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1 treated quantum mechanically, and 35 287, by molecular mechanics).
2 ill provide insight into their functions and molecular mechanics.
3 e size (R) using a proposed hybrid continuum-molecular mechanics.
4 e-grained molecular dynamics simulations and molecular mechanics.
5 identified using a rapid algorithm based on molecular mechanics.
6 ts, because they create flows that alter the molecular mechanics.
8 ime-dependent UV-vis spectroscopy, HPLC, and molecular mechanics analyses revealed an atypical therma
9 in line with excited-state quantum mechanics/molecular mechanics and classical molecular dynamics sim
10 ering method along with optimizations at the molecular mechanics and density functional M06-2X levels
13 iments and theoretically by a combination of molecular mechanics and electronic structure calculation
14 wledge-based scoring functions, and MM-GBSA (molecular mechanics and generalized Born surface area),
21 eved using in vacuo energy minimization with molecular mechanics and statistically derived continuous
22 on (XRD) and computational modeling based on molecular mechanics and two-dimensional XRD simulations
24 solvent molecular dynamics, implicit solvent molecular mechanics, and quantum mechanics with a self-c
25 m force field is a suitable tool for various molecular mechanics applications on large macromolecular
27 tide bond using a combined quantum mechanics/molecular mechanics approach together with adaptive umbr
28 ructure and using a hybrid quantum mechanics/molecular mechanics approach, we investigate the pathway
29 te this reaction step by a quantum-mechanics/molecular-mechanics approach in combination with molecul
30 mechanisms that cannot be captured under the molecular mechanics approximations, and which therefore
31 ular dynamics simulations using ligand-field molecular mechanics are performed to elucidate, for the
32 Thermodynamic values were reproduced using molecular mechanics augmented by ab initio calculations
34 rotocol consists of hybrid quantum mechanics-molecular mechanics-based high temperature Langevin mole
38 oach involves the following steps: (i) using molecular mechanics calculations (with, e.g., MacroModel
43 ecular dynamics and hybrid quantum mechanics/molecular mechanics calculations at the mPW1N/6-311+G(2d
44 e developed a coarse-grained force field for molecular mechanics calculations based on the virtual in
46 ical force field-based and quantum mechanics/molecular mechanics calculations for modeling the nucleo
50 r dynamics simulations and quantum mechanics/molecular mechanics calculations indicated that, for the
51 equirements from ab initio quantum mechanics/molecular mechanics calculations of activation free ener
53 nes in the R series and also on the basis of molecular mechanics calculations performed on the entire
58 g, molecular dynamics, and excitonic quantum/molecular mechanics calculations to examine and rational
59 nctional theory and hybrid quantum mechanics/molecular mechanics calculations to investigate this rea
60 ve survey of the potential energy surface by molecular mechanics calculations using AMBER has provide
62 sotropic displacement parameters (ADPs), and molecular mechanics calculations were used to analyze th
63 ectroscopy, X-ray crystallography, classical molecular mechanics calculations, and normal-coordinate
66 d-flow, rapid-quench flow, quantum/mechanics molecular mechanics calculations, crystallography, and d
67 died by X-ray crystal structure analysis and molecular mechanics calculations, including docking of t
68 computational methods, including docking and molecular mechanics calculations, we have been able to c
69 In the present work, using quantum mechanics/molecular mechanics calculations, we investigate the ele
70 cs simulations, and mixed quantum mechanical/molecular mechanics calculations, yielding a comprehensi
86 ndent forces with efficiencies comparable to molecular-mechanics calculations on the solute alone; as
89 solution were elucidated by combined NMR and molecular mechanics computational techniques, showing th
91 tion of distance constraint information into molecular mechanics conformational searches can be used
93 Boltzmann-weighted probabilities from these molecular mechanics energies compare well with database-
94 , we describe the first tests of the ROSETTA molecular mechanics energy function in the context of ol
96 arious continuum components are derived from molecular-mechanics energy calculations using the CHARMM
97 Design provides a new avenue for testing molecular-mechanics energy functions, and future improve
98 ssively methyl-substituted systems by use of molecular mechanics estimates of differences in strain b
99 re was used for a combined quantum mechanics/molecular mechanics exploration of the reaction mechanis
103 tential multipole moment (EPMM) or classical molecular mechanics force field single-point partial cha
104 Here, we examine the extent to which the molecular mechanics force field used in such simulations
106 next-generation method for the validation of molecular mechanics force fields and chemical shift pred
107 development of the most recent generation of molecular mechanics force fields promises an increasingl
109 to test the ability of a variety of popular molecular mechanics force fields to maintain the native
110 highly relevant for the parameterization of molecular mechanics force fields which form the basis of
112 classical as well as mixed quantum mechanics molecular mechanics force fields, we uncover a possible
116 e (WT) ecDHFR using hybrid quantum mechanics-molecular mechanics free energy simulations with the Met
118 dynamics simulations and binding free energy molecular mechanics-generalized born surface area (MM-GB
120 omputation of interaction energies using the Molecular Mechanics-Generalized Born Surface Area (MM-GB
122 ng free-energy changes, calculated using the molecular mechanics-generalized Born surface area techni
124 rmed using a similarity filter, docking, and molecular mechanics-generalized Born/surface area postpr
125 fts obtained in single point calculations on molecular mechanics geometries without computationally e
126 lly inexpensive single-point calculations on molecular mechanics geometries without time-consuming ab
127 ecular dynamics and hybrid quantum mechanics/molecular mechanics have been used to investigate the me
134 sition state, we performed quantum mechanics/molecular mechanics metadynamics simulations of the glyc
135 d demonstrate, by means of quantum mechanics/molecular mechanics metadynamics simulations, that it is
136 the results from a hybrid quantum mechanics/molecular mechanics method (SORCI+Q//B3LYP/6-31G*:Amber)
138 wn N-layer integrated molecular orbital plus molecular mechanics) method, we report a comprehensive t
139 nstrate that computational quantum mechanics/molecular mechanics methods can provide reasonable value
140 Cr(N=C-t-Bu(2))(4) using density functional/molecular mechanics methods confirmed the qualitative an
141 theoretical framework to combine quantum and molecular mechanics methods, and compute the effect of m
144 cular mechanics package) (quantum mechanical:molecular mechanics) methods to calculate FTIR differenc
145 is determined using X-ray diffraction (XRD), molecular mechanics (MM) and molecular dynamics (MD) sim
146 with imprinted cavities were simulated with molecular mechanics (MM) and molecular dynamics (MD).
147 of these threonine residues with the use of molecular mechanics (MM) and quantum mechanics/molecular
148 tional studies of nucleic acids have applied Molecular Mechanics (MM) approaches using simple pairwis
149 ds that employ quantum mechanics (QM) and/or molecular mechanics (MM) energy calculations to identify
153 oyed QM (density functional theory and MP2), molecular mechanics (MM), and molecular dynamics (MD) me
154 on step, a computational analysis, including molecular mechanics (MMFF94) and semiempirical AM1 geome
159 bation theory to construct quantum-mechanics/molecular-mechanics models of Az48W(*) and ReAz108W(*) c
161 bsorption measurements and quantum mechanics/molecular mechanics molecular dynamics simulations allow
162 called GlmU through hybrid quantum mechanics-molecular mechanics molecular dynamics simulations and f
163 n the context of ab initio quantum mechanics/molecular mechanics molecular dynamics, we examined cert
164 loying ab initio QM/MM-MD (Quantum Mechanics/Molecular Mechanics-Molecular Dynamics) simulations with
166 The interactions among these enzymes and the molecular mechanics of how separation occurs without lys
167 ntitative systems platform that utilizes the molecular mechanics of ion transport, metabolism, and si
168 Our findings provide new insights into the molecular mechanics of mammalian miRNA-mediated gene sil
170 isms of nociception and thermosensation, the molecular mechanics of these ion channels are still larg
171 step toward a detailed understanding of the molecular mechanics of this important signal transductio
173 or a theoretical analysis (quantum mechanics/molecular mechanics) of the mechanism of chemistry witho
174 l methods (ligand docking, quantum mechanics/molecular mechanics optimization, and molecular dynamic
175 own N-layered integrated molecular Orbital + Molecular mechanics package) (quantum mechanical:molecul
177 tive stabilities of the interfaces using the molecular mechanics Poisson-Boltzmann solvent accessible
184 o investigate the sensitivity of the popular molecular mechanics Poisson-Boltzmann surface area (MMPB
185 rmation, we employed two additional methods: Molecular Mechanics Poisson-Boltzmann Surface Area (MMPB
186 intermediate has been characterized using a molecular mechanics Poisson-Boltzmann surface area appro
187 Computational alanine scanning using the molecular mechanics Poisson-Boltzmann surface area metho
188 molecular dynamic simulations combined with Molecular Mechanics-Poisson Boltzmann Surface Area calcu
189 mation rigid docking, solvation docking, and molecular mechanics-Poisson-Boltzmann/surface area (MM-P
191 ute binding free energies were calculated by molecular mechanics/Poisson-Boltzmann surface area (MM/
192 extensive molecular dynamics simulations and molecular mechanics/Poisson-Boltzmann surface area (MM/P
193 igands into a sigma(1) 3D homology model via molecular mechanics/Poisson-Boltzmann surface area calcu
194 evelopment of a CHARMM (Chemistry at Harvard Molecular Mechanics) polarizable force field for simulat
197 and and the 10 primary contact residues, the molecular-mechanics potential is used to redesign a ribo
198 ion method and show that, of the traditional molecular mechanics potentials tested, only one showed a
202 We performed a detailed quantum mechanics/molecular mechanics (QM/MM) and molecular dynamics (MD)
203 ite 8-oxoguanine using the quantum mechanics/molecular mechanics (QM/MM) approach, both from a chemis
211 MD) simulations and hybrid quantum mechanics/molecular mechanics (QM/MM) calculations have been carri
212 MD) simulations and hybrid quantum mechanics/molecular mechanics (QM/MM) calculations have been carri
213 actions were modeled using mixed quantum and molecular mechanics (QM/MM) calculations in the context
214 ctional theory (DFT)-based quantum mechanics/molecular mechanics (QM/MM) calculations of the crystals
215 mics (MD) simulations and quantum-mechanical/molecular mechanics (QM/MM) calculations of the fatty ac
216 unctional theory (DFT) and quantum mechanics/molecular mechanics (QM/MM) calculations on the full enz
218 ) simulations and combined quantum mechanics/molecular mechanics (QM/MM) calculations to elucidate th
219 expensive and specialized quantum mechanics/molecular mechanics (QM/MM) calculations to provide a qu
220 ntegration, and high-level quantum mechanics/molecular mechanics (QM/MM) calculations to study the po
221 variation of selectivity, mixed quantum and molecular mechanics (QM/MM) calculations were carried ou
222 Density functional-based quantum mechanics/molecular mechanics (QM/MM) calculations, employing a mo
228 DNA dodecamer by means of quantum mechanics/molecular mechanics (QM/MM) Car-Parrinello simulations.
230 aracterized at the uniform quantum mechanics/molecular mechanics (QM/MM) computational level using de
231 lecular mechanics (MM) and quantum mechanics/molecular mechanics (QM/MM) computational methods and pu
232 D) simulations, in a mixed quantum mechanics/molecular mechanics (QM/MM) framework, to investigate th
233 se (RNase) H1 using hybrid quantum-mechanics/molecular mechanics (QM/MM) free energy calculations.
235 ording to state-of-the-art quantum mechanics/molecular mechanics (QM/MM) hybrid methods, in conjuncti
240 x geometry by combined quantum mechanics and molecular mechanics (QM/MM) methods, (3) conformational
241 hods in concert with mixed quantum mechanics/molecular mechanics (QM/MM) methods, the hydroxylation o
243 R pK(a) determination with quantum mechanics/molecular mechanics (QM/MM) modeling to study engineered
244 application of hybrid quantum mechanics and molecular mechanics (QM/MM) models is an important appro
245 quantum mechanics (QM) and quantum mechanics/molecular mechanics (QM/MM) models of the UDG active sit
247 eaction carried out in and quantum mechanics/molecular mechanics (QM/MM) simulation, we show that the
249 demonstrated by the hybrid quantum mechanics/molecular mechanics (QM/MM) simulations of light-harvest
250 cs calculations and hybrid quantum mechanics/molecular mechanics (QM/MM) simulations to model a varie
251 onance (EPR) spectroscopy, quantum mechanics/molecular mechanics (QM/MM) simulations, kinetic studies
254 gstrom resolution and used quantum mechanics/molecular mechanics (QM/MM) to investigate its reaction
255 y correlation behavior and quantum mechanics/molecular mechanics (QM/MM) trajectories point to a domi
259 edded PSII with high-level quantum-mechanics/molecular-mechanics (QM/MM) calculations of individual a
260 n n-layered integrated molecular orbital and molecular mechanics(quantum mechanics:quantum mechanics'
262 calculated with a finite cluster model using molecular mechanics revealed a symmetric but nonsinusoid
263 ectroscopy and restrained molecular dynamics/molecular mechanics (rMD/MM) calculations using 179 NOE
265 es and non-adiabatic mixed quantum mechanics/molecular mechanics simulations in the phthalocyanine-fu
266 on is analyzed by means of quantum mechanics/molecular mechanics simulations including solvent effect
267 Our results are pertinent to quantum and molecular mechanics simulations of ligands bound to GPCR
271 , we carried out extensive quantum mechanics/molecular mechanics simulations to calculate stepwise he
272 e density functional theory calculations and molecular mechanics simulations to estimate the strength
274 al models by combining quantum mechanics and molecular mechanics simulations with time-resolved Fouri
275 n of experimental results, quantum mechanics/molecular mechanics simulations, and theoretical analyse
276 Ion mobility measurements, combined with molecular mechanics simulations, are used to study enant
284 g software, HostDesigner, is interfaced with molecular mechanics software, GMMX, providing a tool for
285 g software, HostDesigner, is interfaced with molecular mechanics software, GMMX, providing a tool for
286 In this work we present a quantum mechanics/molecular mechanics study into the mechanism of sulfoxid
287 We report a hybrid density functional theory-molecular mechanics study of the mechanism of the additi
288 e the basis for a detailed quantum mechanics/molecular mechanics study of the path for the complete t
289 Combining accurate mixed quantum mechanics/molecular mechanics techniques and protein structure pre
290 tent-charge density functional tight binding/molecular mechanics, the bond lengths in the concerted m
292 ecular dynamics and hybrid quantum mechanics/molecular mechanics to analyze sequence context-dependen
294 ent-charge density-functional tight binding)/molecular mechanics, umbrella sampling, and the weighted
297 onal theory and multiscale quantum mechanics/molecular mechanics, we report C-terminal cleavage react
298 mics simulation and hybrid quantum mechanics/molecular mechanics, we show that ferric peroxo addition
300 e apply a high-throughput formulation of the molecular mechanics with Poisson-Boltzmann surface area