159 research outputs found
MCPB.py: A Python Based Metal Center Parameter Builder
MCPB.py,
a python based metal center parameter builder, has been
developed to build force fields for the simulation of metal complexes
employing the bonded model approach. It has an optimized code structure,
with far fewer required steps than the previous developed MCPB program.
It supports various AMBER force fields and more than 80 metal ions.
A series of parametrization schemes to derive force constants and
charge parameters are available within the program. We give two examples
(one metalloprotein example and one organometallic compound example),
indicating the program’s ability to build reliable force fields
for different metal ion containing complexes. The original version
was released with AmberTools15. It is provided via the GNU General
Public License v3.0 (GNU_GPL_v3) agreement and is free to download
and distribute. MCPB.py provides a bridge between quantum mechanical
calculations and molecular dynamics simulation software packages thereby
enabling the modeling of metal ion centers. It offers an entry into
simulating metal ions in a number of situations by providing an efficient
way for researchers to handle the vagaries and difficulties associated
with metal ion modeling
Taking into Account the Ion-Induced Dipole Interaction in the Nonbonded Model of Ions
Metal
ions exist in almost half of the proteins in the protein
databank, and they serve as structural, electron-transfer, and catalytic
elements in the metabolic processes of organisms. Molecular dynamics
(MD) simulation is a powerful tool that provides information about
biomolecular systems at the atomic level. Coupled with the growth
in computing power, algorithms like the particle mesh Ewald (PME)
method have become the accepted standard when dealing with long-range
interactions in MD simulations. The nonbonded model of metal ions
consists of an electrostatic plus 12–6 Lennard-Jones (LJ) potential
and is used largely because of its speed relative to more accurate
models. In previous work we found that ideal parameters do not exist
that reproduce several experimental properties for MÂ(II) ions simultaneously
using the nonbonded model coupled with the PME method due to the underestimation
of metal ion-ligand interactions. Via a consideration of the nature
of the nonbonded model, we proposed that the observed error largely
arises from overlooking charge-induced dipole interactions. The electrostatic
plus 12–6 LJ potential model works reasonably well for neutral
systems but does struggle with more highly charged systems. In the
present work we designed and parametrized a new nonbonded model for
metal ions by adding a 1/<i>r</i><sup>4</sup> term to the
12–6 model. We call it the 12–6–4 LJ-type nonbonded
model due to its mathematical construction. Parameters were determined
for 16 +2 metal ions for the TIP3P, SPC/E, and TIP4P<sub>EW</sub> water
models. The final parameters reproduce the experimental hydration
free energies (HFE), ion-oxygen distances (IOD) in the first solvation
shell, and coordination numbers (CN) accurately for most of the metal
ions investigated. Preliminary tests on MgCl<sub>2</sub> at different
concentrations in aqueous solution and Mg<sup>2+</sup>–nucleic
acid systems show reasonable results suggesting that the present parameters
can work in mixed systems. The 12–6–4 LJ-type nonbonded
model is readily adopted into standard force fields like AMBER, CHARMM,
and OPLS-AA with only a modest computational overhead. The new nonbonded
model does not consider charge-transfer effects explicitly and, hence,
may not be suitable for the simulation of systems where charge-transfer
effects play a decisive role
Organocatalytic Enantioselective [1 + 4] Annulation of Morita–Baylis–Hillman Carbonates with Electron-Deficient Olefins: Access to Chiral 2,3-Dihydrofuran Derivatives
A reaction has been developed for
the chiral phosphine-catalyzed enantioselective [1 + 4] annulation
of Morita–Baylis–Hillman carbonates with electron-deficient
olefins via a Michael alkylation process. Morita–Baylis–Hillman
carbonates reacted smoothly with β,γ-unsaturated α-keto
ester and α,β-unsaturated ketone substrates under 1,2-bisÂ[(2<i>R</i>,5<i>R</i>)-2,5-dimethylphospholano]Âbenzene monoxide
catalysis to furnish a wide range of optically active 2,3-dihydrofurans
in high yields (up to 95%) with excellent asymmetric induction (up
to >99% ee, >20:1 dr). This protocol represents an efficient
strategy for the synthesis of optically active multifunctional 2,3-dihydrofurans
via an asymmetric Michael alkylation domino reaction
3‑Center-5-Electron Boryl Radicals with σ<sup>0</sup>π<sup>1</sup> Ground State Electronic Structure
Five-
and six-membered boron heterocycle-based three-center-five-electron
(<b>3c</b>–<b>5e</b>) type boryl radicals with
unusual σ<sup>0</sup>π<sup>1</sup> ground state electronic
structures are predicted theoretically. Compared to σ<sup>1</sup>π<sup>0</sup> analogs, their unique electronic structure leads
to both lower reactivity toward H-atoms and stronger coordination
with Lewis bases. The corresponding Lewis base-stabilized four-center-seven-electron
(<b>4c</b>–<b>7e</b>) type boryl radicals are even
more unreactive toward H-atoms than the conventional <b>4c</b>–<b>7e</b> ones
Double N,B-Type Bidentate Boryl Ligands Enabling a Highly Active Iridium Catalyst for C–H Borylation
Boryl
ligands hold promise in catalysis due to their very high
electron-donating property. In this communication double N,B-type
boryl anions were designed as bidentate ligands to promote an sp<sup>2</sup> C–H borylation reaction. A symmetric pyridine-containing
tetraaminoÂdiborane(4) compound (<b>1</b>) was readily
prepared as the ligand precursor that could be used, in combination
with [IrÂ(OMe)Â(COD)]<sub>2</sub>, to <i>in situ</i> generate
a highly active catalyst for a broad range of (hetero)Âarene substrates
including highly electron-rich and/or sterically hindered ones. This
work provides the first example of a bidentate boryl ligand in supporting
homogeneous organometallic catalysis
Copper-Catalyzed Boron-Selective C(sp<sup>2</sup>)–C(sp<sup>3</sup>) Oxidative Cross-Coupling of Arylboronic Acids and Alkyltrifluoroborates Involving a Single-Electron Transmetalation Process
A rapid and highly selective oxidative
cross-coupling reaction
between readily available and shelf-stable arylboronic acids and primary
or secondary potassium alkyltrifluoroborates was devised and developed,
which works under mild conditions using copperÂ(II) acetate as the
catalyst and silver oxide as the oxidant. Initial experimental results
indicate that a single-electron transmetalation process is involved.
This approach effectively bypasses the problems associated with the
traditional cross-coupling reactions of alkylboronates and thus provides
a complementary method in building CÂ(sp<sup>2</sup>)–CÂ(sp<sup>3</sup>) bonds
Stereocontrolled Construction of the Tricyclic Framework of Tiglianes and Daphnanes by an Oxidative Dearomatization Approach
An appropriately functionalized [5–7–6]
tricyclic
framework of tigliane and daphnane diterpenes containing seven contiguous
stereocenters has been prepared in 10 steps from very simple building
blocks in a modular and stereocontrolled fashion. The key features
of this approach involve an efficient visible light-induced singlet
oxygen oxidative dearomatization and an array of substrate-controlled
highly diastereoselective transformations. This work provides a model
strategy for rapid and diverted synthesis of natural and unnatural
molecules sharing the common skeleton
Computational Analysis of Stable Hard Structures in the Ti–B System
The lowest energy
crystalline structures of various stoichiometric titanium boride (Ti–B)
intermetallic compounds are sought based on density functional theory
combined with the particle-swarm optimization (PSO) technique. Besides
three established experimental structures, i.e., FeB-type TiB, AlB<sub>2</sub>-type, and Ta<sub>3</sub>B<sub>4</sub>-type Ti<sub>3</sub>B<sub>4</sub>, we predict additional six metastable phases at these
stoichiometric ratios, namely, α- and β-phases for TiB,
TiB<sub>2</sub>, and Ti<sub>3</sub>B<sub>4</sub>, respectively. Moreover,
we predict the most stable crystalline structures of four new titanium
boride compounds with different stoichiometric ratios: Ti<sub>2</sub>B–PS<sub>A</sub>, Ti<sub>2</sub>B<sub>3</sub>–PS<sub>B</sub>, TiB<sub>3</sub>–PS<sub>C</sub>, and TiB<sub>4</sub>–PS<sub>D</sub>. Notably, Ti<sub>2</sub>B–PS<sub>A</sub> is shown to have lower formation energy (thus higher stability)
than the previously proposed Al<sub>2</sub>Cu-type Ti<sub>2</sub>B.
The computed convex-hull and phonon dispersion relations confirm that
all the newly predicted Ti–B intermetallic crystals are thermodynamically
and dynamically stable. Remarkably, the predicted α-TiB<sub>2</sub> and β-TiB<sub>2</sub> show semi-metal-like electronic
properties and possess high Vickers hardnesses (39.4 and 39.6 GPa),
very close to the lower limit of <i>superhard materials</i> (40 GPa). Analyses of band structure, density of states, electronic
localization function, and various elastic moduli provide further
understanding of the electronic and mechanical properties of the intermetallic
titanium borides. We hope the newly predicted hard intermetallic titanium
borides coupled with desirable electronic properties and high elastic
modulus will motivate future experimental synthesis for applications
such as high-temperature structural materials
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