30 research outputs found
Internal dynamics of the 3-Pyrroline-N-Oxide ring in spin-labeled proteins
Site-directed spin labeling is a versatile tool to study structure as well as dynamics of proteins using EPR spectroscopy. Methanethiosulfonate (MTS) spin labels tethered through a disulfide linkage to an engineered cysteine residue were used in a large number of studies to extract structural as well as dynamic information on the protein from the rotational dynamics of the nitroxide moiety. The ring itself was always considered to be a rigid body. In this contribution, we present a combination of high-resolution X-ray crystallography and EPR spectroscopy of spin-labeled protein single crystals demonstrating that the nitroxide ring inverts fast at ambient temperature while exhibiting nonplanar conformations at low temperature. We have used quantum chemical calculations to explore the potential energy that determines the ring dynamics as well as the impact of the geometry on the magnetic parameters probed by EPR spectroscopy
Redox-Dependent Structural Transformations of the [4Fe-3S] Proximal Cluster in O<sub>2</sub>âTolerant Membrane-Bound [NiFe]-Hydrogenase: A DFT Study
Broken-symmetry
density functional theory (BS-DFT) has been used to address the redox-dependent
structural changes of the proximal [4Fe-3S] cluster, implicated in
the O<sub>2</sub>-tolerance of membrane-bound [NiFe]-hydrogenase (MBH).
The recently determined structures of the [4Fe-3S] cluster together
with its protein ligands were studied at the reduced [4Fe-3S]<sup>3+</sup>, oxidized [4Fe-3S]<sup>4+</sup>, and superoxidized [4Fe-3S]<sup>5+</sup> levels in context of their relative energies and protonation
states. The observed proximal cluster conformational switch, concomitant
with the proton transfer from the cysteine Cys20 backbone amide to
the nearby glutamate Glu76 carboxylate, is found to be a single-step
process requiring âŒ12â17 kcal/mol activation energy
at the superoxidized [4Fe-3S]<sup>5+</sup> level. At the more reduced
[4Fe-3S]<sup>4+/3+</sup> oxidation levels, this rearrangement has
at least 5 kcal/mol higher activation barriers and prohibitively unfavorable
product energies. The reverse transformation of the proximal cluster
is a fast unidirectional process with âŒ8 kcal/mol activation
energy, triggered by one-electron reduction of the superoxidized species.
A previously discussed ambiguity of the Glu76 carboxylate and âspecialâ
Fe4 iron positions in the superoxidized cluster is now rationalized
as a superposition of two local minima, where Glu76-Fe4 coordination
is either present or absent. The calculated 12.3â17.9 MHz <sup>14</sup>N hyperfine coupling (HFC) for the Fe4-bound Cys20 backbone
nitrogen is in good agreement with the large 13.0/14.6 MHz <sup>14</sup>N couplings from the latest HYSCORE/ENDOR studies
Local Hybrid Functional Applicable to Weakly and Strongly Correlated Systems
The recent idea (WodynÌski, A.; Arbuznikov, A.
V.; Kaupp
M. J. Chem. Phys.2021,155, 144101) to augment local hybrid functionals by a strong-correlation
(sc) factor obtained from the adiabatic connection in the spirit of
the KP16 model has been extended and applied to generate the accurate
sc-corrected local hybrid functional scLH22t. By damping small values
of the ratio between nondynamical and dynamical correlation entering
the correction factor, it has become possible to avoid double counting
of nondynamical correlation for weakly correlated situations and thereby
preserve the excellent accuracy of the underlying LH20t local hybrid
for such cases almost perfectly. On the other hand, scLH22t improves
substantially over LH20t in reducing fractional-spin errors (FSEs),
in providing improved spin-restricted bond dissociation curves, and
in treating some typical systems with multireference character. The
obtained FSEs are similar to those of the KP16/B13 model and slightly
larger than for B13, but performance for weakly correlated systems
is better than for these two related methods, which are also difficult
to use self-consistently. The recent DM21 functional based on the
training of a deep neural network still performs somewhat better than
scLH22t but allows no physical insights into the origins of reduced
FSEs. Examination of local mixing functions (LMFs) for the corrected
scLH22t and uncorrected LH20t functionals provides further insights:
in weakly correlated situations, the LMF remains essentially unchanged.
Strong-correlation effects manifest in a reduction of the LMF values
in certain regions of space, even to the extent of producing negative
LMF values. It is suggested that this is the mechanism by which also
DM21, which may be viewed as a range-separated local hybrid, is able
to reduce FSEs
Quantum-Chemical Approach to NMR Chemical Shifts in Paramagnetic Solids Applied to LiFePO<sub>4</sub> and LiCoPO<sub>4</sub>
A novel
protocol to compute and analyze NMR chemical shifts for
extended paramagnetic solids, accounting comprehensively for Fermi-contact
(FC), pseudocontact (PC), and orbital shifts, is reported and applied
to the important lithium ion battery cathode materials LiFePO<sub>4</sub> and LiCoPO<sub>4</sub>. Using an EPR-parameter-based ansatz,
the approach combines periodic (hybrid) DFT computation of hyperfine
and orbital-shielding tensors with an incremental cluster model for
g- and zero-field-splitting (ZFS) D-tensors. The cluster model allows
the use of advanced multireference wave function methods (such as
CASSCF or NEVPT2). Application of this protocol shows that the <sup>7</sup>Li shifts in the high-voltage cathode material LiCoPO<sub>4</sub> are dominated by spinâorbit-induced PC contributions,
in contrast with previous assumptions, fundamentally changing interpretations
of the shifts in terms of covalency. PC contributions are smaller
for the <sup>7</sup>Li shifts of the related LiFePO<sub>4</sub>, where
FC and orbital shifts dominate. The <sup>31</sup>P shifts of both
materials finally are almost pure FC shifts. Nevertheless, large ZFS
contributions can give rise to non-Curie temperature dependences for
both <sup>7</sup>Li and <sup>31</sup>P shifts
Noncollinear Two-Component Quasirelativistic Description of Spin Interactions in Exchange-Coupled Systems. Mapping Generalized Broken-Symmetry States to Effective Spin Hamiltonians
We
provide a consistent mapping of noncollinear two-component quasirelativistic
DFT energies with appropriate orientations of localized spinor quantization
axes for multinuclear exchange-coupled transition-metal complexes
onto an uncoupled anisotropic effective spin Hamiltonian. This provides
access to the full exchange interaction tensor between the centers
of spin-coupled systems in a consistent way. The proposed methodology
may be best viewed as a generalized broken-symmetry density functional
theory approach (gBS-DFT). While the calculations provided are limited
to trinuclear systems ([M<sub>3</sub>OÂ(OOCH)<sub>6</sub>(H<sub>2</sub>O)<sub>3</sub>]<sup>+</sup>, where M = CrÂ(III), MnÂ(III), FeÂ(III))
with <i>C</i><sub>3</sub> symmetry, the method provides
a general framework that is extendable to arbitrary systems. It offers
an alternative to previous approaches to single-ion zero-field splittings,
and it provides access to the less often examined antisymmetric DzyaloshinskiiâMoriya
exchange interaction. Spinâorbit coupling is included self-consistently.
This will be of particular importance for complexes involving 4d or
5d transition metal centers or possibly also for f-block elements,
where a perturbational treatment of spinâorbit coupling may
not be valid anymore. While a comparison with experimental data was
indirect due to simplifications in the chosen model structures, the
agreement obtained indicates the essential soundness of the presented
approach
Four-Component Relativistic Density Functional Calculations of EPR Parameters for Model Complexes of Tungstoenzymes
For a closer validation
of four-component relativistic DFT methods
within the matrix DiracâKohnâSham (mDKS) framework with
global hybrid functionals for EPR parameter calculations to be applied
in the modeling of tungsten enzymes, we refine a previously suggested
protocol for computations on 5d systems. This is done for a series
of larger, unsymmetrical WÂ(V) complexes thought to closely resemble
enzyme active sites in this oxidation state. Particular focus is placed
on complexes with thiolate and dithiolene ligands, along with an evaluation
of the influence of different amounts of exact-exchange incorporated
in hybrid PBE0-<i>x</i>HF functionals, an implicit solvent
model, and structural changes on the computed EPR parameters. Compared
to previous work, a slightly modified protocol with different optimal
exact-exchange admixtures for electronic <i>g</i>- and hyperfine <i>A</i>-tensors is found to provide the best agreement with experimental
EPR data. It will provide the basis for our subsequent tungsten enzyme
modeling efforts
Validation of the Direct-COSMO-RS Solvent Model for DielsâAlder Reactions in Aqueous Solution
The
modeling of chemical reactions in protic solvents tends to
be far more computationally demanding than in most aprotic solvents,
where bulk solvent effects are well described by dielectric continuum
solvent models. In the presence of hydrogen bonds from a protic solvent
to reactants, transition states or intermediates, a faithful modeling
of the solvent effects usually requires some kind of molecular dynamics
treatment. In contrast, the COSMO-RS (conductor-like screening model
for real solvents) approach has been known for about a decade to describe
protic solvent effects much better than continuum solvents, in spite
of being an implicit solvent model without explicit molecular dynamics.
More recently, the self-consistent use of its potential in electronic-structure
methods has led to the Direct-COSMO-RS approach. It allows, for example,
structure optimization in the presence of a protic solvent, of solvent
mixtures, as well as self-consistent property calculations. In view
of recent successful tests for electron transfer in organic mixed-valence
systems, in this work the wider applicability of D-COSMO-RS for organic
reactivity is evaluated by computation of activation and reaction
free energies, as well as transition-state structures of two prototypical
DielsâAlder reactions, with an emphasis on aqueous solution.
D-COSMO-RS indeed provides substantial improvements over the COSMO
continuum model and in judicious testing compares well with embedded
supermolecular model cluster treatments, without prior knowledge about
the average numbers of hydrogen-bonding interactions present
Gauge effects in local hybrid functionals evaluated for weak interactions and the GMTKN30 test set
<p>The so-called âgauge problemâ, due to the non-uniqueness of exchange-energy densities, is a fundamental challenge for density functionals depending on these energy densities, such as local hybrid functionals. We have recently demonstrated how gauge effects influence the potential-energy curves of the argon dimer, and other quantities depending on ânon-physicalâ Pauli repulsions introduced by incompatible gauges of (semi-)local and exact-exchange energy densities . Introduction of suitable calibration functions depending only on semi-local quantities allowed to correct for these deficiencies and suggested ways to obtain more accurate local hybrid functionals beyond the local spin density approximation (LSDA) exchange-energy density. Here we extend the study of the gauge problem by comparing a number of uncalibrated and calibrated local hybrids for (1) the potential-energy curves of further noble-gas dimers and (2) for the entire GMTKN30 test set and its individual subsets. We find that DFT-D3 dispersion corrections fitted to be compatible with uncalibrated local hybrids have to correct not only for missing London dispersion but also for gauge artefacts that make weak interactions too repulsive. This burden is taken away when using properly calibrated local hybrids, which perform much better for dispersion-sensitive quantities already without D3 corrections, and which require only the physically relevant dispersion to be corrected for. The present results suggest directions for further improvement of calibration functions for local hybrids.</p
MVO-10: A Gas-Phase Oxide Benchmark for Localization/Delocalization in Mixed-Valence Systems
Ten
simple gas-phase, main-group as well as transition-metal, mixed-valence
(MV) oxo complexes are suggested for the screening of electronic-structure
methods for the computational study of localization vs delocalization
of charge and spin density in MV systems, without the usual added
complication of environmental effects. Benchmark coupled-cluster energies
up to CCSDTÂ(Q)/CBS (for Al<sub>2</sub>O<sub>4</sub><sup>â</sup>, Si<sub>2</sub>O<sub>4</sub><sup>+</sup>, Si<sub>2</sub>O<sub>4</sub><sup>â</sup>, ScO<sub>2</sub>, TiO<sub>2</sub><sup>+</sup>) and CCSDÂ(T)/CBS (for Ti<sub>2</sub>O<sub>4</sub><sup>â</sup>, Ti<sub>2</sub>O<sub>4</sub><sup>â</sup>, V<sub>2</sub>O<sub>4</sub><sup>+</sup>, Cr<sub>2</sub>O<sub>6</sub><sup>â</sup>) quality are provided as a basis for screening a variety of density-functional
methods, ranging from a generalized gradient approximation via global
and range-separated to local hybrid functionals. Additionally, experimental
evidence for a delocalized D<sub>2d</sub> structure of the somewhat
larger V<sub>4</sub>O<sub>10</sub><sup>â</sup> is used. None
of the functionals is fully satisfactory when tasked with describing
simultaneously the most extreme cases, the localized Al<sub>2</sub>O<sub>4</sub><sup>â</sup> and the delocalized V<sub>4</sub>O<sub>10</sub><sup>â</sup>. While relatively large exact-exchange
admixtures are required for the former, and for related localized
cases, lower ones are preferable for the latter, as well for other
delocalized d<sup>1</sup>d<sup>0</sup> systems. The overall best combined
performance is provided by a Lh-SVWN (gÂ(<b>r</b>) = 0.670 Ï<sub>W</sub>/Ï) local hybrid, the MN15 global hybrid, and the ÏB97X-D
range-separated hybrid. We also provide vibrational data for comparison
with experiment
Can Zinc Really Exist in Its Oxidation State +III?
Very recently, a thermochemically stable Zn<sup>III</sup> complex
has been predicted by Samanta and Jena (J. Am. Chem. Soc. 2012, 134, 8400â8403). In
contrast to their conclusions we show here by quantum chemical calculations
that (a) ZnÂ(AuF<sub>6</sub>)<sub>3</sub> is not a thermochemically
feasible compound, and (b) even if it could be made, it would not
represent a Zn<sup>III</sup> oxidation state by any valid definition