dimensional tin‐based perovskites. We found that the use of symmetrical imidazolium‐based cations such as benzimidazolium (Bn) and benzodiimidazolium (Bdi) allow the formation of 2D perovskites with relatively narrow band gaps compared to traditional ‐NH3+ amino groups, with optical band gap values of 1.81 eV and 1.79 eV for Bn2SnI4 and BdiSnI4 respectively. Furthermore, we demonstrate that the optical properties in this class of perovskites can be tuned by formation of a quasi 2D perovskite with the formula Bn2FASn2I7. Additionally, we investigate the change in band gap in the mixed Sn/Pb solid solution Bn2SnxPbx−1I4. Devices fabricated with Bn2SnI4 show promising efficiencies of around 2.3 %.
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