The isolation and characterisation of a new type of dimeric adenine photoproduct in UV-irradiated deoxyadenylates

DNA damage in cancer development: special implications in viral oncogenesis

DNA lesions arise from a combination of physiological/metabolic sources and exogenous environmental influences. When left unrepaired, these alterations accumulate in the cells and can give rise to mutations that change the function of important proteins (i.e. tumor suppressors, oncoproteins), or cause chromosomal rearrangements (i.e. gene fusions) that also result in the deregulation of key cellular molecules. Progressive acquisition of such genetic changes promotes uncontrolled cell proliferation and evasion of cell death, and hence plays a key role in carcinogenesis. Another less-studied consequence of DNA damage accumulating in the host genome is the integration of oncogenic DNA viruses such as Human papillomavirus, Merkel cell polyomavirus, and Hepatitis B virus. This critical step of viral-induced carcinogenesis is thought to be particularly facilitated by DNA breaks in both viral and host genomes. Therefore, the impact of DNA damage on carcinogenesis is magnified in the case of such oncoviruses via the additional effect of increasing integration frequency. In this review, we briefly present the various endogenous and exogenous factors that cause different types of DNA damage. Next, we discuss the contribution of these lesions in cancer development. Finally, we examine the amplified effect of DNA damage in viral-induced oncogenesis and summarize the limited data existing in the literature related to DNA damage-induced viral integration. To conclude, additional research is needed to assess the DNA damage pathways involved in the transition from viral infection to cancer. Discovering that a certain DNA damaging agent increases the likelihood of viral integration will enable the development of prophylactic and therapeutic strategies designed specifically to prevent such integration, with an ultimate goal of reducing or eliminating these viral-induced malignancies.

Populations and Dynamics of Guanine Radicals in DNA strands-Direct versus Indirect Generation

Guanine radicals, known to be involved in the damage of the genetic code and aging, are studied by nanosecond transient absorption spectroscopy. They are generated in single, double and four-stranded structures (G-quadruplexes) by one and two-photon ionization at 266 nm, corresponding to a photon energy lower than the ionization potential of nucleobases. The quantum yield of the one-photon process determined for telomeric G-quadruplexes (TEL25/Na⁺) is (5.2 ± 0.3) × 10⁻³, significantly higher than that found for duplexes containing in their structure GGG and GG sequences, (2.1 ± 0.4) × 10⁻³. The radical population is quantified in respect of the ejected electrons. Deprotonation of radical cations gives rise to (G-H1)^• and (G-H2)^• radicals for duplexes and G-quadruplexes, respectively. The lifetimes of deprotonated radicals determined for a given secondary structure strongly depend on the base sequence. The multiscale non-exponential dynamics of these radicals are discussed in terms of inhomogeneity of the reaction space and continuous conformational motions. The deviation from classical kinetic models developed for homogeneous reaction conditions could also be one reason for discrepancies between the results obtained by photoionization and indirect oxidation, involving a bi-molecular reaction between an oxidant and the nucleic acid.

Adenine radicals generated in alternating AT duplexes by direct absorption of low-energy UV radiation

There is increasing evidence that the direct absorption of photons with energies that are lower than the ionization potential of nucleobases may result in oxidative damage to DNA. The present work, which combines nanosecond transient absorption spectroscopy and quantum mechanical calculations, studies this process in alternating adenine-thymine duplexes (AT)n. We show that the one-photon ionization quantum yield of (AT)10 at 266 nm (4.66 eV) is (1.5 ± 0.3) × 10-3. According to our PCM/TD-DFT calculations carried out on model duplexes composed of two base pairs, (AT)1 and (TA)1, simultaneous base pairing and stacking does not induce important changes in the absorption spectra of the adenine radical cation and deprotonated radical. The adenine radicals, thus identified in the time-resolved spectra, disappear with a lifetime of 2.5 ms, giving rise to a reaction product that absorbs at 350 nm. In parallel, the fingerprint of reaction intermediates other than radicals, formed directly from singlet excited states and assigned to AT/TA dimers, is detected at shorter wavelengths. PCM/TD-DFT calculations are carried out to map the pathways leading to such species and to characterize their absorption spectra; we find that, in addition to the path leading to the well-known TA* photoproduct, an AT photo-dimerization path may be operative in duplexes.

Initial excited-state structural dynamics of 2′-deoxyadenosine

Purine nucleobases (adenosine and guanosine) are prone to spontaneous breaking of the nucleosidic bond to form abasic sites in both DNA and RNA. However, the purines also undergo photochemical reactions, including oxidation and cycloaddition, to form damage sites, albeit at lower photochemical quantum yields than the pyrimidines. In this study, we use ultraviolet resonance Raman spectroscopy to measure the initial excited-state structural dynamics in the nucleoside, 2′-deoxyadenosine. The resonance Raman-derived initial excited-state structural dynamics throughout the 260 nm La excited electronic state of adenine are found to be smaller in the nucleoside than in the previously reported 9-methyladenine nucleobase derivative, consistent with what is found for the pyrimidines thymine and uracil. Interestingly, resonance-enhanced vibrational modes in this electronic state also contain internal coordinates localized on the sugar, which may represent a different energy dissipation mechanism than in the pyrimidine nucleosides. The results will be discussed in terms of the initial excited-state photophysics and photochemistry of DNA and RNA.

Formation of UV-induced DNA damage contributing to skin cancer development

UV-induced DNA damage plays a key role in the initiation phase of skin cancer. When left unrepaired or when damaged cells are not eliminated by apoptosis, DNA lesions express their mutagneic properties, leading to the activation of proto-oncogene or the inactivation of tumor suppression genes. The chemical nature and the amount of DNA damage strongly depend on the wavelength of the incident photons. The most energetic part of the solar spectrum at the Earth's surface (UVB, 280-320 nm) leads to the formation of cyclobutane pyrimidine dimers (CPDs) and pyrimidine (6-4) pyrimidone photoproducts (64PPs). Less energetic but 20-times more intense UVA (320-400 nm) also induces the formation of CPDs together with a wide variety of oxidatively generated lesions such as single strand breaks and oxidized bases. Among those, 8-oxo-7,8-dihydroguanine (8-oxoGua) is the most frequent since it can be produced by several mechanisms. Data available on the respective yield of DNA photoproducts in cells and skin show that exposure to sunlight mostly induces pyrimidine dimers, which explains the mutational signature found in skin tumors, with lower amounts of 8-oxoGua and strand breaks. The present review aims at describing the basic photochemistry of DNA and discussing the quantitative formation of the different UV-induced DNA lesions reported in the literature. Additional information on mutagenesis, repair and photoprotection is briefly provided.

Novel adenine/thymine photodimerization channels mapped by PCM/TD-DFT calculations on dApT and TpdA dinucleotides

Despite the biological relevance of AT-rich DNA sequences, the excited state paths associated with the photochemical reactions involving adenine and thymine stacked pairs have never been characterized, and the structure of the most abundant photoproduct in DNA is unknown. PCM/TD-M052X calculations on dApT and TpdA unveil the paths leading to the main photoproduct in TpdA, provide new insights into the reasons why it is not formed in dApT and show the existence of a new photochemical path, which could produce the precursor of the most abundant genomic AT/TA photoproduct. Our calculations confirm that anti/anti conformers are photochemically active and show that the dynamical solvation effects could significantly modulate the reaction yields.

Excited State Pathways Leading to Formation of Adenine Dimers

The reaction intermediate in the path leading to UV-induced formation of adenine dimers A═A and AA* is identified for the first time quantum mechanically, using PCM/TD-DFT calculations on (dA)2 (dA: 2'deoxyadenosine). In parallel, its fingerprint is detected in the absorption spectra recorded on the millisecond time-scale for the single strand (dA)20 (dA: 2'deoxyadenosine).

Electronic coupling between photo-excited stacked bases in DNA and RNA strands with emphasis on the bright states initially populated

In biology the interplay between multiple light-absorbers gives rise to complex quantum effects such as superposition states that are of extreme importance for life, both for harvesting solar energy and likely protecting nucleic acids from radiation damage. Still the characteristics of these states and their quantum dynamics are a much debated issue. While the electronic properties of single bases are fairly well understood, the situation for strands is complicated by the fact that stacked bases electronically couple when photoexcited. These newly arising states are denoted as exciton states and are simply linear combinations of localised wavefunctions that involve N - 1 ground-state bases and one base in its excited state (cf. the Frenkel exciton model). There is disagreement over the number of bases, N, that coherently couple, i.e., the spatial extent of the exciton, and how electronic deexcitation back to the ground state occurs. The importance of dark charge-transfer states has been inferred both from time-resolved fluorescence and transient absorption experiments. These states were suggested to be responsible for long deexcitation times but it is unclear whether 'long' is tens of picoseconds or nanoseconds. In this review paper, we focus on the bright states initially populated and discuss their nature based on information obtained from systematic absorption and circular dichroism experiments on single strands of different lengths. Our results from the last five years are compared with those from other groups, and are discussed in the context of successive deexcitation schemes. Pieces to the puzzle have come from different experiments and theory but a complete description has yet to emerge. As such the story about DNA/RNA photophysical decay mechanisms resembles the tale about the blind men and the elephant where all see the beast in different, correct but incomplete ways.

The variety of UV-induced pyrimidine dimeric photoproducts in DNA as shown by chromatographic quantification methods

Induction of DNA damage is one of the major consequences of exposure to solar UV radiation in living organisms. UV-induced DNA photoproducts are mostly pyrimidine dimers, including cyclobutane pyrimidine dimers, pyrimidine (6-4) pyrimidone photoproducts and Dewar valence isomers. In the last few decades, a large number of methods have been developed for the quantification of these pyrimidine dimers. The present review emphasizes the contribution of chromatographic techniques to our better understanding of the basic DNA photochemistry and the better description of damage in cells.

Physiological aspects of UV-excitation of DNA

Solar ultraviolet (UV) radiation, mainly UV-B (280-315 nm), is one of the most potent genotoxic agents that adversely affects living organisms by altering their genomic stability. DNA through its nucleobases has absorption maxima in the UV region and is therefore the main target of the deleterious radiation. The main biological relevance of UV radiation lies in the formation of several cytotoxic and mutagenic DNA lesions such as cyclobutane pyrimidine dimers (CPDs), 6-4 photoproducts (6-4PPs), and their Dewar valence isomers (DEWs), as well as DNA strand breaks. However, to counteract these DNA lesions, organisms have developed a number of highly conserved repair mechanisms such as photoreactivation, excision repair, and mismatch repair (MMR). Photoreactivation involving the enzyme photolyase is the most frequently used repair mechanism in a number of organisms. Excision repair can be classified as base excision repair (BER) and nucleotide excision repair (NER) involving a number of glycosylases and polymerases, respectively. In addition to this, double-strand break repair, SOS response, cell-cycle checkpoints, and programmed cell death (apoptosis) are also operative in various organisms to ensure genomic stability. This review concentrates on the UV-induced DNA damage and the associated repair mechanisms as well as various damage detection methods.

Formation and Direct Repair of UV-induced Dimeric DNA Pyrimidine Lesions

Direct repair of UV-induced DNA lesions represents an elegant method for many organisms to deal with these highly mutagenic and cytotoxic compounds. Although the participating proteins are structurally well investigated, the exact repair mechanism of the photolyase enzymes remains a vivid subject of current research. In this review, we summarize and highlight the recent contributions to this exciting field.

Probing electronic coupling between adenine bases in RNA strands from synchrotron radiation circular dichroism experiments

Circular dichroism spectra (176-330 nm) of RNA adenine oligomers, (rA)(n) (n = 1-10, 12, 15, and 20), reveal electronic coupling between two bases in short strands. The number of interacting bases in long strands is more and larger than that reported previously for the corresponding DNA strands.

Molecular mechanisms of ultraviolet radiation-induced DNA damage and repair

DNA is one of the prime molecules, and its stability is of utmost importance for proper functioning and existence of all living systems. Genotoxic chemicals and radiations exert adverse effects on genome stability. Ultraviolet radiation (UVR) (mainly UV-B: 280-315 nm) is one of the powerful agents that can alter the normal state of life by inducing a variety of mutagenic and cytotoxic DNA lesions such as cyclobutane-pyrimidine dimers (CPDs), 6-4 photoproducts (6-4PPs), and their Dewar valence isomers as well as DNA strand breaks by interfering the genome integrity. To counteract these lesions, organisms have developed a number of highly conserved repair mechanisms such as photoreactivation, base excision repair (BER), nucleotide excision repair (NER), and mismatch repair (MMR). Additionally, double-strand break repair (by homologous recombination and nonhomologous end joining), SOS response, cell-cycle checkpoints, and programmed cell death (apoptosis) are also operative in various organisms with the expense of specific gene products. This review deals with UV-induced alterations in DNA and its maintenance by various repair mechanisms.

Chemical investigation of light induced DNA bipyrimidine damage and repair

In all organisms, genetic information is stored in DNA and RNA. Both of these macromolecules are damaged by many exogenous and endogenous events, with UV irradiation being one of the major sources of damage. The major photolesions formed are the cyclobutane pyrimidine dimers (CPD), pyrimidine-pyrimidone-(6-4)-photoproducts, Dewar valence isomers and, for dehydrated spore DNA, 5-(α-thyminyl)-5,6-dihydrothymine (SP). In order to be able to investigate how nature's repair and tolerance mechanisms protect the integrity of genetic information, oligonucleotides containing sequence and site-specific UV lesions are essential. This tutorial review provides an overview of synthetic procedures by which these oligonucleotides can be generated, either through phosphoramidite chemistry or direct irradiation of DNA. Moreover, a brief summary on their usage in analysing repair and tolerance processes as well as their biological effects is provided.

A new photoproduct of 5-methylcytosine and adenine characterized by high-performance liquid chromatography and mass spectrometry

The UV portion of sunlight is mutagenic and can modify DNA by producing various photoproducts. UV photodamage often occurs at dipyrimidine sites, to give cyclobutane, pyrimidine-(6-4)-pyrimidone (6-4), and pyrimidine-(6-4)-Dewar pyrimidone (Dewar) photoproducts, and at TA and AA sites. There is no reported evidence, however, of UV photoproduct formation between C or 5-methylC ((m)C) and A. Irradiation of d(GTAT(m)CATGAGGTGC) with UVB light at physiological pH gives an unexpected photoproduct that undergoes fast thermal deamination but does not revert to its original structure under UVC irradiation. Evidence from nuclease P1 digestion coupled with electrospray ionization (ESI)-MS/MS is in accord with product formation between (m)C and A. HPLC analysis indicates that deamination gives a T<>A photoproduct that coelutes on reverse-phase chromatography with the well-known TA* photoproduct, formed from an initial [2 + 2] reaction between C5-C6 and C6-C5 of the adjacent thymine and adenine [as shown by Zhao , X. , et al. ( 1996 ) Nucleic Acids Res. 24 , 1554 - 1560 and Davies , R. J. , et al. ( 2007 ) Nucleic Acids Res. 35 , 1048 - 1053 ]. Furthermore, the deamination product of the unknown (m)C<>A photoproduct and the TA* photoproduct undergo nearly identical fragmentation in tandem MS. The evidence, taken together, indicates that the deamination product of the unknown (m)CA photoproduct has the same chemical structure as the TA* photoproduct. Therefore, the unknown photoproduct is referred to as the (m)CA* photoproduct, which, upon deamination, gives the TA* photoproduct.

High-resolution crystal structure of the intramolecular d(TpA) thymine-adenine photoadduct and its mechanistic implications

A high-resolution crystal structure is reported for d(TpA)*, the intramolecular thymine–adenine photoadduct that is produced by direct ultraviolet excitation of the dinucleoside monophosphate d(TpA). It confirms the presence of a central 1,3-diazacyclooctatriene ring linking the remnants of the T and A bases, as previously deduced from heteronuclear NMR measurements by Zhao et al. (The structure of d(TpA)*, the major photoproduct of thymidylyl-(3′-5′)-deoxyadenosine. Nucleic Acids Res., 1996, 24, 1554–1560). Within the crystal, the d(TpA)* molecules exist as zwitterions with a protonated amidine fragment of the eight-membered ring neutralizing the charge of the internucleotide phosphate monoanion. The absolute configuration at the original thymine C5 and C6 atoms is determined as 5S,6R. This is consistent with d(TpA)* arising by valence isomerization of a precursor cyclobutane photoproduct with cis–syn stereochemistry that is generated by [2 + 2] photoaddition of the thymine 5,6-double bond across the C6 and C5 positions of adenine. This mode of photoaddition should be favoured by the stacked conformation of adjacent T and A bases in B-form DNA. It is probable that the primary photoreaction is mechanistically analogous to pyrimidine dimerization despite having a much lower quantum yield.

Actions of ultraviolet light on cellular structures

Solar radiation is the primary source of human exposure to ultraviolet (UV) radiation. Overexposure without suitable protection (i.e., sunscreen and clothing) has been implicated in mutagenesis and the onset of skin cancer. These effects are believed to be initiated by UV-mediated cellular damage, with proteins and DNA as primary targets due to a combination of their UV absorption characteristics and their abundance in cells. UV radiation can mediate damage via two different mechanisms: (a) direct absorption of the incident light by the cellular components, resulting in excited state formation and subsequent chemical reaction, and (b) photosensitization mechanisms, where the light is absorbed by endogenous (or exogenous) sensitizers that are excited to their triplet states. The excited photosensitizers can induce cellular damage by two mechanisms: (a) electron transfer and hydrogen abstraction processes to yield free radicals (Type I); or (b) energy transfer with O2 to yield the reactive excited state, singlet oxygen (Type II). Direct UV absorption by DNA leads to dimers of nucleic acid bases including cyclobutane pyrimidine species and pyrimidine (6-4) pyrimidone compounds, together with their Dewar isomers. These three classes of dimers are implicated in the mutagenicity of UV radiation, which is typified by a high level of CC-->TT and C-->T transversions. Single base modifications can also occur via sensitized reactions including Type 1 and Type II processes. The main DNA product generated by (1)O2 is 8-oxo-Gua; this is a common lesion in DNA and is formed by a range of other oxidants in addition to UV. The majority of UV-induced protein damage appears to be mediated by (1)O2, which reacts preferentially with Trp, His, Tyr, Met, Cys and cystine side chains. Direct photo-oxidation reactions (particularly with short-wavelength UV) and radicals can also be formed via triplet excited states of some of these side chains. The initial products of (1)O2-mediated reactions are endoperoxides with the aromatic residues, and zwitterions with the sulfur-containing residues. These intermediates undergo a variety of further reactions, which can result in radical formation and ring-opening reactions; these result in significant yields of protein cross-links and aggregates, but little protein fragmentation. This review discusses the formation of these UV-induced modifications and their downstream consequences with particular reference to mutagenesis and alterations in protein structure and function.

Major adenine products from 2-methyl-1,4-naphthoquinone-sensitized photoirradiation at 365 nm

In this article we report the isolation and characterization of major products of adenine in dinucleoside monophosphates upon 2-methyl-1,4-naphthoquinone (menadione)-sensitized UVA irradiation. Our results show that the major products form via the coupling between the menadione moiety and the exocyclic amino group of adenine. Similar reactions were not observed for cytosine. To our knowledge, this is the first report about the direct reaction between a DNA base and a photosensitizer under 365-nm ultraviolet light irradiation. Our results are consistent with previous observation showing that N(6) radical formed on adenine upon UVA irradiation.

Fragmentation of photomodified oligodeoxynucleotides adducted with metal ions in an electrospray-ionization ion-trap mass spectrometer

We report the effect of metal-ion adduction on the fragmentation of oligodeoxynucleotides (ODNs) bearing DNA photoproducts. When protons on backbone phosphates of ODNs are completely replaced with metal ions, cleavages occur readily within the photoproduct moiety, whereas those cleavages do not occur in photomodified ODNs in which the phosphates are associated with protons. For example, thymine/adenine (TA*) photoproducts revert to their undamaged precursors upon collisional activation, the pyrimidine(6-4)pyrimidone product and its Dewar valence isomer show a characteristic neutral loss of C4H3NO3, and dimeric adenine photoproducts show a distinctive loss of NH2CN from the adenine six-membered ring. The product-ion mass spectra of photodamaged ODNs that are adducted to metal ions are complementary in terms of structure information to those spectra of ODNs in which the phosphates are associated with protons. The results also demonstrate that the energy required for strand cleavages is higher for ODNs adducted with metal ions than that for ODNs bound with protons. Furthermore, the loss of a pyrimidine is more favorable than the loss of a purine in the fragmentation of ODNs associated with metal ions.

Direct and indirect effects of UV radiation on DNA and its components

In this survey, emphasis was placed on the main photoreactions of nucleic acid components, involving both direct and indirect effects. The main UVB- and UVA-induced DNA photoproducts, together with the mechanisms of their formation, are described. Information on the photoproduct distribution within cellular DNA is also provided, taking into account the limitations of the different analytical methods applied to monitor the formation of the DNA damage. Thus, the formation of the main DNA dimeric pyrimidine lesions produced by direct absorption of UVB photons was assessed using a powerful HPLC-tandem mass spectrometry assay. In addition, it was found that UVA photooxidation damage mostly involves the guanine residues of cellular DNA as the result of singlet oxygen generation by still unknown endogenous photosensitizers.

Formation and processing of UV photoproducts: effects of DNA sequence and chromatin environment

Cyclobutane pyrimidine dimers and (6-4) photoproducts are the two major classes of lesions produced in DNA by UVB and UVC irradiation. Their distribution along genes is nucleotide sequence-dependent. In vivo, the frequency of these lesions at specific sites is modulated by nucleosomes and other DNA binding proteins. Repair of UV photoproducts is dependent on the transcriptional status of the sequences to be repaired and on the chromatin environment. The formation of DNA photolesions by UV light is responsible for the induction of mutations and the development of skin cancer. To understand the mechanisms of UV mutagenesis, it is important to know how these lesions are formed, by which cellular pathways they are repaired and how they are dealt with by DNA polymerases.

Synthesis and properties of DNA purine dehydrodimers: 8-8-bideoxyribonucleosides and 8-8-bideoxyribonucleotides

Purine dimers are formed by oxidation of DNA. There is evidence that these dimers are not repaired by cells from the human disease xeroderma pigmentosum. It has been suggested that unrepaired purine dimers are involved in the etiogenesis of internal cancers and neural degeneration that are observed in this disease. In order to study the properties and biological consequences of such moieties, these compounds were synthesized: 8-8-(2'-deoxyadenosyl)-2'-deoxyadenosine; 8-8-(2'-deoxyadenosyl)-2'-deoxyadenosine-5'-monophosphate; 8-8-(2'-deoxyadenosyl)-2'-deoxyguanosine; 8-8-(2'-deoxyadenosyl)-2'-deoxyguanosine-5'-monophosphate; 8-8-(2'-deoxyguanosyl)-2'-deoxyguanosine; 8-8-(2'-deoxyguanosyl)-2'-deoxyguanosine-5'-monophosphate; 8-8-(2'-deoxyguanosyl)-2'-deoxyadenosine, and 8-8-(2'-deoxyguanosyl)-2'-deoxyadenosine-5'-monophosphate. Following purification, they were characterized by mass spectrometry and nuclear magnetic resonance studies. Ultraviolet, fluorescence, and circular dichroic spectra of these products were established. The behavior of these photoproducts in various chromatographic systems was elucidated. Syntheses of purine dimers and descriptions of their properties can aid the studies of their possible formation in, and excision from, oxidized DNA.

Photochemistry of DNA and related biomolecules: quantum yields and consequences of photoionization

The reactions of nucleic acids and constituents, which can be induced by laser UV irradiation, are described. Emphasis is placed on the quantum yields of various stable photoproducts of DNA and model compounds upon irradiation at 193, 248, 254 or 266 nm. In particular, those quantum yields and processes are discussed which involve photoionization as the initial step and occur in aqueous solution under well defined conditions, e.g. type of atmosphere. The efficiencies of some photoproducts, with respect to photoionization using irradiation at 193 or 248 nm, are presented. Radical cations of nucleobases are important sources of damage of biological substrates since they can cause lesions other than dimers and adducts, e.g. strand breakage, abasic sites, crosslinks or inactivation of plasmid and chromosomal DNA. While competing photoreactions, such as hydration, dimerization or adduct formation, diminish the selectivity of the photoionization method, a combination with model studies on pyrimidine- and purine-containing constituents of DNA has brought about an enhanced insight into the reaction mechanisms. The knowledge concerning the lethal events in plasmid and cellular DNA has been greatly improved by correlation with the chemical effects obtained by gamma-radiolysis, vacuum-UV (< 190 nm) and low-intensity irradiation at 254 nm.

Damage to uracil- and adenine-containing bases, nucleosides, nucleotides and polynucleotides: quantum yields on irradiation at 193 and 254 nm

Photoreactions, such as base release and decomposition of the base moiety, induced by either 20 ns laser pulses at 193 nm or continuous 254 nm irradiation, were studied for a series of uracil and adenine derivatives in neutral aqueous solution. The quantum yield of chromophore loss (phi cl) depends significantly on the nature of the nucleic acid constituent and the saturating gas (Ar, N2O or O2). In the case of polynucleotides the destruction of nucleotides was measured by high-performance liquid chromatography after hydrolysis; the quantum yields (phi dn) are comparable to those of chromophore loss or larger. The phi cl and phi dn of 0.04-0.1 for poly(U) and poly(dU), obtained for both wavelengths of irradiation, are due to processes originating from the lowest excited singlet state, i.e. formation of photohydrates and photodimers, and a second part from photoionization using lambda irr = 193 nm. Irradiation at 193 nm effectively splits pyrimidine dimers and thus reverts them into monomers. The quantum yield for release of undamaged bases (phi br) from nucleosides, nucleotides and polynucleotides upon irradiation at 254 nm is typically phi br = (0.1-1) x 10(-4). Breakage of the N-glycosidic bond is significantly more efficient for lambda irr = 193 nm, e.g. phi br = 1.1 x 10(-3), 0.8 x 10(-3), 4.3 x 10(-3) and 0.5 x 10(-3) for poly(A), poly(dA), poly(U) and poly(dU) in Ar-saturated solution, respectively. Enhanced phi values for lambda irr = 193 nm, essentially for adenine and its derivatives, are caused by photoprocesses that are initiated by photoionization.

A tertiary interaction in the Tetrahymena intron contributes to selection of the 5' splice site

The utilization of cryptic splice sites has been observed in a number of RNA splicing reactions. In the self-splicing group I intron of Tetrahymena thermophila, point mutations of either A57 or A95 promote cleavage at two sites other than the normal 5' splice site, suggesting that these nucleotides are involved in a common tertiary interaction. These results are unusual since A57 and A95 are neither at nor near the 5' splice site in the sequence or secondary structure. Cleavage at the alternative sites appears to occur by intron cyclization, a reaction with well-established structural and mechanistic similarities to the first step of RNA self-splicing. Alternative docking of P1 (the helix containing the 5' splice site paired to the internal guide sequence of the intron) into the catalytic core accounts for cleavage at the cryptic reaction sites. We propose that the A57/A95 interaction, along with an element implicated previously (J1/2), provide structural connectivity from the reaction site in P1 to the catalytic core of the Tetrahymena intron. It seems likely that RNA splicing in general will require such tertiary interactions to position RNA helices.

Alkali-labile photolesions mapping to purine sites in ultraviolet-irradiated DNA

Gel sequencing experiments with the 5'- and 3'-end-labeled oligonucleotides d(A3GA4GA5GA6GA3G) and d(AT)10 have demonstrated that dimeric adenine photoproducts and thymine-adenine photoadducts constitute alkali-labile lesions in UV-irradiated DNA. On treatment with hot piperidine, DNA strand breakage occurs predominantly at the sites of 5'-adenines in the dimeric photoproducts and of 3'-adenines in the thymine-adenine photoadducts. With 5'-end-labeled oligonucleotides of mixed sequence, major UV-induced loci for alkaline cleavage map to purine bases flanked on their 5'-side by two pyrimidines. This behavior does not arise from enhanced photoreactivity of purines in this sequence context as has been inferred from photofootprinting studies. Instead, as shown by 3'-labeling and selective substitution with 5-methylcytosine, it results from the anomalous electrophoretic mobility of 5'-end-labeled fragments produced by alkaline cleavage of DNA at adjacent pyrimidine (6-4) pyrimidone photoproducts.

The photochemistry of adenosine: intermediates contributing to its photodegradation mechanism in aqueous solution at 298 K and characterization of the major product

The steady-state (254 nm) photolysis of 9-(beta-D-erythropentofuranosyl)adenine (adenosine) in aqueous solution was studied. Photodestruction yields on the order of 1.3 x 10(-3) were determined at room temperature by measuring the initial decrease in the absorption maximum as a function of irradiation time. The use of high performance liquid chromatography (HPLC) permitted a more exact determination of the yield (2.5 x 10(-3). The formation of photoproducts was also studied using HPLC. In the photolysis of 50 microM aqueous solutions of adenosine under anaerobic conditions at least 11 stable photoproducts are formed that absorb at 260 nm, the wavelength of maximum absorption of adenosine. The major photoproduct was also isolated and characterized as adenine; its formation yield was determined to be 4.5 x 10(-4). This yield is affected by the presence of oxygen and by the initial concentration of adenosine employed. Fluorescence emission and excitation spectra were used to monitor the formation of highly fluorescent photoproducts that emit with maxima at 365, 398, and 430 nm and absorb in the wavelength region of 240-380 nm. The reactive species in the photodestruction mechanism were established using substrates that react selectively with the respective short-lived species. Photoionization is a primary photoprocess implied by these studies. The triplet state of adenosine also contributes to the photodestruction mechanism.

Binding of transcription factors creates hot spots for UV photoproducts in vivo

Cyclobutane dipyrimidines and less than mean value of 6-4 dipyrimidines are the two major classes of mutagenic DNA photoproducts produced by UV irradiation of cells. We developed a method to map cyclobutane dipyrimidines at the DNA sequence level in mammalian cells. The frequency of this class of photoproducts was determined at every dipyrimidine along the human phosphoglycerate kinase-1 (PGK1) promoter sequence and was compared to the UV-induced frequency distribution of mean value of 6-4 dipyrimidines. After irradiation of living cells containing active or inactive PGK1 genes, enzymatic or chemical cleavage at UV photoproducts, and amplification by ligation-mediated polymerase chain reaction, photofootprints were seen in all regions which bind transcription factors and appear as DNase I footprints. Photoproduct frequency within transcription factor binding sites was suppressed or enhanced relative to inactive genes or naked DNA with enhancements of up to 30-fold. Since photoproducts are mutagenic, this indicates that photoproduct (mutation?) hot spots may be tissue specific in mammals.

Binding of transcription factors creates hot spots for UV photoproducts in vivo

Cyclobutane dipyrimidines and less than mean value of 6-4 dipyrimidines are the two major classes of mutagenic DNA photoproducts produced by UV irradiation of cells. We developed a method to map cyclobutane dipyrimidines at the DNA sequence level in mammalian cells. The frequency of this class of photoproducts was determined at every dipyrimidine along the human phosphoglycerate kinase-1 (PGK1) promoter sequence and was compared to the UV-induced frequency distribution of mean value of 6-4 dipyrimidines. After irradiation of living cells containing active or inactive PGK1 genes, enzymatic or chemical cleavage at UV photoproducts, and amplification by ligation-mediated polymerase chain reaction, photofootprints were seen in all regions which bind transcription factors and appear as DNase I footprints. Photoproduct frequency within transcription factor binding sites was suppressed or enhanced relative to inactive genes or naked DNA with enhancements of up to 30-fold. Since photoproducts are mutagenic, this indicates that photoproduct (mutation?) hot spots may be tissue specific in mammals.

Adenine photodimerization in deoxyadenylate sequences: elucidation of the mechanism through structural studies of a major d(ApA) photoproduct

The mechanism of the photodimerization of adjacent adenine bases on the same strand of DNA has been elucidated by determining the structure of one of the two major photoproducts that are formed by UV irradiation of the deoxydinucleoside monophosphate d(ApA). The photoproduct, denoted d(ApA)*, corresponds to a species of adenine photodimer first described by Pörschke (Pörschke, D. (1973) J.Am.Chem.Soc. 95, 8440-8446). From a detailed examination of its chemical and spectroscopic properties, including comparisons with the model compound N-cyano-N1-(1-methylimidazol-5-yl)formamidine, it is deduced that d(ApA)* contains a deoxyadenosine unit covalently linked through its C(8) position to C(4) of an imidazole N(1) deoxyribonucleoside moiety bearing an N-cyanoformamidino substituent at C(5). On treatment with acid, d(ApA)* is degraded with high specificity to 8-(5-amino-imidazol-4-yl)adenine whose identity has been confirmed by independent chemical synthesis. It is concluded that the primary event in adenine photodimerization entails photoaddition of the N(7)-C(8) double bond of the 5'-adenine across the C(6) and C(5) positions of the 3'-adenine. The azetidine species thus generated acts as a common precursor to both types of d(ApA) photoproduct which are formed from it by competing modes of azetidine ring fission.

NMR studies of bipyrimidine cyclobutane photodimers

Cyclobutane-type photodimers of dinucleoside monophosphates dCpdT, dTpdC and dTpdT were prepared by ultraviolet irradiation in the presence of acetophenone as photosensitizer. The cytosine-containing derivatives were found to deaminate forming uracil products. Using one- and two-dimensional NMR, the photoproducts were characterized as cis-syn and trans-syn cyclobutane photodimers. On the basis of NOE data the structures of the cis-syn and trans-syn products of dUpdT were determined using distance-geometry and restrained-energy-minimization methods. The cis-syn structures showed (high-ANTI/SYN)/high-ANTI glycosidic linkages while the trans-syn structures were in the SYN-ANTI region. The backbone conformations of both structures were in fair agreement with the coupling-constant-data. The trans-syn structures were found to be very rigid and similar in all three products. For the three cis-syn structures more conformational freedom and more variation among the three structures was observed.

An ultraviolet-inducible adenosine-adenosine cross-link reflects the catalytic structure of the Tetrahymena ribozyme

When a shortened enzymatic version of the Tetrahymena self-splicing intervening sequence (IVS) RNA is placed under catalytic conditions and irradiated at 254 nm, a covalent cross-link forms with high efficiency. The position of the cross-link was mapped by using three independent methods: RNase H digestion, primer extension with reverse transcriptase, and partial hydrolysis of end-labeled RNA. The cross-link is chemically unusual in that it joins two adenosines, A57 and A95. Formation of this cross-link depends upon the identity and concentration of divalent cations present and upon heat-cool renaturation of the IVS in a manner that parallels conditions required for optimal catalytic activity. Furthermore, cross-linking requires the presence of sequences within the core structure, which is conserved among group I intervening sequences and necessary for catalytic activity. Together these correlations suggest that a common folded structure permits cross-linking and catalytic activity. The core can form this structure independent of the presence of P1 and elements at the 3' end of the IVS. The cross-linked RNA loses catalytic activity under destabilizing conditions, presumably due to disruption of the folded structure by the cross-link. One of the nucleotides participating in this cross-link is highly conserved (86%) within the secondary structure of group I intervening sequences. We conclude that A57 and A95 are precisely aligned in a catalytically active conformation of the RNA. A model is presented for the tertiary arrangement in the vicinity of the cross-link.

Two-quantum UV photochemistry of nucleic acids: comparison with conventional low-intensity UV photochemistry and radiation chemistry

The action of high-intensity laser u.v. radiation on nucleic acid molecules and their constituents in vitro and in vivo is compared with the results of low-intensity u.v. photolysis and gamma-radiolysis.

The solution structure of the intramolecular photoproduct of d(TpA) derived with the use of NMR and a combination of distance geometry and molecular dynamics

One and two dimensional NMR techniques have been used together with molecular modelling to obtain the solution structure for the photoproduct d(TpA)*. The NMR data confirm that the cyclobutane linkage is formed between the bonds thymine C6-C5 and adenine C5-C6. The 2D NOE data are used as constraints in a distance geometry calculation. The structures obtained show a trans-syn cyclobutane linkage and the glycosidic angles are SYN and ANTI for thymidine and deoxyadenosine, respectively. The coupling constant data are used to check the backbone torsion angles of the obtained structures. Typical torsion angles are a gamma+ and beta t for the deoxyadenosine residue. A free molecular dynamics simulation of a trans-syn d(TpA) photoproduct confirmed all these structural characteristics.

Origin of ultraviolet damage in DNA

A novel ultraviolet (u.v.) footprinting technique has been used to analyze the formation of u.v. photoproducts at 250 bases of a 5 S rRNA gene under conditions where the gene is either double or single-stranded. Because many more types of u.v. damage can be detected by the u.v. footprinting technique than has been previously possible, we have been able to examine in detail why certain bases in DNA are damaged by u.v. light while others are not. Our measurements demonstrate that the ability of u.v. light to damage a given base in DNA is determined by two factors, the sequence of the DNA in the immediate vicinity of the photoproduct, and the flexibility of the DNA at the site of the photoproduct. For pyrimidines, the predominant photoreaction in double-stranded DNA involves covalent dimerization between adjacent pyrimidine residues. Dimerization is much easier in melted DNA because the geometrical changes required for adjacent pyrimidine residues to dimerize are easier in single-stranded DNA. The absorption of a u.v. photon cannot simultaneously induce the geometrical changes required for adjacent pyrimidines or other bases to dimerize with one another. Rather, upon the absorption of a u.v. photon, only those thermally excited bases that are in a geometry capable of easily forming a photodimer during excitation, can photoreact. In contrast to adjacent pyrimidines, non-adjacent pyrimidines (pyrimidines flanked on either side by a purine) do not readily form u.v. photoproducts in double-stranded DNA. Because photoreactions at non-adjacent pyrimidine residues are greatly enhanced in single-stranded DNA, their failure to form in double-helical DNA is attributed to torsional constraints imposed by the double helix which make it difficult for non-adjacent pyrimidines to adopt a geometry necessary for photoreaction. Although purines are believed to be resistant to u.v. damage, our measurements demonstrate that at moderate u.v. dosages purines which are flanked on their 5' side by two or more contiguous pyrimidines readily form u.v. photoproducts in double-stranded DNA. Flanking pyrimidines appear to activate purine photoreactions by transferring triplet excitation energy to the purine. Melting of the DNA helix greatly inhibits the ability of flanking pyrimidines to activate purine photoreactions, presumably by disrupting intimate orbital overlap required for triplet transfer.

Formation of purine photoproducts in a defined human DNA sequence

The formation of DNA base damages by broad spectrum ultraviolet irradiation (250-400 nm) was investigated using a defined sequence of human DNA. The irradiated, 92 base pair, 3'-end of the human alphoid segment was incubated with an enzyme fraction purified from bacteriophage T4-infected E. coli. As previously reported, analysis of reaction products by sequencing gels showed enzymic incision of purine-containing photoproducts as well as pyrimidine cyclobutane photodimers. The purine-incising activity does not require metal ions and was unaffected by beta-mercaptoethanol or dithiothreitol. The formation of the purine photoproducts is independent of buffer; these lesions are produced by irradiation of DNA in Tris, Hepes or phosphate buffers. They are produced at biologically significant wavelengths between 260 to 300 nm. Only low levels were detected above or below this range. The formation of purine photoproducts is dose dependent with similar yields at some specific loci to pyrimidine dimers. These results suggest that purine-containing photoproducts could be of consequence in ultraviolet carcinogenesis.

Extent of formation of a dimeric adenine photoproduct in polynucleotides and DNA

Quantum yields are reported for the formation of a dimeric adenine photoproduct, A = A, in adenine homopolymers and DNA irradiated at 254 nm. The A = A content of irradiated samples was assayed by using reversed-phase HPLC to isolate the 4,6-diamino-5-guanidinopyrimidine (DGPY) which is produced from A = A on acid hydrolysis. Acid hydrolysates derived from DNA radiolabelled with [14C] 2'-deoxyadenosine were spiked with unlabelled DGPY before fractionation on HPLC and the recovered material was further purified by chromatography on Sephadex G-10 followed by co-crystallization with DGPY sulphate. Although A = A is formed with a relatively high quantum yield of 1.6 X 10(-3) mol einstein-1 in single-stranded poly(dA) the photoaddition reaction is strongly quenched in base-paired poly(dA).poly(dT) and undetectable in poly(rA).poly(dT). Respective quantum yields of 6 X 10(-5) and 9 X 10(-6) were estimated for the formation of A = A in single- and double-stranded E. coli DNA implying that the photoproduct has very limited biological significance. From studies with d(ApG), d(GpA), ApG, GpA, d(A)20 and d(A4G)4 it is concluded that adjacent guanine and adenine bases do not form a photoadduct analogous to A = A and also that guanine residues have no local or long-range quenching effect on photodimerization within A-A doublets.