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. 2015 Oct 1;6(10):5994-6007.
doi: 10.1039/c5sc02051d. Epub 2015 Jul 9.

On-off switch of charge-separated states of pyridine-vinylene-linked porphyrin-C60 conjugates detected by EPR

Affiliations

On-off switch of charge-separated states of pyridine-vinylene-linked porphyrin-C60 conjugates detected by EPR

Sabrina V Kirner et al. Chem Sci. .

Abstract

The design, synthesis, and electronic properties of a new series of D-π-A conjugates consisting of free base (H2P) and zinc porphyrins (ZnP) as electron donors and a fullerene (C60) as electron acceptor, in which the two electroactive entities are covalently linked through pyridine-vinylene spacers of different lengths, are described. Electronic interactions in the ground state were characterized by electrochemical and absorption measurements, which were further supported with theoretical calculations. Most importantly, charge-transfer bands were observed in the absorption spectra, indicating a strong push-pull behavior. In the excited states, electronic interactions were detected by selective photoexcitation under steady-state conditions, by time-resolved fluorescence investigations, and by pump probe experiments on the femto-, pico-, and nanosecond time scales. Porphyrin fluorescence is quenched for the different D-π-A conjugates, from which we conclude that the deactivation mechanisms of the excited singlet states are based on photoinduced energy- and/or electron transfer processes between H2P/ZnP and C60, mediated through the molecular spacers. The fluorescence intensity decreases and the fluorescence lifetimes shorten as the spacer length decreases and as the spacer substitution changes. With the help of transient absorption spectroscopy, the formation of charge-separated states involving oxidized H2P/ZnP and reduced C60 was confirmed. Lifetimes of the corresponding charge-separated states, which ranged from ∼400 picoseconds to 165 nanoseconds, depend on the spacer length, the spacer substitution, and the solvent polarity. Interestingly, D-π-A conjugates containing the longest linkers did not necessarily exhibit the longest charge-separated state lifetimes. The distances between the electron donors and the acceptors were calculated by molecular modelling. The longest charge-separated state lifetime corresponded to the D-π-A conjugate with the longest electron donor-acceptor distance. Likewise, EPR measurements in frozen media revealed charge separated states in all the D-π-A conjugates investigated. A sharp peak with g values ∼2.000 was assigned to reduced C60, while a broader, less intense signal (g ∼ 2.003) was assigned to oxidized H2P/ZnP. On-off switching of the formation and decay of the charge-separated states was detected by EPR at 77 K by repeatedly turning the irradiation source on and off.

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Figures

Chart 1
Chart 1. Above: Porphyrin–fullerene conjugates linked by pyridine-vinylene units at meta- and para-positions 15–20a (H2P-n-mC60, ZnP-n-mC60, n = 1–3) and 15–20b (H2P-n-pC60, and ZnP-n-pC60, n = 1–3). Below: Corresponding porphyrin–pyridine-vinylene references 9–14a (H2P-n-mCHO, ZnP-n-mCHO, n = 1–3) and 9–14b (H2P-n-pCHO, ZnP-n-pCHO, n = 1–3).
Scheme 1
Scheme 1. Synthetic route for the preparation of pyridine-vinylene linkers: top 2–6a and bottom 2–6b. Reagents and conditions: (a) Pd(PPh3)4, tributyl(vinyl)tin, toluene, reflux, 20–22 h, yields 82–86%. (b) 2,6-Dibromopyridine 3, Pd(OAc)2, Bu4NBr, K2CO3, DMF, reflux, 24 h, yields 65–68%. (c) Pd(PPh3)4, tributyl(vinyl)tin, toluene, reflux, 20 h yields 75–80% (d) 2,6-dibromopyridine 3, Pd(OAc)2, Bu4NBr, K2CO3, DMF, reflux, 24 h, yields 62–70%.
Scheme 2
Scheme 2. Synthesis of new porphyrin–fullerene conjugates: top 15–20a (H2P-n-mC60, ZnP-n-mC60, n = 1-3); bottom 15–20b (H2P-n-pC60, ZnP-n-pC60, n = 1–3). Reagents and conditions: (a) C60, N-octylglycine, toluene, reflux, 4–5 h, yields (15a, 32%); (16a, 35%); (17a, 30%); (18a, 38%); (19a, 34%); (20a, 36%); (b) C60, N-octylglycine, toluene, reflux, 4–5 h, yields (15b, 31%); (16b, 38%); (17b, 37%); (18b, 34%); (19b, 45%); (20b, 42%).
Fig. 1
Fig. 1. Left: CVs for porphyrin–fullerene conjugates 15–17a (H2P-n-mC60, n = 1–3) and 15–17b (H2P-n-mC60, n = 1–3) in DCM solutions (0.1 M TBAPF6) at room temperature. Right: CVs for porphyrin–fullerene conjugates 18–20a (ZnP-n-pC60, n = 1–3) and 18–20b (ZnP-n-pC60, n = 1–3) in DCM solutions (0.1 M TBAPF6) at room temperature. Oxidative scans between 0 and 1.25 V; reductive scans between 0 and –2.10 V.
Fig. 2
Fig. 2. Absorption spectra of (18b) ZnP-1-pC60 (cyan); (19b) ZnP-2-pC60 (blue); (20b) ZnP-3-pC60 (navy) and ZnTPP (pink) as the reference in THF at room temperature.
Fig. 3
Fig. 3. Above: Fluorescence spectra of (15a) H2P-1-mC60 (cyan); (16a) H2P-2-mC60 (blue); (17a) H2P-3-mC60 (navy) and H2TPP (pink) (excitation at 420 nm; OD = 0.04) in THF at room temperature. Below: Fluorescence spectra of (18a) ZnP-1-mC60 (cyan); (19a) ZnP-2-mC60 (blue); (20a) ZnP-3-mC60 (navy) and ZnTPP (pink) (excitation at 420 nm; OD = 0.05) in THF at room temperature.
Fig. 4
Fig. 4. Above: Differential absorption spectra (visible and near-infrared) observed upon femtosecond flash photolysis (420 nm, 150 nJ) of 9a (H2P-1-mCHO) in THF with time delays between 0 ps (black) and 7.5 ns (wine) at room temperature. Below: Time-absorption profile of the spectra above at 1070 nm, monitoring the deactivation of the porphyrin singlet excited state.
Fig. 5
Fig. 5. Above: Differential absorption spectra (visible and near-infrared) observed upon femtosecond flash photolysis (387 nm, 200 nJ) of 16a (H2P-2-mC60) in THF with time delays between 0 ps (black) and 7.5 ns (wine) at room temperature. Below: Time-absorption profiles of the 1010 nm decay for (15a) H2P-1-mC60 (cyan); (16a) H2P-2-mC60 (blue) and (17a) H2P-3-mC60 (navy) upon femtosecond flash photolysis (387 nm, 200 nJ) in THF at room temperature, monitoring the charge recombination.
Fig. 6
Fig. 6. Above: Differential absorption spectra (visible) observed upon nanosecond flash photolysis (355 nm, 10 mJ) of 16a (H2P-2-mC60) in THF with time delays between 150 ns (purple) and 2.0 μs (wine) at room temperature under aerobic conditions. Below: Differential absorption spectra (near-infrared) observed upon nanosecond flash photolysis (355 nm, 10 mJ) of 16a (H2P-2-mC60) in THF with time delays between 60 ns (purple) and 2.0 μs (wine) at room temperature under aerobic conditions.
Fig. 7
Fig. 7. Above: Time-absorption profile of the 1010 nm decay – Fig. 6 – of 16a (H2P-2-mC60) upon nanosecond flash photolysis (355 nm, 10 mJ) in THF under aerobic conditions, monitoring the charge recombination process. Below: Time-absorption profile of the 1010 nm decay of 16b (H2P-2-pC60) upon nanosecond flash photolysis (355 nm, 10 mJ) in THF under aerobic conditions, monitoring the charge recombination.
Fig. 8
Fig. 8. Above: Differential absorption spectra (visible and near-infrared) observed upon femtosecond flash photolysis (387 nm, 1 μJ) of 16a (H2P-2-mC60) in THF with time delays between 0 ns (black) and 1.0 μs (wine) at room temperature under aerobic conditions. Below: Time-absorption profile of the spectra above at 1010 nm, monitoring the charge recombination.
Fig. 9
Fig. 9. Above: Differential absorption spectra (visible and near-infrared) observed upon femtosecond flash photolysis (387 nm, 200 nJ) of 19a (ZnP-2-mC60) in THF with time delays between 0 ps (black) and 7.5 ns (wine) at room temperature. Below: Time-absorption profiles of the 1010 nm decay for (18a) ZnP-1-mC60 (cyan); (19a) ZnP-2-mC60 (blue) and (20a) ZnP-3-mC60 (navy) upon femtosecond flash photolysis (387 nm, 200 nJ) in THF at room temperature, monitoring the charge recombination.
Fig. 10
Fig. 10. EPR signals observed under photoirradiation of 15a (H2P-1-mC60) in benzonitrile at 77 K.
Fig. 11
Fig. 11. On–off switch of the EPR signal due to charge separation of 17a (top) and 20a (bottom) in PhCN at 77 K by turning on and off the irradiation from a high-pressure mercury lamp.
Fig. 12
Fig. 12. Lowest-energy conformations of (17a) H2P-3-mC60 (left) and (17b) H2P-3-pC60 (right).

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