Controlling the Photoreactivity of the Photoactive Yellow Protein Chromophore by Substituting at the p-Coumaric Acid Group

• Published in: The journal of physical chemistry. B Vol. 115; no. 21; pp. 7021 - 7028
• Main Authors: Boggio-Pasqua, Martial, Groenhof, Gerrit
• Format: Journal Article
• Language: English
• Published: United States American Chemical Society 02-06-2011
• Subjects: B: Biophysical Chemistry; Bacterial Proteins - chemistry; Coumaric Acids - chemistry; Halorhodospira halophila - chemistry; Molecular Structure; Photochemistry; Photoreceptors, Microbial - chemistry; Propionates; Quantum Theory; Stereoisomerism
• ISSN: 1520-6106; 1520-5207
• DOI: 10.1021/jp108977x

We have performed ab initio CASSCF, CASPT2, and EOM-CCSD calculations on doubly deprotonated p-coumaric acid (pCA2−), the chromophore precursor of the photoactive yellow protein. The results of the calculations demonstrate that pCA2− can undergo only photoisomerization of the double bond. In contrast, the chromophore derivative with the acid replaced by a ketone (p-hydroxybenzylidene acetone, pCK−) undergoes both single- and double-bond photoisomerization, with the single-bond relaxation channel more favorable than the double-bond channel. The substitution alters the nature of the first excited states and the associated potential energy landscape. The calculations show that the electronic nature of the first two (π,π*) excited states are interchanged in vacuo due to the substitution. In pCK−, the first excited state is a charge-transfer (CT π,π*) state, in which the negative charge has migrated from the phenolate ring onto the alkene tail of the chromophore, whereas the locally excited (LE π,π*) state, in which the excitation involves the orbitals on the phenol ring, lies higher in energy and is the fourth excited state. In pCA2−, the CT state is higher in energy due the presence of a negative charge on the tail of the chromophore, and the first excited state is the LE state. In isolated pCA2−, there is a 68 kJ/mol barrier for double-bond photoisomerization on the potential energy surface of this LE state. In water, however, hydrogen bonding with water molecules reduces this barrier to 9 kJ/mol. The barrier separates the local trans minimum near the Franck−Condon region from the global minimum on the excited-state potential energy surface. The lowest energy conical intersection was located near this minimum. In contrast to pCK−, single-bond isomerization is highly unfavorable both in the LE and CT states of pCA2−. These results demonstrate that pCA2− can only decay efficiently in water and exclusively by double-bond photoisomerization. These findings provide a rationale for the experimental observations that pCA2− has both a longer excited-state lifetime and a higher isomerization quantum yield than pCK−.