Open Access Article
D.
Cvejn
a,
E.
Michail
b,
I.
Polyzos
b,
N.
Almonasy
a,
O.
Pytela
a,
M.
Klikar
a,
T.
Mikysek
c,
V.
Giannetas
b,
M.
Fakis
b and
F.
Bureš
*a
aInstitute of Organic Chemistry and Technology, Faculty of Chemical Technology, University of Pardubice, Studentská 573, Pardubice, 53210, Czech Republic. E-mail: filip.bures@upce.cz; Web: http://bures.upce.cz Fax: +420 46 603 7068; Tel: +420 46 603 7099
bDepartment of Physics, University of Patras, GR-26504, Patras, Greece
cDepartment of Analytical Chemistry, Faculty of Chemical Technology, University of Pardubice, Studentská 573, Pardubice, 53210, Czech Republic
First published on 16th June 2015
A series of twelve tripodal push-pull molecules with a central triphenylamine donor and peripheral cyano substituted acceptors has been prepared. These molecules possess systematically altered π-linkers as well as cyano acceptors. Based on the experimental properties measured by differential scanning calorimetry, electrochemistry, one and two photon absorption/emission spectroscopy, supported by the DFT calculations, thorough structure–property relationships were elucidated.
A joint feature of the most successful organic molecules is their push-pull and mostly tripodal (branched, star-shaped or octupolar) arrangement. In a push-pull D–π–A molecule (D = electron donor, π = conjugated system and A = electron acceptor), an intramolecular charge transfer (ICT) from the donor via the π-system to the acceptor occurs and the molecule becomes polarized and constitutes a dipole. The D–A interaction results in the formation of a new molecular orbital in which facile electron excitation by visible light takes place. Hence, push-pull molecules are also called chromophores.9 Apart from N,N-dialkylamino groups used as ordinary donors in linear D–π–A systems, triphenylamine (TPA) proved to be a very useful and readily available precursor for the synthesis of tripodal molecules. The central amino donor in TPA can easily be connected to various peripheral acceptors to gain D(–π–A)3 push-pull systems. In fact, D(–π–A)3 systems are much thoroughly investigated than inverse A(–π–D)3 molecules10 which is most likely due to their tedious and limited synthesis compared to possible modifications of the parent TPA (Fig. 1).
The vast majority of tripodal molecules have been built on TPA and, since late 90s, an admirable number of articles reporting their preparation and 2PA activity have been published.11 These D(–π–A)3 molecules possess peripheral electron withdrawing groups such as nitro, ester, carbonyl, trifluoromethylsulfonyl etc. as well as (hetero)aromatic moieties such as fluorene, perylene diimide, dimesitylboryl, pyridine/pyridinium, triazole, oxadiazole, benzothiazole, benzothiadiazole and porphyrin. Some dendritic molecules have recently appeared as well.12 Further applications of such TPA-derived push-pull molecules range from 3PA,13 organic solar cells,14 molecular glasses,15 intercalates and metal–organic frameworks (MOF)16 to sensors used for the detection of ions,17 amines18 and explosives.19 In contrast to linear D–π–A systems,9,20 less tripodal compounds bearing peripheral cyano-substituted acceptor moieties were prepared and investigated as 2PA-active substances to date.21 Besides their exceptional 2PA activity, a few cyano-substituted TPA molecules were also utilized in solar cells.22
As only a few comprehensive structure–property relationship studies on tripodal TPA molecules were reported to date23 and as an extension of our recent efforts in the field of property tuning in push-pull molecules,9a we report herein on the design, synthesis and further studies of twelve model D(–π–A)3 molecules 1–12 (Fig. 2). These chromophores possess either one or two cyano groups connected to each particular TPA branch and vary in the arrangement, extension and composition of the π-linker. The impacts of such structural changes on the properties of 1–12 were studied by means of differential scanning calorimetry, electrochemistry, one and two photon absorption spectroscopy and were also supported by DFT calculations.
The synthetic details and spectral characterization of precursors and intermediates 14–25 are given in the ESI.† Target tripodal push-pull molecules 1–12 were obtained by a combination of the aforementioned A- and D-precursors, mainly in terms of cross-coupling reactions as shown in Scheme 3. Threefold cyanation27 of triiodotriphenylamine proved to be tedious and, therefore, chromophore 1 was synthesized from trialdehyde 35 (ref. 4g) by a one-pot reaction with hydroxylamine and subsequent Beckmann rearrangement.28 Chromophore 2 was prepared by Heck–Mizoroki cross-coupling reaction of 13 and acrylonitrile 26 with a similar outcome as described by Tian et al.29 The biphenyl π-linker in chromophore 3 has been generated by the Suzuki–Miyaura reaction between 13 and boronic acid 27 (76%).
A Sonogashira reaction of 13 and terminal acetylene 28 provided chromophore 4 in generally lower yield than reported by Ogilby et al. (69 vs. 94%).5d The synthesis of chromophore 5 has been described by Cho et al. via a Horner–Wadsworth–Emmons reaction.21b However, the Suzuki–Miyaura cross-coupling on 13 using boronic acid pinacol ester 29 delivered 5 in a slightly improved yield of 76%. Al2O3-catalyzed Knoevenagel condensation30 of aldehydes 35/16 and malononitrile 30 afforded smoothly target chromophores 6 and 7 with dicyanovinyl (DCV) moieties in the yields of 42 and 94%. Chromophore 6 has also been previously synthesized by the pyridine/acetic acid-catalyzed condensation in a similar yield.11q,31 Target chromophore 8 bearing peripheral dicyanoimidazole (DCI) acceptor moieties was prepared by Heck–Mizoroki olefination of 13 and vinazene 31. Although carried out under optimized conditions (dioxane, elevated temperature and Pd(0) precatalyst), a Sonogashira reaction of triacetylene 14 and halogenated dinitriles 23 and 24 afforded chromophores 9 and 10 only in modest yields. This reaction was complicated by the predominant formation of one- and two-fold cross-coupling products which were tedious to separate and to suppress even in the case of an excess of 23 and 24. Moreover, a similar Sonogashira reaction with trinitrile 25 proved to be unsuccessful at all, which is most likely caused by the presence of chloro instead of bromo substituents (see above). Cross-coupling reactions with thiophene analogues 32 and 33 afforded chromophores 11 and 12 in similar modest yields of 25 and 16%, respectively.
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| Fig. 3 Representative DSC curves of compounds 2 and 9 determined with a scanning rate of 3 °C min−1 under N2. | ||
| Comp. | T m (°C) | T d (°C) | E 1/2(ox1) (V) | E 1/2(red1) (V) | ΔEc (V) | E HOMO (eV) | E LUMO (eV) | λ Amax (nm eV−1) | λ Fmax (nm eV−1) | Φ F (%) | Stokes shift (cm−1) | δ 2PA (GM) |
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| a T m = melting point (the point of intersection of a baseline before the thermal effect with a tangent). b T d = thermal decomposition (pyrolysis in a N2 atmosphere). c E 1/2(ox1) and E1/2(red1) are half-wave potentials of the first oxidation and reduction, respectively; all potentials are given vs. SCE; ΔE = E1/2(ox1) − E1/2(red1). d Electrode surface inhibition. e −EHOMO/LUMO = E1/2(ox1/red1) + 4.429 (ref. 32). f Measured in THF. g The wavelength of the maximum 2PA cross section is shown in parenthesis (measured in THF). | ||||||||||||
| 1 | 343 | — | 1.49 | −2.01 | 3.50 | −5.92 | −2.42 | 339/3.66 | 377/3.29 | 0.62 | 2970 | — |
| 2 | 275 | 317 | 1.12 | −1.74 | 2.86 | −5.55 | −2.69 | 394/3.15 | 460/2.70 | 0.48 | 3640 | 260 (770) |
| 3 | 329 | 340 | 1.02 | −2.02 | 3.04 | −5.45 | −2.41 | 372/3.33 | 448/2.77 | 0.64 | 4560 | 566 (760) |
| 4 | 217 | — | 1.04 | −1.85 | 2.89 | −5.47 | −2.58 | 387/3.20 | 458/2.71 | 0.59 | 4010 | 785 (780) |
| 5 | 291 | 477 | 0.85 | −1.80 | 2.65 | −5.28 | −2.63 | 403/3.08 | 510/2.43 | 0.51 | 5210 | 1100 (810) |
| 6 | 145 | 322 | 1.41 | —d | — | −5.84 | — | 453/2.74 | 549/2.26 | 0.29 | 3860 | 757 (830) |
| 7 | 84 | 176 | 1.29 | —d | — | −5.72 | — | 470/2.64 | 611/2.03 | 0.29 | 4910 | 667 (810) |
| 8 | 188 | 366 | 0.97 | −1.66 | 2.63 | −5.40 | −2.77 | 413/3.00 | 497/2.49 | 0.59 | 4090 | 620 (810) |
| 9 | 327 | 333 | 1.16 | −1.55 | 2.71 | −5.59 | −2.88 | 420/2.95 | 533/2.33 | 0.69 | 5050 | 852 (810) |
| 10 | — | 282 | 1.15 | −1.44 | 2.59 | −5.58 | −2.99 | 414/3.00 | 499/2.48 | 0.55 | 4126 | 631 (810) |
| 11 | 191 | 240 | 1.09 | −1.45 | 2.54 | −5.52 | −2.98 | 397/3.12 | 475/2.61 | 0.46 | 4140 | 148 (750) |
| 12 | 198 | 252 | 1.17 | −1.41 | 2.58 | −5.60 | −3.02 | 412/3.01 | 516/2.40 | 0.49 | 4890 | 375 (830) |
The measured melting points of 1–12 range from 84 to 343 °C. The temperature of decomposition was estimated within the range of 176–477 °C. Compound 1 provided a very sharp peak of melting/crystallization at 343/263 °C and does not undergo decomposition until its boiling point (436 °C). Thermal behaviour of compounds 2, 3, 5–9 and 11–12 is very similar with the melting point peak followed by a subsequent decomposition at a higher temperature. Compound 4 showed a wide enantiotropic solid–solid transition (37–82 °C), melting point at 217 °C and surprisingly no decomposition peak. However, the sample was clearly carbonized after heating up to 500 °C. For compound 10, thermal decomposition preceded the melting point. As can be seen from the whole series (Table 1), DCV-terminated tripodal compounds 6 and 7 showed the lowest melting points and temperatures of thermal decompositions. TPA derivatives substituted with cyanoaromates 3–5 and 9–10 resisted thermal decomposition above 300 °C. Heterocyclic acceptor moieties such as DCI and (di)cyanothiophene as in 8 and 11–12 bring also noticeable thermal stability up to 366 °C, especially for the imidazole-terminated compound 8. The measured DSC data of compounds 1–12 reflect their different molecular structure (varied peripheral acceptors and π-linkers). The following relations can be deduced from the DSC measurements:
• The melting temperatures within the most evaluated subseries of compounds 1–5 are mostly affected by an insertion of multiple bonds. In general, chromophores bearing triple bond proved less stable than the corresponding olefinic derivatives (e.g.4vs.3 and 5vs.3).
• This can be further demonstrated by the DCV acceptor linked to the TPA core via an acetylenic spacer in 7, which lowered the thermal stability very significantly when compared to 6 (ΔTm = 61 °C, ΔTd = 146 °C).
• Chromophores bearing benzene-derived acceptors (e.g.4 or 9/10) are generally more thermally stable than the corresponding thiophene derivatives (e.g.11 and 12).
• Chromophore 8 with the imidazole-based acceptor (DCI) showed the highest thermal resistance among all heterocyclic compounds (8, 11–12) with Td = 366 °C.
The measured half-wave potentials of the first oxidation and reduction (E1/2(ox1) and E1/2(red1)) of chromophores 1–12 were found within the range of 0.85 to 1.49 and −1.41 to −2.02 V, respectively. The first reduction and oxidation are one-electron processes, followed by subsequent oxidations and reductions, and are obviously a function of the peripheral acceptor and the π-linker (Table 1). Whereas the first oxidation can be attributed to the central TPA donor, the first reduction is mostly localized on the peripheral CN groups and the adjacent π-system. The first oxidation potentials of chromophores 1–5 bearing monocyano-substituted acceptor moieties steadily decreased from 1.49 to 0.85 V as a function of the π-system elongation. The first reduction potentials showed similar trends with exception for 3 in which nonplanar biphenyl π-linker allows only reduced ICT. The difference between the first oxidation and reduction potentials (electrochemical gap, ΔE) represents a straightforward way for the evaluation of the ICT. When going from 1 (ΔE = 3.50 V) to 2 (ΔE = 2.86 V), the electrochemical gap decreased by 0.64 V, as a consequence of the insertion of an additional olefinic subunit. However, further π-system extension as in 3 resulted in an increased gap of 3.04 V. This demonstrates “ICT transparency” of the olefinic unit in comparison to the aromatic 1,4-phenyl moiety.33 Further extension and planarization of the π-linker by acetylenic and olefinic subunits (3vs.4 and 5) lowered the electrochemical gap up to 2.65 V. Dicyano-substituted (hetero)aromatic moieties attached to the TPA core affected both the first oxidation and the reduction potentials (8–12, Table 1). The evaluation of the ICT based on the overall electrochemical gap ΔE implies that these (hetero)aromates impart a stronger resonance effect than aromates (ΔE of 2.71–2.54 vs. 3.50–2.65 V for 1–5vs.8–12). Positioning of the CN groups along the (hetero)aromatic scaffold plays also a significant role as can be seen for instance on chromophores 9 and 10. The latter, 2,4-dicyano-substituted chromophore showed a reduced gap by 0.12 V. The lowest electrochemical gap (ΔE = 2.58 V) was measured for chromophore 11 bearing a cyano-acceptor based on polarizable thiophene with the cyano group attached at the resonant and most extended C5 position (as compared to the dicyano acceptor in 12). A comparison of chromophores 4 and 11 also allows comparison of 1,4-phenylene and 2,5-thienylene π-systems.34 With very similar oxidation potentials (1.04 and 1.09 V), the latter showed significantly lowered first reduction potential (−1.45 vs. −1.85 V) as well as the electrochemical gap (ΔE = 2.89 vs. 2.54 V).
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| Fig. 4 Representative absorption (left) and fluorescence (right) spectra of chromophores 5, 7–9 and 11 measured in THF. | ||
Whereas the absorption maxima range from 339 to 470 nm, the emission maxima are red-shifted to 377–611 nm. The absorption spectra are dominated by one intense CT-band whose position is clearly dependent on the nature of the appended cyano-acceptors and the π-system. When considering the monocyano-substituted series of molecules 1–5, the λAmax values showed a very similar trend as seen for the electrochemical gaps ΔE. Namely, extension of the π-system by olefinic (1vs.2) or aromatic units (3vs. 2), planarization (4/5vs.3) and further elongation by acetylenic subunit (4) affected the absorption maxima within the range of 339 to 403 nm. It should be noted that the longest-wavelength absorption maxima of 1–12 correlate very tightly with the measured electrochemical gap ΔE (see the ESI†). Chromophores 6 and 7 bearing strong electron DCV acceptors showed the most bathochromically shifted CT-bands with λAmax at 453 and 470 nm, respectively. In contrast to 1–5, chromophores 8–10 and 12 exhibited red-shifted absorption maxima up to 412–420 as a result of the appended dicyano-substituted (hetero)aromatic acceptor moieties. However, the differences in λAmax are just within the range of 8 nm, which implies that, in contrast to electrochemical gap, the central (hetero)aromatic π-system and positioning of the CN groups do not affect the absorption properties very significantly.
The fluorescence spectra exhibited one single band with λFmax appearing at 377–611 nm. In general, its position is affected by the same structural features as the aforementioned absorption bands. Both positions of the longest-wavelength absorption and fluorescence maxima showed tight correlations (see the ESI†). The quantum yields lie within the range of 0.29 to 0.69. The lowest quantum yields were measured for chromophores 6 and 7 with strongly electron withdrawing DCV moieties. The weaker (di)cyano acceptors in 1–5 and 8–12 lead generally to blue-shifted emission with a high quantum yield. This is in accordance with our previous observations on linear and X-shaped push-pull molecules with strong or weak ICT.20g,h,33a
The 2PA spectra of all compounds, i.e. the 2PA cross-sections (δ2PA) as a function of excitation wavelength, are shown in Fig. 5. For a better comparison of the 2PA properties, target chromophores 1–12 were split into four groups according to the peripheral acceptor moieties. Whereas the first group includes chromophores 2–5 with monocyano acceptors, chromophores 6 and 7 in the second group possess DCV acceptors. The third and fourth group of molecules consist of dicyano aromatic (9 and 10) and (di)cyano heteroaromatic acceptor moieties (8, 11–12), respectively. In all cases, good 2PA properties were observed with the 2PA cross-section exceeding 1000 GM for compound 5. In general, chromophores 4 and 5 with monocyano acceptors displayed a larger 2PA cross section than the other tripodal molecules in the whole series. Moreover, these two chromophores also exhibited good fluorescence quantum yields (>0.50). The 2PA results are summarized in Table 1.
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| Fig. 5 Two-photon absorption cross-sections, δ2PA, of (a) 2, 3, 4, 5 and 11 (b) 6 and 7 (c) 9 and 10 and (d) 8, 11, 12. All compounds have been measured in THF solutions at 10−4 M concentration. | ||
Fig. 5a compares the 2PA spectra of mono-cyano terminated chromophores 2–5 and 11. Compound 1 showed negligible 2PA cross-section within the investigated spectral area. It was observed that by increasing the length of the π-linker, i.e. passing from 2 to 4 and 5, the 2PA cross sections increased. In addition, it is also obvious that upon changing the acetylenic π-conjugated bridge by an olefinic one (4vs.5), the 2PA cross-sections significantly increased up to 1100 GM (at 810 nm) for 5 while this is 785 GM (at 780 nm) for 4. Since the fluorescence quantum yields of 4 and 5 are similar (Table 1), the 2PA action cross-section product Φ × δTPA is again higher for 5 than for 4. This renders molecule 5 as a promising candidate for up-converted lasing or two-photon imaging. A replacement of the 1,4-phenylene moiety in 4 with 2,5-thienylene one (11) led to more than seven-times decrease of the 2PA cross sections (Table 1, 1100 vs. 148 GM). Hence, heteroaromatic polarizable moiety based on thiophene in 11 did not bring the expected higher 2PA activity. Another conclusion drawn from Fig. 5a is that the peaks of the 2PA spectra appear at approximately twice the wavelengths of the one photon absorption spectra. This is in accordance with the two-photon allowed states for octupolar molecules. Specifically, the 2PA spectrum of 4 is blue-shifted compared to 5 while that of 3 is blue shifted compared to 2 as in the case of their one-photon absorption spectra.
The 2PA spectra of chromophores 6 and 7 bearing the strongest DCV acceptor are shown in Fig. 5b. Chromophore 6 exhibited a large 2PA cross-section of 760 GM at 830 nm. Interestingly, an extension of the π-conjugated path by an additional acetylene subunit as in 7 did not lead to enhanced 2PA cross-sections. The fluorescence quantum yields of 6 and 7 are relatively low making the Φ × δ2PA values significantly smaller than those of compounds 4 and 5. However, it should be noted that, according to their one-photon absorption spectra, the maximum of the 2PA spectra of 6 and 7 is expected at wavelengths close to 900 nm, which are not covered by our experiment. On the other hand, chromophore 6 with a DCV acceptor exhibited much larger 2PA cross-section than structurally related 2, which possesses only one cyano group.
Fig. 5c presents the 2PA cross-sections of 9 and 10 bearing dicyano aromatic acceptors with different orientation of the appended CN groups. The position of the cyano groups played significant role as 9 exhibited an approximately 1.35-times larger 2PA cross-sections compared to 10. Moreover, the fluorescence quantum yield is higher for 9 (0.69) compared to 10 (0.55), which provides 9 a larger Φ × δ2PA value. A comparison of the structurally related chromophores 10 and 4, with di- and monocyano aromatic acceptor moieties, reveals that the second cyano group has broadened and red-shifted the 2PA spectra. This is in accordance with one photon absorption spectra, but, on the other hand, it also causes a decrease of the 2PA response.
Finally, the 2PA cross-sections of chromophores 8, 11 and 12 with (di)cyano-heteroaromatic acceptors are compared in Fig. 5d. Chromophores 11 and 12 with thiophene acceptors exhibited relatively small 2PA cross-section values compared to their analogues 4 and 10 having a phenyl ring. Thus, a replacement of 1,4-phenylene by 2,5-thienylene moieties coupled either to cyano or dicyano groups is not a useful strategy towards increasing the 2PA activity in TPA-derived tripodal chromophores. This is in contrast to general trends observed for second order NLO chromophores.34 However, an addition of the second cyano group into 11 leads to 12 with more than three-times higher 2PA cross-section without affecting the florescence quantum yield. This makes the thiophene substituted chromophores 11 and 12 extremely sensitive to the number of cyano groups. On the other hand, 2PA cross-sections measured for the analogous chromophores 4 and 10 with 1,4-phenylene parent moieties showed less sensitivity. Chromophore 8 bearing three peripheral DCI acceptor units exhibited a relative large 2PA cross-section of 620 GM at 810 nm accompanied by a good quantum yield of 0.59. Although, a straightforward comparison of the 2PA properties of the herein studied compounds with literature data is not easy because of various experimental approaches used (sample concentration, solvent used, pulse duration, laser power, spectral range etc.), chromophores 4 and 5 are found to exhibit similar or better 2PA activity compared with other tri-branched compounds with D(–π–A)3 arrangement and similar molecular weight.11b,h
| Comp. | Symmetry group | E HOMO (eV) | E LUMO (eV) | ΔE (eV) | μ (D) |
|---|---|---|---|---|---|
| a Calculated at the DFT B3LYP/6-311++G(2d,p) level. | |||||
| TPA | D 3 | −5.29 | −0.90 | 4.39 | 0.024 |
| 1 | D 3 | −6.53 | −2.53 | 4.00 | 0.000 |
| 2 | C 3 | −6.14 | −2.90 | 3.24 | 0.227 |
| 3 | D 3 | −5.86 | −2.39 | 3.47 | 0.002 |
| 4 | D 3 | −5.80 | −2.67 | 3.13 | 0.001 |
| 5 | C 3 | −5.62 | −2.75 | 2.87 | 0.221 |
| 6 | C 3 | −6.76 | −3.80 | 2.94 | 5.675 |
| 7 | C 3 | −6.49 | −3.81 | 2.68 | 7.199 |
| 8 | C 3 | −6.30 | −3.01 | 3.29 | 7.603 |
| 9 | D 3 | −5.78 | −2.84 | 2.94 | 0.035 |
| 10 | C 3 | −6.05 | −3.17 | 2.88 | 6.034 |
| 11 | C 3 | −5.81 | −2.82 | 2.99 | 5.199 |
| 12 | C 3 | −6.07 | −3.13 | 2.94 | 11.914 |
The calculated energies of the HOMO/LUMO of 1–12 range from −6.76/−3.81 to −5.62/−2.39 eV and are obviously a function of the structure of the particular chromophore. Both energies correlate tightly with the experimental data obtained by the electrochemical measurements (Table 1). Hence, the used DFT method can be considered as a reasonable tool for the description of electronic properties of 1–12 (see the ESI†). When going from parent TPA to molecule 1, the HOMO–LUMO gap decreased from 4.39 to 4.00 eV as a result of attaching three cyano groups and generating a push-pull system. Further extension of the π-system within the series 1–5 affected the HOMO and LUMO levels as well as the gap in very similar way as observed by the electrochemistry. The lowest HOMO–LUMO gap within this subseries has been calculated for 5 bearing a cyano-substituted styryl linker. Further attachment of an additional CN group (4vs.9 and 10) resulted in drop of the calculated gap from 3.13 to 2.94 and 2.88 eV. DCV acceptors in chromophores 6–7 impart also strong ICT and reduce the gaps up to 2.94 and 2.68 eV, respectively. A replacement of the terminal 1,4-phenylene moiety in 4 by 2,5-thienylene one in 11 slightly decreases the HOMO–LUMO gap from 3.13 to 2.99 eV in a similar way as observed by CV measurements. In general, both experimental and calculated HOMO–LUMO gaps correlate tightly as shown in the ESI.†
The calculated ground state dipole moments are almost zero for molecules having the D3 group of symmetry, whereas noticeable values were obtained for molecules 6–8 and 10–12 having branched and unsymmetrical acceptor moieties (DCV, DCI, 2,4-dicyanobenzene and 5(2,4)-(di)cyanothiophene).
The HOMO and LUMO localizations in representative chromophores 5, 7–9 and 11 are shown in Fig. 6. For complete listing see the ESI.† As expected, the HOMO is localized on the central amino donor and adjacent alternating positions of the TPA, whereas the LUMO is spread over the peripheral cyano acceptor and the adjacent π-linker. Fig. 6 shows a clear charge separation and thus confirms the ICT character of chromophores 1–12. As can be seen, the LUMO is predominantly localized over one or two particular branche(s), while the third branch is occupied by the LUMO+1. The HOMO as well the HOMO−1 remained on the central amino donor. This is a common feature of tripodal molecules based on TPA.23b,c,29
Compounds 1–12 showed melting point and subsequent thermal decomposition within the range of 84–343 and 176–477 °C. These values indicate relatively high thermal resistance of TPA derived tripodal molecules.
The electrochemical properties (HOMO and LUMO levels and gap) were mainly affected by the type of peripheral acceptor, length and composition of the π-linker as well as its planarity. Using these structural changes as a tool, the electrochemical HOMO–LUMO gap could be finely tuned by almost 1 V (3.50 to 2.54 V).
One photon absorption and emission properties studied by electronic absorption/emission spectra revealed significant CT-bands appearing between 339/377 and 470/611 nm. Hence, optical tuning could be carried out within the range of 130/230 nm. Quantum yields ranging from 0.29–0.69 were measured for 1–12.
The two photon absorption properties of 1–12 were measured by two-photon excited fluorescence spectroscopy within the spectral range 750 to 850 nm. A critical assessment has been carried out within/across the particular series of chromophores in order to evaluate structure–property relationships. Extension of the π-system and replacement of acetylenic by more polarizable olefinic units led to a significant increase of 2PA activity. Hence, chromophore 5 bearing a cyano substituted styryl linker showed the most enhanced NLO activity within the whole series. An attachment of aromatic acceptors bearing two CN groups (9 and 10) as well as strongly withdrawing DCV units in 6 and 7 did not lead to increased δTPA coefficients compared to 5. A similar conclusion can be made for heterocyclic cyano acceptors such as DCI and 5(2,4)-(di)cyanothiophene.
HOMO and LUMO levels calculated using the DFT and their differences correlate tightly with the linear properties measured by electrochemistry and absorption/emission spectra. Considering all the aforementioned structural features of 1–12, we believe that this work could be treated as a useful guide in designing/tuning tripodal push-pull molecules with a central donor and peripheral acceptors.
:
1). Anhydrous Na2SO4 (350 mg, 2.46 mmol) can eventually be added to accelerate the reaction. The resulting coloured suspension was filtered and the filtrate was concentrated in vacuo. The crude products were purified by column chromatography (SiO2, DCM/EtOAc 10
:
1 or DCM) to afford 6 or 7.
:
1) Mp 145 °C. IR (HATR) νmax/cm−1 3087, 2220 (CN), 1559, 1496, 1269, 1186, 827. 1H-NMR: δH (400 MHz; CD2Cl2) 7.25 (6H, d, 3J 8.8, CHAr), 7.73 (3H, s, CH
C), 7.90 (6H, d, 3J 8.8, CHAr). 13C-NMR: δC (100 MHz; CD2Cl2) 81.6, 113.6, 114.7, 125.4, 128.2, 133.3, 150.7, 158.5. HR-MALDI-MS (DHB): calcd for C30H15N7 (M+) 473.1384 found 473.1385.
C), 7.56 (6H, d, 3J 9.0, CHAr). 13C-NMR: δC NMR (100 MHz; CD2Cl2): 86.2, 93.0, 111.4, 112.47, 114.9, 115.6, 124.5, 135.0, 140.8, 148.5. HR-MALDI-MS (DHB): calcd for C36H15N7 (M+) 545.1384 found 545.1386.
:
3) to afford 8 as orange solid. Yield (144 mg, 42%). Rf 0.4 (SiO2; EtOAc/hexane 1
:
3). Mp 188 °C. IR (HATR), νmax/cm−1 2294, 2231 (CN), 1592, 1506, 1324, 1285, 1179, 972, 818. 1H-NMR: δH (400 MHz; CD2Cl2) 3.83 (9H, s, CH3), 6.77 (6H, d, 3J 16.0, CH
CH), 7.16 (6H, d, 3J 8.5, CHAr), 7.54 (6H, d, 3J 8.5, CHAr), 7.81 (6H, d, 3J 16.0, CH
CH). 13C-NMR: δC (100 MHz; CD2Cl2) 33.2, 109.1, 109.5, 112.8, 113.3, 122.8, 125.0, 129.5, 130.9, 139.7, 148.6, 151.3. HR-MALDI-MS (DCTB): calcd for C42H27N13 (M+) 713.2507 found 713.2526.
:
3 or EtOAc/hexane 3
:
4) to afford target chromophores 9–12.
:
3). Mp 327 °C (dec.). IR (HATR), νmax/cm−1 2921, 2206 (CN), 1593, 1504, 1320, 1289, 1145, 836, 801, 736. 1H-NMR: δH (400 MHz; CD2Cl2) 7.19 (6H, d, 3J 8.8, CHAr), 7.52 (3H, t, 3J 8.0, CHAr), 7.64 (6H, d, 3J 8.8, CHAr), 7.90 (6H, d, 3J 8.0, CHAr). 13C-NMR: δC (100 MHz; CD2Cl2) 83.4, 103.5, 116.2, 116.5, 124.5, 128.3, 131.2, 134.3, 136.4 148.1, 149.5. HR-MALDI-MS (DHB): calcd for C48H21N7 (M+) 695.1853 found 695.1852.
:
3). Mp 282 °C (dec.). IR (HATR), νmax/cm−1 2922, 2204 (CN), 1593, 1503, 1320, 1277, 1145, 836, 800, 735. 1H-NMR: δH (400 MHz; CD2Cl2) 7.24 (6H, d, 3J 8.8, CHAr), 7.66 (6H, d, 3J 8.8, CHAr), 7.81 (3H, d, 3J 8.4, CHAr), 7.92 (3H, dd, 3J 8.4, 4J 1.2, CHAr), 8.04 (3H, d, 4J 1.2, CHAr). 13C-NMR: δC (100 MHz; CD2Cl2) 85.7, 101.1, 112.5, 116.4, 116.7, 116.8, 117.2, 124.9, 132.0, 133.2, 134.3, 136.1, 136.5, 148.4. HR-MALDI-MS (DHB): calcd for C48H21N7 (M+) 695.1853 found 695.1872.
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4). Mp 191 °C. IR (HATR), νmax/cm−1 2925, 2208 (CN), 1593, 1504, 1320, 1291, 834, 808, 737. 1H-NMR: δH (400 MHz; CD2Cl2) 7.18 (6H, d, 3J 8.8, CHAr), 7.31 (3H, d, 3J 4.0, Th), 7.55 (6H, d, 3J 8.8, CHAr), 7.62 (3H, d, 3J 4.0, Th). 13C-NMR: δC (100 MHz; CD2Cl2) 81.2, 97.0, 110.4, 114.1, 117.1, 124.8, 131.2, 132.0, 133.6, 138.0, 147.9. HR-MALDI-MS (DHB): calcd for C39H18N4S3 (M+) 638.0688 found 638.0705.
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4). Mp 198 °C (dec.). IR (HATR), νmax/cm−1 2848, 2236 (CN), 1592, 1472, 1377, 1169, 831, 728, 718. 1H-NMR: δH (500 MHz; CD2Cl2) 7.19 (6H, d, 3J 9.0, CHAr), 7.59 (6H, d, 3J 9.0, CHAr), 7.99 (3H, s, Th). 13C-NMR: δC (100 MHz; CD2Cl2) 78.2, 103.1, 111.8, 111.9, 112.3, 114.9, 115.8, 124.6, 133.7, 135.5, 136.6, 148.0. HR-MALDI-MS (DHB): calcd for C42H27N13 (M+) 713.2507 found 713.2532.
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| † Electronic supplementary information (ESI) available: Synthesis of chromophores 1–5 and all intermediates 13–25, electrochemical and optical data, correlations and NMR spectra. See DOI: 10.1039/c5tc01293g |
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