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. 2022 Oct 15;27(20):6926.
doi: 10.3390/molecules27206926.

Chiral Bis(tetrathiafulvalene)-1,2-cyclohexane-diamides

Affiliations

Chiral Bis(tetrathiafulvalene)-1,2-cyclohexane-diamides

Alexandra Bogdan et al. Molecules. .

Abstract

Chiral bis(TTF) diamides have been obtained in good yields (54-74%) from 1,2-cyclohexane-diamine and the corresponding TTF acyl chlorides. The (R,R)-1 and (S,S)-1 enantiomers have been characterized by circular dichroism and the racemic form by single-crystal X-ray diffraction. The neutral racemic bis(TTF)-diamide shows the formation of a pincer-like framework in the solid state, thanks to the intramolecular S···S interactions. The chemical oxidation in a solution using FeCl3 provides stable oxidized species, while the electrocrystallization experiments provided radical cation salts. In particular, single-crystal resistivity measurements on the racemic donor with AsF6- as a counterion demonstrate semiconductor behavior in this material. The DFT and TD-DFT calculations support the structural and chiroptical features of these new chiral TTF donors.

Keywords: DFT calculations; chirality; chiroptical properties; crystal structure determination; magnetic properties; tetrathiafulvalene.

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Conflict of interest statement

The authors declare no conflict of interest. The funders had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript, or in the decision to publish the results.

Figures

Figure 1
Figure 1
Examples of chiral TTF-amides; 1 is described in the present work.
Scheme 1
Scheme 1
Synthesis of compounds 1.
Figure 2
Figure 2
CD (a) and UV-Vis (b) spectra of compound 1 pair of enantiomers. Green line: (S,S) enantiomer, red line: (R,R) enantiomer.
Figure 3
Figure 3
UV-Vis absorption spectra of (rac)-1 during chemical oxidation by successive addition of FeCl3 in DCM at room temperature.
Figure 4
Figure 4
Cyclic voltammogram of (rac)-1 in 0.1 M Bu4NPF6/CH2Cl2, Pt electrode, scan rate 100 mV s−1. The E1/2 values are shown for both reversible peaks.
Figure 5
Figure 5
Asymmetric unit structure of (rac)-1 (a) and top view of molecule A (b).
Figure 6
Figure 6
Packing of (rac)-1 (a) in the ac plane and the intra- and intermolecular S···S short contacts (b).
Figure 7
Figure 7
H bonding interaction between A- and B-type molecules.
Figure 8
Figure 8
View of crystals (a) and the partial structure of (rac)-1 in the radical cation salt with AsF6 (b). The anions were omitted due to insufficient crystallographic data.
Figure 9
Figure 9
Temperature dependence of the electrical resistivity (blue line) for a single crystal of the radical cation salt of (rac)-1 with AsF6. The red line is the fit to the data with a law of the type ρ = ρ0exp(Ea/T).
Figure 10
Figure 10
Equilibrium geometries of the neutral compound (R,R)-1, optimized at the following DFT levels: (a) B3LYP/Def2-SVPD, (b) B3LYP-D3/Def2-SVPD.
Figure 11
Figure 11
Experimental and theoretical (TD-B3LYP/Def2-SVPD) CD and UV-Vis spectra for neutral compound (R,R)-1.
Figure 12
Figure 12
Most relevant frontier MOs involved in the monoelectronic excitations computed for compound (R,R)-1 at the B3LYP/Def2-SVPD level of theory. Brief description of the MOs: HOMO-3 to HOMO: π orbital on the two TTF units; LUMO and LUMO+1: π* orbitals on the two different arms of compound (R,R)-1; LUMO+2 and LUMO+3: σ* orbital on the TTF units.
Figure 13
Figure 13
NTOs computed for the neutral (R,R)-1 enantiomer, describing the following monoelectronic excitations: (a) S0 → S2, (b) S0 → S4, (c) S0 → S13, (d) S0 → S14, (e) S0 → S16 and (f) S0 → S25.

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