 Open Access Article
 Open Access Article
Cătălin C. Anghelab, 
Ioan Stroiaa, 
Alexandra Popa, 
Atilla Bende c, 
Ion Grosua, 
Niculina D. Hădade
c, 
Ion Grosua, 
Niculina D. Hădade *a and 
Jean Roncali*ad
*a and 
Jean Roncali*ad
aBabeș-Bolyai University, Faculty of Chemistry and Chemical Engineering, Department of Chemistry, SOOMCC, 11 Arany Janos str., 400028, Cluj-Napoca, Romania. E-mail: niculina.hadade@ubbcluj.ro
bUniversity of Bucharest, Faculty of Chemistry, Department of Organic Chemistry, Biochemistry and Catalysis, Research Centre of Applied Organic Chemistry, 90-92 Panduri Street, RO-050663 Bucharest, Romania
cNational Institute for Research and Development of Isotopic and Molecular Technologies, 67-103 Donath str., Cluj-Napoca, RO-400293, Romania
dGroup Linear Conjugated Systems, Moltech Anjou CNRS, University of Angers, 2Bd lavoisier, 49045 Angers, France. E-mail: jeanroncali@gmail.com
First published on 8th March 2021
We report herein our attempt to synthesize an analog of indacenedithiophene (IDT) based on a tetraphenylhexyl substituted, covalently bridged syn-terthienyl unit. Instead of the expected compound the adopted synthetic route led to the formation of an unexpected, new naphtho[2,3-b]thiophene derivative. The structure of this compound was fully characterized by NMR and HRMS as well as single crystal X-ray diffraction and its electronic properties have been analyzed by UV-vis absorption spectroscopy and cyclic voltammetry. A possible mechanism for the formation of this compound is also proposed on the basis of detailed theoretical investigations.
During the past few years, the strong emergence of non-fullerene electron acceptor materials (NFAs) has generated impressive progress in the efficiency of OPV cells.14–16 Intensive research effort in synthetic chemistry has shown that the most efficient NFAs are built around rigid and planar fused ring systems such as indacenodithiophene (IDT) (Fig. 1) which represents the archetype of this kind of building blocks.17,18 It has been shown already that covalent bridging of terthienyl (3T) into a fully planar syn conformation (B3T, Fig. 1) yields to a considerable reduction of the HOMO–LUMO gap, compared to the free analog, due among other factors to a complete elimination of rotational disorder.19 Based on the structural analogy of IDT and B3T we have undertaken the synthesis of compound 2 (Fig. 1, i.e. the B3T analog of the tetra-phenylhexyl substituted IDT 1), which is the building block generally used for practical syntheses due to its higher solubility.15–18 It was anticipated that the lower resonance energy of thiophene vs. benzene could lead to a new class of NFAs with red-shifted absorption. Such IR absorbing acceptors materials are of high potential interest in the context of transparent OPV cells now actively investigated for possible applications in building integrated photovoltaics (BIPV).20–23
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| Fig. 1 Structure of the indacenodithiophene (IDT) and covalently bridged terthienyl (B3T) skeleton (top) as well as the structure of IDT-based NFA 1 and target B3T-based compound 2. | ||
We report herein an attempt to synthesize compound 2. Although, this attempt remained unsuccessful, the adopted synthetic approach led to the formation of an unexpected, new naphtho[2,3-b]thiophene derivative 3 (Scheme 1). Noteworthy, thiophene-functionalized acenes are known to have good optical and electronic properties and also found applications as active materials in opto-electronic devices.24,25 However, to date, there is a limited number of synthetic methods available to build naphtho[2,3-b]thiophene skeleton that usually involve multi-step synthesis.26,27 Therefore, we considered of interest to investigate the structure and properties of this new derivative.
The structure of 3 was clearly identified from 1H-, 13C- and 2D-NMR spectra (Fig. 3 and ESI†) as well as HRMS and single crystal X-ray diffraction. The formation of compound 3 could be explained through the mechanism proposed in Scheme 2: protonation of the tertiary alcohol, elimination of water followed by electrophilic aromatic substitution of the thiophene proton from the closest position to obtain intermediate III. Next, we propose formation of the tertiary, benzyl carbocation IV-a, similar to cation I formed in the first step of the mechanism. However, most probably because of the steric hindrance, instead of the expected electrophilic aromatic substitution of the thiophene ring, the attack does not occur directly onto the carbocation but in the ortho position of one of the phenyl groups (transformation IV-a → V-a). Finally, elimination of the proton afforded compound 3.
In order to gain more insights into the mechanism of formation of compound 3 and to explain the outcome of the cyclization reaction (see Scheme S1 in ESI† for the proposed mechanism for the formation of compound 2), a DFT computational study of the electrophilic aromatic substitution in IV (Scheme 2) has been performed. Since the mechanism involves several reaction steps, our theoretical investigation limits to the description of the IV → V steps, where the structure III already lost the hydroxyl group. Accordingly, the total charge of the systems IV and V was set +1e.
Theoretical calculations results seem to confirm the experimental findings indicating that both activation and reaction enthalpy favor the formation of 3 vs. 2. Thus, intermediate IV was found to display two minima, IV-a (local minimum) and IV-b (global minimum) with only 1.33 kcal mol−1 enthalpy difference (Fig. 2 and Table S1 in ESI.†). Starting from IV-a or IV-b the reaction mechanism can follow two different pathways for the electrophilic substitution step yielding to V-a or V-b, intermediates in the obtaining of 3 and 2 respectively, with activation enthalpy of 24.33 kcal mol−1 and 26.52 kcal mol−1 respectively (Fig. 2). Moreover, calculated global enthalpies for the transformation 7 to 3 and 7 to 2 (see Table S2†), are also in agreement with experimental results, indicating 16.33 lower conformational energy for 3 than 2.
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| Fig. 2 Calculated relative enthalpies profile (298.15 K; 1 atm) for the proposed electrophilic aromatic substitution step in intermediates IV-a and IV-b yielding to 3 (left) and 2 (right). Absolute and relative enthalpies of the intermediates and transition states are given in ESI, (Table S1†). | ||
Careful analysis of 1D and 2D NMR spectra of 3 was in agreement with the formation of a single diastereoisomer. The double bond was found to be in Z configuration as inferred by ROESY-NMR (i.e. correlation between the signal corresponding to Halkene at 7.34 ppm and aromatic protons of ring B at 7.59 ppm, see also Fig. S20†). In addition, 1H-NMR spectrum of 3 (Fig. 3 and S16†), recorded in CD2Cl2, at room temperature, correspond to a rigid structure where the rotation of naphtho[2,3-b]thienyl unit and phenylene ring A is hindered as proved by the heterotopicity of the phenylene groups B and C (signals at 7.59, 7.39 and 7.25 ppm) as well as the diastereotopicity of the protons corresponding to phenylene ring A that give 4 signals at 7.48, 7.39, 7.34 and 7.30 ppm. These data suggest that compound 3 is obtained as a mixture of enantiomers (i.e. atropisomers) formed as result of the hindered rotation of naphtho[2,3-b]thienyl unit. Moreover, the diasteropicity of the protons belonging to ring A is in agreement with a hindered rotation of this unit too. Indeed, the calculated energy for the rotation around the single bond that connect aromatic ring A and naphtho[2,3-b]thienyl unit was found 17.33 kcal mol−1 (see Fig. S3 in ESI†)
Crystals of 3 suitable for single-crystal X-ray diffraction were obtained by slow evaporation from a mixture of DCM and MeCN. The diastereoselective formation of Z isomer of 3 was also confirmed in solid state by single crystal X-ray diffraction (Fig. 4, top). The structure is stabilized by intramolecular edge-to-face interaction between naphtho[2,3-b]thienyl unit and a phenyl ring (i.e. distance from C–H(35) to centroid of phenyl ring is 3.66 Å and the angle between naphtho[2,3-b]thienyl and phenyl units about 75°) and C–H⋯S interaction (i.e. distance C–H(7)–S(3) of 2.83 Å).
Examination of the crystal lattice revealed several interesting features. The enantiomers of 3 forms, by enantioselective recognition, infinite chains through C–H![[dash dash, graph caption]](https://www.rsc.org/images/entities/char_e091.gif) S
S![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif) C interactions (i.e. distance C–H(4) to S(2) is 2.81 Å) as well as hydrophobic interactions between hexyl groups. Two such chains containing the opposite enantiomers are connected through C–H
C interactions (i.e. distance C–H(4) to S(2) is 2.81 Å) as well as hydrophobic interactions between hexyl groups. Two such chains containing the opposite enantiomers are connected through C–H![[dash dash, graph caption]](https://www.rsc.org/images/entities/char_e091.gif) π interactions (distance C–H(16) to centroid 2.77 Å) (Fig. 4, bottom). 3D packing of the crystals (Fig. S1†) displayed double-layer chains of opposite enantiomers connected by hydrophobic interactions between hexyl groups.
π interactions (distance C–H(16) to centroid 2.77 Å) (Fig. 4, bottom). 3D packing of the crystals (Fig. S1†) displayed double-layer chains of opposite enantiomers connected by hydrophobic interactions between hexyl groups.
The optical and electrochemical properties of compound 3 were investigated by absorption and emission spectroscopy as well as cyclic voltammetry. The absorption properties of 3 were determined in dichloromethane solution. The UV-vis absorption spectrum of 3 displays three bands at 273 nm, 370 nm and 516 nm with molecular extinction coefficients of 4.06 × 104, 2.25 × 104 and 4.71 × 103, respectively. Surprisingly, compound 3 does not show any significant emission bands when excited with the absorption maxima wavelength.
Theoretical calculations were also performed in order to assign the observed absorption bands. The experimental and theoretical UV-vis absorption spectra, as well as the electronic excited states are presented in Fig. 5. Theoretical calculations have revealed that the first, relatively broad band from the experimental spectrum, at 519 nm is given by the second electronic excited state (S2). One should mention that the first excited state (S1 = 684 nm) has a very small oscillator strength, thus its peak is missing from the spectrum. The second band from the experimental spectrum around 370 nm is the contribution of the third and fourth electronic excited states with absorption wavelengths of 368 nm and 361 nm. The spectral range of 300–350 nm includes eight further excited states, but their oscillator strengths are weaker so they give only a shoulder to this band. The third, narrow but intense band in the experimental spectrum around 273 nm is the contribution of several higher level electronic excited states. In order to get more details about the nature of the electronic excited states the natural difference orbitals based on the difference density between ground and excited states was also computed for the S2, S3 and S4 electronic states (Fig. 5, top). Analyzing the orbitals shapes, one can conclude that S2 covers the so-called charge-transfer excitation from the naphtho[2,3-b]thienyl unit to the thiophene and C![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif) S fragments, S3 is a mixture of local and charge-transfer excitations effects where mainly the naphtho[2,3-b]thienyl unit and the C
S fragments, S3 is a mixture of local and charge-transfer excitations effects where mainly the naphtho[2,3-b]thienyl unit and the C![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif) S fragment are involved, while S4 shows only a local excitation character. From the charge separation point of view S2 and S3 show the most proper behavior as they allow efficient charge separation induced by the photon absorption.
S fragment are involved, while S4 shows only a local excitation character. From the charge separation point of view S2 and S3 show the most proper behavior as they allow efficient charge separation induced by the photon absorption.
The electrochemical properties of 3 were analyzed in acetonitrile/DCM = 8/2 (v/v) as the solvent, using 0.10 M tetra-n-butylammoniumhexafluorophosphate as the supporting electrolyte (Fig. 5, bottom). The CV traces indicate two successive oxidation processes with anodic peak potentials at 0.94 and 1.35 V tentatively assigned to the cation radical and di-cation of the phenyl-naphtothiophene block respectively. The cathodic wave observed at 0.40 V in the reverse scan suggests the reduction of a product of degradation of the highest oxidized state. The negative potential region displays a reversible reduction process corresponding to the formation of a radical-anion with a cathodic peak potential at −1.15 V. The energy levels of the frontier orbitals of compound 5 (EHOMO = −5.85 eV and ELUMO = −3.94 eV) were calculated from the onset of oxidation and reduction potential, respectively.
In order to calculate the theoretical UV-vis absorption spectrum of 3, the electronic excited states were computed in the framework of density functional theory considering the M06-2X32 exchange-correlation functional and the def2-TZVP33 basis set as is implemented in the Orca34,35 software package. The molecular graphics were created using the Avogadro36 molecular editor and visualizer software. The first 30 excited states were calculated, considering the dichloromethane as the solvent environment. For better comparison with the measured UV-vis absorption spectra, a scaling factor of 1.12 was used for the energy value of each electronic excited state. ESI crystallographic data for this paper, CCDC 2045572.†
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) H2O = 4
H2O = 4![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1, when a white-yellowish solid (0.44 g, 55%) is obtained. 1H-APT-NMR (400 MHz, MeOH-d4)δ (ppm): 7.43 (d, 1H, 3J = 5.8 Hz, HAr), 7.36 (d, 1H, 3J = 5.8 Hz, HAr). 13C-NMR (100 MHz, MeOH-d4) δ (ppm): 164.9, 133.1, 130.6, 127.6, 120.4.
1, when a white-yellowish solid (0.44 g, 55%) is obtained. 1H-APT-NMR (400 MHz, MeOH-d4)δ (ppm): 7.43 (d, 1H, 3J = 5.8 Hz, HAr), 7.36 (d, 1H, 3J = 5.8 Hz, HAr). 13C-NMR (100 MHz, MeOH-d4) δ (ppm): 164.9, 133.1, 130.6, 127.6, 120.4.![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) petroleum ether = 1
petroleum ether = 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 8, Rf = 0.62), when a brownish liquid (0.34 g, 80%) is obtained. 1H-NMR (600 MHz, CDCl3) δ (ppm): 7.36 (d, 1H, 3J = 5.8 Hz, HAr), 7.22 (d, 1H, 3J = 5.8 Hz, HAr), 3.88 (s, 3H, CH3). 13C-APT-NMR (150 MHz, CDCl3) δ (ppm): 162.6, 131.1, 129.5, 126.0, 120.1, 52.1.
8, Rf = 0.62), when a brownish liquid (0.34 g, 80%) is obtained. 1H-NMR (600 MHz, CDCl3) δ (ppm): 7.36 (d, 1H, 3J = 5.8 Hz, HAr), 7.22 (d, 1H, 3J = 5.8 Hz, HAr), 3.88 (s, 3H, CH3). 13C-APT-NMR (150 MHz, CDCl3) δ (ppm): 162.6, 131.1, 129.5, 126.0, 120.1, 52.1.![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) petroleum ether = 1
petroleum ether = 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 8, Rf = 0.32), when an orange crystalline solid is obtained (0.23 g, 62%).
8, Rf = 0.32), when an orange crystalline solid is obtained (0.23 g, 62%).
Mp = 90–92 °C,
1H-NMR (600 MHz, CDCl3) δ (ppm): 7.49 (d, 2H, 3J = 5.4 Hz, HAr), 7.41 (s, 2H, HAr), 7.21 (d, 1H, 3J = 5.4 Hz, HAr), 3.85 (s, 3H, OCH3).
13C-APT-NMR (150 MHz, CDCl3) δ (ppm): 163.6, 142.9, 136.2, 130.7, 129.3, 127.7, 124.3, 51.9.
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) petroleum ether = 1
petroleum ether = 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 8, Rf = 0.42), when an orange viscous oil (1.7 g, 70%) is obtained.
8, Rf = 0.42), when an orange viscous oil (1.7 g, 70%) is obtained.
1H-NMR (600 MHz, CD2Cl2) δ (ppm): 7.11 (overlapped signals, 18H, HAr), 6.43 (d, 2H, 3J = 5.4 Hz, HAr), 6.33 (s, 2H, HAr) 3.11 (s, 2H, OH), 2,59 (t, 8H, 3J = 7.7 Hz, CH2), 1.59 (m, 8H, CH2), 1.34–1.27 (overlapped signals, 24H, CH2), 0.87 (t, 12H, 3J = 6.8 Hz, CH3).
13C-APT-NMR (150 MHz, CD2Cl2) δ (ppm): 146.3, 145.2, 142.8, 137.5, 132.0, 131.9, 129.0, 128.4, 127.9, 124.2, 80.7, 36.1, 32.3, 32.0, 29.6, 23.2, 14.4.
ESI(+)-HRMS (m/z): calculated for C62H76O2S3: 971.4900, found 971.4952 [M + Na+]; 1920.9941, found 1921.0020 [2M + Na+].
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) petroleum ether = 1
petroleum ether = 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 4, Rf = 0.44; DCM
4, Rf = 0.44; DCM![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) petroleum ether
petroleum ether![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) Et3N = 1
Et3N = 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 4
4![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 0.05 for the packing of the column), followed by slow crystallization from DCM/EtOH at low temperature, leading to green-yellow needles (80 mg, 10%).
0.05 for the packing of the column), followed by slow crystallization from DCM/EtOH at low temperature, leading to green-yellow needles (80 mg, 10%).
Mp = 154–156 °C, Rf = 0.44 (DCM![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) petroleum ether = 1
petroleum ether = 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 4).
4).
1H-NMR (600 MHz, CD2Cl2) δ (ppm): 7.82 (d, 1H, 3J = 5.0 Hz, HAr), 7.72 (d, 1H, 3J = 8.8 Hz, HAr), 7.59 (d, 2H, 3J = 8.3 Hz, HAr), 7.48 (dd, 1H, 3J = 7.8 Hz, 4J = 1.7 Hz, HAr), 7.39 (overlapped signals, 3H, HAr), 7.35–7.33 (overlapped signals, 3H, HAr), 7.31–7.28 (overlapped signals, 2H, HAr), 7.25 (d, 4H, 3J = 7.2 Hz, HAr), 7.19 (dd, 1H, 3J = 8.8 Hz, 4J = 1.7 Hz, HAr), 7.14 (d, 1H, 3J = 5.0 Hz, HAr), 7.10 (d, 1H, 3J = 5.7 Hz, HAr), 2.74 (t, 2H, 3J = 7.8 Hz, CH2), 2.67–2.62 (overlapped signals, 4H, CH2), 2.59 (t, 2H, 3J = 7.6 Hz, CH2), 1.73 (m, 2H, CH2), 1.67–1.60 (overlapped signals, 4H, CH2), 1.57 (m, 2H, CH2), 1.44 (m, 2H, CH2), 1.40–1.28 (overlapped signals, 22H, CH2), 0.92 (t, 3H, 3J = 7.0 Hz, CH3), 0.90–0.85 (overlapped signals, 9H, CH3). 13C-APT-NMR (150 MHz, CD2Cl2) δ (ppm): 213.3, 165.8, 158.0, 157.9, 143.03, 143.00, 142.8, 142.7, 141.7, 140.7, 139.6, 138.3, 137.2, 136.5, 135.5, 135.2, 131.3, 131.2, 129.8, 129.22, 129.16, 129.15, 128.9, 128.8, 128.5, 127.4, 127.3, 127.1, 125.7, 124.7, 124.5, 123.3, 64.9, 36.7, 36.4, 36.2, 36.1, 32.4, 32.32, 32.31, 32.1, 32.0, 31.6, 29.8, 29.70, 29.65, 29.6, 23.3, 23.24, 23.21, 23.19, 14.5, 14.4. APCI(+)-HRMS (m/z): calculated for C62H72S3: 913.4869, found 913.4832 [M + H+].
| Footnote | 
| † Electronic supplementary information (ESI) available: Experimental procedures, copies of NMR, HRMS and thin-film UV-vis spectra as well as details of theoretical calculations and X-ray diffraction data (PDF). CCDC 2045572. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/d1ra00659b | 
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