5-Deuterouracil (5-d-U) is an analogue of uracil (RNA) and thymine (DNA), which differ only in the mass of their 5-substituent. Previous work has shown that the initial excited-state structural dynamics primarily lie along C5C6 bond lengthening in thymine, while these dynamics primarily lie along C5 and C6 pyramidalization in uracil. To test whether the 5-substituent mass determines these dynamics, the resonance Raman spectra of 5-d-U, with a 5-substituent mass intermediate between uracil and thymine, is measured at wavelengths throughout its 262 nm absorption band. The resulting spectrum of 5-d-U is intermediate between that of thymine and uracil, indicating both bond-lengthening and pyramidalization motions in the excited state. Self-consistent analysis of the resonance Raman excitation profiles and absorption spectra show that the initial excited-state structural dynamics of 5-d-U are indeed intermediate between those of thymine and uracil, supporting the mass-tuning model of initial excited-state structural dynamics in DNA and RNA pyrimidine nucleobases.

Substituents on the pyrimidine ring of nucleobases appear to play a major role in determining their initial excited-state structural dynamics and resulting photochemistry. To better understand the determinants of nucleobase initial excited-state structural dynamics, we have measured the absorption and resonance Raman excitation profiles of 6-deuterouracil (6-d-U) and 6-methyluracil (6-MeU). Simulation of the resonance Raman excitation profiles and absorption spectrum with a self-consistent, time-dependent formalism shows the effect of the deuterium and methyl group on the photochemically active internal coordinates, i.e. C5C6 stretch and C5X and C6X bends. The methyl group on either the C5 or C6 position of uracil equally increases the excited-state reorganization energies along the C5C6 stretch. However, a lower reorganization energy of the C5X + C6X bends in 6-MeU than uracil and 5-MeU shows that C6 methyl substituents reduce the bending reorganization energy. In addition, deuterium substitution at either C5 or C6 has a much smaller effect on the initial excited-state structural dynamics than methyl substitution, consistent with a mass effect. These results will be discussed in light of the resulting photochemistry of pyrimidine nucleobases.

In this investigation, we show that RNA can be separated from a solution containing DNA and RNA and the isolated RNA can be detected using poly (N-isopropylacrylamide-co-N-(3-aminopropyl) methacrylamide hydrochloride) microgel-based optical devices (etalons). The isolation of RNA was accomplished by using hairpin-functionalized magnetic beads (MMPDNA) and differential melting, based on the fact that the DNA–RNA hybrid duplex is stronger (i.e., high melting temperature) than the DNA–DNA duplex (i.e., low melting temperature). By performing concurrent etalon sensing and fluorescent studies, we found that the MMPDNA combined with differential melting was capable of selectively separating RNA from DNA. This selective separation and simple colorimetric detection of RNA from a mixture will help lead to future RNA-based disease diagnostic devices.

Resonance Raman derived initial excited-state structural dynamics provide insight into the photochemical mechanisms of pyrimidine nucleobases, in which the photochemistry appears to be dictated by the C5 and C6 substituents. The absorption and resonance Raman spectra and excitation profiles of 5,6-dideuterouracil were measured to further test this photochemical dependence on the C5 and C6 substituents. The resulting set of excited-state reorganization energies of the observed internal coordinates were calculated and compared to those of other 5- and 6-substituted uracils. The results show that the initial excited-state dynamics along the C5C6 stretch responds to changes in mass at C5 and C6 in the same manner but that the in-plane bends at C5 and C6 are more sensitive to substituents at the C5 position than at the C6 position. In addition, the presence of two deuterium substituents at C5 and C6 decreases the initial excited-state structural dynamics along these in-plane bends, in contrast to what is observed in the presence of two CH3 groups on C5 and C6. The results are discussed in the context of DNA nucleobase photochemistry.

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