Coumarin–Tetrapyrrolic Macrocycle Conjugates: Synthesis and Applications

This review covers the synthesis of coumarin–porphyrin, coumarin–phthalocyanine and coumarin–corrole conjugates and their potential applications. While coumarin–phthalocyanine conjugates were obtained almost exclusively by tetramerization of coumarin-functionalized phthalonitriles, coumarin–porphyrin and coumarin–corrole conjugates were prepared by complementary approaches: (a) direct synthesis of the tetrapyrrolic macrocycle using formylcoumarins and pyrrole or (b) by functionalization of the tetrapyrrolic macrocycle. In the last approach a range of reaction types were used, namely 1,3-dipolar cycloadditions, hetero-Diels–Alder, Sonogashira, alkylation or acylation reactions. This is clearly a more versatile approach, leading to a larger diversity of conjugates and allowing the access to conjugates bearing one to up to 16 coumarin units.

Due to their exceptional optical properties, coumarins are the focus of an intense research effort in various scientific areas. In particular, in recent years, a large number of coumarin-tetrapyrrolic macrocycle conjugates have been synthesized and their photophysical properties evaluated. Typically, the main objective of those studies is to take advantage from the efficient energy transfer between the coumarin and the tetrapyrrole unit, aiming for light harvesting applications. In this article, we review primarily the synthetic approaches leading to coumarin-porphyrin, coumarin-phthalocyanine, and coumarin-corrole conjugates. A range of other coumarin-chromophore conjugates, such as coumarin-bodipy [18,31], coumarin-fullerene [32][33][34], coumarin-perylene [35][36][37], etc. have also been reported and exhibit highly interesting photophysical properties. However, those systems are not covered in this review.

Coumarin-Porphyrin Dyads
The number of porphyrin derivatives bearing coumarin units at β-pyrrolic positions are scarce.
Examples of such type of compounds were reported in 2011 by Cavaleiro and co-workers [38,39]. The coumarin-porphyrin dyads 4a,b were synthesized via hetero-Diels-Alder The extension of the domino Knoevenagel/hetero-Diels-Alder approach to the zinc(II) complexes of chlorin e6 trimethyl ester and protoporphyrin IX dimethyl ester and the ortho-quinone methides 3a,b afforded the conjugates Zn5a,b and Zn6a,b in excellent yields (81-91%) ( Figure 1) [43]. These complexes were then demetalated to the corresponding free-bases 5a,b and 6a,b. These conjugates were isolated as mixtures of diastereomers and their relative abundances were determined by advanced NMR techniques. The evaluation of their photophysical and electrochemical properties showed that the fluorescence quantum yields of the chlorin e6 derivatives are higher than those of the protoporphyrin conjugates. All conjugates were able to generate singlet oxygen but protoporphyrin IX dyads gave the highest singlet oxygen quantum yields. The free-base chlorin e6 dyads showed an unexpectedly higher ability to generate singlet oxygen when compared with the Zn(II) counterparts due to the higher tendency of the complexes to aggregate. The same group reported the synthesis of six coumarin-porphyrin dyads 8a-f from porphyrin 1 and the ortho-quinone methides 7a-f generated in situ from 4-hydroxycoumarin and suitable aromatic aldehydes. Scheme 1. Route to coumarin-porphyrin dyads [38,39].
The extension of the domino Knoevenagel/hetero-Diels-Alder approach to the zinc(II) complexes of chlorin e 6 trimethyl ester and protoporphyrin IX dimethyl ester and the ortho-quinone methides 3a,b afforded the conjugates Zn5a,b and Zn6a,b in excellent yields (81-91%) ( Figure 1) [43]. These complexes were then demetalated to the corresponding free-bases 5a,b and 6a,b. These conjugates were isolated as mixtures of diastereomers and their relative abundances were determined by advanced NMR techniques. The evaluation of their photophysical and electrochemical properties showed that the fluorescence quantum yields of the chlorin e 6 derivatives are higher than those of the protoporphyrin conjugates. All conjugates were able to generate singlet oxygen but protoporphyrin IX dyads gave the highest singlet oxygen quantum yields. The free-base chlorin e 6 dyads showed an unexpectedly higher ability to generate singlet oxygen when compared with the Zn(II) counterparts due to the higher tendency of the complexes to aggregate. The same group reported the synthesis of six coumarin-porphyrin dyads 8a-f from porphyrin 1 and the ortho-quinone methides 7a-f generated in situ from 4-hydroxycoumarin and suitable aromatic aldehydes. The reactions were carried out under three different conditions, including in water under ohmic heating (Scheme 2) [44]. Comparing the results obtained under the various experimental conditions, the authors concluded that the use of ohmic heating leads to a reduction of the reaction time, higher yields and selectivities. Moreover, the use of water as solvent facilitates the workup and product isolation over traditional organic solvents. Scheme 2. Synthesis of aryl-substituted coumarin-porphyrin dyads [44].
In 2015, Singh and Nath reported the synthesis of β-triazole bridged coumarin-porphyrin conjugates in 84-92% yield by the Cu(I)-catalyzed click reaction between 2-azido-5,10,15,20tetraphenylporphyrinatocopper(II) (9) [45] with various alkyne-substituted coumarins 10-12 (Scheme 3) [46]. The authors also prepared the corresponding free-bases in good yield (71-80%) by demetalation of the copper derivatives. Metalation of the free-bases with zinc(II) acetate afforded the corresponding zinc(II) complexes in 91-96% yield. The photophysical characterization of these conjugates revealed, for some of them, a considerable electronic communication between both units. Additionally, in some of these dyads it was observed a significant intramolecular energy transfer between both chromophores. The reactions were carried out under three different conditions, including in water under ohmic heating (Scheme 2) [44]. Comparing the results obtained under the various experimental conditions, the authors concluded that the use of ohmic heating leads to a reduction of the reaction time, higher yields and selectivities. Moreover, the use of water as solvent facilitates the workup and product isolation over traditional organic solvents. The reactions were carried out under three different conditions, including in water under ohmic heating (Scheme 2) [44]. Comparing the results obtained under the various experimental conditions, the authors concluded that the use of ohmic heating leads to a reduction of the reaction time, higher yields and selectivities. Moreover, the use of water as solvent facilitates the workup and product isolation over traditional organic solvents. Scheme 2. Synthesis of aryl-substituted coumarin-porphyrin dyads [44].
In 2015, Singh and Nath reported the synthesis of β-triazole bridged coumarin-porphyrin conjugates in 84-92% yield by the Cu(I)-catalyzed click reaction between 2-azido-5,10,15,20tetraphenylporphyrinatocopper(II) (9) [45] with various alkyne-substituted coumarins 10-12 (Scheme 3) [46]. The authors also prepared the corresponding free-bases in good yield (71-80%) by demetalation of the copper derivatives. Metalation of the free-bases with zinc(II) acetate afforded the corresponding zinc(II) complexes in 91-96% yield. The photophysical characterization of these conjugates revealed, for some of them, a considerable electronic communication between both units. Additionally, in some of these dyads it was observed a significant intramolecular energy transfer between both chromophores.
Using a similar strategy, the same authors also described the synthesis of zinc(II) β-triazolylmethylbridged coumarin-porphyrin dyads 17-19 (Scheme 4) [47]. In these conjugates the porphyrin and the triazole units are separated by a methylene spacer. Their synthesis involved the 1,3-dipolar cycloaddition between the 2-azidomethyl-5,10,15,20-tetraphenylporphyrinatozinc(II) (16) and the alkyne-substituted coumarins 10-12. The reported yields for the dyads are in the range 84-92%. Demetalation of the zinc(II) complexes afforded the corresponding dyads with free-base porphyrins in 69-79% yield. Again, the photophysical characterization of the new compounds allowed verifying an intramolecular energy transfer between both units for some of the conjugates.
Lin et al. reported the synthesis of symmetric and asymmetric porphyrins bearing coumarin units at the meso positions ( Figure 2) [49]. The monoand meso-tetrakis(coumarin-4-yl)porphyrins 25-27 were obtained in yields between ca. 5% and 13% from the reaction of pyrrole and an adequate molar ratio of benzaldehyde/coumarin-4-carbaldehydes 24a-c. Depending on the coumarin−carbaldehyde used, the porphyrins where synthesized under Adler (refluxing propionic acid) [50] or Lindsey (BF 3 ·OEt 2 or TFA, CHCl 3 , room temperature, then p-chloranil) [51] conditions. The symmetrical meso-tetrakis(coumarin-4-yl)porphyrins 26b and 27b, isolated in 5.3% and 2.7% yield, respectively, were obtained from the reaction between pyrrole and coumarin−carbaldehydes 24b and 24c under Lindsey conditions. The absorption and photoluminescent spectra of these dyads in dilute THF solutions and as solid films (obtained by spin-coating the derivatives in quartz plates) demonstrated that the energy transfer from the coumarin substituents to the porphyrin core is more efficient in solid film than in solution. The best results were obtained with the dyads 27a,b bearing the 7-diethylaminocoumarin moiety. This efficiency was justified by the high electron-donating ability of the amino substituent and also considering that in the solid state, the stacking porphyrins reduce the torsion angle between the porphyrin core and the coumarin substituent, forcing them to be coplanar and thus enhancing the conjugation extent of the porphyrin core and the coumarin substituent, facilitating the energy transfer from the coumarin units to the porphyrin core. solution. The best results were obtained with the dyads 27a,b bearing the 7-diethylaminocoumarin moiety. This efficiency was justified by the high electron-donating ability of the amino substituent and also considering that in the solid state, the stacking porphyrins reduce the torsion angle between the porphyrin core and the coumarin substituent, forcing them to be coplanar and thus enhancing the conjugation extent of the porphyrin core and the coumarin substituent, facilitating the energy transfer from the coumarin units to the porphyrin core. The Lindsey experimental conditions were also used for the condensation of coumarin-3carbaldehydes 28a-d with pyrrole (Scheme 6) [52]. The resulting meso-tetrakis(4-chlorocoumarin-3yl)porphyrins 29a-d were obtained in ca. 20% yield as mixtures of four atropisomers. The authors were able to determine the ratio of the atropisomers by high-performance thin-layer chromatography (HPTLC) (UV-detector). The metalation of the free-bases with zinc(II) acetate in CHCl3-MeOH at room temperature afforded the corresponding zinc(II) complexes Zn29a-d in 80-86% yield.
Fréchet and co-workers reported the synthesis of branched star polymers consisting of a central porphyrin core and 16 coumarin units (Scheme 7) [53][54][55]. The compounds were prepared via esterification of meso-tetrakis(3,5-dihydroxyphenyl)porphyrin (30) with acetonide-protected 2,2-bis(hydroxymethyl)propanoic acid followed by deprotection of the diol functionalities under acidic conditions. The reaction of the resulting hexadecahydroxy-functionalized porphyrin 31 with coumarin-3-carboxylic acid chloride gave the hexadecacoumarin-functionalized porphyrin 32. Bulk polymerization of ε-caprolactone with the initiator 31, with tin(II) 2-ethylhexanoate as the catalyst, followed by esterification of the resulting polymer with coumarin-3-carboxylic acid chloride gave 33 in quantitative yield. Polymers 33 with varying chain lengths were prepared in almost quantitative yields by adjusting the monomer-to-initiator ratio. The 16 coumarin units in compounds 32 and 33 are responsible for the large absorption in the UV region of the spectrum. It was found that the presence of coumarin donor chromophores in these systems was particularly useful to evaluate the isolation of the core functionalities by using fluorescence resonance energy transfer (FRET). When the coumarin units were excited selectively at λ = 350 nm, the emission from both the coumarin donor and the porphyrin acceptor was observed demonstrating that in these systems FRET was facile but not quantitative. It was verified that as the chain length of the polymer increases the donor emission intensity increases as the result of the reduced probability of FRET. In compound 32, due to the extremely short average donor-acceptor distance, a quantitative FRET was observed. Besides the chain length, it was verified that poor solvents seem to further increase the degree of site isolation due to a structural collapse of the polymer backbone giving rise to a more densely packed structure around the core unit and a reduced average donor-acceptor distance. This observation was supported by Scheme 6. Route to meso-tetrakis(4-chlorocoumarin-3-yl)porphyrins reported by Amaravathi et al. [52].
Bulk polymerization of ε-caprolactone with the initiator 31, with tin(II) 2-ethylhexanoate as the catalyst, followed by esterification of the resulting polymer with coumarin-3-carboxylic acid chloride gave 33 in quantitative yield. Polymers 33 with varying chain lengths were prepared in almost quantitative yields by adjusting the monomer-to-initiator ratio. The 16 coumarin units in compounds 32 and 33 are responsible for the large absorption in the UV region of the spectrum. It was found that the presence of coumarin donor chromophores in these systems was particularly useful to evaluate the isolation of the core functionalities by using fluorescence resonance energy transfer (FRET). When the coumarin units were excited selectively at λ = 350 nm, the emission from both the coumarin donor and the porphyrin acceptor was observed demonstrating that in these systems FRET was facile but not quantitative. It was verified that as the chain length of the polymer increases the donor emission intensity increases as the result of the reduced probability of FRET. In compound 32, due to the extremely short average donor-acceptor distance, a quantitative FRET was observed. Besides the chain length, it was verified that poor solvents seem to further increase the degree of site isolation due to a structural collapse of the polymer backbone giving rise to a more densely packed structure around the core unit and a reduced average donor-acceptor distance. This observation was supported by Scheme 7. Route to coumarin-porphyrin conjugates reported by Fréchet and co-workers [53,54].
Bulk polymerization of ε-caprolactone with the initiator 31, with tin(II) 2-ethylhexanoate as the catalyst, followed by esterification of the resulting polymer with coumarin-3-carboxylic acid chloride gave 33 in quantitative yield. Polymers 33 with varying chain lengths were prepared in almost quantitative yields by adjusting the monomer-to-initiator ratio. The 16 coumarin units in compounds 32 and 33 are responsible for the large absorption in the UV region of the spectrum. It was found that the presence of coumarin donor chromophores in these systems was particularly useful to evaluate the isolation of the core functionalities by using fluorescence resonance energy transfer (FRET). When the coumarin units were excited selectively at λ = 350 nm, the emission from both the coumarin donor and the porphyrin acceptor was observed demonstrating that in these systems FRET was facile but not quantitative. It was verified that as the chain length of the polymer increases the donor emission intensity increases as the result of the reduced probability of FRET. In compound 32, due to the extremely short average donor-acceptor distance, a quantitative FRET was observed. Besides the chain length, it was verified that poor solvents seem to further increase the degree of site isolation due to a structural collapse of the polymer backbone giving rise to a more densely packed structure around the core unit and a reduced average donor-acceptor distance. This observation was supported by pulsed field gradient spin-echo (PGSE) NMR experiments that allowed the direct determination of the polymers molecular sizes in different solvents.
Mao and Song also used meso-tetrakis(3,5-dihydroxyphenyl)porphyrin (30) as a platform to synthesize three porphyrin-core dendrimers bearing eight coumarin units (Scheme 8) [56]. Dendrimer 36 was prepared in 85% yield by reacting porphyrin 30 with the coumarin derivative 34. Dendrimers 37a and 37b were synthesized in 73-75% yield by coupling porphyrin 30 with the carboxylic acid terminated coumarins 35a,b in the presence of DCC (N,N -dicyclohexylcarbodiimide) and DPTS (4-(dimethylamino)pyridinium p-toluenesulfonate). The study of the photophysical properties of the dendrimers in CH 2 Cl 2 solutions and in thin neat films revealed an intramolecular energy transfer from the coumarin units to the porphyrin core. The best energy-transfer efficiencies were found for the dendrimers 37a and 37b due to a better spectral overlap between the emission spectrum of the coumarin units and the absorption spectrum of the porphyrin moiety than in dendrimer 36. Comparing the optical properties of both dendrimers 37, it was found that the energy-transfer efficiency is better for 37b than 37a in both solid film and solution, probably due to the presence of the longer alkyl side-chain which improves its solubility and consequently prevents the coumarins from self-quenching. All dendrimers emit red light with higher fluorescence quantum yields than the free-base porphyrin. It was remarked that these systems could be applied as light-harvesting antenna. pulsed field gradient spin-echo (PGSE) NMR experiments that allowed the direct determination of the polymers molecular sizes in different solvents. Mao and Song also used meso-tetrakis (3,5-dihydroxyphenyl)porphyrin (30) as a platform to synthesize three porphyrin-core dendrimers bearing eight coumarin units (Scheme 8) [56]. Dendrimer 36 was prepared in 85% yield by reacting porphyrin 30 with the coumarin derivative 34. Dendrimers 37a and 37b were synthesized in 73-75% yield by coupling porphyrin 30 with the carboxylic acid terminated coumarins 35a,b in the presence of DCC (N,N′-dicyclohexylcarbodiimide) and DPTS (4-(dimethylamino)pyridinium p-toluenesulfonate). The study of the photophysical properties of the dendrimers in CH2Cl2 solutions and in thin neat films revealed an intramolecular energy transfer from the coumarin units to the porphyrin core. The best energy-transfer efficiencies were found for the dendrimers 37a and 37b due to a better spectral overlap between the emission spectrum of the coumarin units and the absorption spectrum of the porphyrin moiety than in dendrimer 36.
Comparing the optical properties of both dendrimers 37, it was found that the energy-transfer efficiency is better for 37b than 37a in both solid film and solution, probably due to the presence of the longer alkyl side-chain which improves its solubility and consequently prevents the coumarins from self-quenching. All dendrimers emit red light with higher fluorescence quantum yields than the free-base porphyrin. It was remarked that these systems could be applied as light-harvesting antenna. Scheme 8. Synthesis of three porphyrin-core dendrimers with eight coumarin units [56].
Marcos and co-workers reported a new class of porphyrin-core dendrimers bearing 12 coumarin units via acylation of meso-tetrakis(4-hydroxyphenyl)porphyrin 38 with the coumarin-substituted benzoic acid derivative 39 (Scheme 9) [57]. The resulting compound 40 was obtained in 55% yield. Metalation of the free-base dendrimer 40 with zinc(II) acetate or with copper(II) acetate in CHCl3-MeOH afforded the corresponding zinc(II) or copper(II) complexes. All dendrimers formed nematic discotic mesophases and the charge mobility values of these materials are the highest ever reported for a nematic discotic phase. Excitation of the coumarin moieties (λexc = 320 nm) leaded to energy transfer Scheme 8. Synthesis of three porphyrin-core dendrimers with eight coumarin units [56].
Marcos and co-workers reported a new class of porphyrin-core dendrimers bearing 12 coumarin units via acylation of meso-tetrakis(4-hydroxyphenyl)porphyrin 38 with the coumarin-substituted benzoic acid derivative 39 (Scheme 9) [57]. The resulting compound 40 was obtained in 55% yield. Metalation of the free-base dendrimer 40 with zinc(II) acetate or with copper(II) acetate in CHCl 3 -MeOH afforded the corresponding zinc(II) or copper(II) complexes. All dendrimers formed nematic discotic mesophases and the charge mobility values of these materials are the highest ever reported for a nematic discotic phase. Excitation of the coumarin moieties (λ exc = 320 nm) leaded to energy transfer to the porphyrin core. However, emission from both the coumarin units and the porphyrin acceptor was observed, thus demonstrating that FRET was facile but not quantitative in these systems [57]. to the porphyrin core. However, emission from both the coumarin units and the porphyrin acceptor was observed, thus demonstrating that FRET was facile but not quantitative in these systems [57].
Lin and co-workers also used meso-tetrakis(4-hydroxyphenyl)porphyrin (38) as a platform to synthesize a coumarin-porphyrin dyad (Scheme 10) [58]. This platform was alkylated with ethyl bromoacetate and the carboxylic acid 42 was obtained after hydrolysis of the ester group. The new dyad 43 was then prepared in 68% yield by coupling the amine-functionalized coumarin 41 with the carboxylic acid 42 in the presence of benzotriazol-1-yloxytris(dimethylamino)phosphonium hexafluorophosphate (BOP) and triethylamine. The dyad is highly selective and sensitive to thiols, exhibiting a remarkable change in emission colour from red to blue, being suitable for ratiometric fluorescence imaging of thiols in living cells.
Lin and co-workers also used meso-tetrakis(4-hydroxyphenyl)porphyrin (38) as a platform to synthesize a coumarin-porphyrin dyad (Scheme 10) [58]. This platform was alkylated with ethyl bromoacetate and the carboxylic acid 42 was obtained after hydrolysis of the ester group. The new dyad 43 was then prepared in 68% yield by coupling the amine-functionalized coumarin 41 with the carboxylic acid 42 in the presence of benzotriazol-1-yloxytris(dimethylamino)phosphonium hexafluorophosphate (BOP) and triethylamine. The dyad is highly selective and sensitive to thiols, exhibiting a remarkable change in emission colour from red to blue, being suitable for ratiometric fluorescence imaging of thiols in living cells.
Marcos and co-workers reported the formation of supramolecular system based on hydrogenbonding between a porphyrin core and carboxylic acid dendrons functionalized with coumarin units (Scheme 12) [61]. The supramolecular porphyrin-coumarin dendrimers were prepared by mixing a dichloromethane solution of meso-tetra(4-pyridyl)porphyrin (46), or its Zn(II) complex (Zn46), and Scheme 10. A coumarin-porphyrin dyad reported by Weiying Lin and co-workers [58]. Marcos and co-workers reported the formation of supramolecular system based on hydrogenbonding between a porphyrin core and carboxylic acid dendrons functionalized with coumarin units (Scheme 12) [61]. The supramolecular porphyrin-coumarin dendrimers were prepared by mixing a dichloromethane solution of meso-tetra(4-pyridyl)porphyrin (46), or its Zn(II) complex (Zn46), and Scheme 11. Synthesis of a donor-acceptor system [60].
Marcos and co-workers reported the formation of supramolecular system based on hydrogen-bonding between a porphyrin core and carboxylic acid dendrons functionalized with coumarin units (Scheme 12) [61]. The supramolecular porphyrin-coumarin dendrimers were prepared by mixing a dichloromethane solution of meso-tetra(4-pyridyl)porphyrin (46), or its Zn(II) complex (Zn46), and four equivalents of the carboxylic acid 47. The slow evaporation of the solvent by stirring at room temperature afforded the dendrimers 48 and Zn48. Their stoichiometry in the condensed phase is 1:4, as corroborated by NMR spectroscopy. These supramolecular complexes do not show liquid crystalline behaviour and their absorption and emission spectra are a combination of the spectra of the corresponding building blocks. The lack of energy transfer between the two chromophores is probably due to the long distance between them. four equivalents of the carboxylic acid 47. The slow evaporation of the solvent by stirring at room temperature afforded the dendrimers 48 and Zn48. Their stoichiometry in the condensed phase is 1:4, as corroborated by NMR spectroscopy. These supramolecular complexes do not show liquid crystalline behaviour and their absorption and emission spectra are a combination of the spectra of the corresponding building blocks. The lack of energy transfer between the two chromophores is probably due to the long distance between them.
Gust and co-workers reported the synthesis of a molecular hexad 50 comprising two porphyrin moieties and four coumarin antenna chromophores, all organized by a central hexaphenylbenzene core (Scheme 13) [62]. The metalated hexad self-assembles with a pyridyl-bearing fullerene moiety, through coordination with the zinc atoms of the porphyrins, to yield the artificial photosynthetic reaction center 51.
It was shown that light absorbed by any of the coumarins in hexad 50 is transferred to a porphyrin on the 1-10 ps time scale, depending on the site of initial excitation. The quantum yield of singlet energy transfer is 1.0. In heptad 51, energy transfer to the porphyrins is followed by photoinduced electron transfer to the fullerene, resulting in a charge-separated state (P •+ -C60 •− ) with an overall quantum yield of 1.0 [62].
Compound 50 was prepared in 90% yield by coupling compound 49 with coumarin 343 using 1-ethyl-3-(3-dimethylaminopropyl)carbodiimide (EDCI) and 4-dimethylaminopyridine (DMAP). The synthesis of other compounds of type 50, with one or two coumarin units (52-54, Figure 3), was also reported [62]. Gust and co-workers reported the synthesis of a molecular hexad 50 comprising two porphyrin moieties and four coumarin antenna chromophores, all organized by a central hexaphenylbenzene core (Scheme 13) [62]. The metalated hexad self-assembles with a pyridyl-bearing fullerene moiety, through coordination with the zinc atoms of the porphyrins, to yield the artificial photosynthetic reaction center 51.
It was shown that light absorbed by any of the coumarins in hexad 50 is transferred to a porphyrin on the 1-10 ps time scale, depending on the site of initial excitation. The quantum yield of singlet energy transfer is 1.0. In heptad 51, energy transfer to the porphyrins is followed by photoinduced electron transfer to the fullerene, resulting in a charge-separated state (P •+ -C 60 •− ) with an overall quantum yield of 1.0 [62].
Compound 50 was prepared in 90% yield by coupling compound 49 with coumarin 343 using 1-ethyl-3-(3-dimethylaminopropyl)carbodiimide (EDCI) and 4-dimethylaminopyridine (DMAP). The synthesis of other compounds of type 50, with one or two coumarin units (52-54, Figure 3), was also reported [62].    These studies allowed to conclude that in spite of the relatively long, flexible ester linkages between the coumarins and the hexaphenylbenzene ring, coumarin moieties are well suited as antennas in the 400−460 nm spectral range for porphyrin based artificial photosynthetic reaction centers. The high transfer rates, and therefore efficiencies, are ensured by coumarin singlet excited state lifetimes of several ns and high fluorescence quantum yields.

Coumarin-Phthalocyanine Dyads
Several coumarin-phthalocyanine conjugates have been reported in the last years. Many of those conjugates were synthesized from substituted 7-hydroxycoumarins 55 following the synthetic route shown in Scheme 14. Typically the first step involves the formation of a coumarin-substituted phthalonitrile, usually by nucleophilic displacement of a nitro group in 3-or 4-nitrophthalonitrile, and the resulting phthalonitriles 56 are then converted into metallophthalocyanines 57 by cyclotetramerization in 2-(dimethylamino)ethanol in the presence of a metal salt. The coumarins and phthalonitriles used in many of these reactions, and the metals in the phthalocyanine complexes, are shown in Table 1  . These studies allowed to conclude that in spite of the relatively long, flexible ester linkages between the coumarins and the hexaphenylbenzene ring, coumarin moieties are well suited as antennas in the 400−460 nm spectral range for porphyrin based artificial photosynthetic reaction centers. The high transfer rates, and therefore efficiencies, are ensured by coumarin singlet excited state lifetimes of several ns and high fluorescence quantum yields.
A recent study report the preparation of four coumarin-phthalocyanine conjugates bearing only one coumarin unit in which the coumarin moiety is linked to the phthalocyanine core at position 1 or 2 via a tri(ethylene glycol) spacer (63, Scheme 17) [105]. These conjugates were evaluated as potential anticancer agents with dual photodynamic and chemotherapy activity. Upon illumination at 670 nm, they show substantial cytotoxicity against HepG2 human hepatocarcinoma cells, with IC 50 values in the range of 0.014-0.044 µM. The conjugate bearing the coumarin substituent at position 1 of the phthalocyanine (and R 1 = H) exhibits high photocytotoxicity and significant chemocytotoxicity (IC 50 = 4.43 µM). The results indicate that the coumarin and the phthalocyanine components of this conjugate work in a cooperative fashion [105]. A recent study report the preparation of four coumarin-phthalocyanine conjugates bearing only one coumarin unit in which the coumarin moiety is linked to the phthalocyanine core at position 1 or 2 via a tri(ethylene glycol) spacer (63, Scheme 17) [105]. These conjugates were evaluated as potential anticancer agents with dual photodynamic and chemotherapy activity. Upon illumination at 670 nm, they show substantial cytotoxicity against HepG2 human hepatocarcinoma cells, with IC50 values in the range of 0.014-0.044 µM. The conjugate bearing the coumarin substituent at position 1 of the phthalocyanine (and R 1 = H) exhibits high photocytotoxicity and significant chemocytotoxicity (IC50 = 4.43 µM). The results indicate that the coumarin and the phthalocyanine components of this conjugate work in a cooperative fashion [105]. Scheme 17. Synthesis of coumarin-phthalocyanine conjugates [105].
Bulut and co-workers reported the synthesis of the axial coumarin-substituted titanium(IV) phthalocyanines 66a,b and their characterization by IR, UV-Vis, fluorescence, 1 H-NMR, and MALDI-TOF MS [106]. The new conjugates were obtained in high yields from the reaction of the ortho-dihydroxyphenylcoumarin derivatives 64a,b with the oxotitanium(IV) phthalocyanine 65 (Scheme 18). The UV-Vis spectra revealed small red-shifts of the Q-bands of the conjugates 66a,b when compared to the Q-band of the oxotitanium(IV) phthalocyanine 65. They also suggested that the conjugates have low aggregation tendency in nonpolar solvents. The fluorescence studies showed that Scheme 17. Synthesis of coumarin-phthalocyanine conjugates [105].
Bulut and co-workers reported the synthesis of the axial coumarin-substituted titanium(IV) phthalocyanines 66a,b and their characterization by IR, UV-Vis, fluorescence, 1 H-NMR, and MALDI-TOF MS [106]. The new conjugates were obtained in high yields from the reaction of the ortho-dihydroxyphenylcoumarin derivatives 64a,b with the oxotitanium(IV) phthalocyanine 65 (Scheme 18). The UV-Vis spectra revealed small red-shifts of the Q-bands of the conjugates 66a,b when compared to the Q-band of the oxotitanium(IV) phthalocyanine 65. They also suggested that the conjugates have low aggregation tendency in nonpolar solvents. The fluorescence studies showed that the emission intensity is diminished by the axial coumarin substituents. Metal-insulatorsemiconductor capacitors incorporating spin coated films of phthalocyanines 65 and 66a,b as the insulating layer showed a rectification behavior.

Coumarin-Corrole Conjugates
Corroles display highly interesting and unusual photophysical and chemical properties. The methods for their functionalization were reviewed recently [107]. Despite the importance of such tetrapyrrolic compounds, published works on the synthesis of coumarin-corrole conjugates are scarce. In fact, the first synthesis of coumarin-corrole conjugates was reported only in 2010 by Gryko and co-workers [108]. These authors used two distinct approaches to synthesize the coumarin-corrole conjugates: (a) direct synthesis of the conjugates from the condensation of a dipyrromethane with a coumarincarbaldehyde (Scheme 19) or (b) functionalization of an ethynyl-substituted corrole with a bromocoumarin derivative via a Sonogashira reaction (Scheme 20).
The method used to prepare conjugates 69a-c, that bear a direct link between both chromophores, involved the condensation of 5-(pentafluorophenyl)dipyrromethane 67 [109] with the coumarincarbaldehydes 68a-c in CH2Cl2/trifluoroacetic acid (TFA) followed by oxidation with DDQ, according to established conditions [110]. The authors justified the relative low yields obtained in the [2 + 1] strategy for corroles 69a-c due to a competitive Michael addition of the dipyrromethane to the coumarin α,β-unsaturated system.

Coumarin-Corrole Conjugates
Corroles display highly interesting and unusual photophysical and chemical properties. The methods for their functionalization were reviewed recently [107]. Despite the importance of such tetrapyrrolic compounds, published works on the synthesis of coumarin-corrole conjugates are scarce. In fact, the first synthesis of coumarin-corrole conjugates was reported only in 2010 by Gryko and co-workers [108]. These authors used two distinct approaches to synthesize the coumarin-corrole conjugates: (a) direct synthesis of the conjugates from the condensation of a dipyrromethane with a coumarincarbaldehyde (Scheme 19) or (b) functionalization of an ethynyl-substituted corrole with a bromocoumarin derivative via a Sonogashira reaction (Scheme 20).
The method used to prepare conjugates 69a-c, that bear a direct link between both chromophores, involved the condensation of 5-(pentafluorophenyl)dipyrromethane 67 [109] with the coumarincarbaldehydes 68a-c in CH 2 Cl 2 /trifluoroacetic acid (TFA) followed by oxidation with DDQ, according to established conditions [110]. The authors justified the relative low yields obtained in the [2 + 1] strategy for corroles 69a-c due to a competitive Michael addition of the dipyrromethane to the coumarin α,β-unsaturated system.
The method used to prepare conjugates 69a-c, that bear a direct link between both chromophores, involved the condensation of 5-(pentafluorophenyl)dipyrromethane 67 [109] with the coumarincarbaldehydes 68a-c in CH2Cl2/trifluoroacetic acid (TFA) followed by oxidation with DDQ, according to established conditions [110]. The authors justified the relative low yields obtained in the [2 + 1] strategy for corroles 69a-c due to a competitive Michael addition of the dipyrromethane to the coumarin α,β-unsaturated system. The dyad 73 was synthesized by coupling the ethynyl-corrole 71 with the adequate bromoketobiscoumarin 72 under copper-free Sonogashira conditions (Scheme 20) [108]. Corrole 71 was obtained from the reaction of the TMS-protected ethynylbenzaldehyde 70 [111] with dipyrromethane 67 in aqueous methanol in the presence of HCl, followed by oxidation with DDQ [112] and then removal of the protecting group with tetrabutylammonium fluoride (TBAF).
Spectroscopic studies revealed that in all dyads the electronic coupling between the components is weak. In addition, there is a quantitative and extremely fast energy transfer from the coumarin moiety to the corrole unit [108]. This behaviour was justified considering the significant Stokes shift and the resulting overlap of coumarin emission with corrole absorption as well as the short spacer between the two units. The energy transfer was ascribed to a dipole-dipole mechanism. In dyad 69b it was detected an electron-transfer from the excited corrole to the coumarin, yielding the low lying charge separated state Cum − -Corr + .
The same group extended the copper-free Sonogashira approach to the synthesis of dyads 74 and 75 (Figure 4) [113]. The coupling involved the ethynyl-corrole 71 and the adequate 6bromocoumarins. The cross-coupling reactions were performed in DMF in the presence of Pd(AcO)2, PPh3 and Cs2CO3 and the dyads were obtained in moderate yields.
In the same article it was also reported the synthesis of a series of coumarin-corrole dyads (76-Scheme 20. Coumarin-corrole dyad obtained under copper-free Sonogashira conditions [108]. The dyad 73 was synthesized by coupling the ethynyl-corrole 71 with the adequate bromoketobiscoumarin 72 under copper-free Sonogashira conditions (Scheme 20) [108]. Corrole 71 was obtained from the reaction of the TMS-protected ethynylbenzaldehyde 70 [111] with dipyrromethane 67 in aqueous methanol in the presence of HCl, followed by oxidation with DDQ [112] and then removal of the protecting group with tetrabutylammonium fluoride (TBAF).
Spectroscopic studies revealed that in all dyads the electronic coupling between the components is weak. In addition, there is a quantitative and extremely fast energy transfer from the coumarin moiety to the corrole unit [108]. This behaviour was justified considering the significant Stokes shift and the resulting overlap of coumarin emission with corrole absorption as well as the short spacer between the two units. The energy transfer was ascribed to a dipole-dipole mechanism. In dyad 69b it was detected an electron-transfer from the excited corrole to the coumarin, yielding the low lying charge separated state Cum − -Corr + .
The same group extended the copper-free Sonogashira approach to the synthesis of dyads 74 and 75 ( Figure 4) [113]. The coupling involved the ethynyl-corrole 71 and the adequate 6-bromocoumarins. The cross-coupling reactions were performed in DMF in the presence of Pd(AcO) 2 , PPh 3 and Cs 2 CO 3 and the dyads were obtained in moderate yields.
In the same article it was also reported the synthesis of a series of coumarin-corrole dyads (76-80, Figure 5) via condensation of dipyrromethane 67 with suitable formylcoumarins [113]. These condensations were performed in CH 2 Cl 2 /trifluoroacetic acid followed by oxidation with DDQ and again the competitive Michael addition of the dipyrromethane to the α,β-unsaturated coumarins was considered responsible by the low yields of the desired dyads.   Gryko, Wróbel and co-workers reported the synthesis of several trans-A2B-corroles, where A is the C6F5 group and B is an aryl or hetaryl group, and their use in a comparative study of their spectroscopic features [114]. One of those compounds was the coumarin-corrole 82 that was obtained from the reaction of dipyrromethane 67 with the coumarin-4-carbaldehyde 81 (Scheme 21). The yield obtained (16%) is much higher than the ones of related systems reported in previous studies (ca. 5-8%) [108,113]. This result was attributed to the much weaker polarization of 7,8-dimetoxycoumarin-4-carbaldehyde 81 and consequently the side reactions were minimized. Spectroscopic studies (absorption and   Gryko, Wróbel and co-workers reported the synthesis of several trans-A2B-corroles, where A is the C6F5 group and B is an aryl or hetaryl group, and their use in a comparative study of their spectroscopic features [114]. One of those compounds was the coumarin-corrole 82 that was obtained from the reaction of dipyrromethane 67 with the coumarin-4-carbaldehyde 81 (Scheme 21). The yield obtained (16%) is much higher than the ones of related systems reported in previous studies (ca. 5-8%) [108,113]. This result was attributed to the much weaker polarization of 7,8-dimetoxycoumarin-4-carbaldehyde Gryko, Wróbel and co-workers reported the synthesis of several trans-A 2 B-corroles, where A is the C 6 F 5 group and B is an aryl or hetaryl group, and their use in a comparative study of their spectroscopic features [114]. One of those compounds was the coumarin-corrole 82 that was obtained from the reaction of dipyrromethane 67 with the coumarin-4-carbaldehyde 81 (Scheme 21). The yield obtained (16%) is much higher than the ones of related systems reported in previous studies (ca. 5-8%) [108,113]. This result was attributed to the much weaker polarization of 7,8-dimetoxycoumarin-4-carbaldehyde 81 and consequently the side reactions were minimized. Spectroscopic studies (absorption and excitation emission and fluorescence life-time values) of this dye in chloroform allowed to rule out the formation of aggregates even in highly concentrated solutions. The experimental data were supported by quantum chemical calculations (TD-DFT) of the HOMO and the LUMO. The electron spin resonance (ESR) studies before and after light illumination demonstrated that an unpaired electron is localized on the corrole core but not on the substituent. Neves and co-workers developed a new strategy to prepare coumarin-corrole dyads where the coumarin unit is linked to a β-pyrrolic position of the corrole [39]. The new method involved a hetero-Diels-Alder reaction between the 3-vinylcorrole 83 [115] with o-quinone methides generated in situ from 4-hydroxycoumarins 2a,b and paraformaldehyde (Scheme 22). The reactions were performed in refluxing dioxane and the cycloadducts 84a,b were obtained in excellent yields.
The characterization of the photophysical properties of these dyads in various solvents (dichloromethane, DMSO, toluene, and ethanol) showed a strong solvatochromic effect for compound 84b, easily detected by naked eye (Figure 6): a bathochromic shift of the absorption bands occurs with the increase of the solvent polarity. The sensorial ability of the coumarin-corrole dyads 84a,b towards spherical (F − , Cl − ), linear (CN − ), and bulky (CH3COO − ) anions was evaluated by UV-vis and fluorescence measurements and the more drastic alterations were detected for fluoride, cyanide and acetate. Scheme 21. Synthesis of the dyad 82 [114].
Neves and co-workers developed a new strategy to prepare coumarin-corrole dyads where the coumarin unit is linked to a β-pyrrolic position of the corrole [39]. The new method involved a hetero-Diels-Alder reaction between the 3-vinylcorrole 83 [115] with o-quinone methides generated in situ from 4-hydroxycoumarins 2a,b and paraformaldehyde (Scheme 22). The reactions were performed in refluxing dioxane and the cycloadducts 84a,b were obtained in excellent yields. Neves and co-workers developed a new strategy to prepare coumarin-corrole dyads where the coumarin unit is linked to a β-pyrrolic position of the corrole [39]. The new method involved a hetero-Diels-Alder reaction between the 3-vinylcorrole 83 [115] with o-quinone methides generated in situ from 4-hydroxycoumarins 2a,b and paraformaldehyde (Scheme 22). The reactions were performed in refluxing dioxane and the cycloadducts 84a,b were obtained in excellent yields.
The characterization of the photophysical properties of these dyads in various solvents (dichloromethane, DMSO, toluene, and ethanol) showed a strong solvatochromic effect for compound 84b, easily detected by naked eye (Figure 6): a bathochromic shift of the absorption bands occurs with the increase of the solvent polarity. The sensorial ability of the coumarin-corrole dyads 84a,b towards spherical (F − , Cl − ), linear (CN − ), and bulky (CH3COO − ) anions was evaluated by UV-vis and fluorescence measurements and the more drastic alterations were detected for fluoride, cyanide and acetate. Scheme 22. Synthesis of coumarin-corrole conjugates via hetero-Diels-Alder reactions [39].
The characterization of the photophysical properties of these dyads in various solvents (dichloromethane, DMSO, toluene, and ethanol) showed a strong solvatochromic effect for compound 84b, easily detected by naked eye (Figure 6): a bathochromic shift of the absorption bands occurs with the increase of the solvent polarity. The sensorial ability of the coumarin-corrole dyads 84a,b towards spherical (F − , Cl − ), linear (CN − ), and bulky (CH 3 COO − ) anions was evaluated by UV-vis and fluorescence measurements and the more drastic alterations were detected for fluoride, cyanide and acetate.
The characterization of the photophysical properties of these dyads in various solvents (dichloromethane, DMSO, toluene, and ethanol) showed a strong solvatochromic effect for compound 84b, easily detected by naked eye (Figure 6): a bathochromic shift of the absorption bands occurs with the increase of the solvent polarity. The sensorial ability of the coumarin-corrole dyads 84a,b towards spherical (F − , Cl − ), linear (CN − ), and bulky (CH3COO − ) anions was evaluated by UV-vis and fluorescence measurements and the more drastic alterations were detected for fluoride, cyanide and acetate.