9 research outputs found
Neighboring base sequence effect on DNA damage
Guanine is the most strongly oxidized base in DNA; generation of a guanine radical cation as an intermediate in an oxidation reaction leads to migration through a resulting cationic hole in the DNA π-stack until it is trapped by irreversible reaction with water or other free radicals. In the case of normal sequences, the primary position of Guanine oxidations by one-electron oxidants such as carbonate radical anions, BPT(7,8,9,10-tetrahydroxytetrahydrobenzo[a]pyrene), and riboflavin are 5′-G in GG doublets and the central G in a GGG triplet. According to results, the properties of guanine oxidation on abasic site containing sequences are independent from the position of AP(apurinic/apyrimidinic) site in the presence of carbonate radical anions under a short irradiation time, although this radical is exposed to solvent by the existence of an abasic site. The lack of abasic site effect on guanine oxidative damage by the carbonate radical may be due to a sequence-independent property of the initial electron transfer rate in the hole injection step, or may relate to an electron transfer mechanism with large reorganization energy dependency. Consequently, the carbonate radical anions may easily migrate to another single G in the charge re-distribution step. Meanwhile, there is a strong dependency on the presence of an AP(apurinic/apyrimidinic) site in the cleavage patterns of guanine oxidations by physically large oxidizing agents, such as BPT(7,8,9,10-tetrahydroxytetrahydrobenzo[a]pyrene) and riboflavin. These radicals show strong AP(apurinic/apyrimidinic) site dependency and clear G-site selectivity. Communicated by Ramaswamy H. Sarma</p
Interaction of G‑Quadruplex with RecA Protein Studied in Bulk Phase and at the Single-Molecule Level
As in the human genome there are
numerous repeat DNA sequences
to adopt into non-B DNA structures such as hairpin, triplex, Z-DNA,
G-quadruplex, and so on, an understanding of the interaction between
DNA repair proteins and a non-B DNA forming sequence is very important.
In this regard, the interaction between RecA protein and human telomeric
5′-TAGGG-(TTAGGG)<sub>3</sub>-TT-3′ sequence and the
G-quadruplex formed from this sequence has been investigated in bulk
phase and at the single-molecule level. The RecA@ssDNA filament, which
is formed by the interaction between RecA protein and a G-rich sequence,
was dissociated by the addition of K<sup>+</sup> ions, and the dissociated
G-rich sequence was quickly folded to a G-quadruplex structure, indicating
that the G-quadruplex structure is more favorable than the RecA@ssDNA
filament in the presence of K<sup>+</sup> ions. In addition, we demonstrate
that the conformation of the G-quadruplex, which is heterogeneous
in the absence of RecA, converged to the specific G-quadruplex with
one double-chain-reversal loop upon association of RecA protein
Chiral Selective Stacking of a Cationic Porphyrin along Z‑Form Poly[d(A-T)<sub>2</sub>]
In this study, the binding mode of porphyrin-free single-stranded
poly[d(AT)] and <i>trans</i>-BMPyP was observed in the Z-form <i>trans</i>-BMPyP–poly[d(A-T)<sub>2</sub>] complex induced
by extensive stacking depending on the temperature and concentration
through circular dichroism (CD). The Z-form <i>trans</i>-BMPyP–poly[d(A-T)<sub>2</sub>] complex (<i>R</i> = 0.30) retained the Z-form DNA structure
at a low temperature (20 °C) by the <i>trans</i>-BMPyP
molecules. When the temperature was increased to 60 °C, the DNA
was almost unfolded as a single-stranded poly[d(AT)], but the extensive
stacking binding mode of <i>trans</i>-BMPyP was maintained
and the shape of the porphyrin Soret band was symmetrically changed
in comparison with the shape of the Z-form DNA. However, when the
temperature was raised to 80 °C, the extensive stacking binding
mode of <i>trans</i>-BMPyP was also unfolded almost completely.
The binding mode of the <i>trans</i>-BMPyP-single-stranded
poly[d(AT)] complex was very similar to the already known binding
mode of porphyrins and a double-stranded DNA. The binding mode was
dependent on the concentration ratio ([porphyrin]/[DNA]): a monomeric
binding mode at a concentration ratio of 0.04, a moderate groove binding
mode at a concentration ratio between 0.08 and 0.16, and extensive
stacking at a concentration ratio between 0.20 and 0.30. The same
result was obtained when the temperature of the Z-form DNA (<i>R</i> = 0.30) was increased to 60 °C. However, those binding
modes were not found in <i>cis</i>-BMPyP, which was because,
in the extensive stacking of <i>trans</i>-BMPyP along the
DNA skeleton, the distance between the two positive methylpyridine
ions at the trans site and thymine, one of the DNA bases, is decreased,
creating a much more hydrophobic environment. In addition, the poly
AT sequences found from the CD spectra for the binding of <i>trans</i>-BMPyP–poly[d(A-T)<sub>2</sub>] and <i>trans</i>-BMPyP–poly[d(AT)] (<i>R</i> = 0.30)
showed that both of them underwent effective extensive stacking and
that the chirality of extensive stacking was dependent on the form
of DNA
Effect of periphery cationic substituents of porphyrin on the B-Z transition of poly[d(A-T)<sub>2</sub>], poly[d(G-C)<sub>2</sub>] and their binding modes
The binding mode of cationic porphyrin (trans-BMPyP) with poly[d(G-C)2] and poly[d(A-T)2] was examined according to the site of the periphery cationic methyl pyridine ion of the cationic porphyrin (o-, m-, p-) as well as the possibility of a B-Z transition depending on the binding modes by measuring the absorption spectrum and circular dichroism (CD). The negative band found in the soret region showed the intercalation mode of m- and p-trans-BMPyP-poly[d(G-C)2] to the DNA base pairs, but no B-Z transition was induced. On the other hand, the distinctive bisignate band found in the soret region of the CD spectrum for m- and p-trans-BMPyP-poly[d(A-T)2] suggests that m- and p-trans-BMPyP have an effective extensive stacking-based binding mode along with the skeleton of poly[d(A-T)2], wherein the B-Z transition was induced through extensive stacking. The difference in binding mode was attributed to the difference in the molecular structure depending on the site of the periphery cationic methyl pyridine ion in the cationic porphyrin. In other words, o-trans-BMPyP is nonplanar because of the steric hindrance of the cationic methyl pyridine ion at the o-site. In contrast, m- and p-trans-BMPyP are planar, but not all porphyrins with a planar structure undergo the B-Z transition. In conclusion, a B-Z transition is induced if the structure of a porphyrin is planar and the binding mode allows the porphyrins to be stacked effectively along the DNA skeleton, not in a binding mode where the porphyrin is intercalated to the DNA. Communicated by Ramaswamy H. Sarma</p
Binding mode of a cationic porphyrin to parallel and antiparallel thrombin binding aptamer G-quadruplex
The spectral properties of meso-tetrakis (N-methylpyridinium-4-yl)porphyrin (TMPyP) in the presence of parallel and antiparallel G-quadruplexes formed from a thrombin-binding aptamer G-quadruplex (5′-G3T2G3TGTG3T2G3) were investigated in this study. Red shift and hypochromism in the Soret absorption band of TMPyP were observed after binding to both parallel and antiparallel G-quadruplexes. The extent of changes in the absorption spectra were similar for both conformers. No circular dichroism spectrum was induced in the Soret region for both parallel and antiparallel G-quadruplexes. This is suggest that there is no or very weak interaction between electric transitions of nucleobases and porphyrin molecule. The accessibility of the neutral quencher I2 to the G-quadruplex-bound TMPyP was similar for both parallel and antiparallel G-quadruplexes. All these observations suggest that TMPyP was bound at the outside of the quadruplexes, and conceivably interacted with the phosphate group via a weak electrostatic interaction. Communicated by Ramaswamy H. Sarma</p
Photoinduced Reduction of Manganese(III) <i>meso</i>-Tetrakis(1-methylpyridinium-4-yl)porphyrin at AT and GC Base Pairs
The photoreduction of water-soluble
cationic manganese(III) <i>meso</i>-tetrakis(1-methylpyridium-4-yl)porphyrin
(Mn<sup>III</sup>(TMPyP)<sup>4+</sup>) bound to a synthetic polynucleotide,
either
poly[d(A-T)<sub>2</sub>] or poly[d(G-C)<sub>2</sub>], was examined
by conventional absorption and circular dichroism (CD) spectroscopy,
transient absorption, and transient Raman spectroscopy. Upon binding,
Mn<sup>III</sup>(TMPyP)<sup>4+</sup> produced a positive CD signal
for both polynucleotides, suggesting external binding. In the poly[d(A-T)<sub>2</sub>]–Mn<sup>III</sup>(TMPyP)<sup>4+</sup> adduct case,
an interaction between the bound porphyrin was suggested. The transient
absorption spectral features of Mn<sup>III</sup>(TMPyP)<sup>4+</sup> in the presence of poly[d(A-T)<sub>2</sub>] and poly[d(G-C)<sub>2</sub>] were similar to those of the photoreduced products, Mn<sup>II</sup>(TMPyP)<sup>4+</sup>, whereas Mn<sup>III</sup>(TMPyP)<sup>4+</sup> in the absence of polynucleotides retained its oxidation
state. This indicated that both poly[d(A-T)<sub>2</sub>] and poly[d(G-C)<sub>2</sub>] act as electron donors, resulting in photo-oxidized G and
A bases. The transient Raman bands (ν<sub>2</sub> and ν<sub>4</sub>) that were assigned to porphyrin macrocycles exhibited a
large downshift of ∼25 cm<sup>–1</sup>, indicating the
photoreduction of Mn<sup>III</sup> to Mn<sup>II</sup> porphyrins when
bound to both polynucleotides. The transient Raman bands for pyridine
were enhanced significantly, suggesting that the rotation of peripheral
groups for binding with polynucleotides is the major change in the
geometry expected in the photoreduction process. These photoinduced
changes do not appear to be affected by the binding mode of porphyrin
Solvent-to-Polymer Chirality Transfer in Intramolecular Stack Structure
Solvent-to-polymer chirality transfer was examined using
conjugated polymer with intramolecular stack structure (IaSS). When
achiral poly(diphenylacetylene)s (PDPAs) dissolved in limonene, the
solvent chirality was successfully transferred to the side phenyl
stack structure, leading to intramolecular axial chirality. The phenyl–phenyl
IaSS was under thermodynamic control to readily undergo asymmetric
changes in chiral limonene, leading to optical activity in the isotropic
structure between the main chain and resonant side phenyl rings. The
axial chirality was significantly affected by the chain length and
substitution position of the side alkyl groups. The longer alkyl chains
and bulkier alkyl group prevented direct intermolecular interactions
between the side phenyl rings and the chiral limonene molecules. PDPA
with sterically congested, highly stable, and regulated IaSS was not
favorable for efficient solvent-to-polymer chirality transfer
Photosensitized Oxidative DNA Damage: From Hole Injection to Chemical Product Formation and Strand Cleavage
Oxidatively generated damage to DNA induced by a pyrenyl photosensitizer residue (Py)
covalently attached to a guanine base in the DNA sequence context 5‘-d(CAT[G1Py]CG2TCCTAC) in aerated
solutions was monitored from the initial one-electron transfer, or hole injection step, to the formation of
chemical end-products monitored by HPLC, mass spectrometry, and high-resolution gel electrophoresis.
Hole injection into the DNA was initiated by two-photon excitation of the Py residue with 355 nm laser
pulses, thus producing the radical cation Py•+ and hydrated electrons; the latter are trapped by O2, thus
forming the superoxide anion O2•-. The decay of the Py•+ radical is correlated with the appearance of the
G•+/G(−H)• radical on microsecond time scales, and O2•- combines with guanine radicals at G1 to form
alkali-labile 2,5-diamino-4H-imidazolone lesions (Iz1Py). Product formation in the modified strand is smaller
by a factor of 2.4 in double-stranded than in single-stranded DNA. In double-stranded DNA, hot piperidine-mediated cleavage at G2 occurs only after G1Py, an efficient hole trap, is oxidized thus generating tandem
lesions. An upper limit of hole hopping rates, khh 3 s-1 from G1•+−Py to G2 can be estimated from
the known rates of the combination reaction of the G(−H)• and O2•- radicals. The formation of Iz products
in the unmodified complementary strand compared to the modified strand in the duplex is ∼10 times smaller.
The formation of tandem lesions is observed even at low levels of irradiation corresponding to “single-hit”
conditions when less than ∼10% of the oligonucleotide strands are damaged. A plausible mechanism for
this observation is discussed
Bioconjugation of l-3,4-Dihydroxyphenylalanine Containing Protein with a Polysaccharide
We describe the simple bioconjugation strategy in combination of periodate chemistry and unnatural amino acid incorporation. The residue specific incorporation of 3,4-dihydroxy-l-phenylalanine can alter the properties of protein to conjugate into the polymers. The homogeneously modified protein will yield quinone residues that are covalently conjugated to nucleophilic groups of the amino polysaccharide. This novel approach holds great promise for widespread use to prepare protein conjugates and synthetic biology applications
