Publication date: 21st July 2025
Chiral organic–inorganic hybrid metal halides are emerging as a promising class of materials for spin-controlled optical and optoelectronic applications. Their lattice chirality can be tuned via the incorporation of enantiopure organic cations.1-3 However, materials crystallizing in enantiomorphic space groups, where the R- and S-configured structures are non-superimposable mirror images, remain rare. In my talk, I will present novel chiral zero-dimensional (0D) (R-/S-MBA)₂SnBr₆ (MBA = methylbenzylammonium) crystals with enantiomorphic helical space groups P6₅ (M-helix) and P6₁ (P-helix). The helicity of the inorganic framework arises from 60° helical rotational alignment along the six-fold screw axis, stabilized by strong N–H···Br and C–H···π interactions. This cooperative assembly induces long-range chirality in the lattice, supported by DFT calculations showing strong electronic coupling between MBA ligands and SnBr₆²⁻ units. The chiral crystals and thin films exhibit mirrored circular dichroism (CD) spectra with a relatively high gCD factor of 3.5 × 10⁻². Interestingly, the crystals does not the Cotton effect a rare phenomenon in chiral metal halides. Additionally, the materials demonstrate broadband second harmonic generation (SHG) from 875 to 1200 nm, with a dissymmetry factor (gCP–SHG) up to 0.44 under 1030 nm excitation. Alloying with Pb induces a structural transition to a non-helical chiral space group (P2₁2₁2₁), highlighting that helicity is intrinsic to specific metal–halide combinations. These results introduce a new family of chiral halides with unique linear and nonlinear optical activity, opening exciting opportunities in spin-optoelectronics and chiroptical photonics.
Figure 1. Helical crystal structures of (R-/S-MBA)₂SnBr₆ viewed along the b-axis. Blue helices are guides to the eye, illustrating the continuous propagation of chirality throughout the lattice. |
Keywords:
Chiral metal halides, enantiomorphic space group, helical framework, circular dichroism, second harmonic generation
This work has received funding from the Spanish Agencia Estatal de Investigación (AEI/MCIN) through grants: TED2021-131628A-I00, CNS2022-135531 and PID2023-147567NB-I00, funded by MICIU/AEI/10.13039/501100011033 and European Union Next Generation EU/PRTR.