Abstract
Ruthenium(II) polypyridyl complexes can be harnessed for photodynamic therapy. In this work, diprotic ligands which can be deprotonated to change the metal complexes from dicationic to neutral are combined with extended π systems for light absorption at longer wavelengths. Herein, the diprotic ligands are 4,4′-dhbp = 4,4′-dihydroxybipyridine or 4,7-dhphen = 4,7-dihydroxy-1,10-phenanthroline and the π-expanded ligands are bphen = bathophenanthroline, dppz = dipyrido[3,2-a:2′,3′-c]phenazine, and dppn = benzodipyrido[3,2-a:2′,3′-c]phenazine. This report describes the synthesis and characterization of [(bphen)2Ru(4,4′-dhbp)]Cl2 (1A), [(dppz)2Ru(4,4′-dhbp)]Cl2 (2A), [(dppn)2Ru(4,4′-dhbp)]Cl2 (3A), [(bphen)2Ru(4,7-dhphen)]Cl2 (4A), [(dppz)2Ru(4,7-dhphen)]Cl2 (5A), and [(dppn)2Ru(4,7-dhphen)]Cl2 (6A). Single crystal X-ray diffraction data are reported for 1A, 2A, and two known precursor compounds: [(ղ6-p-cymene)RuCl(diprotic ligand)]Cl (P1, P2 where diprotic ligand = 4,4′-dhbp and 4,7-dhphen, respectively). Compounds 1A-6A have been studied for their photocytotoxicity vs. breast and melanoma cancer cells, lipophilic vs. hydrophilic properties, thermodynamic acidities (pKa values), singlet oxygen quantum yields, and luminescence which is heavily influenced by the nature of the π expanded ligand. Four compounds (bearing bphen and dppn ligands) have promising photocytotoxicity including activity with green light and one compound has a phototherapeutic index (PI) as high as 145.
Keywords: photodynamic therapy, ruthenium complexes, protic ligands, dihydroxybipyridine, π-expanded ligands, photoluminescence
Graphical Abstract

INTRODUCTION
We have been interested in determining the photophysical and biological properties of ruthenium(II) tris diimine complexes which can be used for photodynamic therapy (PDT) applications. PDT involves using visible light and a photosensitizer to generate cytotoxic singlet oxygen (1O2).1 PDT can be inherently cancer selective by shining the light directly on the tumor for spatio and temporal control. Several Ru(II) complexes have shown promise for PDT applications vs. cancer cells,2, 3 with TLD-1433 (Chart 1) having very potent light driven toxicity and advancing to Phase II clinical trials for non-muscle-invasive bladder cancer.1 Typically, a type II PDT process generates singlet oxygen by energy transfer from 3MLCT, but it can also involve energy transfer from other excited states (3ILCT, etc.).4 However, very little work has been done on using protic ligands for PDT.5, 6 Our group has been interested in using ligands bearing OH groups (e.g. dihydroxybipyridine) for investigation of how ligand charge and protonation state influences the cellular uptake7 and excited state properties.8–10
Chart 1.

Structure of TLD-1433 which is in clinical trials for bladder cancer. One enantiomer is shown, but it is used as a racemic mixture of both enantiomers.
We have studied complexes of the type: [(N,N)2Ru(diprotic ligand)]2+ in this work (Figure 1). The (N,N) ligand was chosen from bathophenanthroline (bphen), dipyrido[3,2-a:2′,3′-c]phenazine (dppz), and benzodipyrido[3,2-a:2′,3′-c]phenazine (dppn) for their lipophilic and π extended structures. Bphen ligands are lipophilic and can favor Ru(II) complex accumulation in the mitochondria of cancer cells, as demonstrated in past work.9, 11 Ru(II) complexes of dppz and dppn have extended π systems and are known to intercalate between DNA base pairs.12–16 Dppn, having an extended π-system when compared to its dppz parent, introduces a low-lying π-orbital resulting in a long-lived non-emissive 3π-π* excited state that can generate 1O2 more efficiently.14, 15, 17–21 Ru(II) complexes of dppz, dppn, and related ligands have been explored by Turro, McFarland, and others for promising PDT effects vs. cancer cells in vitro.4, 5, 22
Figure 1.

Ruthenium complexes used in this study are shown in both their acidic (XA = OH bearing) and basic (XB = O− bearing) forms.
Very little has been done to understand the role of acid-base chemistry in the behavior of photosensitizers (PSs). The hydroxy groups in the 4,4′-dihydroxybipyridine (4,4′-dhbp) ligand typically have pKa values of 5–6 in aqueous solution with simultaneous removal of both protons.8, 10, 23 For complex 1A, we previously measured a pKa value of 5.9(3).8 These complexes are typically isolated as the acidic form (XA = 1A, 2A, 3A) which is dicationic and more hydrophilic.7 The pKa values lead to the neutral and more lipophilic form of the complex (XB) being the major species in solution at the physiological pH of 7.4. This also influences the photochemistry, with the OH bearing form having longer lived excited states vs. O−.8 In the current work, we investigated the role of increased π conjugation on the diprotic ligand by using 4,7-dihydroxy-1,10-phenanthroline (dhphen) in 4A, 5A, and 6A. This ligand has been used in the catalysis literature,24, 25 but it has not been used for PDT studies to the best of our knowledge.
RESULTS AND DISCUSSION
Synthesis and Characterization.
Complexes 1A and 4A were synthesized from the reaction of cis-(bphen)2RuCl2 with 4,4′-dhbp and 4,7-dhphen, respectively, using the previously published procedure for 1A.9 A different procedure was effective for the synthesis of 2A, 3A, 5A, and 6A in which the half sandwich complexes [(ղ6-p-cymene)RuCl(diprotic ligand)]Cl (P1, P2 where diprotic ligand = 4,4′-dhbp and 4,7-dhphen, respectively) were treated with dppz or dppn (Figure 2). These half sandwich complexes are known in the literature,26, 27 but the crystal structures of these compounds are new. The 1H-NMR spectra of the five newly synthesized compounds were fully assigned using COSY, HSQC, and HMBC. Single crystal X-ray diffraction (SC XRD), IR, and MS were used to confirm the structures. The purity of the six compounds was analyzed using RP-HPLC. All the spectra and chromatograms obtained for characterization are in the Supporting Information.
Figure 2.

Synthetic procedures used to obtain complexes 1A-6A.
Single Crystal X-Ray Diffraction.
Complexes P1 and P2 are known in the literature and were synthesized by a slight modifications of known procedures in 83% and 80% yields, respectively.26, 27 Single crystals of both P1 and P2 were grown by vapor diffusion of diethyl ether into methanolic solutions of each compound (Figure 3). The bond lengths and angles shown for P1 and P2 (Table 1) are similar to other Ru(II) half sandwich complexes in the literature25, 28 including [(ղ6-p-cymene)RuCl(phen′)]Cl where phen′ is phenanthroline bearing an epoxide substituent.27
Figure 3.

Molecular diagrams of P1 and P2 from the crystallographic data (ellipsoids shown at 50% probability). The chloride counter anions and water solvent (for P2) are removed for clarity. Grey = carbon, blue = nitrogen, red = oxygen, green = chlorine, teal = ruthenium.
Table 1.
Selected bond lengths (Å) and angles (°) for P1 and P2.
| P1 | P2 | |
|---|---|---|
| Bond lengths | ||
| Ru1-arene (centroid) | 1.674 | 1.676 |
| Ru1-Cl1 | 2.397(1) | 2.385(1) |
| Ru1-N1 | 2.087(1) | 2.093(1) |
| Ru1-N2 | 2.096(2) | 2.098(1) |
| O1-C3 | 1.346(2) | 1.336(2) |
| O2-C15 for P1 O2-C8 for P2 |
1.337(2) | 1.340(2) |
| Bond angles | ||
| N1-Ru1-N2 | 76.8(1) | 77.6(1) |
| Nl-Ru1-Cl1 | 84.3(1) | 85.8(1) |
| N2-Ru1-Cl1 | 82.6(1) | 84.2(1) |
Red single crystals of 1A and 4A suitable for X-ray diffraction were grown by diethyl ether vapor diffusion into saturated methanol solutions of the respective compound. The molecular diagrams are shown in Figure 4 with selected bond lengths and angles in Table 2. Overall, the octahedral Ru(II) centers show minimal distortion from an ideal octahedral geometry. The view with the protic ligand planar (left of Figure 4) shows minimal twisting of the OH substituted rings for 4,4′-dhbp or 4,7-dhphen. In contrast, the published structure of [(bphen)2Ru(6,6′-dhbp)]Cl2 shows more twisting of the OH substituted rings.9 The Ru-N bond distances involving the protic ligands are slightly shorter for 1A (2.074(6) Å) vs. in [(bphen)2Ru(6,6′-dhbp)]Cl2 (2.100(2) Å) because the 6,6′-dihydroxybipyridine ligand introduces steric strain near the metal center.9 For 1A and 4A, the average C-O bond distance is ~1.33 Å, indicating an average bond order between single and double due to the resonance effect of the pyridinol ring. These values are very similar to other dhbp complexes.9, 23
Figure 4.

Molecular diagrams of 1A and 4A from the crystallographic data (ellipsoids shown at 50% probability). Two views are shown for each molecule. The chloride counter anions, hydrogen atoms, and water solvent (for 4A) are removed for clarity. Grey = carbon, blue = nitrogen, red = oxygen, green = chlorine, teal = ruthenium.
Table 2.
Selected bond lengths (Å) and angles (°) for 1A and 4A.
| 1A | 4A | |
|---|---|---|
| Bond lengths | ||
| Ru-N (protic ligand)avg | 2.074(6) | 2.089(2) |
| Ru-N (bphen)avg | 2.068(5) | 2.056(2) |
| C-Oavg | 1.338(8) | 1.333(3) |
| Bond angles | ||
| Bphen N-Ru-Ncis (within chelate) | 79.4(2) | 79.39(9) |
| Protic ligand N-Ru-Ncis (within chelate) | 79.3(3) | 79.3(1) |
| N-Ru-Ntrans (avg trans angles) | 171.5(2) | 172.5(1) |
Optical Absorption Spectroscopy.
The electronic spectra of compounds 1A-6A in dry acetonitrile display singlet metal-to ligand charge transfer (1MLCT) bands between 429–483 nm (Table 3 and Figure 5). These bands undergo a red shift upon deprotonation of the protic ligands in acetonitrile, for example, with a shift from 475 nm for 1A to 525 nm for 1B8, 9 and from 483 nm for 4A to 515 nm for 4B (Figure S38). Similar changes are also observed for 4A (broad shoulder at ~485 nm) red shifting to form 4B (537 nm) in aqueous solution (90% aqueous, 10% ethanol added for solubility, see Figure S65). The red shift and broadening observed on deprotonation in the absorption spectra have been attributed to the generation of the singlet ligand-to-ligand charge transfer excited state (1LLCT) by the mixing of the 4,4′-dhbp or 4,7-dhphen orbitals with the bphen orbital.
Table 3.
Optical absorption spectral data of compounds 1A-6A, dppz, and dppn as measured in dry acetonitrile. The molar absorptivities have estimated errors of (+/−)1000 M−1cm−1.
| Compound | λmax (nm) | Charactera | ε (M−1cm−1) |
|---|---|---|---|
| 1 A | ~300 | π- π* | n.d.b |
| 445 | MLCT | 17,000 | |
| 475 | MLCT | 15,700 | |
| 2 A | 359 | π- π* | 22,000 |
| 370 | π- π* | 22,000 | |
| 429 | MLCT | 13,000 | |
| 480 | MLCT | 12,000 | |
| 3 A | 389 | π- π* | 5,000 |
| 410 | π- π* | 6,000 | |
| 461 | MLCT | 4,000 | |
| 4 A | ~300 | π- π* | n.d.b |
| 440 | MLCT | 20,000 | |
| 483 | MLCT | 18,000 | |
| 5 A | 359 | π- π* | 50,000 |
| 370 | π- π* | 52,000 | |
| 425 | MLCT | 28,000 | |
| 483 | MLCT | 22,000 | |
| 6 A | 389 | π- π* | 7,000 |
| 410 | π- π* | 12,000 | |
| 468 | MLCT | 7,000 | |
| dppz c | 359 | π- π* | 14,000 |
| 379 | π- π* | 14,000 | |
| dppn c | 389 | π- π* | 10,000 |
| 411 | π- π* | 13,000 |
Some of these π - π * transitions may also have n - π * character.
Extinction coefficient not available due to the peak being off scale for 1A and 4A (below 300 nm).
Similar to a literature report.29
Figure 5.

Absorption spectra of compounds 1A to 6A in dry acetonitrile.
Complexes 2A and 5A with the dppz ligand show two π-π* transitions (at 359 and 370 nm in acetonitrile, Figure 5) in the same positions as those for the dppz free ligand. MLCT bands for 2A and 5A are located at ~430 and 480 nm in acetonitrile. A similar pattern is observed for 3A, 6A, and the dppn free ligand with π-π* transitions at 389 and 410 nm. Thus, these ligand-based transitions are not perturbed significantly by the presence of the Ru(II) metal center. Extending the π conjugation from dppz to dppn resulted in a 30–40 nm red-shift in the π-π* transitions due to the extra aryl ring. Upon deprotonation of 3A or 6A to form 3B or 6B in aqueous solution, we observe a red shift of the charge transfer bands at low energy, with no significant changes to the dppn ligand based π-π* transitions (Figures S64 and S66).
Thermodynamic Acidity Measurements.
The deprotonation events described above have been studied in aqueous solution to measure pKa values (Table 4) for the most potent light activated anticancer compounds: 1, 3, 4, and 6 (see below). Compound 1 was studied in past work by pH dependent UV-Vis, and an apparent pKa value of 5.9(3) was observed for removal of both protons; therein 1% ethanol in aqueous solution was used to afford sufficient solubility.8 In the potentiometric titrations used herein, 10% ethanol was required to dissolve the complexes in the solution phase. Both individual proton removals for 3A, 4A, and 6A are observed with pKa1 values ranging from 4.2 to 5.3 and pKa2 values ranging from 6.0 to 6.6 (Figure S61–S63, Table 4). While we have not measured the pKa values for 2 and 5, we expect them to be in a similar range based upon similar structures to 3 and 6. As such, all compounds are expected to be fully deprotonated (present as the “basic” B forms) in cellular studies at physiological pH of 7.4 These are apparent pKa values due to the use of ethanol (10%) as a co-solvent and pH is defined as being in 100% aqueous solution. Therefore, these values should not be compared directly with pKa values for 1 (1% ethanol) or for compounds measured in pure aqueous solution.8
Table 4.
Emission data, singlet oxygen quantum yields, and log(Do/w) values for 1A-6A.
| Compound | λem (nm)a | Stokes shift (eV)a | Φlum (%)a | τlum (μS)a | ΦΔ (%)a | log(Do/w) (UV-Vis)b | log(Do/w) (RP HPLC)b,c | pKa |
|---|---|---|---|---|---|---|---|---|
| 1 A | 642 | 0.65 | 18.7 | 3.45 | 46 | >3 | 3.3(3) | 5.9(3)d |
| 2 A | 671 | 0.78 | 4.2 | 0.11, 0.52 | 17 | >3 | n.d. | n.d. |
| 3 A | 566 | 0.86 (PLE) / 0.52 (abs) | 0.46 | 0.04 | 65 | >3 | n.d. | 4.8(3), 6.4(3)e |
| 4 A | 653 | 0.65 | 9.4 | 3.12 | 17 | >3 | 3.7(2) | 4.2(2), 6.0(2)e |
| 5 A | 680 | 0.82 | 0.44 | 0.01, 0.07, 0.62 | 5 | >3 | n.d. | n.d. |
| 6 A | 571 | 0.88 (PLE) / 0.52 (abs) | 4.65 | 0.04 | 32 | >3 | n.d. | 5.3(2), 6.6(2)e |
Measured in dry acetonitrile under argon. See the experimental section for further details.
Measured with the aqueous phase as pH 7.4 buffer.
Poor solubility for 2A, 3A, 5A, and 6A hindered our studies by reverse phase (RP) HPLC (n.d. = not determined).
Apparent pKa for removal of both protons as measured in prior work, with 1% ethanol in aqueous solution.8
Apparent pKa1 and pKa2 measured with 10% ethanol in aqueous solution (Figures S61–S63).
Light Stability.
Typically, octahedral Ru(II) complexes lacking steric bulk near the metal center (e.g. 1-6) do not undergo photodissociation upon light irradiation. This was confirmed for 1 in past work,9 and for compounds 3, 4, and 6 in this work. White light irradiation (90–120 min) of samples of 3, 4, or 6 dissolved in pH 7.4 aqueous buffer with ethanol (8–16%) added for solubility resulted in no significant changes in the UV-Vis spectra with some slight ground state bleaching (Figure S60). MS analysis confirmed that the samples are intact after irradiation, thus ruling out ligand loss. Based upon a similar structure, we expect the same properties for 2 and 5.
Photoluminescence spectroscopy.
The photoluminescence spectra of compounds 1A-6A in dry acetonitrile display a triplet metal-to-ligand charge transfer (3MLCT) band between 566 and 680 nm (see Table 4 and Figures S42–S46). Compounds 1A and 4A, display typical Stokes shifts of 0.65 eV (Table 4). Compounds 2A and 5A display typical Stokes shifts of 0.78 – 0.82 eV (Table 4), which indicates that emission occurs after relaxation of an excited state. In contrast, 3A and 6A display smaller Stokes shifts of around 0.52 eV. This suggests that emission occurs from an excited state that is closer in energy to the initial excitation, which led us to investigate the origin of these 3MLCT excited states, as described below.
Complex 4B is used as a representative example of a deprotonated compound. Absorption and luminescence studies show broadening and a red shift in the absorption and emission bands of 4B, indicating the presence of a 1LLCT and a lower energy 3LLCT (Figures S38 and S44). Introducing a 3LLCT excited state to the native 3MLCT excited state results from the electron-donating O− group in the 4,7-dhphen ligand of 4B which can quench the emission by a photoinduced electron transfer mechanism (PET) as described previously.30, 31 Our previous work has shown that formation of the deprotonated O− bearing complex (e.g. in 1B) leads to more rapid quenching of the excited state resulting in shorter photoluminescence lifetimes and lower quantum yields.8, 9
Photoluminescence excitation measurement (PLE).
It is noteworthy that 3A and 6A were excited at the wavelengths corresponding to their UV-Vis absorption bands for 1MLCT and π-π* states, and the steady-state luminescence spectrum observed displays an emission spectrum that is similar to that of the free ligand (Figure 6). This begs the question: from what excited state(s) does the emission arise? Is the emission a result of 1) the population of a triplet excited state from a ligand-centered singlet state, i.e., 1π-π* to the 3MLCT, or 2) an overlap of the 3MLCT and the 3π-π* excited state, or 3) just the relaxation of 3MLCT excited state? To investigate these possibilities, a PLE measurement was carried out on compounds 1A-6A to investigate the excited state(s) involved in the emission of the compounds. The photoluminescence excitation spectrum almost always retraces the electronic transitions present in the absorption spectrum of the investigated compound. During PLE experiments, the range of the wavelengths in the absorption spectrum of the investigated compound is scanned while the emission wavelength is held constant.
Figure 6.

Optical absorption, steady-state photoluminescence (PL) spectra, and photoluminescence excitation (PLE) spectra in dry acetonitrile of free ligands dppn, dppz, and compounds 1A-6A. For each corresponding metal complex (1A-6A): black = absorbance, red = PL, and green = PLE. The blue curves show the absorbance of the free ligands: bphen for 1A and 4A, dppz for 2A and 5A, and dppn for 3A and 6A.
The PLE measurements showed that the dppn compounds (3A and 6A) display PLE spectra that retrace the free ligand absorption spectra. In contrast, the dppz and bphen compounds (1A, 2A, 4A, and 5A) all display PLE spectra that retrace the absorption spectra of the parent Ru(II) compound (Figure 6). Since the dppn compounds have PLE spectra that are replicates of the free ligand electronic spectra (Figure 6), it appears that dppn affords compounds 3A and 6A a low-lying 3π-π* deactivation pathway, which is populated from the 3MLCT state. The triplet excited state in the dppz compounds (2A and 5A) is believed to arise from overlap of the 3π-π* and the 3MLCT states. In contrast, the 3MLCT state for compounds 1A and 4A is populated from the 1MLCT state. However, the exact energies of these triplet states have not been experimentally observed.
Photoluminescence quantum yield (ϕlum).
The photoluminescence quantum yields range from 18.7% to 0.44% for compounds 1A-6A. These range from brightly emissive with 1A (18.7%) > 4A (9.4%) to moderately emissive 2A and 6A (4–5%) to non-emissive 3A and 5A (<1%). There is no clear pattern with respect to the protic ligand (4,4′-dhbp vs. 4,7-dhphen), and it seems that the π-expanded ligand plays a greater role. Bathophenanthroline-derived compounds show greater luminescence quantum yields vs. dppz and dppn compounds. No clear trend is apparent for comparing dppz and dppn complexes. The 3π-π* state is a dark and non-emissive relaxation pathway that may lead to a lower photoluminescence quantum yield for Ru(II) complexes of dppz and dppn (2A, 3A, 5A, and 6A).
Using 4B as a representative example of the deprotonated species, its photoluminescence quantum yield is low, with a value of less than 0.24% at room temperature. This is due to quenching of the 3MLCT state by the low-emissive 3LLCT state.8, 9 The 3LLCT excited state of complex 4B is populated via direct photoexcitation in the 1LLCT absorption band or through internal conversion from the photoexcited 3MLCT state.32
Photoluminescence dynamics studies.
The time-resolved photoluminescence measurements (Table 5) show a relatively long lifetime value of over 3 μs for the bphen compounds, 1A and 4A. Much shorter lifetimes are observed for all other compounds. Four compounds show monoexponential decay, but compound 2A has a biexponential decay, and compound 5A has a triexponential decay, indicating multiple emission channels. This suggests that an emissive 3MLCT state for 2A and 5A transforms into other triplet emissive states. Similarly, the representative deprotonated species 4B also shows a biexponential decay (see Figure S50).
Table 5.
Cytotoxicity and photocytotoxicity of compounds 1A-6A vs. MCF7 and MDA-MB-231 cells under normoxia (~18.5% O2) via tetrazolium cell viability assay.a
| Compound | MCF7 | MDA-MB-231 | ||||
|---|---|---|---|---|---|---|
| EC50_dark (μM) | EC50_vis (μM) | PI | EC50_dark (μM) | EC50_vis (μM) | PI | |
| 1 A | 3.8 ± 0.9 | 0.1 ± 0.1 | 29 | 12.3 ± 4.7 | 0.7 ± 0.5 | 19.4 |
| 2 A | >100 | >100 | N/A | n.d.b | n.d.b | n.d.b |
| 3 A | >100 | 0.7 ± 0.1 | >145 | >100 | 3.8 ± 2.3 | >35 |
| 4 A | 11.0 ± 5.0 | 3.8 ± 2.2 | 2.9 | 36.1 ± 4.9 | 1.6 ± 0.5 | 23.8 |
| 5 A | 3.9 ±0.3 | 2.5 ±0.8 | 1.7 | n.d.b | n.d.b | n.d.b |
| 6 A | >100 | n.d.c | N/A | n.d.b | n.d.b | n.d.b |
Photocytotoxicity in MCF7 and MDA-MB-231 breast cancer cells were measured by irradiation for 2 h with white light (irradiance: 40 mW cm−2, total fluence: 288 J cm−2).
These values were “not determined” (n.d.) because the screening data showed no toxicity at 5 μM under dark and light conditions vs. MDA-MB-231.
These values were “not determined” (n.d.) because the cellular viability (normalized absorbance) vs. log[Ru] curve had an unusual shape in all three replicates.
Singlet Oxygen Quantum Yields and Tests for Other Reactive Oxygen Species (ROS).
Singlet oxygen (1O2) is a product of the triplet excited states interacting with molecular oxygen, 3O2. Therefore, the relaxation pathways, whether radiative or non-radiative, influence 1O2 generation. Complexes 3A, 1A and 6A are relatively efficient at 1O2 generation with ΦΔ values of 65, 46, and 32%, respectively (Table 4). Lower quantum yields of 17 and 5% are seen for the remaining compounds. Generally, the 4,4′-dhbp compounds have better singlet oxygen quantum yields as compared with 4,7-dhphen compounds if the other ligand (bphen, dppz, or dppn) is held constant. No clear trend emerges from comparing the singlet oxygen quantum yields to luminescence quantum yields or lifetimes.
To test for other reactive oxygen species (ROS), a sample of compound 3 or 6 in aqueous phosphate buffer (pH 7.5) was irradiated for one hour with white light under head space of air (see Experimental Section). These compounds were chosen for study as two of our most toxic compounds upon light irradiation (see below). After one hour, the sample was treated with catalase. Catalase converts peroxide to O2,33 and the amount of dissolved O2 was quantified with a Clark electrode. Comparison with a control sample lacking the Ru complex showed no increased oxygen production (Figure S67). This suggests that peroxide is not produced by these Ru complexes. Furthermore, because superoxide undergoes rapid disproportionation to form peroxide,34 this also suggests that superoxide was not present. This suggests that the major ROS present is 1O2. However, we caution that these experiments lack all the components of biological media, and this does not rule out the formation of superoxide or peroxide (perhaps from 1O2 reduction) in cell studies.
Lipophilic vs. Hydrophilic Properties of the Compounds.
Lipophilic compounds typically have better cellular uptake by passive diffusion and are often preferred for cellular studies.35–38 The partitioning of a compound between octanol and water can be used to estimate the ability of a compound to diffuse through the phospholipid bilayer. The distribution coefficient, log(Do/w), is used for ionizable compounds and is defined here as the log([Ru]octanol/[Ru]aq) where aq = aqueous buffer at pH 7.4. These compounds had good solubility in octanol but poor solubility in aqueous buffer, therefore, initially the log(Do/w) values were all estimated as >3 (undetectable in aqueous solution by UV-Vis method, Table 4). We were able to determine log(Do/w) values by reverse phase (RP) HPLC also, using a calibration curve in octanol solution. Values for log(Do/w) of 3.3 and 3.7 were obtained for 1A and 4A, respectively, indicating that these compounds are very lipophilic. Similar log(Do/w) measurements by RP HPLC were not possible for 2A, 3A, 5A, and 6A due to poor solubility; these compounds exhibited no solubility in aqueous buffer and while they would dissolve in octanol they also precipitated from octanol over time.
Cytotoxicity and Photocytotoxicity Cancer Cell Studies.
Compounds 1A-6A were evaluated for cytotoxicity and photocytotoxicitiy vs. MCF7 and MDA-MB-231 breast cancer cells (Table 5). These compounds were isolated as the OH bearing “A forms”, but at pH 7.4 in cell media, they are all expected to be predominantly deprotonated based on the measured pKa values (above, see Table 4).8–10, 23 MCF7 are differentiated mammary epithelium cells, whereas MDA-MB-231 is a triple-negative breast cancer cell line with stem-cell like characteristics. All compounds were tested in MCF7 cells, but for MDA-MB-231, we only measured EC50 values on compounds that showed toxicity at 5 μM under light and dark conditions. The phototherapeutic index (PI) is the ratio of EC50 dark to EC50 light, and this is our key metric for assessing the potential of these compounds for PDT. Only compounds 3A, 1A, and 4A are promising vs. MCF7 with a PI value as high as >145 for 3A with no observed dark toxicity up to 100 μM and EC50 = 0.7 μM with visible light. Exactly why these three compounds perform best is unclear, but it appears to be correlated to good quantum yields for singlet oxygen (ΦΔ = 65, 46, and 17% for 3A, 1A, and 4A, respectively) and favorable cellular uptake. Similarly, the PI values are promising for these three compounds vs. MDA-MB-231 with a PI as high as >35 for 3A.
Similarly, compounds 1A-6A were tested in a metastatic melanoma cell line, SKMEL28 (Table 6). These studies were performed in dark conditions and under irradiation with visible, blue, green, or red light. Only three compounds (4A, 1A, and 6A) showed significant PI values greater than 1 with visible light, with the highest PI being 43 for 4A. When considering longer wavelengths of light which penetrate tissue more deeply, only compounds 1A and 4A have significant photocytotoxicity with green light (PI = 14 and 9, respectively). These values may relate to favorable singlet oxygen quantum yields, which were 46, 32, and 17% for 1A, 6A, and 4A, respectively.
Table 6.
Cytotoxicity and photocytotoxicity of the compounds 1A-6A against SKMEL28 cells under normoxia (~18.5% O2) via resazurin cell viability assay.
| Compound | EC50 ± SEM (μM) | PIe | |||||||
|---|---|---|---|---|---|---|---|---|---|
| Dark | Visiblea | Blueb | Greenc | Redd | Visiblea | Blueb | Greenc | Redd | |
| 1 A | 31.3 ± 5.1 | 0.869 ± n.d. | 1.74 ± 0.23 | 2.25 ± 0.10 | 14.8 ± 0.7 | 36 | 18 | 14 | 2 |
| 2 A | 53.0 ± 2.1 | 56.9 ± 1.5 | 56.0 ± 1.0 | 49.9 ± 1.3 | 55.3 ± 2.1 | 1 | 1 | 1 | 1 |
| 3 A | 43.0 ± 1.8 | 50.8 ± 1.8 | 50.0 ± 1.1 | 43.4 ± 1.8 | 47.8 ± 1.9 | 1 | 1 | 1 | 1 |
| 4 A | 39.8 ± 1.9 | 0.933 ± 0.025 | 2.36 ± 0.09 | 4.52 ± 0.33 | 39.6 ± 1.6 | 43 | 17 | 9 | 1 |
| 5 A | 39.7 ± 1.6 | 50.7 ± n.d. | 50.9 ± 1.7 | 42.9 ± 1.9 | 42.2 ± 2.0 | 1 | 1 | 1 | 1 |
| 6 A | 50.6 ± 1.9 | 3.02 ± 0.20 | 4.07 ± 0.33 | 51.7 ± 1.7 | 52.1 ± 2.4 | 17 | 12 | 1 | 1 |
Light treatments were approximately 100 J cm−2 delivered at 19–24 mW cm−2 with a cool white Visible (400–700 nm), b Blue (453 nm), c Green (523 nm), d Red (633 nm), and e PI = phototherapeutic index.
n.d. = SEM not determined due to steep slope.
Since the studies using breast cancer cells and melanoma cells were done in different laboratories using different lamps, we are cautious about making comparisons. Nonetheless, a few general trends are apparent. The bphen compounds (1A and 4A) had good photocytotoxicity across assays in both breast and melanoma cell lines, and this may partially relate to better solubility (cf. the dppz and dppn compounds, 2A, 3A, 5A, and 6A) and long-lived excited states which may promote energy transfer to 3O2 and good 1O2 quantum yields. No clear advantage is seen for 4,4′-dhbp vs. 4,7-dhphen as both 1A and 4A behave similarly and the structures are quite similar. The dppz and dppn Ru(II) compounds tended to aggregate and form a precipitate upon letting a solution sit for minutes to hours, and this may have impacted cellular studies and subcellular localization. This was especially problematic for the dppn compounds (3A and 6A). In particular, we were unable to obtain an EC50 under visible light for 6A vs. MCF7 cells, and we suspect that aggregation may have caused these studies to produce an unusual curve shape for plots of cellular viability vs. log[Ru].
CONCLUSIONS
In conclusion, several compounds have been synthesized, fully characterized, examined for their photophysical properties, and tested in cell culture for their photocytotoxicity. Comparing compounds containing either the 4,4′-dhbp or 4,7-dhphen ligand (e.g. comparing 1A to 4A, 2A to 5A, or 3A to 6A) showed similar photophysical properties, including photoluminescence and photoluminescence excitation spectra. Slightly improved singlet oxygen quantum yields are seen for the 4,4′-dhbp vs. 4,7-dhphen complexes. These similarities make sense as the 4,4′-dhbp and 4,7-dhphen ligands are very similar in structure. However, spectral changes are seen upon modifying the aprotic ligand from bphen to dppz to dppn. An expanded π system in dppn leads to a PLE spectrum that retraces that of the free ligand. Four compounds are promising for photocytotoxicity with visible light and these include 1A, 3A, 4A, and 6A. In a melanoma cell line, the bphen compounds (1A and 4A) were most promising and showed some activation with green light, but in breast cancer cells, compound 3A, a dppn compound, was most promising. The reasons for this are unclear, but we note that the dppn compounds are prone to aggregation and low solubility, which may influence their subcellular localization.
EXPERIMENTAL SECTION
General.
All of the organic ligands (except dppz and dppn) and metal sources were purchased from commercial sources (VWR, Sigma Aldrich, etc.) and used as received. Dppz,39 and dppn40 were synthesized according to published procedures. NMR spectra were recorded in a Bruker AVANCE 360 (360 MHz, 1H frequency) or AVANCE 500 (500 MHz, 1H frequency) and the Neo Cryoprobe 500 (500 MHz, 1H frequency) at room temperature if not mentioned otherwise. UV-Vis spectra were recorded on a Jasco V-780 spectrophotometer using a quartz cuvette of 1 cm path length. FT-IR spectra were recorded using a Bruker Alpha ATR-IR spectrophotometer. Mass spectra were obtained using a Waters AutoSpec-Ultima NT mass spectrometer or a Waters Xero G2-XS QTOF. HPLC studies were performed using an Agilent 1260 Infinity II HPLC system with with a diode array detector, vial sampler, quaternary pump, and column oven using an Agilent analytical column (poroshell 120 EC-C18, 4.6 × 150 mm, 2.7 μm).
All of the photophysics data presented in this study were performed in deaerated and dry acetonitrile. HPLC grade acetonitrile, HPLC grade methanol, and HPLC grade water, reagent grade formic acid (FA), sodium phosphate dibasic heptahydrate, sodium phosphate monobasic monohydrate, and octanol were purchased from VWR. Deuterated DMSO for NMR was purchased from Cambridge Isotope Laboratories. All synthesized Ru(II) complexes were in their racemic forms if chiral.
Synthesis and Characterization data.
Synthesis of [(ղ6-p-cymene)RuCl(4,4′-dhbp)]Cl (P1).
A modification of the published procedure was performed.26 [ղ6-p-cymene)RuCl2]2 (0.282 g, 0.713 mmol, 1.0 equiv.) and 4,4ʹ-dhbp (0.282 g, 1.496 mmol, 2.1 equiv.) were added to an oven-dried Schlenk flask equipped with a stir bar and a septum. The Schlenk flask was then evacuated and refilled thrice with N2. MeOH (15 mL) was then added to the Schlenk flask, and the solution was stirred under N2 at 50 °C for 8 h. The red solution was cooled, filtered, and evaporated to dryness. The solid was rinsed with 10 mL of methanol, 10 mL of dichloromethane, 15 mL of hexanes, and 20 mL of diethyl ether. The reddish-yellow residue was left to air dry. (Yield: 0.285 g, 0.810 mmol, 81%). 1H-NMR: 12.32 ppm (2H, s), 9.12 ppm (2H, d, 6.50 Hz), 7.81 ppm (2H, d, 2.59 Hz), 7.15 ppm (2H, dd, 6.55 and 2.60 Hz), 6.07 ppm (2H, d, 6.33 Hz), 5.84 ppm (2H, d, 6.32 Hz), 2.57 ppm (1H, m), 2.17 ppm (3H, s), 0.97 ppm (6H, d). Single crystals were grown by vapor diffusion of diethyl ether into methanolic solution of the compound.
Synthesis of [(ղ6-p-cymene)RuCl(4,7-dhphen)]Cl (P2).
A modification of the published procedure was performed.27 [(ղ6-p-cymene)RuCl2]2 (0.302 g, 0.493 mmol, 1.0 equiv.) and 4,7-dhphen (0.220 g, 1.035 mmol, 2.1 equiv.) were added to an oven-dried Schlenk flask equipped with a stir bar and a septum. The Schlenk flask was then evacuated and refilled thrice with N2. MeOH (15 mL) was then added to the Schlenk flask, and the solution was stirred under N2 at 50 °C for 8 h. The red solution was cooled, filtered, and evaporated to dryness. The solid was rinsed with 10 mL of methanol, 10 mL of dichloromethane, 15 mL of hexanes, and 20 mL of diethyl ether. The reddish-yellow residue was then left to air dry. (Yield: 0.217 g, 0.419 mmol, 85%). 1H NMR spectra for this compound match the literature values:: 13.40 ppm (2H, s), 9.44 ppm (2H, d, 6.18 Hz), 8.14 ppm (2H, s), 7.42 ppm (2H, d, 6.21 Hz), 6.15 ppm (2H, d, 6.17 Hz), 5.94 ppm (2H, d, 6.24 Hz), 2.59 ppm (1H, m), 2.16 ppm (3H, s), 0.92 ppm (6H, d, 6.89 Hz). Single crystals were grown by vapor diffusion of diethyl ether into methanolic solution of the compound.
Synthesis of 1A ([(bphen)2Ru(4,4′-dhbp)]Cl2).
This compound has been previously synthesized, characterized, and reported.9 Herein, we used the published procedure and report 100% purity by HPLC (see the SI).
Synthesis of 2A ([(dppz)2Ru(4,4′-dhbp)]Cl2).
[(ղ6-p-cymene)RuCl(4,4′-dhbp)]Cl (0.075 g, 0.152 mmol, 1.0 equiv.), and dppz (0.096 g, 0.289 mmol, 1.9 equiv.) were added to an oven-dried Schlenk flask equipped with a stir bar and a septum. The Schlenk flask was then evacuated and refilled thrice with N2. DMF (10 mL) dispensed from the solvent purification system (SPS) was then cannula transferred into the Schlenk flask. The reaction mixture was stirred at 140 °C under N2 for 6 d. The reaction mixture was then cooled to room temperature and stored in the freezer for 10 h. The dark purple solution was filtered and washed with copious amounts of ice-cold water. The dark solid residue was washed with 2 mL of methanol and 10 mL of dichloromethane, followed by 20 mL of diethyl ether and 10 mL of hexanes. The solid was then allowed to dry under vacuum. (Yield: 0.091 g, 0.098 mmol, 53%). 1H-NMR: 12.23 ppm (2H, s), 9.68 ppm (2H, d, 8.3 Hz), 9.55 ppm (2H, d, 8.2 Hz), 8.54 ppm (4H, m), 8.46 ppm (2H, d, 5.4 Hz), 8.26 ppm (2H,d, 5.4 Hz), 8.21 ppm (4H, t, 9.5 Hz, 4.8 Hz), 8.16 ppm (2H, d, 3.2 Hz), 8.14 ppm (2H,d, 5.6 Hz), 7.87 ppm (2H, q, 5.4 Hz, 2.8 Hz), 7.46 ppm (2H, d, 6.4 Hz), 6.95 ppm (2H, dd, 6.6 Hz, 2.5 Hz). HRMS: M = C46H28N10O2RuCl2, m/z for [M-2Cl−]2+ calcd: 427.0721, found: 427.07, [M-H+−2Cl−]+ calcd: 853.1374, found: 853.1360. IR (cm−1) 3363 (OH str), 3073, 2666, 2558 (CH str), 1617, 1564 (C=C & C=N), 1490, 1442, 1419, 1354, 1301, 1266, 1227, 1115, 1110, 1030 (C-O & =CH def), 975, 870, 845, 815, 766, 722, 575 (oop vib). HPLC was used to determine a purity of 97.6% by peak area.
Synthesis of 3A ([(dppn)2Ru(4,4′-dhbp)]Cl2).
[(ղ6-p-cymene)RuCl(4,4′-dhbp)]Cl (0.075 g, 0.152 mmol, 1.0 equiv.), and dppn (0.096 g, 0.289 mmol, 1.9 equiv.) were added to an oven-dried Schlenk flask equipped with a stir bar and a septum. The Schlenk flask was then evacuated and refilled thrice with N2. DMF (10 mL) dispensed from the SPS was then cannula transferred into the Schlenk flask. The reaction mixture was stirred at 140 °C under N2 for 6 d. Then, the reaction mixture was cooled to room temperature and stored in the freezer for 10 h. The dark purple solution was filtered and washed with copious amounts of ice-cold water. The dark solid residue was washed with 2 mL methanol and 10 mL dichloromethane, followed by 20 mL diethyl ether and 10 mL hexanes. The solid was allowed to dry in a vacuum. (Yield: 0.122 g, 0.119 mmol, 71%). 1H-NMR: 12.25 ppm (2H, s), 9.65 ppm (2H, d, 8.2 Hz, 1.1 Hz), 9.54 ppm (2H, d, 8.3 Hz, 1.1 Hz), 9.26 ppm (4H, d, 15 Hz), 8.48 ppm (2H, overlaid or embedded doublet), 8.44 ppm (4H, m), 8.29 ppm (4H, m), 8.18 ppm (2H, m, 2.6 Hz), 8.14 ppm (2H, q, 8.3 Hz, 4.1 Hz), 7.88 ppm (2H, q, 8.2 Hz, 4.1 Hz), 7.80 ppm (4H, q, 9.6 Hz), 7.52 ppm (2H, d, 6.5 Hz), 6.98 ppm (2H, dd, 6.4 Hz, 2.5 Hz). HRMS: M = C54H32N10O2RuCl2, m/z for [M-2Cl−]2+ calcd: 477.09, found: 477.09. IR (cm−1) 3347 (OH str), 3045 (CH str), 1619 (C=N str), 1452, 1348, 1313 (C=C str & C=N), 1215, 1109, 1070 (C-O str & =CH def), 881 (oop vib). HPLC was used to determine a purity of 97.4% by peak area.
Synthesis of 4A ([(bphen)2Ru(4,7-dhphen)]Cl2).
This compound was synthesized using the literature procedure but substituting 4,7-dhphen for 4,4′-dhbp.9 The compound (bphen)2RuCl2 (0.359g, 0.429 mmol) and 4,7-dhphen (0.100 g, 0.472 mmol, 1.1 equiv) were added to an oven-dried Schlenk flask equipped with a stir bar and a septum. The flask was then evacuated and refilled with N2 thrice, after which a mixture of degassed 17 mL ethanol and 17 mL distilled deionized H2O was added. The purple solution was refluxed at 120 °C for 72 h under N2. The red solution was allowed to cool to room temperature and filtered to remove excess 4,7-dhphen. The product was precipitated out of solution using three drops of concentrated HCl. The product was washed with a copious amount of water, 10 mL diethyl ether, and 10 ml hexanes. The product was then air-dried. (Yield: 0.356 g, 0.339 mmol, 71 %). 1H NMR: 13.07 ppm (2H, s), 8.35 ppm (2H, d, 4 Hz), 8.34 ppm (2H, d 4 Hz), 8.30 ppm (2H, s), 8.25 ppm (4H, s), 7.80 ppm (2H, d, 4 Hz), 7.78 ppm (2H, d, 4 Hz), 7.75 ppm (2H, d, 4.4 Hz), 7.68 ppm (8H, m), 7.64 ppm (4H, m), 7.61 ppm (8H, m), 7.29 ppm (2H, d, 4.5 Hz). HRMS: M = C60H40N6O2RuCl2, m/z for [M-H-2Cl−]+ calcd: 977.22, found: 977.22. IR (cm−1) 3383 (OH str), 3057 (CH str), 1572 (C=C str & C=N str), 1356, 1221, 1074, 1001, 905 (C-O str & =CH def), 850, 762, 695, 573, 445 (oop vib). HPLC was used to determine a purity of 100% by peak area.
Typical isolation of the deprotonated complex (4B).
Compound 4A (50 mg) was treated with 50 mL of basic MeOH at pH = 8.2 (prepared by methanol mixed with aqueous NaOH) and stirred for 3 h. The dark purple solution was filtered and evaporated to dryness. The dark purple solid was then dissolved in 2 mL dry EtOH and 40 mL dry acetonitrile. The purple solution was dried with magnesium sulfate and filtered. The solution was evaporated to dryness. The dark purple solid was then washed with diethyl ether and hexanes. The solid was dried under vacuum. The yield of 4B was 66 %. The purity and identity of 4B was confirmed by 1H-NMR.
Synthesis of 5A ([(dppz)2Ru(4,7-dhphen)]Cl2).
[(ղ6-p-cymene)RuCl(4,7-dhphen)]Cl (0.075 g, 0.15 mmol, 1.0 equiv.) and dppz (0.082 g, 0.29 mmol, 2.0 equiv.) were added to an oven-dried Schlenk flask equipped with a stir bar and a septum. The Schlenk flask was then evacuated and refilled thrice with N2. Dimethyl formamide (10 mL) dispensed from the SPS was then cannula transferred into the Schlenk flask. The reaction mixture was stirred at 140 °C under N2 for 6 d. The reaction mixture was then cooled to room temperature and stored in the freezer for 10 h. The dark purple solution was filtered and washed with copious amounts of ice-cold water. The dark solid residue was then washed with 2 mL methanol and 10 mL dichloromethane, followed by 20 mL diethyl ether and 10 mL hexanes. The solid was then dried under vacuum. (Yield: 0.090 g, 0.09 mmol, 59 %). 1H NMR: 13.09 ppm (2H, s), 9.58 ppm (4H, d, 5.9 Hz), 8.52 ppm (4H, m), 8.39 ppm (2H, d, 3.8 Hz), 8.29 ppm (2H, s), 8.20 ppm (4H,q, 2.5 Hz, 4.8 Hz), 7.93 ppm (4H, m), 7.79 ppm (2H, d, 4.5 Hz), 7.25 ppm (2H,d, 4.5 Hz). HRMS: M = C48H28N10O2RuCl2, m/z for [M-2Cl−]2+ calcd: 439.0721, found: 439.0720, m/z for [M-H+−2Cl−]+ calcd: 877.1375, found: 877.1352. IR (cm−1) 3342 (OH str), 3047–2333 (CH str), 1603, 1572, 1527, 1505, 1411 (C=C & C=N), 1350, 1205, 1115 (C-O str & =CH def), 824, 807, 756, 720, 577 (oop vib). HPLC was used to determine a purity of 97.6% by peak area.
Synthesis of 6A ([(dppn)2Ru(4,7-dhphen)]Cl2).
[(ղ6-p-cymene)RuCl(4,7-dhphen)]Cl (0.075 g, 0.145 mmol, 1.0 equiv.) and dppn (0.096 g, 0.275 mmol, 1.9 equiv.) were added to an oven-dried Schlenk flask equipped with a stir bar and a septum. The Schlenk flask was then evacuated and refilled thrice with N2. DMF (10 mL) dispensed from the SPS was then cannula transferred into the Schlenk flask. The reaction mixture was stirred at 140 °C under N2 for 6 d. The reaction mixture was then cooled to room temperature and stored in the freezer for 10 h. The dark purple solution was then filtered and washed with copious amounts of ice-cold water. The dark solid residue was then washed with 2 mL methanol and 10 mL dichloromethane followed by 20 mL diethyl ether and 10 mL hexanes. The solid was then allowed to dry in vacuum. (Yield: 0.152 g, 0.144 mmol, 82%). 1H NMR: 13.05 ppm (2H, s), 9.59 ppm (4H, d, 8.10 Hz), 9.26 ppm (4H, d, 5.33 Hz), 8.47 ppm (4H), 8.42 ppm (2H, d, 5.44 Hz), 8.32 ppm (2H, s), 8.30 ppm (2H,d, 5.47 Hz), 7.95 ppm (4H, m), 7.86 ppm (2H, d, 6.1 127 Hz), 7.80 ppm (4H, q), 7.24 ppm (2H, d, 6.1 Hz). HRMS: M = C56H32N10O2RuCl2 m/z for [M-2Cl−]2+ calcd: 489.0879, found: 489.1134, m/z for [M-H+−2Cl−]+ calcd: 977.1690, found: 977.2155. IR (cm−1) 3371 (OH str), 3067 (CH str), 1550 (C=C), 1417, 1348, 1297, 1264, 1258, 1213, 1107, 1070 (C=C & C=N), 869, 817 (C-O str & -CH def), 724, 575, 490 (oop vib). HPLC was used to determine a purity of 100% by peak area.
Single Crystal X-ray Diffraction.
CCDC Deposition Numbers 2479506–2479509 contain the supplementary crystallographic data for this paper. These data are provided free of charge by the joint Cambridge Crystallographic Data Centre and Fachinformationszentrum Karlsruhe Access Structures service www.ccdc.cam.ac.uk/structures. Single clear red block-shaped crystals of 1A and 4A and yellowish orange irregular shaped crystals of P1 and P2 were obtained by vapor diffusion of diethyl ether into a saturated methanolic solution of respective compounds. Suitable crystals 0.19×0.14×0.09 mm3 (1A), 0.17×0.15×0.07 mm3 (4A), 0.17×0.13×0.09 mm3 (P1), and 0.23×0.20×0.09 mm3 (P2) were selected and mounted on a suitable support on an XtaLAB Synergy R, DW system, HyPix diffractometer. The crystals were kept at a steady T = 100.01(16) K during data collection.
The structures were solved with the ShelXT 2018/241 (Sheldrick, 2018) (1A) and ShelXT 2014/542 (4A, P1, P2) structure solution program using the Intrinsic Phasing solution method and by using Olex243 as the graphical interface. The models were refined with version 2016/6 of ShelXL 2016/644 using Least Squares minimization.
Data were measured using ω scans of 0.5° per frame for 2.8/11.1 s (1A) and 5.2/15.0 s (4A) using Cu Ka radiation and ω scans of 0.5° per frame for 4.3s (P1) and 3.0s (P2) using Mo Ka radiation. The diffraction patterns were indexed and the total number of runs and images were based on the strategy calculation from the program CrysAlisPro45 for 1A, CrysAlisPro46 for 4A, and CrysAlisPro47 for P1 and P2. The maximum resolution for achieved for each data collection is Θ = 77.221° (0.79 Å) (1A), 77.111° (0.79 Å) (4A), 32.469° (0.66 Å) (P1), 33.398° (0.65 Å) (P2).
The diffraction patterns were indexed, and the total number of runs and images were based on the strategy calculation from the program CrysAlisPro. The unit cell for 1A was refined using CrysAlisPro41 on 25109 reflections, 44% of the observed reflections. The Unit cell for 4A was refined using CrysAlisPro42 on 44674 reflections, 37% of the observed reflections. The unit cell for P1 and P2 were refined using CrysAlisPro43 on 25841 (P1) and 25896 (P2) reflections with the used reflections comprising 78% and 74% of the total observed reflections, respectively.
Data reduction, scaling, and absorption corrections were performed using CrysAlisPro. The final completeness is 100.00 % out to 77.221° in Θ for 1A and 4A and 99.90 % out to 32.469° and 99.90 % out to 33.398° for P1 and P2. A gaussian absorption correction was performed using CrysAlisPro. Numerical absorption correction based on gaussian integration over a multifaceted crystal absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm. For 1A, the absorption coefficient μ of this material is 3.635 mm−1 at this wavelength (λ = 1.542Å) and the minimum and maximum transmissions are 0.449 and 0.728. For 4A The absorption coefficient μ of this material is 4.111 mm−1 at this wavelength (λ = 1.542Å) and the minimum and maximum transmissions are 0.621 and 0.903. For P1 The absorption coefficient μ of this material is 1.007 mm−1 at this wavelength (λ = 0.771Å) and the minimum and maximum transmissions are 0.892 and 1.000. For P2 The absorption coefficient μ of this material is 0.985 mm−1 at this wavelength (λ = 0.771Å) and the minimum and maximum transmissions are 0.820 and 1.000.
The structure for 1A was solved and the space group C222 (# 21) determined by the ShelXT 2018/241 structure solution program using Intrinsic Phasing and refined by Least Squares using version 2016/6 of ShelXL 2016/6.44
The structure for 4A was solved and the space group I41/acd (# 142) determined by the ShelXT 2014/542 structure solution program using Intrinsic Phasing and refined by Least Squares using version 2016/6 of ShelXL 2016/6.44 All non-hydrogen atoms were refined anisotropically. Hydrogen atom positions were calculated geometrically and refined using the riding model.
The structure for P1 was solved and the space group P21/n (# 14) determined by the ShelXT 2014/542 structure solution program using Intrinsic Phasing and refined by Least Squares using version 2016/6 of ShelXL 2016/6.44 All non-hydrogen atoms were refined anisotropically. Hydrogen atom positions were calculated geometrically and refined using the riding model.
The structure for P2 was solved and the space group P21/c (# 14) determined by the ShelXT 2014/542 structure solution program using Intrinsic Phasing and refined by Least Squares using version 2016/6 of ShelXL 2016/6.44 All non-hydrogen atoms were refined anisotropically. Hydrogen atom positions were calculated geometrically and refined using the riding model.
Purity determination.
The analyte solutions (1A-6A) were made in methanol and stirred at room temperature for 2 h. The solution was filtered using a polytetrafluoroethylene (PTFE) filter (13 mm, 0.2 μm). The method employed three mobile phases for the gradient elution. Water plus 0.1% formic acid (FA) (v/v) and methanol were used in solvent lines A and B, respectively. At time t = 0, solvent line A was 100 % at the pump, and this was held for elution at a flow rate of 1.0 mL/min. This method employed needle wash to avoid cross-contamination between sample injections. At the sampler, the method also employs an injection volume of 5.0 μL, a draw speed of 100 μL/min, eject speed of 400 μL/min, a wait time after draw of 1.2 s, and a sample flush-out factor of 5.0 times injection volume. In the column, the analysis was set to run at 25 °C. At the diode array detector (DAD), the wavelengths acquired are 250, 270, 300, 320, and 350 nm. The wavelength with the highest response area is used for the purity determination. The full spectrum of the chromatogram was collected at a bandwidth of 4 nm. This method is tabulated in Table S3.
HPLC determination of lipophilic vs. hydrophilic properties.
The lipophilicity analysis by HPLC (log(Do/w) values) was performed on an Agilent 1260 HPLC with a diode array detector (DAD), vial sampler, quaternary pump, and column oven. An Agilent analytical column (poroshell 120 EC-C18, 4.6 × 150 mm, 2.7 μm) was used. The dwell volume was measured according to the method in Table S2 and Figure S29.
HPLC reagent methanol, and HPLC grade water were obtained from VWR, reagent grade formic acid (FA), sodium phosphate dibasic heptahydrate, sodium phosphate monobasic monohydrate, octanol. Phosphate buffer (pH 7.4) was prepared and filtered using the Agilent InfinityLab filtration assembly system. The pH was measured using a calibrated Mettler Toledo pH meter. Stock solutions (100 μM) of the compounds 1A and 4A were made in pH 7.4 phosphate buffer pre-saturated octanol. The solution was filtered using a polytetrafluoroethylene (PTFE) filter (13 mm, 0.2 μm). The octanol layer (1 mL) was then transferred into a 2 mL HPLC vial to determine the concentration of Ru in octanol. The solution was stirred at room temperature for 18 h. The stock solution was filtered using a polytetrafluoroethylene (PTFE) filter (13 mm, 0.2 μm). Six dilutions from the stock solution were made up with pre-saturated octanol for the lipophilicity experiments. For the log(Do/w) experiments, 5 mL of concentration ([Xoct]i), where X is 1A or 4A from the diluted series (10 μM to 80 μM), is added to 5 mL pre-saturated pH 7.4 phosphate buffer. The 10 mL solution was stirred at room temperature for 48 h. For efficient separation, the solution was then centrifuged for 2 h. A sample from the octanol layer (1 mL) was then transferred into a 2 mL HPLC vial ([Xoct]f). The quaternary solvent pump was used for gradient elution with two mobile phases. Water with 0.1% TFA (v/v) an methanol were used in solvent lines A and B, respectively. At time t = 0, solvent line A was 100 % at the pump, and this was held for isocratic elution at a flow rate of 1.5 mL/min. From t = 1 to 15 min, a linear gradient from 90% A to 0% A and 10% B to 100% B was applied at the pump at a flow rate of 1.0 mL/min. This method employed needle wash to avoid cross-contamination between sample injections. At the sampler, the method employs an injection volume of 1.0 μL, a draw speed of 100 μL/min, eject speed of 400 μL/min, a wait time after draw of 1.2 s and a sample flush-out factor of 5.0 times injection volume. At the column the analysis was set to run at 25.0 °C. At the DAD, the absorptions are acquired at 250, 270, 300, 320, 350, and 370 nm wavelengths. The wavelength with the highest response factor (peak area) is used for the calibration curve. The full spectrum of the chromatogram was collected at a bandwidth of 4 nm. A single phase (octanol) was analyzed because no response was recorded on the chromatogram for the aqueous phosphate buffer phase. A calibration curve of concentration versus area of response for each of the six compounds was obtained using the six dilutions, and the concentration of the analyte in the octanol ([Xoct]f) is calculated from the calibration curve. Due to the insolubility of the compounds 1A and 4A in aqueous buffer, the final concentration of the compounds in aqueous buffer [XAq]f was calculated as [Xoct]i-[Xoct]f. This method was developed to determine the lipophilicity of compounds 1A and 4A and verified using compounds with reported lipophilicity values. The lipophilicity of the compounds is calculated as log(Do/w) = Log ([Xoct]f)/([XAq]f).
Absorption and Photoluminescence Studies.
The compounds were prepared in the glovebox using dry acetonitrile dispensed from the solvent purification system. The solution was then filtered using a 5-μm syringe filter to remove undissolved compounds. The absorption spectra of these solutions were recorded on a Jasco V-780 spectrophotometer from 250 nm to 800 nm. The photoluminescence spectra of the compounds were recorded on a Horiba Fluoromax+ fluorimeter The same samples used for absorption studies were utilized for luminescence studies. The samples were excited at the absorption maxima of the complexes, as obtained from electronic spectroscopy. The emission spectra were collected from 500 nm to 900 nm using appropriate band filters to avoid reabsorption. The emission and excitation splits were both 10 nm.
Photoluminescence quantum yield measurements.
The photoluminescence quantum yield (PLQY) of compound 1A-6A was measured using the Horiba Fluoromax. The sample solutions were prepared in the glovebox using acetonitrile dispensed from the solvent purification system (SPS). These compounds were dissolved, and the solution was transferred into a fluorescence cuvette equipped with a septum. The cuvette was wrapped with parafilm to prevent air and moisture from entering, after which the absorbance and absorption wavelength were measured. The sample solution was prepared such that the maximum absorbance of the samples is below 0.4 to avoid the inner filter effect. Although this may not pose a problem to our compounds because of the large Stokes shift,48, 49 absorbance correction was factored into the calculations to remove errors due to lamp output.
The quantum yield of luminescence measurements was calculated using the relative method, which compares the absorbance and emission of the standard with that of the sample under the same irradiance condition, and was calculated using equation (1), which calculates the quantum yield of the unknown as a product of the luminescence quantum yield of the standard (ɸs) and the integrated emission area (I), the corrected absorbance fractions (F) and the solvents refractive index (n) of the unknown (X) and the standard [(bpy)3Ru]Cl2.48, 49
| (1) |
Photoluminescence excitation measurement (PLE).
Samples were prepared in the same manner as mentioned above for photoluminescence experiments. The monitored wavelengths for the PLE experiments are 642 nm (1A), 671 nm (2A), 566 nm (3A), 653 nm (4A), 680 nm (5A), and 571 nm (6A).
Luminescence lifetime measurements.
Luminescence lifetime measurements of compounds 1A-6A were carried out on the Horiba Delta Flex fluorescence lifetime system using the time-correlated single-photon counting method (TCSPC) with the 404 nm excitation and 0.1 ns resolution.
Quantum Yield of Singlet Oxygen.
Using [Ru(bpy)3]2+ as the standard (ΦΔ = 0.56 in aerated MeCN), quantum yields (ΦΔ) were calculated per the actinometric method described by eq. 2, where I denote the integration of the emission band, A is the solution UV-Vis absorption at the excitation wavelength, and η is the solvent’s refractive index (η2/ηS2=1 here, as MeCN was used in both). The [Ru(bpy)3]2+ standard is denoted by the subscript S.
| (2) |
Emission spectra were measured on a PTI Quantamaster emission spectrometer equipped with a Hamamatsu R550942 near-infrared photomultiplier tube behind a 1000 nm long-pass filter. The emission and excitation spectra were corrected for lamp output and detector response nonlinearities. The longest wavelength in the excitation spectrum with the most intense emission at 1276 nm was selected as the excitation wavelength. The emission spectra were collected over 1200–1350 nm and integrated with baseline correction. Values were generally reproducible within ± 5%.
Cytotoxicity and photocytotoxicity.
Compounds 1A-6A were assessed for their biological activity in the light and in the dark against human skin melanoma cells (SK-MEL-28), hormone receptor-positive breast cancer cells (MCF-7), and triple-negative breast cancer cells (MDA-MB-231). The cells were cultured as 2D monolayer cells.
MCF-7 and MDA-MB-231.
Experiments to determine photocytotoxicity in MCF-7 and MDA-MB-231 were performed in triplicates. Breast epithelial adenocarcinoma cell lines MDA-MB-231 and MCF-7 (ATCC, Manassas, VA) were seeded in 96-well plates at a density of 10,000 cells per well using a 100 μL Dulbecco’s Modified Eagle Media phenol red-free (Gibco, Waltham, MA) supplemented with 10% v/v fetal bovine serum (Gibco) media. The compounds were dissolved in 1% v/v DMSO and diluted with cell media. The final DMSO concentration in the solution was kept at < 1% to prevent the cytotoxicity of DMSO to cells.
For initial screening, the cells were treated with 5 μM of the compounds. For EC50 determination, the cells were treated with varying concentrations of the compounds. The compounds were incubated with the cells for 48 h in the dark. The incubated cells were then gently washed with phosphate-buffered saline (pH 7.2, 3 × 200 μL; Gibco) and left in the dark for additional 2 h (for EC50 dark) or irradiated for 2 h with white light (STASUN 200 W LED flood light, 100–256 V, 20,000 lm, 40,000 lx, irradiance: 40 mW cm−2, total fluence: 288 J cm−2, irradiation time of approximately 2 h) (for EC50 light). All cells were incubated in fresh media (200 μL per well) for 20 h in the dark.
Cell viability was measured using Cell Counting Kit-8 at 450 nm according to the manufacturer’s protocol (Enzo Life Sciences, Farmingdale, NY). The EC50 of the compounds was then determined using a nonlinear regression fit of the dose-response curve with the following formula (eq 3) using GraphPad Prism (v10.0.3, La Jolla, CA):
| (3) |
where Aobs is the observed absorbance, Amax and Amin are the maximum and minimum absorbance, respectively.
Normoxia in SKMEL28.
Compounds 1A-6A were screened for their dark and light cytotoxicities toward SK-MEL-28 human melanoma cells under normoxia (~18.5 O2). The cells (passage 11) growing in the log phase were first seeded in 384-well plates and incubated for 2–3 h before dosing with compound (1 nM to 300 μM). Stock solutions were made in 10% DMSO in water at 5mM, and the dilutions (1 nM – 300 uM) were made in DPBS.
Light treatment was delivered after PS addition with a drug-to-light interval (DLI) of 19 h, using a fluence of 100 J/cm2 and irradiance of 19–24 mW/cm2 (irradiation time of approximately 1 h) delivered from broadband visible (450 nm maxima, 400–700 nm) light source or LEDs emitting blue (453 nm), green (523 nm) or red (633 nm) light. The light-treated cells were then incubated for 23 h (post-PDT incubation) before measuring cell viability using the resazurin assay. Spectramax m2e fluorescent microplate reader was used for reading the plates after 4 h incubation with resazurin. EC50 values, the effective concentration to reduce relative cell viability by 50%, were obtained from logistic fits of the dose-response curves for the dark and light conditions. Phototherapeutic indices (PIs) were calculated as the ratio of dark to light EC50 values and reflect amplification of cytotoxic effects by light and is the appropriate parameter to use for comparing PS potencies.
Reactive Oxygen Species (ROS) Assay: Peroxide.
A 10 mM stock solution of 3 or 6 was prepared in pH 7.5 phosphate buffer and each compound was tested separately. Samples of each compound and corresponding buffer-only controls were irradiated for 1 h at a fixed distance of 6 inches from the light source. Following irradiation, catalase (5 μM) was added to all samples and controls to convert photogenerated hydrogen peroxide into molecular oxygen. Oxygen evolution was quantified using a Clark-type O2 electrode, and the corrected O2 signal (sample minus control) was used to evaluate peroxide formation by each compound under these conditions.
Thermodynamic acidity (pKa values) measurements.
Ten milligrams of compound 3A, 4A, or 6A was dissolved in 10 % EtOH (with the other solvent being DI water). Five equivalents of HCl was added via 0.1M HCl to obtain a pH of ~2.6 to ensure protonation of the complex at the start and the UV-Vis spectra were taken (Figures S64–S66). A sample of the solution was then titrated against 0.00576 M of NaOH (standardized with KHP) to provide pKa values (Figures S61–S63). A sample from the titration was used to provide a UV-Vis spectrum at pH of 9.8 for 3B, 4B and 6B (Figures S64–S66).
Supplementary Material
The Supporting Information is available free of charge on the ACS Publications website at DOI: xxxx.
Experimental details including spectra and HPLC analysis (PDF)
ACKNOWLEDGMENT
This research was funded by the National Institute of General Medical Sciences (R15-GM132803) to ETP and YK; National Science Foundation MRI grants at the University of Alabama (CHE 1726812, 1828078, 1919906) for MS, SC XRD, and NMR instruments; and the National Cancer Institute (R01CA222227) to SAM for support in part of this work. We acknowledge undergraduates in the Kim group for their technical assistance in cell studies. We thank Annie Garness, Yifei Sun, Eli Chambers, and Spenser Brown for preliminary experiments and Brad Pierce for helpful discussions and use of a Clark Electrode. IF thanks UA for startup funds. We thank Qiaoli Liang for MS experimental work. We thank Ken Belmore for assistance with the NMR experiments. The content in this paper is solely the responsibility of the authors and does not necessarily represent the official views of the National Institutes of Health.
Footnotes
CONFLICT OF INTEREST STATEMENT
S.A.M. has a potential research conflict of interest due to a financial interest with Theralase Technologies, Inc. and PhotoDynamic, Inc. A management plan has been created to preserve objectivity in research in accordance with UTA policy.
References
- (1).Monro S; Colón KL; Yin H; Roque J; Konda P; Gujar S; Thummel RP; Lilge L; Cameron CG; McFarland SA Transition Metal Complexes and Photodynamic Therapy from a Tumor-Centered Approach: Challenges, Opportunities, and Highlights from the Development of TLD1433. Chem. Rev 2019, 119, 797–828. DOI: 10.1021/acs.chemrev.8b00211. [DOI] [PMC free article] [PubMed] [Google Scholar]
- (2).Dickerson M; Sun Y; Howerton B; Glazer EC Modifying Charge and Hydrophilicity of Simple Ru(II) Polypyridyl Complexes Radically Alters Biological Activities: Old Complexes, Surprising New Tricks. Inorg. Chem 2014, 53, 10370–10377. DOI: 10.1021/ic5013796. [DOI] [PMC free article] [PubMed] [Google Scholar]
- (3).Karges J; Kuang S; Ong YC; Chao H; Gasser G One- and Two-Photon Phototherapeutic Effects of RuII Polypyridine Complexes in the Hypoxic Centre of Large Multicellular Tumor Spheroids and Tumor-Bearing Mice. Chem. Eur. J 2021, 27, 362–370. DOI: 10.1002/chem.202003486. [DOI] [PubMed] [Google Scholar]
- (4).Toupin NP; Nadella S; Steinke SJ; Turro C; Kodanko JJ Dual-Action Ru(II) Complexes with Bulky π-Expansive Ligands: Phototoxicity without DNA Intercalation. Inorg. Chem 2020, 59, 3919–3933. DOI: 10.1021/acs.inorgchem.9b03585. [DOI] [PMC free article] [PubMed] [Google Scholar]
- (5).Reichardt C; Monro S; Sobotta FH; Colón KL; Sainuddin T; Stephenson M; Sampson E; Roque J; Yin H; Brendel JC; Cameron CG; McFarland S; Dietzek B Predictive Strength of Photophysical Measurements for in Vitro Photobiological Activity in a Series of Ru(II) Polypyridyl Complexes Derived from π-Extended Ligands. Inorg. Chem 2019, 58, 3156–3166. DOI: 10.1021/acs.inorgchem.8b03223. [DOI] [PMC free article] [PubMed] [Google Scholar]
- (6).Reichardt C; Sainuddin T; Wächtler M; Monro S; Kupfer S; Guthmuller J; Gräfe S; McFarland S; Dietzek B Influence of Protonation State on the Excited State Dynamics of a Photobiologically Active Ru(II) Dyad. J. Phys. Chem. A 2016, 120, 6379–6388. DOI: 10.1021/acs.jpca.6b05957. [DOI] [PubMed] [Google Scholar]
- (7).Park S; Gray JL; Altman SD; Hairston AR; Beswick BT; Kim Y; Papish ET Cellular uptake of protic ruthenium complexes is influenced by pH dependent passive diffusion and energy dependent efflux. J. Inorg. Biochem 2020, 203, 110922. DOI: 10.1016/j.jinorgbio.2019.110922. [DOI] [PMC free article] [PubMed] [Google Scholar]
- (8).Oladipupo OE; Prescott MC; Blevins ER; Gray JL; Cameron CG; Qu F; Ward NA; Pierce AL; Collinson ER; Hall JF; Park S; Kim Y; McFarland SA; Fedin I; Papish ET Ruthenium Complexes with Protic Ligands: Influence of the Position of OH Groups and pi Expansion on Luminescence and Photocytotoxicity. Int. J. Mol. Sci 2023, 24, 5980. DOI: 10.3390/ijms24065980. [DOI] [PMC free article] [PubMed] [Google Scholar]
- (9).Oladipupo O; Brown SR; Lamb RW; Gray JL; Cameron CG; DeRegnaucourt AR; Ward NA; Hall JF; Xu Y; Petersen CM; Qu F; Shrestha AB; Thompson MK; Bonizzoni M; Webster CE; McFarland SA; Kim Y; Papish ET Light-responsive and Protic Ruthenium Compounds Bearing Bathophenanthroline and Dihydroxybipyridine Ligands Achieve Nanomolar Toxicity towards Breast Cancer Cells. Photochem. Photobiol 2022, 98, 102–116. DOI: 10.1111/php.13508. [DOI] [PMC free article] [PubMed] [Google Scholar]
- (10).Qu F; Lamb RW; Cameron CG; Park S; Oladipupo O; Gray JL; Xu Y; Cole HD; Bonizzoni M; Kim Y; McFarland SA; Webster CE; Papish ET Singlet Oxygen Formation vs Photodissociation for Light-Responsive Protic Ruthenium Anticancer Compounds: The Oxygenated Substituent Determines Which Pathway Dominates. Inorg. Chem 2021, 60, 2138–2148. DOI: 10.1021/acs.inorgchem.0c02027. [DOI] [PMC free article] [PubMed] [Google Scholar]
- (11).Karges J; Heinemann F; Jakubaszek M; Maschietto F; Subecz C; Dotou M; Vinck R; Blacque O; Tharaud M; Goud B; Viñuelas Zahínos E; Spingler B; Ciofini I; Gasser G Rationally Designed Long-Wavelength Absorbing Ru(II) Polypyridyl Complexes as Photosensitizers for Photodynamic Therapy. J. Am. Chem. Soc 2020, 142, 6578–6587. DOI: 10.1021/jacs.9b13620. [DOI] [PubMed] [Google Scholar]
- (12).Friedman AE; Chambron JC; Sauvage JP; Turro NJ; Barton JK A molecular light switch for DNA: Ru(bpy)2(dppz)2+. J. Am. Chem. Soc 1990, 112, 4960–4962. DOI: 10.1021/ja00168a052. [DOI] [Google Scholar]
- (13).Hartshorn RM; Barton JK Novel dipyridophenazine complexes of ruthenium(II): exploring luminescent reporters of DNA. J. Am. Chem. Soc 1992, 114, 5919–5925. [Google Scholar]
- (14).Brennaman MK; Meyer TJ; Papanikolas JM [Ru(bpy)2dppz]2+ Light-switch mechanism in protic solvents as studied through temperature-dependent lifetime measurements. J. Phys. Chem. A 2004, 108, 9938–9944. [Google Scholar]
- (15).Brennaman MK; Alstrum-Acevedo JH; Fleming CN; Jang P; Meyer TJ; Papanikolas JM Turning the [Ru(bpy)2dppz]2+ light-switch on and off with temperature. J. Am. Chem. Soc 2002, 124, 15094–15098. DOI: 10.1021/ja0279139. [DOI] [PubMed] [Google Scholar]
- (16).Wachter E; Glazer EC Mechanistic Study on the Photochemical “Light Switch” Behavior of [Ru(bpy)2dmdppz]2+. J. Phys. Chem. A 2014, 118, 10474–10486. DOI: 10.1021/jp504249a. [DOI] [PubMed] [Google Scholar]
- (17).Önfelt B; Olofsson J; Lincoln P; Nordén B Picosecond and Steady-State Emission of [Ru(phen)2dppz]2+ in Glycerol: Anomalous Temperature Dependence. J. Phys. Chem. A 2003, 107, 1000–1009. [Google Scholar]
- (18).Sun Y; Joyce LE; Dickson NM; Turro C DNA photocleavage by an osmium(II) complex in the PDT window. Chem. Commun 2010, 46, 6759–6761. DOI: 10.1039/c0cc02571b. [DOI] [Google Scholar]
- (19).Sun Y; Lutterman DA; Turro C Role of electronic structure on DNA light-switch behavior of Ru(II) intercalators. Inorg. Chem 2008, 47, 6427–6434. DOI: 10.1021/ic800560x. [DOI] [PubMed] [Google Scholar]
- (20).Liu Y; Chouai A; Degtyareva NN; Lutterman DA; Dunbar KR; Turro C Chemical control of the DNA light switch: cycling the switch ON and OFF. J. Am. Chem. Soc 2005, 127, 10796–10797. DOI: 10.1021/ja052648n. [DOI] [PubMed] [Google Scholar]
- (21).Foxon SP; Alamiry MA; Walker MG; Meijer AJ; Sazanovich IV; Weinstein JA; Thomas JA Photophysical properties and singlet oxygen production by ruthenium(II) complexes of benzo[i]dipyrido[3,2-a:2’,3’-c]phenazine: spectroscopic and TD-DFT study. J. Phys. Chem. A 2009, 113, 12754–12762. DOI: 10.1021/jp906716g. [DOI] [PubMed] [Google Scholar]
- (22).Sainuddin T; McCain J; Pinto M; Yin H; Gibson J; Hetu M; McFarland SA Organometallic Ru(II) Photosensitizers Derived from π-Expansive Cyclometalating Ligands: Surprising Theranostic PDT Effects. Inorg. Chem 2016, 55, 83–95. DOI: 10.1021/acs.inorgchem.5b01838. [DOI] [PubMed] [Google Scholar]
- (23).Qu F; Park S; Martinez K; Gray JL; Thowfeik FS; Lundeen JA; Kuhn AE; Charboneau DJ; Gerlach DL; Lockart MM; Law JA; Jernigan KL; Chambers N; Zeller M; Piro NA; Kassel WS; Schmehl RH; Paul JJ; Merino EJ; Kim Y; Papish ET Ruthenium Complexes are pH-Activated Metallo Prodrugs (pHAMPs) with Light-Triggered Selective Toxicity Toward Cancer Cells. Inorg. Chem 2017, 56, 7519–7532. DOI: 10.1021/acs.inorgchem.7b01065. [DOI] [PubMed] [Google Scholar]
- (24).Giordano PJ; Bock CR; Wrighton MS Excited State Proton Transfer of Ruthenium(II) Complexes of 4,7-Dihydroxy-1,10-phenanthroline. Increased Acidity in the Excited State. J. Am. Chem. Soc 1978, 100, 6960–6965. [Google Scholar]
- (25).Himeda Y Conversion of CO2 into Formate by Homogeneously Catalyzed Hydrogenation in Water: Tuning Catalytic Activity and Water Solubility through the Acid–Base Equilibrium of the Ligand. Eur. J. Inorg. Chem 2007, 2007, 3927–3941. DOI: 10.1002/ejic.200700494. [DOI] [Google Scholar]
- (26).Martinez K; Koehne SM; Benson K; Paul JJ; Schmehl RH Bimolecular Excited-State Proton-Coupled Electron Transfer within Encounter Complexes. J. Am. Chem. Soc 2023, 145, 4462–4472. DOI: 10.1021/jacs.2c10165. [DOI] [PMC free article] [PubMed] [Google Scholar]
- (27).Valladolid J; Hortigüela C; Busto N; Espino G; Rodríguez AM; Leal JM; Jalón FA; Manzano BR; Carbayo A; García B Phenanthroline ligands are biologically more active than their corresponding ruthenium(II) arene complexes. Dalton Trans. 2014, 43, 2629–2645. DOI: 10.1039/c3dt52743c. [DOI] [PubMed] [Google Scholar]
- (28).Ogo S; Abura T; Watanabe Y pH-Dependent Transfer Hydrogenation of Ketones with HCOONa as a Hydrogen Donor Promoted by (η6-C6Me6)Ru Complexes. Organometallics 2002, 21, 2964–2969. DOI: 10.1021/om011059x. [DOI] [Google Scholar]
- (29).Meshcheryakova VA; Grivin VP; Mikheylis AV; Tsentalovich YP; Kokorenko AA; Pozdnyakov IP; Ershov KS; Baklanov AV; Zazulya AE; Vasilchenko DB; Melnikov AA; Chekalin SV; Glebov EM Photophysical properties of benzo[i]dipyrido[3,2-a:2′,3′-c] phenazine (dppn) - A prospective ligand for light-activated anticancer complexes. J. Lumin 2024, 275, 120804. DOI: 10.1016/j.jlumin.2024.120804. [DOI] [Google Scholar]
- (30).Passalacqua R; Loiseau F; Campagna S; Fang YQ; Hanan GS In search of ruthenium(II) complexes based on tridentate polypyridine ligands that feature long-lived room-temperature luminescence: the multichromophore approach. Angew. Chem. Int. Ed. Engl 2003, 42, 1608–1611. DOI: 10.1002/anie.200250613. [DOI] [PubMed] [Google Scholar]
- (31).Wang X.-y.; Guerzo AD; Schmehl RH Photophysical behavior of transition metal complexes having interacting ligand localized and metal-to-ligand charge transfer states. J. Photochem. Photobiol. C: Photochem. Rev 2004, 5, 55–77. [Google Scholar]
- (32).Verma S; Kar P; Das A; Ghosh HN Photophysical properties of ligand localized excited state in ruthenium(ii) polypyridyl complexes: a combined effect of electron donor–acceptor ligand. Dalton Trans. 2011, 40, 9765–9773. DOI: 10.1039/C1DT10266D. [DOI] [PubMed] [Google Scholar]
- (33).Alfonso-Prieto M; Biarnés X; Vidossich P; Rovira C The Molecular Mechanism of the Catalase Reaction. Journal of the American Chemical Society 2009, 131, 11751–11761. DOI: 10.1021/ja9018572. [DOI] [PubMed] [Google Scholar]
- (34).Bielski BHJ; Allen AO Mechanism of the disproportionation of superoxide radicals. The Journal of Physical Chemistry 1977, 81, 1048–1050. DOI: 10.1021/j100526a005. [DOI] [Google Scholar]
- (35).Tardito S; Bassanetti I; Bignardi C; Elviri L; Tegoni M; Mucchino C; Bussolati O; Franchi-Gazzola R; Marchiò L Copper Binding Agents Acting as Copper Ionophores Lead to Caspase Inhibition and Paraptotic Cell Death in Human Cancer Cells. J. Am. Chem. Soc 2011, 133, 6235–6242. DOI: 10.1021/ja109413c. [DOI] [PubMed] [Google Scholar]
- (36).Che C-M; Sun RW-Y Therapeutic applications of gold complexes: lipophilic gold(III) cations and gold(I) complexes for anti-cancer treatment. Chem. Commun 2011, 47, 9554–9557. DOI: 10.1039/c1cc10860c. [DOI] [Google Scholar]
- (37).Svensson FR; Matson M; Li M; Lincoln P Lipophilic ruthenium complexes with tuned cell membrane affinity and photoactivated uptake. Biophys. Chem 2010, 149, 102–106. DOI: 10.1016/j.bpc.2010.04.006. [DOI] [PubMed] [Google Scholar]
- (38).Murphy MP Targeting lipophilic cations to mitochondria. Biochim. Biophys. Acta - Bioenerg 2008, 1777, 1028–1031. DOI: 10.1016/j.bbabio.2008.03.029. [DOI] [Google Scholar]
- (39).Savic A; Kaczmarek AM; Van Deun R; Van Hecke K DNA Intercalating Near-Infrared Luminescent Lanthanide Complexes Containing Dipyrido[3,2-a:2’,3’-c]phenazine (dppz) Ligands: Synthesis, Crystal Structures, Stability, Luminescence Properties and CT-DNA Interaction. Molecules 2020, 25, 5309. DOI: 10.3390/molecules25225309. [DOI] [PMC free article] [PubMed] [Google Scholar]
- (40).Foxon SP; Green C; Walker MG; Wragg A; Adams H; Weinstein JA; Parker SC; Meijer AJHM; Thomas JA Synthesis, Characterization, and DNA Binding Properties of Ruthenium(II) Complexes Containing the Redox Active Ligand Benzo[i]dipyrido[3,2-a:2′,3′-c]phenazine-11,16-quinone. Inorg. Chem 2011, 51, 463–471. DOI: 10.1021/ic201914h. [DOI] [PubMed] [Google Scholar]
- (41).SHELXL-2018. Program for Crystal Structure Refinement; University of Göttingen: Göttingen., 2018. [Google Scholar]
- (42).SHELXL-2014/1, Program for Crystal Structure Refinement.; University of Göttingen: Göttingen, 2014. [Google Scholar]
- (43).Dolomanov OV; Bourhis LJ; Gildea RJ; Howard JAK; Puschmann H OLEX2: a complete structure solution, refinement and analysis program. J. Appl. Cryst 2009, 42, 339–341. DOI: 10.1107/S0021889808042726. [DOI] [Google Scholar]
- (44).Sheldrick GM Crystal structure refinement with SHELXL. Acta Cryst. 2015, A71, 3–8. [Google Scholar]
- (45).Rigaku, V1.171.42.60a, 2022
- (46).Rigaku, V1.171.43.121a, 2024
- (47).Rigaku, V1.171.41.118a, 2021
- (48).Ishida H; Tobita S; Hasegawa Y; Katoh R; Nozaki K Recent advances in instrumentation for absolute emission quantum yield measurements. Coord. Chem. Rev 2010, 254, 2449–2458. DOI: 10.1016/j.ccr.2010.04.006. [DOI] [Google Scholar]
- (49).Suzuki K; Kobayashi A; Kaneko S; Takehira K; Yoshihara T; Ishida H; Shiina Y; Oishi S; Tobita S Reevaluation of absolute luminescence quantum yields of standard solutions using a spectrometer with an integrating sphere and a back-thinned CCD detector. Phys. Chem. Chem. Phys 2009, 11, 9850–9860. DOI: 10.1039/B912178A. [DOI] [PubMed] [Google Scholar]
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