Sung Wook Han

Classification of CD and absorption spectra in the Soret band of H2TMPyP bound to various synthetic polynucleotides

The binding mode of porphyrins, namely meso-tetrakis(N-methyl pyridinium-4-yl)porphyrin (H(2)TMPyP), was classified in this work by absorption and circular dichroism(CD) spectroscopy. The three binding modes of intercalation, minor groove binding and external stacking exhibit their own characteristic absorption and CD spectra. Intercalation occurs for this porphyrin when bound to GC-rich polynucleotides at a low mixing ratio, as expected. This binding mode produces hypochromism and a red shift in the absorption band and a negative CD band in the Soret absorption region. When it is complexed with AT-rich polynucleotides at a low mixing ratio, hypochromism and a red shift in the absorption band and a positive CD peak is apparent, and this species can easily be assigned to the minor groove-binding mode. For both AT- and GC-rich polynucleotides at a high binding ratio, an excitonic CD was apparent. The sign of excitonic CD depends on the order of the DNA bases; the CD spectra of H(2)TMPyP complexed with non-alternating homopolymer (disregarding the nature of base pairs, i.e. AT or GC) are characterized by a positive band at short wavelengths followed by a negative band at long wavelengths. In contrast, those complexed with alternating polynucleotide were opposite to those of non-alternating homopolymers.

Binding of meso-Tetrakis(N-methylpyridinium-4-yl)porphyrin to AT Oligomers: Effect of Chain Length and the Location of the Porphyrin Stacking

Circular dichroism (CD) spectra of meso-tetrakis(N-methylpyridinium-4-yl)porphyrin (TMPyP) that are associated with various duplex and triplex AT oligomers were investigated in this study. A strong positive CD was apparent for both the TMPyP complexed with duplex d[(A-T)(12)](2), d(A)(12).d(T)(12) and triplex d(A)(12).d[(T)(12)](2) at a low mixing ratio. As the mixing ratio increased, bisignate excitonic CD was produced for TMPyP complexed with duplexes, whereas the positive CD signal remained the same for the TMPyP-d(A)(12).d[(T)(12)](2) complex. This difference in the CD spectrum in the presence of duplex and triplex oligomers indicates that the moderate stacking of TMPyP occurs at the major groove of the duplex and the monomeric binding occurs in (or near) the minor groove. When TMPyP forms a complex with duplex d[(A-T)(6)](2) only excitonic CD was observed, even at a very low mixing ratio. Therefore, at least seven or more basepairs are required for TMPyP to exhibit a monomeric CD spectrum. After close analysis of the CD spectrum, the TMPyP-poly[d(A-T)(2)] complex could be explained by a combination of the CD spectrum of the monomeric, moderately stacked, and extensively stacked TMPyP.

Effect of the Position and Number of Positive Charges on the Intercalation and Stacking of Porphyrin to Poly[d(G-C)2], Poly[d(A-T)2], and Native DNA

The effect of the number and position of the positive charges on porphyrin with respect to the mode of binding to poly[d(G-C)2] and poly[d(A-T)2] were investigated by absorption and polarized spectroscopy, including circular and linear dichroism (CD and LD). Meso-tetrakis(N-methylpyridinium-4-yl)porphyrin (TMPyP), which possesses four positive charges on the periphery pyridinium rings, produces a negative CD and wavelength-independent reduced LD (LDr) spectra in the Soret absorption region when it associates with poly[d(G-C)2]. These spectral characteristics have been considered as diagnostic for intercalation. In contrast, both trans- and cis-bis(N-methylpyridinium-4-yl)diphenylporphyrin (trans- and cis-BMPyP), where the number of positive charges was reduced to two, multisignate CD and strong wavelength-dependence of the LDr spectra were observed, indicating that these porphyrins do not intercalate. Therefore, four positive charges are required for TMPyP intercalation. When associated with poly[d(A-T)2], trans-BMPyP exhibited a positive CD signal at a low [porphyrin]/[nucleobase] ratio with the appearance of a bisignate CD upon increase of the mixing ratio, suggestive of binding at the groove of the double helix at low mixing ratios, and stacking at increasing mixing ratios. Conversely, no monomeric binding was evident in the bis-BMPyP bisignate CD spectrum; hence, only the stacking mode was found for cis-BMPyP, even at the lowest [porphyrin]/[nucleobase] ratio, suggesting the importance of the position of the positive charges in determining monomeric groove binding or stacking. The binding geometries of trans- and cis-BMPyP were similar when associated with poly[d(A-T)2], as determined from the similar LDr spectrum. When associated with DNA, TMPyP exhibited similar spectral properties with that of the TMPyP-poly[d(G-C)2] complex, indicating intercalation of TMPyP between the DNA base pairs. Conversely, CD and LDr characteristics of both trans- and cis-BMPyP-DNA complexes resembled those that complexed with poly[d(A-T)2] at a high [porphyrin]/[DNA] ratio, suggesting that both porphyrins were stacked along the DNA stem.

Retained binding mode of various DNA-binding molecules under molecular crowding condition

Meso-tetrakis(N-methyl pyridinium-4-yl)porphyrin (TMPyP) intercalates between the base-pairs of DNA at a low [TMPyP]/[DNA base] ratio in aqueous solutions and molecular crowding conditions, which is induced by the addition of Poly(ethylene glycol) (PEG). Studied DNA-binding drugs, including TMPyP, 9-aminoacridine, ethidium bromide, and DAPI (4′,6-diamidino-2-phenylindole) showed similar binding properties in the presence or absence of PEG molecules which is examined by circular and linear dichroism. According to the LDr (reduced linear dichroism) results of the binding drugs examined in this work, PEG molecules induced no significant change compared to their binding properties in aqueous buffering systems. These results suggest that the transition moments are not expected to be perturbed significantly by PEG molecules. In this study, the experimental conditions of PEG 8000 were maintained at 35% (v/v) of total reaction volume, which is equal to the optimal molar concentration (0.0536 M as final concentration for PEG 8000) to maintain suitable cell-like conditions. Therefore, there was no need to focus on the conformational changes of the DNA helical structure, such as forming irregular aggregate structures, induced by large quantities of molecular crowding media itself at this stage.

Enantioselective light switch effect of Δ- and Λ-[Ru(phenanthroline)2 dipyrido[3,2-a:2′, 3′-c]phenazine]2+ bound to G-quadruplex DNA

The interaction of Δ- and Λ-[Ru(phen)2DPPZ]2+ (DPPZ = dipyrido[3,2-a:2′, 3′-c]phenazine, phen = phenanthroline) with a G-quadruplex formed from 5′-G2T2G2TGTG2T2G2–3′(15-mer) was investigated. The well-known enhancement of luminescence intensity (the ‘light-switch’ effect) was observed for the [Ru(phen)2DPPZ]2+ complexes upon formation of an adduct with the G-quadruplex. The emission intensity of the G-quadruplex-bound Λ-isomer was 3-fold larger than that of the Δ-isomer when bound to the G-quadruplex, which is opposite of the result observed in the case of double stranded DNA (dsDNA); the light switch effect is larger for the dsDNA-bound Δ-isomer. In the job plot of the G-quadruplex with Δ- and Λ-[Ru(phen)2DPPZ]2+, a major inflection point for the two isomers was observed at x ≈ .65, which suggests a binding stoichiometry of 2:1 for both enantiomers. When the G base at the 8th position was replaced with 6-methyl isoxanthopterin (6MI), a fluorescent guanine analog, the excited energy of 6-MI transferred to bound Δ- or Λ-[Ru(phen)2DPPZ]2+, which suggests that at least a part of both Ru(II) enantiomers is close to or in contact with the diagonal loop of the G-quadruplex. A luminescence quenching experiment using [Fe(CN)6]4- for the G-quadruplex-bound Ru(II) complex revealed downward bending curves for both enantiomers in the Stern–Volmer plot, which suggests the presence of Ru(II) complexes that are both accessible and inaccessible to the quencher and may be related to the 2:1 binding stoichiometry.