2-Aminopurine (2AP) is a fluorescent analog of guanosine and adenosine and has been used to probe nucleic acid structure and dynamics. Its spectral features in nucleic acids have been interpreted phenomenologically, in the absence of a rigorous electronic description of the context-dependence of 2AP fluorescence. Now, by using time-dependent density functional theory, we describe the excited-state properties of 2AP in a B-form dinucleotide stacked with guanosine, adenosine, cytosine, or thymine. Calculations predict that 2AP fluorescence is quenched statically when stacked with purines, because of mixing of the molecular orbitals in the ground state. In contrast, quenching is predicted to be dynamic when 2AP is stacked with pyrimidines, because of formation of a low-lying dark excited state. The different quenching mechanisms will result in different experimentally measured fluorescence lifetimes and quantum yields.T he nucleotide 2-aminopurine (2AP) has been used as a site-specific probe of nucleic acid structure and dynamics (1-11) because it base pairs with cytosine in a wobble configuration (4,5,12) or with thymine in a Watson-Crick geometry (7,11). Thermodynamic measurements of DNAs containing 2AP:C or 2AP:T show that the former pairing is more destabilizing (11,12). Incorporating 2AP into DNA quenches its fluorescence (2, 8, 11), reducing its quantum yield from that of the free nucleoside (0.65 in aqueous solution). This reduction is attributed to stacking interactions with nearest neighbor nucleobases, and, therefore, fluorescence properties of 2AP have been used to probe the equilibrium stacking properties of DNA duplexes containing these mismatched pairs (2,8,10). Although the fluorescence decay of 2AP in solution is single exponential, with a lifetime of Ϸ10 ns, in the context of a DNA molecule, four decay components, from 50 ps to 8 ns, are typically needed to describe its lifetime (2). The short decay time observed for 2AP in a duplex is attributed to the fully stacked state, whereas the longest lifetime comes from unstacked 2AP (2, 7). The distribution of stacked states can be altered by temperature, solvent, flanking bases, and bound protein, and so all of these conditions can be probed by using 2AP fluorescence. Dynamics of stacked bases adjacent to a mutagenic mismatch in DNA (such as 2AP:C and 2AP:T) may be part of the recognition mechanism by replication͞repair enzymes (3, 13), so interpretation of 2AP fluorescence data is critical for describing these environments.To understand the effect of base stacking on fluorescent properties of 2AP, we have used time-dependent density functional theory (TDDFT) (14, 15) to calculate the excited-state properties of 2AP alone and in stacked B-and A-form dinucleotides (dimers). Analysis of monomer calculations indicates the accuracy with which TDDFT describes spectral properties: excited-state transition energies, transition dipole directions, and oscillator strengths for 2AP, thymine, cytosine, adenine, and guanine (see figures) are in excellent agreement w...