Open Access Article
Vy-Phuong
Tran
a,
Arup
Kundu
b,
Madelyn N.
Scott
b,
Ainsley
Iwanicki
b,
Phattananawee
Nalaoh
c,
James R.
Diers
d,
Masahiko
Taniguchi
a,
David F.
Bocian
d,
Gabriela S.
Schlau-Cohen
*b and
Jonathan S.
Lindsey
*a
aDepartment of Chemistry, North Carolina State University, Raleigh, NC 27695, USA. E-mail: jlindsey@ncsu.edu
bDepartment of Chemistry, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA. E-mail: gssc@mit.edu
cDepartment of Chemistry, University of Tennessee, Knoxville, TN 37996, USA. E-mail: pnalaoh@utk.edu
dDepartment of Chemistry, University of California, Riverside, California 92521-0403, USA. E-mail: david.bocian@ucr.edu
First published on 14th January 2026
A self-assembly paradigm is provided in green photosynthetic bacteria by the chlorin macrocycle bacteriochlorophyll (BChl) c, which contains a 3-(1-hydroxyethyl) substituent, central magnesium ion, and 13-keto group. The assembled BChl c structure is a powerful light-harvesting apparatus that can support life even under extreme low-light conditions. Here, inspired by the work of Balaban, two far simpler porphyrins have been synthesized, 5,15-bis(hydroxymethyl)-10,20-diphenylporphinatozinc(II) (Ph/CH2OH) and 5,15-bis(hydroxymethyl)porphinatozinc(II) (H/CH2OH), and analogues wherein ethyl replaces hydroxymethyl (Ph/Et and H/Et). Examination of Ph/CH2OH and H/CH2OH by time-resolved spectroscopy showed an ∼2-fold enhancement in the singlet excited-state lifetime compared to meso-tetraphenylporphinatozinc(II) (ZnTPP). The single-crystal X-ray diffraction revealed distinct packing patterns. Porphyrin Ph/CH2OH exhibited double staircases wherein (1) each zinc is pentacoordinate (by apical coordination of one hydroxymethyl group of a porphyrin in the same staircase), (2) the second hydroxymethyl group is hydrogen-bonded to an apically coordinated hydroxymethyl oxygen atom in the adjacent staircase, (3) the porphyrins in a given staircase are coplanar but cofacially offset with each other, and (4) the adjacent staircases are oriented approximately 72° relative to each other. Porphyrin H/CH2OH assembled wherein (1) each zinc is hexacoordinate by ligation of hydroxymethyl moieties, (2) each hydroxymethyl –OH is hydrogen-bonded with an acetonitrile solvent molecule in the lattice, and (3) the planes of the four nearest neighbor porphyrins are essentially perpendicular to a given porphyrin. Study of the solid-state packing patterns of sparsely substituted porphyrins enables insights into how the structural design of tetrapyrroles can guide their aggregate self-assembly.
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| Fig. 1 Native bacteriochlorophyll c and proposed molecular interactions in the self-assembly.4 Many substituents are omitted for clarity. | ||
Much effort has been devoted to understand the essential structural features that undergird the assembly into functional light-harvesting antennas. Tamiaki has employed semisynthesis with derivatives of natural pigments to create diverse macrocycles for probing the role of structural substituents on the self-assembly pattern.5–12 Balaban pioneered the design and synthesis of a set of far simpler porphyrins, which upon self-assembly give broad and red-shifted absorption maxima.9,13–21 The evolution of the Balaban design is shown in the 10,20-diaryl family by the 3,13-substitution pattern of I,14 the 3,15-substitution pattern of II15 and III,4 and the 5,15-substitution pattern of IV,14V,14 and VI22 (Chart 1). The 3,13-substitution pattern also was examined in the β-substituted porphyrin VII.14 In all cases, the zinc chelate was employed as a chemically more robust surrogate for magnesium. Among this set, porphyrins III,4IV,16 and VI4 have been characterized by single-crystal X-ray diffraction (SCXRD) analysis. The pioneering work of Balaban (1958–2016) was left undeveloped owing to his untimely passing.23
The question of interest here is whether even simpler molecular designs can afford chlorosomal-like assemblies. In this work, four meso-substituted zinc(II)porphyrins have been synthesized (Chart 1). Two porphyrins contain 5,15-dihydroxymethyl groups with the presence of 10,20-diphenyl groups (Ph/CH2OH) or with the lack of 10,20-diphenyl group (H/CH2OH). Two other porphyrins (Ph/Et, H/Et) have identical substitution patterns but with an ethyl group in place of the hydroxymethyl substituent. The electronic properties and dynamics of the synthetic porphyrins have been characterized by steady-state and time-resolved spectroscopy. All four porphyrins were also analyzed by SCXRD for comparative assessment of their structural packing patterns. The results provide insights into the relationship between the structure and assembly of simple compounds as putative analogs of chlorosomal bacteriochlorophylls.
For the synthesis of porphyrin H/CH2OH, dipyrromethane 1 was treated with Eschenmoser's reagent to give the 1,9-bis(dimethylaminomethyl)-substituted dipyrromethane as the bis(hydroiodide) salt. Treatment of the reaction mixture with saturated aqueous NaHCO3 liberated the free base dipyrromethane 1-Esch from the bis(hydroiodide) salt. Dipyrromethane 1-Esch was not characterized but was reacted in situ with dipyrromethane 1 in the standard way25 to form zinc porphyrin 5 in 11.5% yield. Deprotection with TBAF gave zinc porphyrin H/CH2OH in 90% yield.
An established route to dipyrromethane-1-carbinols was applied for the synthesis of porphyrin Ph/Et. The meso-ethyldipyrromethane266 was treated with EtMgBr followed by pyridyl thioester277 to obtain 1-acyldipyrromethane 8 in 90% yield (Scheme 2). Reduction of 8 gave the dipyrromethane-1-carbinol, which was condensed in the presence of InCl3 to afford the trans-A2B2-porphyrin, 5,15-diethyl-10,20-diphenylporphyrin (9), in 37% yield. Subsequent reaction with Zn(OAc)2 gave the target zinc(II) chelate Ph/Et in (80%).
The meso-ethyldipyrromethane266 also was treated with the Eschenmoser reagent to give the 1,9-bis(N,N-dimethylaminomethyl)dipyrromethane 6-Esch. Treatment to the standard conditions established in the Eschenmoser route with dipyrromethane 6 gave zinc porphyrin H/Et in 8.3% yield.
Each porphyrin was characterized by 1H NMR spectroscopy, 13C{1H} NMR spectroscopy, high-resolution mass spectrometry via electrospray ionization-time-of-flight (HRMS via ESI-TOF), matrix-assisted laser desorption ionization mass spectrometry (MALDI-MS),28 and absorption and fluorescence spectroscopy. The symmetry and sparse substitution of each of the four porphyrins afford simple and readily interpretable 1H NMR spectra (Fig. S1). The results from absorption and fluorescence spectroscopy are described in the next section.
All of the following data for the four zinc porphyrins were obtained in aerated neat THF solution. Each porphyrin exhibits the characteristic B-band (Soret or S0 → S2) and Q-band (S0 → S1) transitions. The Q-band transitions exhibit a vibronic progression, denoted as Q(0,0) and Q(1,0) for the transitions with zero and one vibrational quanta (respectively), with a spacing ranging from ∼950–1280 cm−1 for each porphyrin (Fig. 2). Expanded spectra are provided in Fig. S2–S6. The spectral features are summarized in Table 1. Several trends are evident.
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| Fig. 2 Absorption spectra (solid lines) of the Q-band region and fluorescence spectra (dashed lines) of the four synthetic porphyrins in aerated THF solution at room temperature. | ||
| Sample | λ abs, nm | λ em, nm | I B(0,0)/IQ(1,0)b | Stokes shift, cm−1 | I Q(1,0)/IQ(0,0)b | |||
|---|---|---|---|---|---|---|---|---|
| B | Q(1,0) | Q(0,0) | Q(0,0) | Q(0,1) | ||||
| a All data were obtained in aerated THF solution at room temperature. b Ratio of peak intensities. | ||||||||
| Ph/CH2OH | 421 | 555 | 594 | 602 | 654 | 23 | 224 | 5.7 |
| Ph/Et | 424 | 558 | 601 | 607 | 661 | 28 | 164 | 2.4 |
| H/CH2OH | 408 | 543 | 578 | 582 | 637 | 29 | 119 | 3.7 |
| H/Et | 410 | 546 | 576 | 591 | 645 | 30 | 441 | 9.0 |
| ZnTPP | 423 | 555 | 595 | 603 | 655 | 31 | 223 | 3.2 |
• First, the porphyrins with four meso-substituents (Ph/CH2OH, Ph/Et) exhibit B (421, 424 versus 408, 410 nm) and Q(1,0) (555, 558 versus 543, 546 nm) bands at longer wavelength than porphyrins with two meso-substituents (H/CH2OH, H/Et). Such shifts are consistent with the previous observation of a systematic bathochromic shift in the absorption spectra of zinc porphyrins with an increase in the number of substituted phenyl groups.29
• Second, the addition of an ethyl group instead of a hydroxymethyl group generally causes a bathochromic shift of several nanometers for the B and Q bands, although one apparent exception is the Q(0,0) band of H/Et (576 nm) versusH/CH2OH (578 nm); this may simply reflect the relatively very weak band Q(0,0) band on the tail of the more intense Q(1,0) band of H/Et.
• Third, the relative intensity of the Q(0,0) band is sensitive to the nature of the substituents, as is seen by the ratio of the intensities of the Q(1,0) and Q(0,0) bands, which ranges from 2.4 for Ph/Et to 9.0 for H/Et.
| Sample | τ (ns) | Φ f | τ° (ns) | k r (s−1) | k nr (s−1) |
|---|---|---|---|---|---|
| a All data were obtained in aerated THF solution at room temperature. Lifetimes were obtained from time-correlated single-photon counting (TCSPC) measurements. Fluorescence lifetime, τ; fluorescence quantum yield, ΦF; radiative lifetime, τ°; radiative decay rate, kr; nonradiative decay rate, knr. | |||||
| Ph/CH2OH | 3.7 | 0.039 | 100 | 1.0 × 107 | 26 × 107 |
| Ph/Et | 2.03 | 0.026 | 78 | 1.3 × 107 | 48 × 107 |
| H/CH2OH | 4.2 | 0.042 | 102 | 0.98 × 107 | 23 × 107 |
| H/Et | 3.0 | 0.024 | 130 | 0.77 × 107 | 33 × 107 |
| ZnTPP | 1.87 | 0.026 | 72 | 1.4 × 107 | 52 × 107 |
Time-resolved fluorescence measurements were performed in aerated THF. The decay curves were well-fit with a monoexponential function (Fig. S7). The extracted decay timescales were 3.7 ns and 4.2 ns for the hydroxymethylporphyrins Ph/CH2OH and H/CH2OH, respectively. For analogues Ph/Et and H/Et, where the hydroxymethyl groups were replaced by ethyl groups, the timescales were slightly shorter, 2.03 and 3.0 ns, respectively. The reference compound ZnTPP exhibited a lifetime value of 1.87 ns, which closely resembles the reported consensus value of 2.0 ns (in aerated toluene).30
To understand the origin of the enhanced fluorescence observed in Ph/CH2OH and H/CH2OH, the measured emission lifetime and fluorescence quantum yield of each compound were used to calculate the radiative and nonradiative decay rates of the singlet excited state (eqn (S1)–(S3); Table 2). The nonradiative decay rates for Ph/CH2OH and H/CH2OH (26 × 107 s−1 and 23 × 107 s−1, respectively) were diminished with respect to ZnTPP (52 × 107 s−1). Further, the radiative decay rates also decreased for Ph/CH2OH and H/CH2OH (1.0 × 107 s−1 and 0.98 × 107 s−1, respectively) relative to ZnTPP (1.4 × 107 s−1). The porphyrin analogues Ph/Et and H/Et follow a similar trend, albeit to a lesser degree than Ph/CH2OH and H/CH2OH. These distinctions are attributed to differences in the nonradiative rates, which has two components, internal conversion (IC) and intersystem crossing (ISC). The rate of IC often approximately scales with the number of normal modes, but no correlation was observed between the nonradiative rate and the number of normal modes, and indeed, the overall Q(1,0) vibronic structure was similar for all four porphyrins. The yield of ISC, which is quite high in zinc porphyrins (88% for ZnTPP)29 is likely the dominant factor, although the rationale for this is not clear.
To resolve the initial excited-state dynamics, porphyrins Ph/CH2OH and H/CH2OH in aerated THF were examined by femtosecond transient absorption (fs-TA) measurements. The excited-state dynamics of the porphyrin solutions were probed using a broadband white light supercontinuum (∼400 nm to 800 nm) subsequent to 400 nm excitation, resonant with the B band. Fig. 3a shows the fs-TA spectra traces for Ph/CH2OH and H/CH2OH at representative time delays from −1 ps to 1000 ps. The timescales of the dynamics were extracted with multiexponential kinetic fitting (Fig. 3b).
After initial photoexcitation, a broad excited-state absorption (ESA) feature was present in the spectral region of 415 nm to 780 nm for both the porphyrins, along with a strong ground-state bleach (GSB) of the Q bands at 548 nm for Ph/CH2OH and 536 nm for H/CH2OH, respectively. The initial broad ESA feature is assigned to a photoexcited S2 state, which evolves to the S1 state via IC. The IC of the S2 → S1 was observed as a rise in a sharp ESA feature associated with the S1 state around 450 nm and a concomitant decay of the stimulated emission (SE) feature of the S2 state around 545 nm to 690 nm (Fig. 3a, left panel). Time constants of 0.8 ps and 1 ps were extracted for S2 → S1 IC in Ph/CH2OH and H/CH2OH, respectively. The subsequent two time constants were assigned to intramolecular vibrational relaxation (IVR) in the S1 state (4.6 ps and 134 ps for Ph/CH2OH, 5.2 ps and 90 ps for H/CH2OH). The slowest time constant (>2 ns) was assigned to the formation of a long-lived triplet state via ISC. These dynamics are summarized in Fig. 3c and are consistent with earlier reports on zinc porphyrins.31,32 Timescales obtained through the fs-TA measurements were consistent with those obtained via time-resolved fluorescence, revealing that these zinc porphyrins show an enhancement of up to 2-fold in the singlet excited-state lifetime as compared to traditional ZnTPP systems. The long-lived excited-state has the potential to enhance energy transport for synthetic light-harvesting systems and other optoelectronic applications.
The absorption spectra of the four porphyrins were simulated using the Gouterman module in PhotochemCAD.35 This calculation utilizes the four frontier MOs shown in Table 3. The calculations faithfully reproduce the relative energies of the B(0,0) and Q(0,0) bands of the four porphyrins (Fig. S8–S10). In particular, the calculations reproduce the observed bathochromic shift of the 10,20-phenyl-substitued molecules (Ph/CH2OH and Ph/Et) relative to those that lack these substituents (H/CH2OH and H/Et), as well as the additional bathochromic shifts observed upon ethyl replacement of the hydroxymethyl groups: larger in Ph/EtversusPh/CH2OH than in H/EtversusH/CH2OH. More interestingly, the calculation reproduces the observed relative intensities of the Q(0,0) bands of the four porphyrins Ph/Et > H/CH2OH > Ph/CH2OH > H/Et (Table 1). This pattern reflects the observation that ethyl replacement of the hydroxymethyl groups in the 10,20-phenyl-substituted porphyrins (Ph/EtversusPh/CH2OH) increases the intensity of the Q(0,0) absorption, whereas this substitution in the porphyrins that lack the phenyl groups (H/EtversusH/CH2OH) decreases the intensity of the Q(0,0) band. The rank ordering of the porphyrins on the basis of the relative intensity of the Q(0,0) absorption transition (Ph/Et > H/CH2OH > Ph/CH2OH > H/Et) nearly parallels that of the magnitude of the radiative rate constant (kf, Table 2) (Ph/Et > Ph/CH2OH ∼ H/CH2OH > H/Et).
A given coordination polymer of apical-ligated porphyrins is aligned alongside a second polymer of apical-ligated porphyrins. The angle between the two staircases is 72.66(3)° (Fig. 4b). The meso-phenyl groups are neither coplanar nor orthogonal with respect to the plane of the porphyrin, as is typical; here, both phenyl groups are tilted in the same direction with dihedral angles of 115.15(7)° and 108.82(7)° (Fig. S11a). The plane of the phenyl group on the porphyrin from the second staircase is rotated 75.37(10)° versus that from the first one, affording a putative CH/π interaction (2.687(3) Å) between two phenyl groups from adjacent staircases, along with the distance to the centroid belonging to the mentioned phenyl group at 3.4440(12) Å (Fig. 4b).
Although the planes of porphyrins in adjacent staircases are not parallel, the planes of every other staircase are parallel giving an overall herringbone arrangement. The two adjacent macrocycles are slipped from a completely cofacial alignment to give only partial overlap of the π clouds (Fig. 4c). The distance along the normal between the mean planes of two porphyrins in a coordination polymer is 3.4142(11) Å (Fig. 4d). The resulting translation is such that the centroid offset of porphyrins in adjacent steps is 5.3177(11) Å (Fig. S11a). The two infinite polymers thus constitute a side-by-side or double staircase comprised of cofacially offset porphyrins, which altogether affords a zigzag shape. A model for the assembly showing the key interactions of the central zinc metal and two hydroxymethyl groups is provided in Fig. 4d.
The two hydroxymethyl groups of a given porphyrin are oriented in a trans-configuration with respect to each other. The O–H bonds are not uncompensated due to the presence of molecules of acetonitrile in the crystal lattice (two CH3CN per porphyrin; in other words, one CH3CN for each hydroxymethyl group). Each hydroxymethyl group serves as a hydrogen-bond donor with the nitrogen atom of a molecule of acetonitrile (Fig. 5c). The H⋯N distances are 2.14(3) Å. The acetonitrile molecules are aligned in pairs with dipoles in opposite directions, with a distance of 3.983(4) Å from the methyl carbon of one acetonitrile molecule to the nitrogen atom of the other acetonitrile molecule (Fig. 5b). The oppositely aligned dimers of acetonitrile are solvent molecules in the porphyrin lattice.
The four adjacent, apically coordinated porphyrins form a square-shaped arrangement around a central porphyrin. Although such nearest neighbors have essentially orthogonal planes, the next-nearest neighbor porphyrins are coplanar with each other but are translated such that there is essentially no cofacial overlap. A model for the assembly showing the key interactions of the central zinc metal, two hydroxymethyl groups, and the presence of the acetonitrile molecules, is provided in Fig. 5c.
Here, zinc porphyrins are employed rather than magnesium chlorins (as in the native systems, e.g., BChl c). Both porphyrins Ph/CH2OH and H/CH2OH contain 5,15-bis(hydroxymethyl) substituents but contain or lack 10,20-diphenyl substituents. Both afford infinite coordination polymers by ligation of a hydroxymethyl group at the apical zinc site. But otherwise the crystal packing patterns are fundamentally different. In Ph/CH2OH, where phenyl groups are present, each zinc is pentacoordinate and a double staircase results in which adjacent porphyrins within a staircase are aligned along the 5,15-axis, with separation of mean planes of the two porphyrins of 3.4142(11) Å and a cofacial offset of 5.3177(11) Å; the adjacent staircases are linked by hydrogen-bonding. In H/CH2OH, where phenyl groups are absent, each zinc is hexacoordinate, the four nearest neighbors coordinated to a given porphyrin display orthogonal planes in a square-like architecture, and two molecules of acetonitrile per porphyrin in the crystal lattice serve as hydrogen-bond acceptors of the O–H derived from apical coordination; there is no cofacial π-overlap of adjacent porphyrins. Whether incorporation of acetonitrile (or another moiety) is essential for this pattern of solid-state assembly remains to be determined. More broadly, a next step concerns the all-important second question – the extent to which these, or any other crystalline-like assemblies – can support the remarkable light-harvesting features found in native systems.
:
2 with 0.5% triethylamine)] yielded a yellow viscous oil (2.92 g, 54%). 1H NMR (CDCl3, 500 MHz) δ −0.14 (s, 6H), 0.61 (t, J = 7.3 Hz, 3H), 0.84 (s, 2H), 0.96–1.03 (m, 2H), 1.12–1.18 (m, 2H), 1.31–1.36 (m, 4H), 1.56–1.62 (m, 4H), 1.77–1.81 (m, 2H), 3.78 (d, J = 7.3 Hz, 2H), 4.46 (t, J = 7.3 Hz, 1H), 6.44 (d, J = 3.7 Hz, 2H), 7.11 (d, J = 3.7 Hz, 2H), 7.49–7.58 (m, 6H), 7.90–7.91 (m, 4H); 13C{1H} NMR (CDCl3, 125 MHz) δ −5.7, 13.7, 13.8, 18.6, 23.2, 25.5, 25.9, 26.1, 26.8, 27.2, 27.8, 43.7, 71.3, 116.1, 123.9, 128.5, 129.2, 131.7, 136.3, 137.9, 150.0, 184.6. HRMS (ESI-TOF) m/z: [M + H]+ calcd for C38H51N2O3SiSn 731.2691; found 731.2700.
:
1, 40 mL). The progress of the reaction was followed by TLC. The reaction was complete in 40 min, at which point the reaction mixture was quenched by the addition of water and then poured into CH2Cl2. The organic phase was separated, washed with water, dried (Na2SO4), and concentrated to give the dipyrromethane-1,9-dicarbinol as a yellow oil. The latter was immediately subjected to condensation with dipyrromethane 1 (200 mg, 0.690 mmol) in the presence of InCl3 (19.1 mg, 0.0863 mmol) in CH2Cl2 (80 mL) for 90 min. Then, DDQ (680 mg, 3 mmol) was added to the reaction mixture. The reaction mixture was stirred for 20 min. Then, triethylamine (5 mL) was added. The crude mixture was concentrated to dryness and then purified by chromatography [silica, hexanes/CH2Cl2 (1
:
1)] to obtain a purple solid (26 mg, 5%). The title compound could not be dissolved in CH2Cl2, CHCl3, DMSO or THF but was analyzed by mass spectrometry and absorption spectroscopy. MALDI-MS (CHCA) obsd 750.31, calcd 750.38 (C46H54N4O2Si2); λabs (toluene) 416, 514, 544, 592 nm.
:
3 with 0.5% triethylamine)] yielded a purple solid (12.8 mg, 68%). 1H NMR (CDCl3, 600 MHz) δ 0.22 (s, 12H), 0.98 (s, 18H), 7.04 (s, 4H), 7.77–7.80 (m, 6H), 8.22 (d, J = 7.2 Hz, 4H), 9.03 (d, J = 3.0 Hz, 4H), 9.68 (d, J = 3.6 Hz, 4H). 13C{1H} NMR (CDCl3, 175 MHz) δ −4.5, 26.2, 29.9, 64.9, 117.0, 120.7, 126.7, 127.6, 129.5, 132.6, 134.6, 143.0, 150.1, 150.8. The title compound was not highly soluble in CDCl3. MALDI-MS (CHCA) obsd 812.08, calcd 812.29 (C46H52N4O2Si2Zn); λabs (toluene + two drops of THF) 422, 554, 586 nm.
:
1 with 0.5% triethylamine] afforded a purple solid (38 mg, 11.5%). 1H NMR (DMSO-d6, 500 MHz) δ 0.25 (s, 12H), 0.93 (s, 18H), 7.12 (s, 4H), 9.57 (d, J = 4.5 Hz, 4H), 9.82 (d, J = 4.0 Hz, 4H), 10.29 (s, 2H)); 13C{1H} NMR (DMSO-d6, 175 MHz) δ −4.7, 18.1, 25.9, 64.3, 105.5, 115.1, 129.8, 132.2, 148.7, 149.9; MALDI-MS (CHCA) obsd 660.19, calcd 660.23 (C34H44N4O2Si2Zn). HRMS (ESI-TOF) m/z: [M + HCOO]− calcd for C35H45N4Si2O6 705.2276; found 705.2287; λabs (toluene + two drops of THF) 412, 544, 580 nm.
:
3)] showed complete consumption of the pyridyl thioester after 20 min, so the cooling bath was removed. The reaction mixture was poured into a mixture of saturated aqueous NH4Cl solution and ethyl acetate. The organic layer was separated, washed with brine, dried (Na2SO4), and concentrated to afford a yellow oil. Purification by flash column chromatography [silica; neat CH2Cl2 to CH2Cl2/ethyl acetate (100
:
3)] afforded a yellow oil (441 mg, 90%). 1H NMR (CDCl3, 500 MHz) δ 0.95 (t, J = 7.5 Hz, 3H), 2.09–2.15 (m, 2H), 4.03 (t, J = 8.0 Hz, 1H), 6.05–6.07 (m, 1H), 6.10 (dd, J = 3.5 Hz, 6.0 Hz, 1H), 6.18 (dd, J = 2.5 Hz, 3.5 Hz, 1H), 6.83 (dd, J = 2.5 Hz, 4.0 Hz, 1H), 7.47 (t, J = 8.0 Hz, 2H), 7.56 (t, J = 7.5 Hz, 1H), 7.84–7.85 (m, 2H), 8.91 (brs, 1H), 10.47 (brs, 1H); 13C{1H} NMR (CDCl3, 125 MHz) δ 12.6, 27.3, 40.2, 105.5, 108.2, 109.3, 117.4, 122.3, 128.5, 129.0, 130.4, 131.9, 132.2, 138.7, 144.5, 185.1; HRMS (ESI-TOF) m/z: [M + Na]+ calcd for C18H18N2ONa 301.1317; found 301.1312.
:
1, 10 mL). Analysis by TLC [silica; hexanes/ethyl acetate (9
:
1)] showed complete consumption of 8 after 20 min, so the reaction mixture was quenched by the addition of water and CH2Cl2. The organic layer was separated, washed with brine, dried (Na2SO4), and concentrated to afford the dipyrromethane-1-carbinol as a yellow oil. The crude dipyrromethane-1-carbinol was immediately dissolved in acetonitrile (100 mL), and TFA (231 µL, 3 mmol, 30 mM) was added. After 10 min, DDQ (227 mg, 1 mmol) was added, and the mixture was stirred at room temperature for 1 h. Then, triethylamine (417 µL, 3 mmol) was added. The crude mixture was concentrated to dryness and then purified by chromatography [alumina, hexanes/CH2Cl2 (1
:
1)] to afford a purple solid (48 mg, 37%). 1H NMR (CDCl3, 700 MHz) δ −2.69 (s, 2H), 2.13 (t, J = 7.7 Hz, 6H), 5.02 (q, J = 7.7 Hz, 4H), 7.75–7.81 (m, 6H), 8.20 (d, J = 7.0 Hz, 4H), 8.87 (d, J = 4.2 Hz, 4H), 9.45 (d, J = 4.2 Hz, 4H); 13C{1H} NMR (CDCl3, 175 MHz) δ 22.9, 28.8, 119.0, 121.3, 126.7, 127.7, 134.6, 134.7, 142.8, resonances from the α- and β-carbons of the porphyrin were not observed; MALDI-MS (CHCA) obsd 518.24, calcd 518.25 (C36H30N4); λabs (toluene) 419, 516, 549, 653 nm.
:
1) with 0.5% triethylamine] gave a solid. The solid was washed several times with hexanes/CH2Cl2 (5
:
1) to remove impurities, affording a purple solid (27 mg, 8.3%). 1H NMR (THF-d8, 700 MHz) δ 2.16 (t, J = 7.7 Hz, 6H), 5.19 (q, J = 7.7 Hz, 4H), 9.40 (d, J = 4.2 Hz, 4H), 9.71 (d, J = 4.9 Hz, 4H), 10.08 (s, 2H); 13C{1H} NMR (THF-d8, 175 MHz) δ 23.8, 29.5, 105.4, 121.2, 129.6, 132.6, 149.9, 150.9; MALDI-MS (CHCA) obsd 428.10, calcd 428.10 (C24H20N4Zn); HRMS (ESI-TOF) m/z: [M]+ calcd for C24H20N4Zn 428.0979; found 428.0978; λabs (toluene + two drops of THF) 413, 546 nm. A single crystal obtained from THF/acetone was examined by SCXRD analysis.
:
1) to remove impurities, affording a purple solid (10 mg, 80%). 1H NMR (THF-d8, 700 MHz) δ 2.11 (t, J = 7.7 Hz, 6H), 5.12 (q, J = 7.7 Hz, 4H), 7.73–7.78 (m, 6H), 8.18 (d, J = 7.0 Hz, 4H), 8.85 (d, J = 4.2 Hz, 4H), 9.56 (d, J = 4.2 Hz, 4H); 13C{1H} NMR (THF-d8, 175 MHz) δ 23.7, 29.7, 120.3, 122.5, 127.2, 128.1, 129.1, 132.7, 135.5, 145.1, 150.4, 151.0; MALDI-MS (CHCA) obsd 580.21, calcd 580.16 (C36H28N4Zn); HRMS (ESI-TOF) m/z: [M]+ calcd for C36H28N4Zn 580.1605; found 580.1608; λabs (toluene + two drops of THF) 426, 557 nm. A single crystal obtained from THF/hexane was examined by SCXRD analysis.
(ii) Fluorescence lifetime measurements from time-correlated single photon counting (TCSPC). Fluorescence lifetimes were measured for 20 µM solutions of Ph/CH2OH and H/CH2OH in a 10-mm excitation and 2-mm emission pathlength cuvette. A 20 µM solution of ZnTPP was also prepared in THF solution for comparison. All the porphyrin solutions were excited at 550 nm using a 10-nm band pass filter. To generate the excitation pulse, an 800 nm centered femtosecond 80 MHz pulse, produced by a mode-locked Ti:sapphire pulsed laser (Mai Tai HP, Spectra Physics) was first focused into a nonlinear photonic crystal fiber (FemtoWhite800, NKT Photonics) to generate a white light supercontinuum. This beam was passed through a 10-nm band pass filter at 550 nm, selected for the excitation wavelength of 550 nm. The emission from the sample was isolated using another 10-nm bandpass filter (ZnTPP and Ph/CH2OH at 650 nm; H/CH2OH at 635 nm). Single photons from the fluorescence emission were then detected by a single-photon avalanche diode (Micro Photon Devices) connected to a time-correlated single photon module (PicoHarp 300, Picoquant) to record the arrival times, producing a histogram of photon events up to ∼12 ns.
The impulse response function (IRF) was similarly measured with a colloidal silica (LUDOX) solution sample. The fluorescence lifetimes were then calculated by performing a reconvolution of the IRF with an exponential fit optimized by a least-squares regression.
(iii) Ultrafast transient absorption (TA) measurements. Solutions of Ph/CH2OH and H/CH2OH (100 µM in THF) were used for femtosecond TA measurements. Both samples were measured using a 2-mm flow-cuvette set up to control photodegradation. Both porphyrins were measured with pump powers of 20 nJ per pulse with time delays from −25 ps to 1.3 ns. The experimental apparatus has been described.37,38 In brief, the femtosecond transient absorption measurements were taken with a femtosecond 400 nm pump pulse and a broadband white light supercontinuum probe. The instrument response function measured through the pump–probe cross-correlation from a frequency-resolved optical gating (FROG) experiment was ∼250 fs. Both pulses were sourced from the 800 nm mode-locked output of a Ti:Sapphire laser (Coherent Libra) with a repetition rate of 5 kHz. Splitting this output in two, one path was sent through an argon tube pressurized at 20 psi to generate the broadband white light continuum used as the probe. The second beam path was used to generate the pump pulse at 400 nm through second harmonic generation after passing through a BBO crystal. The pump was chopped using a 2.5 kHz optical chopper to create a repetition rate half that of the probe to obtain the delta absorbance (ΔA) signal. The time delay between the pump and probe pulses was set by a motorized delay stage (Aerotech) which controlled the path length of the pump. For the transient absorption measurements, both pulses were then focused and spatially overlapped onto the sample. The transmitted probe was then dispersed using a holographic grating (450 grooves per mm, Wasatch Photonics) and detected by a 2048-pixel CCD camera (e2v Aviiva EM4). All data analysis was done using home-built code in MATLAB-R2023a.
CCDC 2496240 (H/CH2OH), 2496241 (Ph/Et), 2496247 (H/Et), and 2496248 (Ph/CH2OH) contain the supplementary crystallographic data for this paper.43a–d
All other data are contained in the paper.
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