2008
DOI: 10.1021/jp802058k
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Charge-Transfer Excited States in a π-Stacked Adenine Dimer, As Predicted Using Long-Range-Corrected Time-Dependent Density Functional Theory

Abstract: The lowest few electronic excitations of a pi-stacked adenine dimer in its B-DNA geometry are investigated, in the gas phase and in a water cluster, using a long-range-corrected version of time-dependent density functional theory (TD-DFT) that asymptotically incorporates Hartree-Fock exchange. Long-range correction is shown to eliminate the catastrophic underestimation of charge-transfer (CT) excitation energies that plagues conventional TD-DFT, at the expense of introducing one adjustable parameter, mu, that … Show more

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Cited by 176 publications
(184 citation statements)
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References 49 publications
(96 reference statements)
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“…20,35,40,42,50,52,53,[59][60][61][65][66][67][68][69][70][71][72][73][74][75][76][77][78][79][80][81][82] The accuracy of optimally tuned range-separated functionals was critically tested in ref 61 for basis set variation as well as prediction of relative energies of spin states, binding energies, and the form of potential energy surfaces.…”
Section: Optimally Tuned Rangeseparated Functionalsmentioning
confidence: 99%
“…20,35,40,42,50,52,53,[59][60][61][65][66][67][68][69][70][71][72][73][74][75][76][77][78][79][80][81][82] The accuracy of optimally tuned range-separated functionals was critically tested in ref 61 for basis set variation as well as prediction of relative energies of spin states, binding energies, and the form of potential energy surfaces.…”
Section: Optimally Tuned Rangeseparated Functionalsmentioning
confidence: 99%
“…It has also been proposed to use in this scheme an empirically modified correlation density functional depending on the range-separation parameter [14]. The CAM-B3LYP scheme and other similar schemes have also been applied in linear-response theory for calculating excitation energies [11,[15][16][17][18][19][20][21][22][23][24][25][26]. In all these schemes, the presence of long-range HF exchange greatly improves Rydberg and charge-transfer excitation energies, in comparison to time-dependent Kohn-Sham (TDKS) calculations using standard local or semilocal density-functional approximations in which they are strongly underestimated (see, e.g., Ref.…”
Section: Introductionmentioning
confidence: 99%
“…[5][6][7][8][9] This failure of TD-DFT stems from the approximate (adiabatic) exchange-correlation functional, 10,11 and recent work in quantum chemistry has created new functionals that add in exact Hartree-Fock exchange at long-distance by partitioning the Coulomb operator. [12][13][14][15][16][17][18][19][20][21][22][23][24] These so-called longa) Electronic mail: subotnik@sas.upenn.edu.…”
Section: Introductionmentioning
confidence: 99%