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33747772053
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34447520716
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See Supporting Information for details
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See Supporting Information for details.
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4243943295
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The geometry of the stacked quartets was constructed using the standard global helical parameters of B-DNA. These gas phase calculations included the sugar-phosphate groups and six Na+ counter ions (three on each strand) located near the phosphate groups. The calculations used density functional theory (spin-density functional for the radical cations) with the generalized gradient approximation GGA, Perdew, J. P, Burke, K, Ernzerhof, M. Phys. Rev. Lett. 1996, 77, 3865-3868, and norm conserving soft pseudopotentials
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+ counter ions (three on each strand) located near the phosphate groups. The calculations used density functional theory (spin-density functional for the radical cations) with the generalized gradient approximation (GGA) [Perdew, J. P.; Burke, K.; Ernzerhof, M. Phys. Rev. Lett. 1996, 77, 3865-3868.] and norm conserving soft pseudopotentials.
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17
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0001496730
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A piane-wave basis (cut-off energy of 68 Ry) was used, with no supercell periodic replication of the ions, thus enabling accurate treatment of charged systems: Barnett, R. N.; Landman, U. Phys. Rev. B 1993, 48, 2081-2097.
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A piane-wave basis (cut-off energy of 68 Ry) was used, with no supercell periodic replication of the ions, thus enabling accurate treatment of charged systems: Barnett, R. N.; Landman, U. Phys. Rev. B 1993, 48, 2081-2097.
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18
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0029011701
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The MD simulations were carried out at T = 300 K, for 10 ns each with a time step of 1 fs, using the Amber 96 potentials: Cornell, W. D.; Cieplak, P.; Bayly, C. I.; Gould, I. R.; Merz, K. M.; Ferguson, D. M.; Spellmeyer, D. C.; Fox, T.; Caldwell, J. W.; Kollman, P. A. J. Am. Chem. Soc. 1995, 117, 5179-5197.
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The MD simulations were carried out at T = 300 K, for 10 ns each with a time step of 1 fs, using the Amber 96 potentials: Cornell, W. D.; Cieplak, P.; Bayly, C. I.; Gould, I. R.; Merz, K. M.; Ferguson, D. M.; Spellmeyer, D. C.; Fox, T.; Caldwell, J. W.; Kollman, P. A. J. Am. Chem. Soc. 1995, 117, 5179-5197.
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19
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34447558746
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The partial charges of uracil where taken as those fitted for simulations of RNA. TIP3P potentials [Jorgensen, W. L.; Chandrasekhar, J.; Madura, J. D.; Impey, R. W.; Klein, M. L. J. Chem. Phys. 183, 79, 926.] were used for water. No cutoffs were used for either the electrostatic or Lennard-Jones interactions.
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The partial charges of uracil where taken as those fitted for simulations of RNA. TIP3P potentials [Jorgensen, W. L.; Chandrasekhar, J.; Madura, J. D.; Impey, R. W.; Klein, M. L. J. Chem. Phys. 183, 79, 926.] were used for water. No cutoffs were used for either the electrostatic or Lennard-Jones interactions.
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20
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34447524186
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The samples were irradiated for 10 min (single hit conditions) at 350 nm, where only AQ absorbs, in air-saturated sodium phosphate buffer solution (pH 7) at ambient temperature. In the quantitative analyses of relative reactivity, interference caused by end effects was eliminated by considering only the four central identical GG steps, but including the others does not change the conclusion.
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The samples were irradiated for 10 min (single hit conditions) at 350 nm, where only AQ absorbs, in air-saturated sodium phosphate buffer solution (pH 7) at ambient temperature. In the quantitative analyses of relative reactivity, interference caused by end effects was eliminated by considering only the four central "identical" GG steps, but including the others does not change the conclusion.
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1542377678
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Liu, C.-S.; Hernandez, R.; Schuster, G. B. J. Am. Chem. Soc. 2004, 126, 2877-2884.
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(2004)
J. Am. Chem. Soc
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Liu, C.-S.1
Hernandez, R.2
Schuster, G.B.3
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0035913970
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While the dynamically fluctuating hydrating environment and counterion distribution may influence the IP values and hole distributions e.g, hole localization, Barnett, R. N, Cleveland, C. L, Joy, A, Landman, U, Schuster, G. B. Science 2001, 294, 567-571, they are likely to remain largely sequence independent, leaving our conclusions unchanged
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While the dynamically fluctuating hydrating environment and counterion distribution may influence the IP values and hole distributions (e.g., hole localization) [Barnett, R. N.; Cleveland, C. L.; Joy, A.; Landman, U.; Schuster, G. B. Science 2001, 294, 567-571.], they are likely to remain largely sequence independent, leaving our conclusions unchanged.
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