2010
DOI: 10.1002/qua.22957
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Development of force field parameters for oxyluciferin on its electronic ground and excited states

Abstract: Construction of force field parameters of the oxyluciferin molecule on its electronic ground and excited states is presented. Several new approaches are introduced for more reliable parameterization: argon-scanning, Hessian matching, and constrained-group parameterization. The Ar-scanning approach is for fitting Lennard-Jones parameters so that the constructed force field can mimic the changes in ab initio energy of oxyluciferin-argon pair at various argon positions. The Hessian matching procedure is to closel… Show more

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Cited by 31 publications
(36 citation statements)
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References 102 publications
(98 reference statements)
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“…Orientation of water dipoles and lipid head group dipoles at the water‐membrane interface can be one reason for the appearance of the membrane electrostatic potential. Ions and membrane‐associated molecules are other parts of the system that significantly affect the value of the electrostatic potentials of the lipid bilayers . Charge density distribution along the Z ‐axis ρ(z) is related to the electrostatic potential ψ(z) by the Poisson equation: d 2 Ψ ( z ) d z 2 = ρ ( z ) ɛ 0 where ε 0 is the vacuum permittivity (the relative permittivity is set to 1 in atomistic simulations).…”
Section: Resultsmentioning
confidence: 99%
“…Orientation of water dipoles and lipid head group dipoles at the water‐membrane interface can be one reason for the appearance of the membrane electrostatic potential. Ions and membrane‐associated molecules are other parts of the system that significantly affect the value of the electrostatic potentials of the lipid bilayers . Charge density distribution along the Z ‐axis ρ(z) is related to the electrostatic potential ψ(z) by the Poisson equation: d 2 Ψ ( z ) d z 2 = ρ ( z ) ɛ 0 where ε 0 is the vacuum permittivity (the relative permittivity is set to 1 in atomistic simulations).…”
Section: Resultsmentioning
confidence: 99%
“…32,47,48 However, some doubt can be shed to this statement by a recent force-field parameterization developed for the ground and excited state of Keto- (21), which revealed that exist some differences between the ground and the excited state. 60 However, this study do not demonstrated that these differences result in different effects caused by the same intermolecular forces in both states, as no excitation or emission energies were calculated. For the contrary, the calculation of emission energies of Keto- (21) in complex with small molecules or active site molecules, withdrawn from the ''closed'' conformation of Luc, support our conclusions regarding the effects exerted by ionic interactions and hydrogen bonding.…”
Section: Evaluation Of the Interactions Present In The Active Site Ofmentioning
confidence: 55%
“…[23] Just like in QM/ MM, we can calculate (1) the electrostatic interaction between the IM and MM regions by computing the electric field from the IM region and (2) the dispersion interaction between the two regions by assigning Lennard-Jones parameters to the IM atoms. [25] If we ignore the polarizability of the IM part, we can calculate the electric field based on atomic partial charges that are obtained by fitting to electrostatic potential map of the IM part. This simple idea, supplemented by additional tweaks for extending the simulation timescales such as adding bounding potentials for stabilizing trajectory integrations, [22] was shown to be quite satisfactory in reproducing spectroscopic features of a solvated chromophore [22] with quantitatively reliable excited state vibrational frequencies and good agreements in their dephasing timescales.…”
Section: Early Developments: Gas Phase Reactionsmentioning
confidence: 99%