Glen R. Loppnow

Excited-state structure and isomerization dynamics of the retinal chromophore in rhodopsin from resonance Raman intensities

Resonance Raman excitation profiles have been measured for the bovine visual pigment rhodopsin using excitation wavelengths ranging from 457.9 to 647.1 nm. A complete Franck-Condon analysis of the absorption spectrum and resonance Raman excitation profiles has been performed using an excited-state, time-dependent wavepacket propagation technique. This has enabled us to determine the change in geometry upon electronic excitation of rhodopsins 11-cis-retinal protonated Schiff base chromophore along 25 normal coordinates. Intense low-frequency Raman lines are observed at 98, 135, 249, 336, and 461 cm-1 whose intensities provide quantitative, mode-specific information about the excited-state torsional deformations that lead to isomerization. The dominant contribution to the width of the absorption band in rhodopsin results from Franck-Condon progressions in the 1,549 cm-1 ethylenic normal mode. The lack of vibronic structure in the absorption spectrum is shown to be caused by extensive progressions in low-frequency torsional modes and a large homogeneous linewidth (170 cm-1 half-width) together with thermal population of low-frequency modes and inhomogeneous site distribution effects. The resonance Raman cross-sections of rhodopsin are unusually weak because the excited-state wavepacket moves rapidly (approximately 35 fs) and permanently away from the Franck-Condon geometry along skeletal stretching and torsional coordinates.

Excited-state dynamics of alizarin-sensitized TiO2 nanoparticles from resonance Raman spectroscopy

Resonance Raman spectra of alizarin-sensitized TiO2 nanoparticles have been obtained at excitation wavelengths throughout the 488-nm charge transfer absorption band. The resonance Raman spectrum of the alizarin-sensitized TiO2 nanoparticle is significantly different from the spectrum of free alizarin, consistent with a chemisorption-type interaction. This interaction is probably chelation of surface titanium ions by the hydroxy groups of alizarin, supported by the observed enhancement of bridging C–O modes at 1326 cm−1. In contrast to resonance Raman intensity analysis of homogeneous electron transfer where vibrations of both the donor and acceptor are observed, self-consistent analysis of the resulting resonance Raman excitation profiles and absorption spectrum using the time-dependent wave packet propagation formalism show mode-specific reorganization along alizarin vibrations exclusively; no resonance-enhanced vibrations attributable to the TiO2 moiety are observed. Therefore, the total resonance Raman...

pH-dependent UV resonance Raman spectra of cytosine and uracil.

Cytosine is a nucleobase found in both DNA and RNA, while uracil is found only in RNA. Uracil has abstractable protons at N3 and N1. Cytosine has only one abstractable proton at N1 but can also accept a proton at N3. The pKa values of these protons are well-known, but the effect of the change in protonation on the rest of the molecule is not well understood and is very important in base stacking, base pairing, and protein-nucleic acid interactions. In this paper, UV resonance Raman (UVRR) spectroscopy is used to probe the structures of both cytosine and uracil at varying pH to determine the structural changes that take place. The results show that cytosine has increased electronic delocalization when moving to either basic or acidic environments, whereas uracil shows no significant change in acidic environment but increases its electronic delocalization in basic environment.

Initial excited-state structural dynamics of uracil from resonance Raman spectroscopy are different from those of thymine (5-methyluracil).

To explore the origin of the differences in UV photochemistry of uracil (RNA) and thymine (DNA) nucleobases, we have measured the UV resonance Raman spectra of uracil in aqueous solution at wavelengths throughout the lowest-energy absorption band and analyzed the resulting resonance Raman excitation profiles and absorption spectra using a time-dependent wave-packet formalism to obtain the initial excited-state structural changes. In contrast to thymine, which differs from uracil only by the presence of a methyl group at C(5), most of the resonance Raman intensity and resulting initial excited-state structural dynamics for uracil occur along in-plane hydrogen-bond angle deformation, ring stretching, and carbonyl vibrational modes. Weaker intensities and less significant structural dynamics are observed along the C=C stretching mode. These results suggest that the initial excited-state structural dynamics of uracil occur along a carbon pyramidalization coordinate. These dynamics are different from those of thymine, which distorts primarily along a C(5)=C(6) bond lengthening coordinate. These differences in initial excited-state structural dynamics can explain the different primary photoproducts observed for these two pyrimidine nucleobases.

Initial excited-state structural dynamics of 9-methyladenine from UV resonance Raman spectroscopy.

The photophysics and photochemistry of nucleobases are the factors governing the photostability of DNA and RNA, since they are the UV chromophores in nucleic acids. Because the formation of photoproducts involves structural changes in the excited electronic state, we study here the initial excited-state structural dynamics of 9-methyladenine (9-MeA) by using UV resonance Raman (UVRR) spectroscopy. UV resonance Raman intensities are sensitive to the initial excited-state structural dynamics of molecules. Therefore, information about the initial structural changes in the excited-state of a given molecule can be obtained from its UVRR intensities. The resonance Raman spectra of 9-MeA at wavelengths throughout its 262 nm absorption band were measured, and a self-consistent analysis of the resulting resonance Raman excitation profiles and absorption spectrum was performed using a time-dependent wave packet formalism. We found that the initial structural dynamics of this molecule primarily lie along the N3C4, C4C5, C5C6, C5N7, N7C8, and C8N9 stretching vibrations and CH(3) deformation vibrations. These results are discussed in the context of photochemistry and other deactivation processes.

Molecular Beacon Probes of Photodamage in Thymine and Uracil Oligonucleotides

Abstract Molecular beacons (MB) are becoming more common as sequence-selective detectors of nucleic acids. Although they can easily detect single-base mismatches, they have never been used to directly detect DNA or RNA damage. To measure the degree of ultraviolet (UV) light damage in oligonucleotides, we report a novel MB approach for general detection of photoproducts in UV-irradiated rU17 and dT17 oligonucleotides. With monochromatic UV light irradiation at ca 280 nm under anoxic conditions, the oligonucleotide absorption decays with a single-exponential time constant of 123 ± 1 min for rU17 and with double-exponential time constants of 78 ± 0.5 min (99%) and 180 ± 5 min (0.05%) for dT17 oligonucleotides. Under the same conditions, the MB fluorescence decays more quickly, with single-exponential time constants of 19 ± 2 and 26 ± 3 min for rU17 and dT17, respectively. Similar kinetics were observed with broadband UV light irradiation of oligonucleotides. The differences in the UV damage kinetics of dT17 and rU17 and their detection by absorption and fluorescence techniques will be discussed in the context of differential instabilities introduced in the nucleic acid–MB duplex by the different photoproducts formed.

Self-quenching smart probes as a platform for the detection of sequence-specific UV-induced DNA photodamage

Molecular beacons (MBs) are sensitive probes for many DNA sequence-specific applications, such as DNA damage detection, but suffer from technical and cost limitations. We have designed smart probes with self-quenching properties as an alternative to molecular beacons to monitor sequence-specific UV-induced photodamage of oligonucleotides. These probes have similar stem-loop structural characteristics as molecular beacons, but quenching is achieved instead via photoinduced intramolecular electron transfer by neighboring guanosine residues. Our results indicate that the probes are sensitive enough to detect nanomolar target concentrations and are specific enough to discriminate single-base damage. When the probes were used to monitor UV-induced photodamage in oligonucleotide sequences that differ by a single-base mismatch, the photodamage time constant was higher for the perfectly complementary target sequences than for the mismatch sequences, indicating that these probes are specific for each target sequence. In addition, time constants obtained for oligonucleotide target sequences with both stem and loop base mismatches are lower than those with only loop mismatches, suggesting that these sequences are also specifically distinguished by the smart probes. These probes thus constitute robust, sensitive, specific, and cheaper alternatives to MBs for sequence-specific DNA damage detection.

2-Aminopurine hairpin probes for the detection of ultraviolet-induced DNA damage.

Nucleic acid exposure to radiation and chemical insults leads to damage and disease. Thus, detection and understanding DNA damage is important for elucidating molecular mechanisms of disease. However, current methods of DNA damage detection are either time-consuming, destroy the sample, or are too specific to be used for generic detection of damage. In this paper, we develop a fluorescence sensor of 2-aminopurine (2AP), a fluorescent analogue of adenine, incorporated in the loop of a hairpin probe for the quantification of ultraviolet (UV) C-induced nucleic acid damage. Our results show that the selectivity of the 2AP hairpin probe to UV-induced nucleic acid damage is comparable to molecular beacon (MB) probes of DNA damage. The calibration curve for the 2AP hairpin probe shows good linearity (R(2)=0.98) with a limit of detection of 17.2 nM. This probe is a simple, fast and economic fluorescence sensor for the quantification of UV-induced damage in DNA.

Initial excited-state structural dynamics of 5,6-dimethyluracil from resonance Raman spectroscopy.

In order to understand the effect of methyl substitution patterns on the initial excited-state structural dynamics of uracil derivatives, we measured the resonance Raman spectra of 5,6-dimethyluracil (5,6-DMU). The results show that the resonance Raman spectrum is a combination of that of 5-methyl- and 6-methyluracil. The resonance Raman excitation profiles (RREPs) and absorption spectrum are simulated with a self-consistent, time-dependent formalism to yield the excited-state slopes and broadening parameters. The initial excited-state structural dynamics occur primarily along the C5═C6 stretching mode, as expected, but with lesser excited-state slopes along each mode compared to 5-methyluracil and 6-methyluracil. This study along with previous experiments with different uracil derivatives show that the presence and positions of the methyl groups seems to determine the partitioning of initial excited-state structural dynamics.

Raman spectroscopy: a structural probe of solute-solvent interactions in ethyl 4-(dimethylamino)benzoate

Abstract Raman spectra of ethyl 4-(dimethylamino)benzoate (DMABEE) were recorded in 18 solvents of varying polarity and hydrogen bonding strength to elucidate the molecular mechanism of solute-solvent interactions in condensed phase. Frequency shifts were observed in the vibrational frequencies of the CO stretching, the CO stretching and the OCO bending modes, as a function of increasing solvent acceptor number. A molecular model of DMABEE-solvent interaction is proposed based on solute-solvent hydrogen bonding and π-π interactions. These results suggest that vibrational spectroscopy provides a mode-specific measure of solute-solvent interactions.