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      De Novo Generation of Singlet Oxygen and Ammine Ligands by Photoactivation of a Platinum Anticancer Complex**

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          Abstract

          The potential for spacial selectivity, as offered by photoactivation, together with novel excited-state chemistry and accompanying mechanisms of action make exploration of photoactivated metal chemotherapeutic complexes attractive for cancer therapy.1We have been studying PtIV-diazidodihydroxido anticancer complexes, [Pt(N3)2(OH)2(Am1)(Am2)] (Am1/Am2=am(m)ines),2 which, in the absence of light, exhibit minimal cytotoxicity towards cancer cells and do not react with glutathione (GSH), 5′-guanosine monophosphate (5′-GMP), or DNA in either cell-free media or aqueous solutions. By contrast, upon irradiation with UVA or visible (blue/green) light, these complexes display potent cytotoxicity towards a range of cancer cell lines. The reported photodecomposition products include azide anions (N3 −), azidyl radicals (N3 .), nitrogen gas (N2), and oxygen gas (O2).3 A particularly potent photocytotoxic anticancer complex is trans,trans,trans-[Pt(N3)2(OH)2(MA)(Py)] (1, MA=methylamine, Py=pyridine).4 Herein we report the unprecedented oxidation of 5′-GMP by 1 upon irradiation with UVA and the identification of some unexpected reaction pathways involving singlet oxygen (1O2) and nitrene (Pt-N) intermediates. The source of the 1O2 was also investigated. The photoreaction of 1 with 5′-GMP upon irradiation with blue light with a wavelength of 450 nm for 1 h gave (SP-4-2)-[Pt(N3)(MA)(Py)(5′-GMP)]+ (1 a +) as the major product and trans-[Pt(MA)(Py)(5′-GMP)2]2+ (1 b 2+) as the minor product (Figure 1 A). A similar result has been reported for 1 under slightly different conditions, and for related compounds.2a, 4, 4 However, when the reaction mixture was irradiated at 420 nm for 30 min, two new photoproducts, 1 c and 1 e, were observed by HPLC (Figure 1 B). When the sample was irradiated with UVA (365 nm) for 15 min, one more species, 1 d, was found (Figure 1 C). The isotopic distributions observed in the ESI-MS analysis revealed that the singly charged cations of 1 c (m/z=718.1), 1 d (m/z=684.1), and 1 e (m/z=700.1) all contain a Pt atom. A control experiment with 5′-GMP in the absence of 1 and UVA irradiation for 15 min showed no reaction (Figure 1 D), thus suggesting that 5′-GMP is stable under these conditions. The photoreaction of 1 and 5′-GMP under an atmosphere of argon gave similar results, thereby excluding the possibility that dissolved oxygen is the oxidant. Hence, 1 c, 1 d, and 1 e are all produced by the photoreaction of 1. Figure 1 Chromatograms for the photoreactions of 1 (0.67 mm) with 5′-GMP (1.0 mm) in aqueous solution upon irradiation with A) 450 nm light, 50 mW cm−2, 60 min; B) 420 nm, 4.3 mW cm−2, 30 min; C) UVA (365 nm), 3.5 mW cm−2, 15 min; D) 5′-GMP (1.0 mm) only, UVA, 15 min. High-resolution MS of 1 a, 1 c, 1 d, and 1 e, as well as their tandem MS (CID), were performed to examine further the structure of each species (see Figures S1 and S2 in the Supporting Information). They are all assigned as PtII complexes, and their structures are listed in Table 1, while fragment ions are listed in Tables S1–S4 in the Supporting Information, together with their assignments. Table 1 Positive ions for complexes 1 a, 1 c, 1 d, and 1 e observed by HRMS and the corresponding assignments. Found m/z 710.1205 718.1337 684.1228 700.1235 Proposed chemical structure ([1 a]+) ([1 c−H]+) ([1 d−H]+) ([1 e−H]+) Theoretical m/z 710.1164 718.1314 684.1260 700.1209 Error [ppm] 5.8 3.2 4.7 3.7 Curiously, species 1 c, 1 d, and 1 e all have an NH3 ligand, which was not present in the reactants. A reasonable source of the NH3 is the {Pt-N3} fragment, which can lose N2 upon irradiation with light to form a {Pt-N} nitrene intermediate.6 This postulation was verified by using 1*, azide trans,trans,trans-[Pt(N3 *)2(OH)2(MA)(Py)], where N3 *=[15N=14N=14N], and hence each bound N atom from the azide is now 50 % 15N. The photoreaction of 1* with 5′-GMP, carried out under identical conditions, gave an identical chromatogram as that shown in Figure 1 C. The ESI-MS spectra for 1 a*, 1 c*, 1 d*, and 1 e*, which have the same retention times as 1 a, 1 c, 1 d, and 1 e, are shown in Figure S5 in the Supporting Information. The molecular weight of compound 1 a* was 1 Da larger than 1 a, thus suggesting that it has an intact N3 * − ligand. The isotope distributions of 1 c*, 1 d*, and 1 e* indicate that they are all 50 %/50 % mixtures of [M] and [M+1], so they are all considered as {Pt-NH3 *} fragments derived from {Pt-N3*} (NH3 *=50 % 15NH3/50 % 14NH3). This result suggests that N2 gas is released directly from {Pt-N3}, thereby generating a {Pt-N} intermediate. The release of N2 on photolysis of 1 was verified by 14N NMR spectroscopy (see Figure S6 in the Supporting Information); signals for free azide (N3 −) were also detected (see the Supporting Information for details). N2 may be released directly from {Pt-N3} and also may be formed from the recombination of the azidyl radicals (N3 .) generated in this photoreaction.7 The release of N3 . was confirmed by EPR spectroscopy by using 5,5-dimethylpyrroline-N-oxide (DMPO) as the spin trap. Signals for the DMPO-14N3 spin adduct were detected (see Figure S7 in the Supporting Information), but hydroxyl radicals OH. were not trapped. It is evident that 5′-GMP is not oxidized by N3 ., as its presence did not affect the trapping of N3 . radicals (see the Supporting Information for details). Species 1 e contains an 8-hydroxyguanine (8-OH-G) fragment, equivalent to 8-oxoguanine (8-oxo-G), which is one of the most common products of DNA oxidation.8 The possibility that the oxidation of guanine by photoactivated 1 involved singlet oxygen or nitrene intermediates was investigated. Product 1 c has a similar structure as 1 e, but the 8-OH-G is replaced by RedSp (N-formylamidoiminohydantoin),8a hydrolyzed 8-OH-G (shown in Scheme S1 in the Supporting Information). During the photoreaction of 1 and 5′-GMP with irradiation at 450 nm the yellow color of the solution became darker, and gas bubbles formed (see Figure S8 in the Supporting Information). Similar results were obtained when the reaction was triggered with UVA. The evolution of the gases O2 and N2 was verified by GC-MS performed in 18O-labeled water under an argon atmosphere, with the aim also of examining the source of the O atoms in the generated O2. After the photolysis of 1, the gas phase was analyzed by GC-MS (see Figure S9 and the Supporting Information for details), and 16O2 (m/z=32) and N2 (m/z=28) were both found. No 18O-substituted O2 was detected. This result verified the release of N2 and O2 and, moreover, provided evidence that the two oxygen atoms in the generated O2 are both from 1 rather than from the solvent. The nature of the released oxygen was investigated using a fluorescence probe for singlet oxygen: SOSG. SOSG is a highly selective sensor for 1O2 without any appreciable response to hydroxyl radicals or superoxide.9 In the absence of 1O2, SOSG exhibits low fluorescence, but in the presence of 1O2, strong green fluorescence can be observed with λ ex=504 nm and λ em=525 nm. Solutions containing 1 and SOSG were stable in the dark or even upon irradiation at λ≥504 nm. However, when exposed to weak irradiation at 365 nm (21 μW cm−2), the intensity of the fluorescence at 525 nm increased rapidly, thus indicating that 1O2 was generated (Figure 2). The dose-dependent efficiency of generating 1O2 upon irradiation was higher the shorter the wavelength (UVA>420 nm>450 nm, see Figure S10 in the Supporting Information). Control experiments carried out in the dark or in the absence of 1 showed no change in the fluorescence intensity (see Figure S10 in the Supporting Information). A sample saturated with argon was irradiated at 365 nm and gave stronger fluorescence (Figure 2). This result revealed that the 1O2 was not generated from the dissolved O2 through energy transfer from a photosensitizer. N2 had a similar effect as argon. Neither argon nor N2 itself could trigger the fluorescence of SOSG. The release of singlet oxygen from a PtIV-diazidodihydroxido complex upon irradiation with light in the absence of any exogenous source of oxygen gas appears to be unprecedented. Figure 2 Time-dependent fluorescence (λ ex/λ em=504/525 nm) from 1 (50 μm) and SOSG (1 μm) in H2O (3 % MeOH) upon weak irradiation at 365 nm (21 μW cm−2) (293 K). ▪: no additive; □: 50 % D2O; ▴: saturated with argon; •: 0.1 mm l-ascorbic acid (AscA). All the data points were the average of 2–4 independent experiments. The lifetime of 1O2 in D2O is known to be much longer than that in H2O.10 Indeed, the fluorescence intensity arising from the reaction of 1 with SOSG in 50 % D2O with λ irr=365 nm was three- to fourfold higher than that of the reaction carried out in H2O alone (Figure 2). The reaction was repeated in the presence of 100 μm l-ascorbic acid (AscA) as a 1O2 scavenger. Complex 1 does not react with AscA in the absence of light, even though AscA is a strong reductant. However, upon irradiation at 365 nm, the fluorescence was totally quenched (Figure 2). These results again confirmed the generation of 1O2. Guanine and the other nucleobases may be oxidatively damaged by reactive oxygen species (ROS), radicals, and ionizing/UVA radiation.11 The oxidation of guanine usually leads to DNA damage so as to cause lethality, aging, and mutagenicity.8 Although it has been reported that several PtIV-tetrachlorido complexes can directly oxidize guanine,12 we report here for the first time that the photodecomposition of a PtIV-diazidodihydroxido complex can oxidize guanine. Complexes containing PtII and oxidized guanine as 8-OH-G and RedSp were detected (Table 1). Two pathways can be proposed for the oxidation of guanine. The first involves a nitrene intermediate (Scheme 1, Mechanism 1). This can arise from loss of N2 from the {Pt-N3} fragment upon irradiation with UVA.6 Two electrons are transferred from guanine to the nitrene, and the guanine itself is oxidized to give 8-OH-G on addition of H2O. The nitrene is reduced and finally forms the ammine adduct {Pt-NH3}. Another possible oxidant is singlet oxygen. The 1O2 generated by photolysis of 1 can oxidize guanine to 8-OH-G by a direct [4+2] cycloaddition (Scheme 1, Mechanism 2).8a Scheme 1 Two possible mechanisms for the oxidation of 5′-GMP. Charges are omitted for clarity. Singlet oxygen (1O2) is a highly reactive and toxic species in biological systems. It is considered the principal antiproliferative species in photodynamic therapy (PDT), in which it reacts with many biomolecules, including nucleic acids, proteins, and lipids, thereby causing cancer cell death.8, 13 A common method to generate 1O2 is photosensitization, which produces 1O2 by energy transfer from a photoexcited sensitizer to ground-state triplet oxygen (3O2). This strategy is the basis of current PDT, but requires the presence of oxygen at the target site. However, tumor cells are often hypoxic. In contrast, the generation of 1O2 from trans,trans,trans-[Pt(N3)2(OH)2(MA)(Py)] upon irradiation with UVA/blue light does not require any exogenous source of oxygen gas (Figure 2). This feature may be beneficial for the potential clinical application of 1 and killing of hypoxic cancer cells. Moreover, the wavelength can be tuned to control its photocytotoxicity, as shorter wavelengths generate more 1O2. Since neither of the oxygen atoms in the released 1O2 originate from water, the most plausible source is the OH groups of 1. Furthermore, solvent substitution at PtIV is not likely to occur before its reduction to PtII. A possible photolysis mechanism is given in Scheme 2. Upon irradiation with short-wavelength light, such as UVA, photodecomposition of 1 in the presence of 5′-GMP may occur through two pathways. In the first, two azidyl radicals (N3 .) are lost and PtIV is reduced to PtII. The OH groups are protonated and thus are substituted by 5′-GMP to give product 1 b. The second pathway is more complicated, but perhaps more likely. The integration of the HPLC peaks in Figure 1 C suggested that about 92 % of the Pt species were produced through this pathway. Complex 1 loses one azide ligand (N3 −) and the OH ligands donate one electron each to reduce the PtIV to PtII; they then rapidly recombine to generate oxygen gas, as singlet oxygen, through H2O2 formation.14 Then the binding of 5′-GMP to Pt produces 1 a, which can be further transformed to 1 e by loss of N2 gas from the N3 ligand, as in Scheme 1. Alternately, if N2 is expelled from the N3 ligand before 5′-GMP binds, 1 d is produced, which can also be transformed to 1 e by reacting with 1O2 (Scheme 1). Scheme 2 Possible mechanisms for the photoreaction of 1 with 5′-GMP upon irradiation with UVA. Species in square brackets are unstable intermediates. Charges are omitted for clarity. Species percentages are average HPLC integrations for four experiments with UVA irradiation (Figure 1 C). There are a number of reports of the chemical reduction of PtIV to PtII, and it is widely accepted that a concerted two-electron transfer from, for example, ascorbate, GSH, or guanine, to PtIV is involved.12, 15 However, the photoreduction of 1 may not follow the above pathway. PtIV is more likely to gain one electron from each of the two N3 or two OH ligands and give rise to N3 . or OH. radicals, respectively. We were not able to trap OH. radicals, perhaps because their lifetime is too short. The in situ formation of an NH3 ligand can give rise to potential hydrogen-bonding interactions with DNA. DNA adducts of the type 1 d, for example, may strongly inhibit RNA polymerase II and nucleotide excision repair.16 Nitrenes are highly reactive intermediates and are reported to be responsible for a wide range of DNA lesions.17 N3 . is a relatively mild and selective oxidant that can oxidize amino acids such as tryptophan.3b N3 − is a mitochondrial inhibitor, and a myeloperoxidase and catalase inhibitor. These species, together with 1O2, could all contribute to the potent photo-antiproliferative effect of 1 on cancer cells. In summary, we observed the unexpected oxidation of guanine during the photoreaction of complex 1 (trans,trans,trans-[Pt(N3)2(OH)2(MA)(Py)]) with 5′-GMP. The photodecomposition of 1 involves Pt-nitrene intermediates and formation of singlet oxygen, free azide, azidyl radicals, and nitrogen gas. The oxidation of guanine is likely to arise from reactions of singlet oxygen and nitrene intermediates. The generation of singlet oxygen in the absence of oxygen gas and the oxidative damage to guanine may contribute to the potent photocytotoxic effects of this complex.

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          Most cited references56

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          Singlet oxygen: there is indeed something new under the sun.

          Singlet oxygen, O(2)(a(1)Delta(g)), the lowest excited electronic state of molecular oxygen, has been known to the scientific community for approximately 80 years. It has a characteristic chemistry that sets it apart from the triplet ground state of molecular oxygen, O(2)(X(3)Sigma), and is important in fields that range from atmospheric chemistry and materials science to biology and medicine. For such a "mature citizen", singlet oxygen nevertheless remains at the cutting-edge of modern science. In this critical review, recent work on singlet oxygen is summarized, focusing primarily on systems that involve light. It is clear that there is indeed still something new under the sun (243 references).
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            Optimization of an AMBER Force Field for the Artificial Nucleic Acid, LNA, and Benchmarking with NMR of L(CAAU)

            Locked Nucleic Acids (LNAs) are RNA analogues with an O2′-C4′ methylene bridge which locks the sugar into a C3′-endo conformation. This enhances hybridization to DNA and RNA, making LNAs useful in microarrays and potential therapeutics. Here, the LNA, L(CAAU), provides a simplified benchmark for testing the ability of molecular dynamics (MD) to approximate nucleic acid properties. LNA χ torsions and partial charges were parametrized to create AMBER parm99_LNA. The revisions were tested by comparing MD predictions with AMBER parm99 and parm99_LNA against a 200 ms NOESY NMR spectrum of L(CAAU). NMR indicates an A-Form equilibrium ensemble. In 3000 ns simulations starting with an A-form structure, parm99_LNA and parm99 provide 66% and 35% agreement, respectively, with NMR NOE volumes and 3 J-couplings. In simulations of L(CAAU) starting with all χ torsions in a syn conformation, only parm99_LNA is able to repair the structure. This implies methods for parametrizing force fields for nucleic acid mimics can reasonably approximate key interactions and that parm99_LNA will improve reliability of MD studies for systems with LNA. A method for approximating χ population distribution on the basis of base to sugar NOEs is also introduced.
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              Oxidation of DNA: damage to nucleobases.

              All organisms store the information necessary to maintain life in their DNA. Any process that damages DNA, causing a loss or corruption of that information, jeopardizes the viability of the organism. One-electron oxidation is such a process. In this Account, we address three of the central features of one-electron oxidation of DNA: (i) the migration of the radical cation away from the site of its formation; (ii) the electronic and structural factors that determine the nucleobases at which irreversible reactions most readily occur; (iii) the mechanism of reaction for nucleobase radical cations. The loss of an electron (ionization) from DNA generates an electron "hole" (a radical cation), located most often on its nucleobases, that migrates reversibly through duplex DNA by hopping until it is trapped in an irreversible chemical reaction. The particular sequence of nucleobases in a DNA oligomer determines both the efficiency of hopping and the specific location and nature of the damaging chemical reaction. In aqueous solution, DNA is a polyanion because of the negative charge carried by its phosphate groups. Counterions to the phosphate groups (typically Na(+)) play an important role in facilitating both hopping and the eventual reaction of the radical cation with H(2)O. Irreversible reaction of a radical cation with H(2)O in duplex DNA occurs preferentially at the most reactive site. In normal DNA, comprising the four common DNA nucleobases G, C, A, and T, reaction occurs most commonly at a guanine, resulting in its conversion primarily to 8-oxo-7,8-dihydroguanine (8-OxoG). Both electronic and steric effects control the outcome of this process. If the DNA oligomer does not contain a suitable guanine, then reaction of the radical cation occurs at the thymine of a TT step, primarily by a tandem process. The oxidative damage of DNA is a complex process, influenced by charge transport and reactions that are controlled by a combination of enthalpic, entropic, steric, and compositional factors. These processes occur over a broad distribution of energies, times, and spatial scales. The emergence of a complete picture of DNA oxidation will require additional exploration of the structural, kinetic, and dynamic properties of DNA, but this Account offers insight into key elements of this challenge.
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                Author and article information

                Journal
                Angew Chem Int Ed Engl
                Angew. Chem. Int. Ed. Engl
                anie
                Angewandte Chemie (International Ed. in English)
                WILEY-VCH Verlag (Weinheim )
                1433-7851
                1521-3773
                16 December 2013
                25 October 2013
                : 52
                : 51
                : 13633-13637
                Affiliations
                Department of Chemistry, University of Warwick, CV4 7AL (United Kingdom)
                Beijing National Laboratory for Molecular Sciences, CAS Key Laboratory of Analytical Chemistry for Living Biosystems, Institute of Chemistry, Chinese Academy of Sciences, Beijing 100190 (P.R. China)
                Author notes
                [**]

                Y.Z. and H.L. thank the University of Warwick for PhD scholarships (WPRS and ORSAS awards). Y.Z., P.J.S., and N.J.F. thank he EPSRC (EP/G006792/1) and the ERC (award no. 247450). We thank Science City/AWM/ERDF for funding the mass spectrometers; Dr. Lijiang Song, Prof. Alison Rodger, Dr. Ivan Prokes, and Dr. Mark E. Newton for assistance with instruments; and members of EC COST Actions D39 and CM1105 for stimulating discussions. Y.Z. and .Y.W. thank the NSFC (Grant Nos.: 21020102039) for support.

                Article
                10.1002/anie.201307505
                4230391
                24167018
                a28b37c8-08e4-419b-8d5b-5197e1e35907
                © 2013 The Authors. Published by Wiley-VCH Verlag GmbH & Co. KGaA. This is an open access article under the terms of the Creative Commons Attribution License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited.
                History
                : 26 August 2013
                Categories
                Communications

                Chemistry
                antitumor agents,bioinorganic chemistry,guanine oxidation,photoactivation,singlet oxygen
                Chemistry
                antitumor agents, bioinorganic chemistry, guanine oxidation, photoactivation, singlet oxygen

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