Fixed-charge phosphine ligands to explore gas-phase coinage metal-mediated decarboxylation reactions

2013 ◽  
Vol 42 (18) ◽  
pp. 6440 ◽  
Author(s):  
Krista Vikse ◽  
George N. Khairallah ◽  
J. Scott McIndoe ◽  
Richard A. J. O'Hair
Keyword(s):  
Gas Phase ◽  
Phosphine Ligands ◽  
Fixed Charge ◽  
Coinage Metal

Syntheses and Structures of d10 Coinage Metal Complexes of Electron-Accepting Phosphine Ligands Featuring a 3,3,4,4,5,5-Hexafluorocyclopentene Framework

2018 ◽  
Vol 57 (15) ◽  
pp. 9105-9114 ◽  
Author(s):  
Tomohiro Agou ◽  
Nao Wada ◽  
Kiyoshi Fujisawa ◽  
Takaaki Hosoya ◽  
Yoshiyuki Mizuhata ◽  
...  
Keyword(s):  
Metal Complexes ◽  
Phosphine Ligands ◽  
Coinage Metal

Keep it tight: a crucial role of bridging phosphine ligands in the design and optical properties of multinuclear coinage metal complexes

2021 ◽  
Author(s):  
Aleksandra V. Paderina ◽  
Igor O Koshevoy ◽  
Elena V. Grachova
Keyword(s):  
Optical Properties ◽  
Metal Complexes ◽  
Crucial Role ◽  
Phosphine Ligands ◽  
Bridging Ligands ◽  
Coinage Metal ◽  
Metal Interactions ◽  
Metal Metal ◽  
State 1

The copper subgroup metal ions in the oxidation state +1 are classical candidates for the aggregation via non-covalent metal–metal interactions, which are supported by a number of the bridging ligands....

Benchmarking Electronic Structure Methods for Accurate Fixed-Charge Electrostatic Models

2019 ◽  
Author(s):  
Alex Zhou ◽  
Michael Schauperl ◽  
Paul Nerenberg
Keyword(s):  
Electronic Structure ◽  
Gas Phase ◽  
Condensed Phase ◽  
Force Fields ◽  
Dipole Moments ◽  
Fixed Charge ◽  
Basis Set ◽  
Atomic Charges ◽  
Molecular Dipole ◽  
Partial Atomic Charges

<p>The accuracy of classical molecular mechanics (MM) force fields used for condensed phase molecular simulations depends strongly on the accuracy of modeling nonbonded interactions between atoms, such as electrostatic interactions. Some popular fixed-charge MM force fields use partial atomic charges derived from gas phase electronic structure calculations using the Hartree-Fock method with the relatively small 6-31G* basis set (HF/6-31G*). It is generally believed that HF/6-31G* generates fortuitously overpolarized electron distributions, as would be expected in the higher dielectric environment of the condensed phase. Using a benchmark set of 47 molecules we show that HF/6-31G* overpolarizes molecules by just under 10% on average with respect to experimental gas phase dipole moments. The overpolarization of this method/basis set combination varies significantly though and, in some cases, even leads to molecular dipole moments that are lower than experimental gas phase measurements. We further demonstrate that using computationally inexpensive density functional theory (DFT) methods, together with appropriate augmented basis sets and a continuum solvent model, can yield molecular dipole moments that are both more strongly and more uniformly overpolarized. These data suggest that these methods – or ones similar to them – should be adopted for the derivation of accurate partial atomic charges for next-generation MM force fields.<br></p>

Gas-phase propene epoxidation over coinage metal catalysts

2011 ◽  
Vol 38 (1) ◽  
pp. 1-24 ◽  
Author(s):  
Jiahui Huang ◽  
Masatake Haruta
Keyword(s):  
Gas Phase ◽  
Metal Catalysts ◽  
Coinage Metal

Benchmarking Electronic Structure Methods for Accurate Fixed-Charge Electrostatic Models

2019 ◽  
Author(s):  
Alex Zhou ◽  
Michael Schauperl ◽  
Paul Nerenberg
Keyword(s):  
Electronic Structure ◽  
Gas Phase ◽  
Condensed Phase ◽  
Force Fields ◽  
Dipole Moments ◽  
Fixed Charge ◽  
Basis Set ◽  
Atomic Charges ◽  
Molecular Dipole ◽  
Partial Atomic Charges

<p>The accuracy of classical molecular mechanics (MM) force fields used for condensed phase molecular simulations depends strongly on the accuracy of modeling nonbonded interactions between atoms, such as electrostatic interactions. Some popular fixed-charge MM force fields use partial atomic charges derived from gas phase electronic structure calculations using the Hartree-Fock method with the relatively small 6-31G* basis set (HF/6-31G*). It is generally believed that HF/6-31G* generates fortuitously overpolarized electron distributions, as would be expected in the higher dielectric environment of the condensed phase. Using a benchmark set of 47 molecules we show that HF/6-31G* overpolarizes molecules by just under 10% on average with respect to experimental gas phase dipole moments. The overpolarization of this method/basis set combination varies significantly though and, in some cases, even leads to molecular dipole moments that are lower than experimental gas phase measurements. We further demonstrate that using computationally inexpensive density functional theory (DFT) methods, together with appropriate augmented basis sets and a continuum solvent model, can yield molecular dipole moments that are both more strongly and more uniformly overpolarized. These data suggest that these methods – or ones similar to them – should be adopted for the derivation of accurate partial atomic charges for next-generation MM force fields.<br></p>

scholarly journals Coinage Metal–Sulfur Complexes: Stability on Metal(111) Surfaces and in the Gas Phase

2019 ◽  
Author(s):  
Jiyoung Lee ◽  
Theresa L. Windus ◽  
Patricia A. Thiel ◽  
James W. Evans ◽  
Da-Jiang Liu
Keyword(s):  
Gas Phase ◽  
Coinage Metal
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