Open Access Article
Luis
Martín-Gomis
a,
Georgios
Rotas
b,
Kei
Ohkubo
c,
Fernando
Fernández-Lázaro
a,
Shunichi
Fukuzumi
*cd,
Nikos
Tagmatarchis
*b and
Ángela
Sastre-Santos
*a
aÁrea de Química Orgánica Instituto de Bioingeniería, Universidad Miguel Hernández, Elche, Spain. E-mail: asastre@umh.es; Fax: +34 966658408; Tel: +34 966658351
bTheoretical and Physical Chemistry Institute, National Hellenic Research Foundation, 48 Vassileos Constantinou Avenue, Athens 116 35, Greece. E-mail: tagmatar@eie.gr
cDepartment of Material and Life Science, Graduate School of Engineering, Osaka University, ALCA, Japan Science and Technology Agency (JST), Suita, Osaka 565-0871, Japan. E-mail: fukuzumi@chem.eng.osaka-u.ac.jp
dDepartment of Bioinspired Science, Ewha Womans University, Seoul, 120-750, Korea
First published on 16th March 2015
The first perylenediimide (PDI) covalently linked to an azafullerene (C59N) is described. PDI-C59N and PDI-C60 dyads where PDI acts as an electron-donor moiety have been synthesized by connection of the balls to the PDI 1-bay position. Photoexcitation of the PDI unit in both systems results in formation of the charge-separated state by photoinduced electron transfer from the singlet excited state of the PDI moiety to the C59N or to the C60 moiety. The charge-separated state has a lifetime of 400 ps in the case of PDI-C59N and 120 ps for the PDI-C60 dyad in benzonitrile at 298 K. This result has significant implications for the design of organic solar cells based on covalent donor–acceptor systems using C59N as an electron acceptor, indicating that longer-lived charge-separated states can be attained using C59N systems instead of C60 systems.
On the other hand, perylenediimides (PDI) comprise an outstanding family of perylene derivatives that, due to an extreme synthetic versatility and an easily tunable electronic character, have become one of the most promising classes of molecular materials in organic photovoltaic devices.11 In this context, we can find only a few examples where PDI derivatives have been successfully employed as an electron-donor moiety in fullerene-based systems, eventually undergoing photoinduced electron and/or energy transfer.12
Here we present the synthesis, characterization and photophysical properties of a new photoexcitable molecular system, consisting of an electron-donor PDI moiety, carrying a pyrrolidinyl substituent in the 1-bay position, which also acts as a linker to the C59N counterpart (Scheme 1). The obtained donor–acceptor PDI-C59N dyad 1, upon selective excitation of the PDI subunit in benzonitrile, shows efficient intramolecular photoinduced electron transfer, generating a 400 ps-lived charge-separated state (CSS). Together with two covalently linked porphyrin-C59N dyads,7 this is the longest CSS lifetime value obtained so far for a C59N-based donor–acceptor dyad in a polar solvent. Moreover, in order to study the effect of the nitrogen atom on the photophysics, the analogous PDI-C60 dyad 2 (Scheme 1) was synthesized, as reference material, obtaining a 3-times shorter CSS lifetime than for the PDI-C59N dyad 1, thus, highlighting the role of nitrogen in the photoinduced electron-transfer processes.
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| Scheme 1 Synthetic routes for preparing PDI-C59N 1 and PDI-C602 dyads as well as PDI-based reference material 6. | ||
9 gave rise to PDI-C59N dyad 1 in 8% yield. A similar esterification process, involving 2,2-[60]fullerenylacetic acid 5a
14 and PDI-based 3 was followed, affording in 43% yield PDI-C60 dyad 2. Furthermore, PDI derivative 6 was also synthesized in 75% yield, through an acylation of 3 with acetic anhydride in acidic media, in order to be used as a reliable reference to evaluate optical, electrochemical and photophysical properties.
All new compounds were fully characterised using standard analytical techniques such as 1H and 13C NMR, HR-MS, FT-IR, electronic absorption and photoluminescence. Fig. 1 compares the aromatic region of the 1H NMR spectra for 1, 2 and 6 in CDCl3 as solvent. Taking as reference the C1 of the PDI core (the substituted one), and comparing the signals of analogous hydrogens in compounds 1, 2 and 6, it is worth noting that the chemical displacement of the nearby hydrogens (H2, H11 and H12) is significantly shifted in dyad's spectra, while the contrary trend is observed in the displacement of H5, H6, H7 and H8. For example, the H2 signal goes from 8.69 to 9.19 and 9.18 ppm (in 2 and 1 respectively), while H6 goes from 8.45 to 8.40 ppm. Furthermore, the fullerene influence is slightly larger when C59N is present instead of C60, and it can be recognised in the H12 displacement, which changes from 8.11 ppm in 6, to 8.29 and 8.40 ppm in dyads 2 and 1, respectively. Fig. 2 shows the aliphatic regions of the spectra, where some differences can also be found due to the presence of the covalently attached fullerene. For example, the signals corresponding to the hydrogens labeled as HB, HC and HE, which appear as broad signals in the spectrum of PDI-based 6, split into two in the corresponding spectra of PDI-fullerene dyads 1 and 2. All these differences in the 1H NMR spectra of dyads and reference material can be explained by considering the electron-withdrawing character of the fullerene sphere, which is more intense in the case of C59N as compared with C60, and also assuming a pseudo-fixed molecular conformation in PDI-fullerene dyads caused by an electrostatic interaction between the PDI and the fullerene moiety including a concave–convex interaction3l,15 that causes a different influence of the sphere on the chemical shift of the pyrrolidine-linker geminal protons. HR MALDI-TOF (negative mode) experiments clearly confirm the structure of PDI-C59N and PDI-C60 dyads 1 and 2, respectively, showing base peaks due to the molecular ions at 1476.463 amu and 1474.302 amu, with isotopical distributions that exactly match the simulated isotope patterns for C106H52N4O6 and C107H51N3O6, respectively (see ESI, Fig. S1†).
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| Fig. 1 Partial 1H NMR (9.30–8.00 ppm) spectra of (a) PDI-based reference material 6, (b) PDI-C602, and (c) PDI-C59N 1. | ||
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| Fig. 2 Partial 1H NMR (5.50–1.60 ppm) spectra in CDCl3 as solvent of (a) PDI-based reference material 6, (b) PDI-C602, and (c) PDI-C59N 1. | ||
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| Fig. 3 UV/vis spectra of PDI-C59N 1 and PDI-C602, reference compounds 4b and 5a and PDI-based reference 6 registered in benzonitrile as solvent. | ||
On the other hand, Fig. 4 shows the fluorescence emission spectra of PDI-C59N 1 and PDI-C602 dyads, when selectively excited at 429 nm. As can be seen, the fluorescence spectrum of 6 clearly shows three different emission bands, centered at 480, 512 and 691 nm. When the emission spectra of PDI-C59N and PDI-C60 dyads 1 and 2 are compared to that of the reference compound, the first and second bands are partially quenched while the third one is extinguished. The latter is indicative of intra-dyad electronic interactions between the two components of the dyad (i.e., PDI and fullerene) at the excited state. The strong fluorescence quenching of the 691 nm band in both 1 and 2 as compared to 6, supports electron and/or energy transfer as the decay mechanism of the PDI-centred singlet excited state. This effect is slightly more pronounced in the case of PDI-C59N dyad 1 (see inset Fig. 4).
The electrochemical data of PDI-C59N 1 and PDI-C602 dyads, as well as 6, 4b and 5b as reference materials for PDI-C59N, and C60, respectively, in benzonitrile using Fc/Fc+ as an internal standard are listed in Table 1 (see differential pulse voltammograms in ESI, Fig. S13†). The measurements for PDI 6 reveal a one-electron oxidation and two one-electron reduction processes centred at 0.55, −1.15 and −1.35 V respectively, while the measurements for fullerene reference compounds show two one-electron reversible reduction processes at −1.01 and −1.42 V. The voltammograms of dyads 1 and 2 are very similar, in spite of the nitrogen atom in dyad 1, and can be considered as a combination of the already mentioned electrochemical processes assigned to PDI and fullerene electroactive moieties. A slight influence of the fullerene sphere (either C59N or C60) over the PDI moiety can be recognised, and it is highlighted by a 20–30 mV anodic displacement of the oxidation wave and a 40 mV cathodic displacement of the second reduction process, which is attributed to the PDI counterpart. As contrary to previous results reported by us,9,10 the similar first reduction values obtained for PDI-C60 and PDI-C59N might come from the use of different solvents. Based on the redox data shown in Table 1 and neglecting the Coulombic interactions, the electrochemical band gap for 1 is calculated as 1.59 eV (1.61 eV for 2).
| E 3red (V) | E 2red (V) | E 1red (V) | E ox (V) | |
|---|---|---|---|---|
| PDI-6 | −1.35 | −1.15 | 0.55 | |
| PDI-C602 | −1.39 | −1.19 | −1.03 | 0.58 |
| PDI-C59N 1 | −1.38 | −1.19 | −1.01 | 0.58 |
| C60-ref 5b | −1.42 | −1.01 | ||
| C59N-ref 4b | −1.42 | −1.01 |
Femtosecond laser flash photolysis on a deaerated benzonitrile solution of 1 and 2 indicates the formation of a charge-separated state, providing solid evidence for the electron-transfer deactivation mechanism in 1 and 2, after selective excitation of the perylene moiety. The transient absorption spectrum taken at 1 ps after laser pulse irradiation of the absorption band of the PDI moiety at 490 nm exhibits an absorption maximum at 900 nm, which is assigned to the singlet excited state of C59N of PDI-C59N dyad 1 (Fig. 5a). No indication of the PDI singlet excited state was observed in spite of the selective excitation of PDI, indicating that the rate of energy transfer from the singlet excited state of the PDI moiety to the C59N moiety is too fast to be followed even with the use of femtosecond laser flash photolysis (fwhm = 130 fs). Then, electron transfer from PDI to the singlet-excited state of C59N takes place to form PDI˙+-C59N˙− as the charge-separated state. The transient absorption band decayed with a rate constant of 5.5 × 1010 s−1 giving rise to an absorption band at λmax = 1030 nm due to the C59N˙− radical anion,9,10 which indicates the formation of the charge-separated state. From the decay of the absorption band at 1030 nm, a 400 ps lifetime (k = 2.5 × 109 s−1) was obtained for the charged-separated state (Fig. 5b), being the first example of a charge-separated state in a donor–acceptor dyad based on PDI and azafullerene.
When benzonitrile was replaced by toluene, the rate constant of charge separation became much larger (3.9 × 1011 s−1), whereas the rate constant of charge recombination became smaller (1.3 × 109 s−1) as shown in Fig. S14 (ESI†). The faster charge separation in toluene than in benzonitrile may result from the smaller solvent reorganization energy of toluene than that of the more polar benzonitrile in the Marcus normal region, where the charge separation becomes faster with decreasing the solvent reorganisation energy of electron transfer.1d,18 By the same token, the slower charge recombination in toluene than in benzonitrile results from the smaller solvent reorganisation energy of toluene than that of benzonitrile in the Marcus inverted region, where the charge recombination becomes slower with decreasing the solvent reorganisation energy of electron transfer.1d,18
On the other hand, a similar transient absorption spectral change was observed for PDI-C60 dyad 2 as shown in Fig. 6a. The transient absorption recorded at 1 ps after femtosecond laser pulse irradiation is assigned to the singlet excited state of C60, indicating that ultrafast energy transfer from the singlet excited state of PDI to the C60 moiety also occurs in PDI-C60. Then, electron transfer from PDI to the singlet excited state of C60 takes place to form the charge-separated state. The rate constant for electron transfer is determined to be 8.6 × 1010 s−1 from the rise of the absorbance at 1000 nm (inset of Fig. 6b). This rate is slightly faster than that of PDI-C59N (vide supra). The lifetime of the charge-separated state was determined to be 120 ps from the decay of absorbance at 1000 nm as shown in Fig. 6b. It is worth to mention the much shorter lifetime of the CSS in PDI-C60, less than one third of that in PDI-C59N, pointing to the remarkable influence of the nitrogen atom in C59N, which is not explained only by an increased electron-accepting character as the reduction potentials of 1 and 2 indicate. In both cases, the decay of the charge-separated state by back electron transfer yields the ground state rather than the triplet excited state of PDI as indicated by no triplet transient absorption of 1 and 2 in nanosecond laser flash photolysis measurements (Fig. S14 in ESI†).
tert-Butyl (2,2-[60]fullerenyl)acetate 5b
14 and ethyl (2-azafullerenyl)acetate 4b, used as C60 and C59N reference compounds, respectively, in electrochemistry measurements, were prepared as reported earlier.
:
1) to obtain 52 mg (51%) of the desired product as a green powder. 1H NMR (300 MHz, 25 °C): 8.46 (1H, s, H-PDI), 8.42–8.35 (2H, m, 3 × H-PDI), 8.18 (1H, d, J = 8.2 Hz, H-PDI), 8.02–7.89 (2H, m, 2 × H-PDI), 7.55–7.47 (1H, m, 2 × H-PDI), 4.51–4.39 (1H, m, CHN-pyrrolidine), 4.31 (1H, t, J = 12.7 Hz, CHH-OH), 4.21–4.03 (4H, m, 2 × CH2-N-alkyl chain), 3.98 (1H, t, J = 12.7 Hz, CHH-OH), 3.57–3.41 (1H, m, CHHN-pyrrolidine), 2.30–2.09 (2H, m, CH2-pyrrolidine), 2.07–1.91 (2H, m, CHH-pyrrolidine + CH-alkyl chain), 1.90–1.76 (1H, m, CH-alkyl chain), 1.71–1.59 (2H, m, CHHN-pyrrolidine + CHH-pyrrolidine) 1.54–1.21 (16H, m, 8 × CH2-alkyl chain) and 1.06–0.78 (12H, m, 4 × CH3-alkyl chain) ppm; 13C NMR (75 MHz, CDCl3, 25 °C):164.2, 163.9, 163.3, 163.3, 147.2, 134.8, 134.2, 132.0, 131.5, 129.7, 129.7, 128.3, 128.1, 126.6, 126.2, 124.6, 123.2, 123.0, 122.5, 122.3, 120.6, 120.0, 118.0, 116.2, 62.0, 60.2, 56.2, 44.3, 43.9, 38.1, 38.1, 37.8, 30.9, 30.7, 29.6, 28.8, 28.6, 27.9, 25.2, 24.1, 24.0, 23.1, 14.1, 10.7 and 10.6 ppm; IR-FT (KBr) ν/cm−1: 3467, 2956, 2927, 2858, 1691, 1652, 1586, 1427, 1338, 1242, 807, 748; UV/vis (CH2Cl2), λmax/nm (log
ε): 431 (4.16), 637 (4.36); HR-MS (MALDI-TOF, dithranol): m/z = 713.349, [M]−, calcd for C45H51N3O5: 713.383.
O), 2.11–1.88 (4H, m, CH2-pyrrolidine + 2 × CH-alkyl chain), 1.50–1.24 (16H, m, 8 × CH2-alkyl chain) and 1.01–0.84 (12H, m, 4 × CH3-alkyl chain) ppm; 13C NMR (75 MHz, CDCl3, 25 °C): 170.9, 164.3, 164.1, 147.8, 135.9, 135.2, 133.2, 131.3, 129.2, 129.1, 127.6, 127.5, 124.6, 124.0, 123.9, 123.3, 122.9, 122.6, 122.1, 121.0, 119.8, 118.9, 65.3, 57.5, 56.4, 44.5, 38.1, 31.0, 29.1, 28.9, 25.4, 24.3, 23.2, 21.0, 14.3, 10.9, 10.8; IR-FT (KBr) 2956, 2927, 2857, 1744, 1693, 1654, 1587, 1419, 1336, 1240, 808, 748 ν/cm−1; UV/vis (CH2Cl2), λmax/nm (log
ε):332 (3.80), 430 (4.17), 624 (4.36); HR-MS (MALDI-TOF, dithranol): m/z = 755.385, [M]−, calcd for C45H51N3O5: 755.393.
C60), 4.22–3.99 (4H, m, 2 × CH2-N-alkyl chain), 3.90–3.76 (1H, m, CHHN-pyrrolidine), 2.60–2.48 (1H, m, NCH-CHH-pyrrolidine), 2.27–1.76 (6H, m, CHHN-pyrrolidine + NCH-CHH-pyrrolidine + CH2-pyrrolidine + 2 × CH-alkyl chain), 1.50–1.22 (16H, m, 8 × CH2-alkyl chain) and 1.01–0.82 (12H, m, 4 × CH3-alkyl chain) ppm; 13C NMR (75 MHz, CDCl3, 25 °C): 165.8, 164.3, 164.0, 163.9, 148.8, 148.0, 147.0, 145.5, 145.4, 145.2, 145.1, 145.0, 144.9, 144.8, 144.6, 144.5, 144.4, 144.3, 144.2, 144.1, 143.9, 143.7, 143.6, 143.5, 143.4, 143.3, 143.1, 142.9, 142.8, 142.7, 142.5, 142.2, 142.1, 142.0, 141.9, 141.8, 141.2, 141.0, 140.7, 140.2, 140.0, 139.9, 139.2, 136.3, 136.1, 135.6, 135.1, 133.6, 131.5, 131.1, 129.5, 129.0, 127.8, 127.5, 124.9, 124.5, 124.0, 123.7, 123.1, 122.5, 122.1, 121.1, 120.0, 119.4, 70.2, 70.0, 68.9, 57.1, 44.5, 44.4, 44.3, 38.5, 38.2, 38.0, 30.9, 28.9, 28.8, 28.7, 25.4, 24.2, 23.3, 23.2, 14.3 and 10.9; IR-FT (KBr) 2951, 2923, 2854, 1740, 1693, 1655, 1417, 1333, 1242, 1182, 1152, 807, 747, 527 ν/cm−1; UV/vis (CH2Cl2), λmax/nm (log
ε): 327 (4.60), 428 (4.18), 628 (4.35); HR-MS (MALDI-TOF, dithranol): m/z = 1473.302, [M]−, calcd for C107H51N3O6: 1473.378.
:
1). The first green fraction was collected and further purified in preparative HPLC (buckyprep, toluene, 10 ml min−1. R.t. = 18.6 min) yielding 1 as green dust (3 mg, 8%). 1H NMR (300 MHz, CDCl3, 25 °C): 9.19 (1H, s, H-PDI), 8.69 (1H, d, J = 8.1 Hz, H-PDI), 8.59 (1H, d, J = 8.0 Hz, H-PDI), 8.44–8.35 (4H, m, 4 × H-PDI), 5.21–5.27 (2H, m, CHN-pyrrolidine + CHH-O2C), 4.87–4.77 (1H, m; CHH-O2C), 4.71 (1H, d, J = 16.2 Hz, O2C-CHH-C59N), 4.63 (1H, d, J = 16.2 Hz, O2C-CHH-C59N), 4.24–4.03 (4H, m, 2 × CH2-N-alkyl chain), 3.95–3.83 (1H, m, CHHN-pyrrolidine), 2.62–2.48 (1H, m, NCH-CHH-pyrrolidine), 2.28–1.76 (6H, m, CHHN-pyrrolidine + NCH-CHH-pyrrolidine + CH2-pyrrolidine + 2 × CH-alkyl chain), 1.48–1.22 (16H, m, 8 × CH2-alkyl chain) and 1.02–0.80 (12H, m, 4 × CH3-alkyl chain) ppm; 13C NMR (75 MHz, CDCl3, 25 °C): 169.5, 164.5, 164.3, 164.1, 164.0, 154.7, 154.4, 148.5, 147.8, 147.6, 147.5, 147.4, 147.1, 147.0, 146.7, 146.6, 146.5, 146.4, 146.3, 145.9, 145.8, 145.7, 145.1, 145.0, 144.8, 144.6, 144.3, 143.8, 143.6, 143.5, 142.7, 142.1, 141.7, 141.6, 141.1, 140.9, 140.8, 140.6, 139.4, 139.2, 137.0, 136.9, 135.8, 135.2, 134.2, 133.7, 133.6, 131.6, 131.1, 129.4, 129.0, 127.9, 127.6, 124.8, 124.3, 124.1, 123.9, 123.8, 123.6, 123.0, 122.4, 122.0, 121.0, 120.0, 119.2, 78.4, 68.4, 57.4, 57.1, 46.9, 44.5, 44.3, 38.2, 37.9, 30.9, 29.8, 29.1, 28.9, 28.8, 28.7, 25.3, 24.2, 23.3, 23.2, 14.3, 10.9 and 10.8 ppm; IR-FT (KBr) ν/cm−1: 3425, 2953, 2925, 2856, 1747, 1694, 1656, 1588, 1421, 1334, 1242, 1185, 808, 748, 525; UV/vis (CH2Cl2), λmax/nm (log
ε): 321 (4.59), 431 (4.27), 632 (4.37); HR-MS (MALDI-TOF, dithranol): m/z = 1476.463, [M]−, calcd for C106H52N4O6: 1476.389.
Footnote |
| † Electronic supplementary information (ESI) available: Characterization spectra of the new compounds. See DOI: 10.1039/c5nr00308c |
| This journal is © The Royal Society of Chemistry 2015 |