Mixing ratio-dependent energy transfer from DNA-bound 4′,6-diamidino-2-phenylindole to [Ru(1,10-phenanthroline)2dipyrido[3,2-a:2′,3′-c]phenazine]2+

Ji Yeon Choi, Jeong Mi Lee, Hyosun Lee, Maeng Joon Jung, Seog K. Kim, Jong Moon Kim

Research output: Contribution to journalArticlepeer-review

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Abstract

The binding mode of Δ- and Λ-[Ru(1,10-phenanthroline)2dipyrido[3,2-a:2′,3′-c]phenazine]2+ ([Ru(phen)2DPPZ]2+) to DNA in the presence of 4′,6-diamidino-2-phenylindole (DAPI) at a low and high [DAPI]/[DNA base] ratio (0.02 and 0.20, respectively) was investigated using electric absorption and circular dichroism spectroscopy. The spectral properties of both the Δ- and Λ-[Ru(phen)2DPPZ]2+ were not altered in the presence of DAPI disregarding the [DAPI]/[DNA] ratio, suggesting that the presence of DAPI in the minor groove of DNA does not affect the binding mode of the [Ru(phen)2DPPZ]2+ complex to DNA. The transferring excited energy of DAPI to both Δ- and Λ-[Ru(phen)2DPPZ]2+ occurs through Förster type resonance when they both spontaneously bound to DNA. At a high [DAPI]/[DNA] ratios, an upward bending curve in the Stern-Volmer plot, and a shortening the DAPI fluorescence decay time with increasing [Ru(phen)2DPPZ]2+ concentration were found. These results indicate that the quenching of the DAPI's fluorescence occurs through both the static and dynamic mechanisms. In contrast, the quenching mechanism at a low [DAPI]/[DNA] ratios was found to be purely static. The static quenching constant decreased linearly with respect to the [DAPI]/[DNA] ratio. Decrease in quenching efficiency can be explained by the association constant of [Ru(phen)2DPPZ]2+ to DNA while being within a quenchable distance from a DAPI molecule.

Original languageEnglish
Pages (from-to)56-63
Number of pages8
JournalBiophysical Chemistry
Volume134
Issue number1-2
DOIs
StatePublished - Apr 2008

Keywords

  • [Ru(1,10-phenanthroline)dipyrido[3,2-a:2′,3′-c]phenazine]
  • DNA, 4′,6-diamidino-2-phenylindole
  • Energy transfer
  • Luminescence
  • Spectroscopy

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