Extended Data Fig. 7: Computation of IR spectra. | Nature Chemistry

Extended Data Fig. 7: Computation of IR spectra.

From: Ultrafast proton-coupled isomerization in the phototransformation of phytochrome

Extended Data Fig. 7

Computation of IR spectra. Selected QM/MM calculated (*) and experimental vibrational frequencies of vibrational modes diagnostic of the chromophore geometry for the Pfr models as well as Lumi-F model in H2O and D2O. Frequencies are given in cm−1. (*) The crystal structure of Agp2 in the Pfr state (PDB:6G1Y) was used as template for generating the initial structure for the Pfr and Lumi-F models. Unresolved regions in the crystal were restored by three-dimensional homology modelling using SWISS MODEL and hydrogens were added to the crystallographic structure according to predictions based on Karlsberg2 + . His248 and His278 were modeled as charge neutral each with a proton at Ne position. The Lumi-F model was generated based on the Pfr model by simply rotating the pyrrole ring D around 180 degrees. The chromophore binding site of the energy minimized- and thermally equilibrated solvated protein models were geometry optimized at QM/MM level. Accordingly, the biliverdin chromophore, the side chains of Cys13 and the pyrrole water were treated quantum mechanically at the B3LYP/6-31 G* level of theory while the protein matrix, solvent water and ions were described molecular mechanically using CHARMM36 force field. Relaxation during the minimization was allowed only for atoms located within a 20 Å-radius sphere centered at N22 of the BV cofactor. The charge-shifted scheme in combination with the electrostatic embedding approach was used to couple the QM and the MM region. The QM/MM optimized geometries were further used as input for subsequent frequency calculation of exclusively the QM fragment. These computations were performed at B3LYP/6-31 G* level of theory using GAUSSIAN09 following the same protocol as described previously in ref. 79. Scaling of force constants, normal mode analysis as well as correction of the QM Hessian matrix were performed using the programs developed in our group.

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