Antimony(+5) insertion induces both electron-rich and electron-poor parts within the porphyrin structure resulting in a push–pull style intramolecular charge transfer.

Emissive covalent organic frameworks (COFs) have recently emerged as next-generation porous materials with attractive properties such as tunable topology, porosity, and inherent photoluminescence. Among the different types of COFs, substoichiometric frameworks (so-called Type III COFs) are especially attractive due to the possibility of not only generating unusual topology and complex pore architectures but also facilitating the introduction of well-defined functional groups at precise locations for desired functions. Herein, the first example of a highly emissive (PLQY 6.8%) substoichiometric 2D-COF (COF-SMU-1) featuring free uncondensed aldehyde groups is reported. In particular, COF-SMU-1 features a dual-pore architecture with an overall bex net topology, tunable emission in various organic solvents, and distinct colorimetric changes in the presence of water. To gain further insights into its photoluminescence properties, the charge transfer, excimer emission, and excited state exciton dynamics of COF-SMU-1 are investigated using femtosecond transient absorption spectroscopy in different organic solvents. Additionally, highly enhanced atmospheric water-harvesting properties of COF-SMU-1 are revealed using FT-IR and water sorption studies.The findings will not only lead to in-depth understanding of structure-property relationships in emissive COFs but also open new opportunities for designing COFs for potential applications in solid-state lighting and water harvesting.

To study the photophysical and redox properties as a function of meso-aryl units, a series of hypervalent phosphorus­(V) porphyrins, PP­(OMe)2·PF6, PMP­(OMe)2·PF6, PDMP­(OMe)2·PF6, P345TMP­(OMe)2·PF6, and P246TMP­(OMe)2·PF6, with phenyl (P), 4-methoxyphenyl (MP), 3,5-dimethoxyphenyl (DMP), 3,4,5-trimethoxyphenyl (345TMP), and 2,4,6-trimethoxyphenyl (246TMP) units, respectively, have been synthesized. The P­(+5) in the cavity makes the porphyrin ring electron-poor, whereas the methoxy groups make the meso-phenyl rings electron-rich. The presence of electron-rich and electron-poor portions within the porphyrin molecule promoted an intramolecular charge transfer (ICT). Also, the study suggests that the ICT depends on the number and position of the methoxy groups. The ICT is more prominent in m-methoxy-substituted phosphorus­(V) porphyrins (PDMP­(OMe)2.PF6, P345TMP­(OMe)2·PF6) and almost no ICT was found in no-methoxy, o-methoxy, and/or p-methoxy phosphorus­(V) porphyrins (PP­(OMe)2·PF6, PMP­(OMe)2·PF6, P246TMP­(OMe)2·PF6). Transient absorption studies indicate that the ICT takes place on the picosecond time scale. The most striking results come from P246TMP­(OMe)2·PF6, where each phenyl ring carries three methoxy units, like the P345TMP­(OMe)2·PF6, but it failed to induce the ICT process. Electrochemical studies and time-dependent density functional theory (TD-DFT) calculations were used to support the experimental results. This study extensively explores why and how slight variations in meso-aryl substitutions lead to intricate changes in the photophysical and redox properties of phosphorus­(V) porphyrins.

Copper and silver tritolylcorroles (TTC) are symmetrically functionalized to carry two tetracyanobutadiene (TCBD) entities via [2 + 2] cycloaddition-retroeletrocyclization reaction involving ethynyl functionalized corroles with an electron acceptor, tetracyanoethylene (TCNE) in excellent yields, as the first examples of corrole-TCBD push-pull systems. The strong push-pull effect resulted in charge polarization in the ground state resulting in a considerable hypsochromic shift of the spectrum extending it into the near-IR region. Electrochemical studies coupled with computational studies revealed considerable interactions between the two TCBD entities via the corrole π-system and the degree of such interactions was found to depend on the metal ion present in the corrole cavity. Energy considerations suggested charge transfer (CT) from the S 2 or vibrationally hot S 1 state but not the relaxed S 1 state in the case of CuTTC(TCBD) 2 while CT to occur from all these states in the case of AgTTC(TCBD) 2 . Additionally, the high-energy CT states populate the low-lying triplet states. Systematic femtosecond pump-probe studies provided the ultimate proof for the occurrence of excited CT as a function of excitation wavelength followed by the efficient population of the triplet states. The present study brings out the significance of charge transfer in efficiently populating the triplet states in rather unusual copper and silver corroles carrying two TCBD entities.

A series of fluorinated antimony­(V) porphyrins, SbTPP­(OMe)2·PF6, SbTPP­(OTFE)2·PF6, SbT­(4F)­PP­(OMe)2·PF6, SbT­(35F)­PP­(OMe)2·PF6, SbT­(345F)­PP­(OMe)2·PF6, SbT­(4CF3)­PP­(OMe)2·PF6, SbT­(35CF3)­PP­(OMe)2·PF6, and SbT­(35CF3)­PP­(OTFE)2·PF6, have been synthesized with phenyl [P], 4-fluorophenyl [(4F)­P], 3,5-difluorophenyl [(35F)­P], 3,4,5-difluorophenyl [(345F)­P], 4-trifluoromethylphenyl [(4CF3)­P], and 3,5-bis­(trifluoromethyl)­phenyl [(35CF3)­P], in the meso-positions. Additionally, the SbTPP­(OTFE)2·PF6 and SbT­(35CF3)­PP­(OTFE)2·PF6 carry trifluoroethoxy units in their axial-positions. The fluorination on the porphyrin peripherals ranges from zero fluorine atoms in SbTPP­(OMe)2·PF6 to 30 fluorine atoms in SbT­(35CF3)­PP­(OTFE)2·PF6. X-ray crystallography confirmed the structures of the investigated antimony­(V) porphyrins. The absorption spectra depend on the number of fluorine atoms as it is blue-shifted with increasing fluorination. The series also exhibited rich redox chemistry with two reduction processes and one oxidation process. Remarkably, these porphyrins manifested the lowest reduction potentials reported among the main-group porphyrins, which are as low as −0.08 V vs SCE for SbT­(35CF3)­PP­(OTFE)2·PF6. On the contrary, the oxidation potentials were found to be very large, that is equal to 2.20 V vs SCE or even higher for SbT­(4CF3)­PP­(OMe)2·PF6 or SbT­(35CF3)­PP­(OMe)2·PF6 and SbT­(35CF3)­PP­(OTFE)2·PF6, respectively. These unprecedented potentials are due to a combination of two factors: (i) the +5-oxidation state of antimony in the porphyrin cavity and (ii) the presence of the strong electron-withdrawing fluorine atoms on the porphyrin peripherals. Density functional theory (DFT) calculations were used to support the experimental results. The systematic study of antimony­(V) porphyrins, especially their high potentials, make them ideal for the construction of photoelectrodes and excellent electron acceptors for photoelectrochemical cells and artificial photosynthetic systems, respectively, for solar energy conversion and storage applications.