2 research outputs found
A Direct, Quantitative Connection between Molecular Dynamics Simulations and Vibrational Probe Line Shapes
A quantitative
connection between molecular dynamics simulations
and vibrational spectroscopy of probe-labeled systems would enable
direct translation of experimental data into structural and dynamical
information. To constitute this connection, all-atom molecular dynamics
(MD) simulations were performed for two SCN probe sites (solvent-exposed
and buried) in a calmodulin-target peptide complex. Two frequency
calculation approaches with substantial nonelectrostatic components,
a quantum mechanics/molecular mechanics (QM/MM)-based technique and
a solvatochromic fragment potential (SolEFP) approach, were used to
simulate the infrared probe line shapes. While QM/MM results disagreed
with experiment, SolEFP results matched experimental frequencies and
line shapes and revealed the physical and dynamic bases for the observed
spectroscopic behavior. The main determinant of the CN probe frequency
is the exchange repulsion between the probe and its local structural
neighbors, and there is a clear dynamic explanation for the relatively
broad probe line shape observed at the “buried” probe
site. This methodology should be widely applicable to vibrational
probes in many environments
Overcoming the Failure of Correlation for Out-of-Plane Motions in a Simple Aromatic: Rovibrational Quantum Chemical Analysis of <i>c</i>‑C<sub>3</sub>H<sub>2</sub>
Truncated,
correlated, wave function methods either produce imaginary
frequencies (in the extreme case) or nonphysically low frequencies
in out-of-plane motions for carbon and adjacent atoms when the carbon
atoms engage in π bonding. Cyclopropenylidene is viewed as the
simplest aromatic hydrocarbon, and the present as well as previous
theoretical studies have shown that this simple molecule exhibits
this behavior in the two out-of-plane bends (OPBs). This nonphysical
behavior has been treated by removing nearly linear dependent basis
functions according to eigenvalues of the overlap matrix, by employing
basis sets where the <i>spd</i> space saturatation is balanced
with higher angular momentum functions, by including basis set superposition/incompleteness
error (BSSE/BSIE) corrections, or by combining standard correlation
methods with explicitly correlated methods to produce hybrid potential
surfaces. However, this work supports the recently described hypothesis
that the OPB problem is both a method and a basis set effect. The
correlated wave function’s largest higher-order substitution
term comes from a π → π* excitation where constructive
interference of both orbitals artificially stabilizes the OPB. By
employing schema to overcome this issue, the symmetric OPB ν<sub>9</sub> is the predicted to be the second-brightest transition, and
it will be observed very close to 775 cm<sup>–1</sup>. However,
more work from the community is required to formulate better how carbon
atoms interact with their adjacent atoms in π-bonded systems.
Such bonds are ubiquitous in all of chemistry and beyond