戻る
「早戻しボタン」を押すと検索画面に戻ります。

今後説明を表示しない

[OK]

コーパス検索結果 (1語後でソート)

通し番号をクリックするとPubMedの該当ページを表示します
1 -) and theoretically by investigation of its electronic structure.
2 ly sensitive to changes in the excited-state electronic structure.
3 tic BaMnSb2 is a 3D Weyl semimetal with a 2D electronic structure.
4 harge compensation and hence a change in the electronic structure.
5 ntion though the years, largely due to their electronic structure.
6 s confirmed by computational modeling of the electronic structure.
7 polymer series differing in architecture and electronic structure.
8 dical but will have a classical closed-shell electronic structure.
9 u-(Mes)PDI(Me)) (3-(t)Bu), displays the same electronic structure.
10 rom 2 h to over 20 days without altering its electronic structure.
11  selectivity without a drastic alteration of electronic structure.
12 QD but also, in some cases, its ground state electronic structure.
13 orption spectroscopy demonstrate a change in electronic structure.
14  provide access to materials with engineered electronic structure.
15 y the lack of knowledge about the low-energy electronic structure.
16 ls of high electrical conductivity and of 1D electronic structure.
17 e effect of subtle ligand flexibility on the electronic structure.
18 al and interfacial complexity in determining electronic structure.
19 ring properties associated with the modified electronic structure.
20 ted with the local active site geometric and electronic structure.
21 actors responsible for the tunability of MOF electronic structures.
22 lexes and provide further insight into their electronic structures.
23 n of these molecules and their corresponding electronic structures.
24 P compounds as verified by analyses of their electronic structures.
25 been interest in understanding their diverse electronic structures.
26  the characterization of their molecular and electronic structures.
27 ionship between the morphology evolution and electronic structures.
28 nt of hybrid porous materials with desirable electronic structures.
29 n experimentally defining highly delocalized electronic structures.
30 se materials possess significantly different electronic structures.
31 es that are nearly identical in diameter and electronic structure, (6,5)- and (7,3)-SWCNTs, we are ab
32  bonds, while xenon possesses a closed-shell electronic structure: a direct consequence of which rend
33 cal account of the interrelation between MHP electronic structure, absorption, emission, carrier dyna
34                         The evolution of the electronic structure across the transition reveals the r
35         Here we show the real space image of electronic structures across the bilayer-monolayer inter
36                                        These electronic structure-activity relations provide a promis
37  a combination of varying steric demands and electronic structure among the different anchor groups.
38                  Here we demonstrate a novel electronic structure analysis technique that predicts an
39  first-principles microkinetic modeling, and electronic structure analysis to elucidate the metal/met
40  = Bi, Sb, As, and P) using first principles electronic structure and Boltzmann transport calculation
41 e our understanding of the spatially varying electronic structure and bonding in ceria-based nanopart
42                                          The electronic structure and charge distribution of this mol
43 these connections and discusses the bonding, electronic structure and chemical transformations at nan
44 itations of conventional XAS to identify the electronic structure and coordination environment of met
45 e trilayer nickelate La4Ni3O10 revealing its electronic structure and correlations, finding strong re
46 s dictates the properties as they pertain to electronic structure and defect tolerance.
47 that the Stokes shift is intrinsic to the NC electronic structure and does not arise from extrinsic e
48 bridge, which may increase the tunability of electronic structure and film morphology.
49 rption states are described in terms of both electronic structure and geometry.
50 oscopy, we map the spin-polarized unoccupied electronic structure and identify a surface resonance wh
51 -chemical calculations, the orbital-specific electronic structure and its ultrafast dynamics accessed
52                                          The electronic structure and metal-metal bonding of 2, 6, 8,
53 fferences in the electron transfer rate with electronic structure and morphology, achieved with sub-2
54                                          The electronic structure and optical spectrum of Ag67 were c
55              Theory is combined to probe the electronic structure and orbitals responsible for the bo
56 ties of La(1-x)Sr(x)CoO(3-delta) through the electronic structure and participation of lattice oxygen
57 ies yielded information about the unoccupied electronic structure and postexcitation relaxation behav
58 2-) in ZnO brings about major changes in the electronic structure and properties, the composition, ev
59 troelectrochemical experiments elucidate the electronic structure and redox thermodynamics of Ni-only
60 tion plays a role in determining the surface electronic structure and semiconducting properties of hy
61 @C80 at Gd N 4,5-edges to directly study the electronic structure and spin flip excitations of Gd 4f
62               Combined with state-of-the-art electronic structure and statistical calculations, the r
63 rovides a detailed account of the synthesis, electronic structure and stoichiometric reactivity of di
64  the cooperative interplay between molecular electronic structure and strong electron correlations pl
65 r mechanics calculations, we investigate the electronic structure and the dynamics of the P(D1)P(D2)
66  the synergistic effects of Ag and In on the electronic structure and the improved electrical transpo
67 om phase approximation calculation using the electronic structure and the momentum dependence of the
68    DFT and TD-DFT calculations elucidate the electronic structure and the photophysical behavior.
69 analogues based on a detailed study of their electronic structure and the pseudo Jahn-Teller effect (
70                   Calculations of the ribbon electronic structure and theoretical transport studies s
71 hrene ligand, which drastically modifies the electronic structure and tunes the stability of the Pd(I
72  we implement sparse sampling to capture the electronic structure and ultrafast dynamics of molecular
73 NRs and heterostructures, we introduce their electronic structures and dynamics of exciton and carrie
74 tional theory provides a rich picture of the electronic structures and dynamics of these biomolecules
75 's perimeter model, to analyze trends in the electronic structures and optical properties of expanded
76                                Trends in the electronic structures and optical properties of isomeric
77 ew cations are used to probe their molecular electronic structures and optical properties.
78 fect types can generate greatly varied local electronic structures and that the formation energies an
79                Surface chemical composition, electronic structure, and bonding characteristics determ
80 /Ru catalyst is attributed to changes in the electronic structure, and thus the altered adsorption pr
81 cuprates leads to significant changes in the electronic structure, and was later found to be accompan
82 to their high specific surface areas, exotic electronic structures, and fascinating physical and chem
83 r vacancies for metal-insulator transitions, electronic structures, and introducing magnetism in non-
84 pectroscopic characterisation, molecular and electronic structures, and properties of these intriguin
85          We show that this transient valence electronic structure arises within 60 +/- 20 fs after ul
86            The material has an unprecedented electronic structure arising from its ultrathin walls.
87 ectroscopy data also shows the change in the electronic structure around 12 GPa.
88 xplained by the evolution of the crystal and electronic structure as a function of the sulfur content
89  is the much wider prevalence of noninnocent electronic structures as well as full-fledged corrole(*2
90 of a first complete study of the crystal and electronic structures as well as of properties of a stab
91 ects of intrinsic changes in the flavin ring electronic structure, as well as perturbations in the ap
92 be exploited as probes of distortions in the electronic structure at the nanoscale.
93 ces requires a detailed understanding of the electronic structure at this interface; however, this un
94 ed kinetic isotope effects and corresponding electronic-structure-based transition-state theory calcu
95  replacement given its electron mobility and electronic structure, but LBSO cannot be synthesized as
96 mance, such that detailed calculations using electronic structure calculations (e.g., density functio
97                                              Electronic structure calculations agree with the experim
98                                          The electronic structure calculations also demonstrate that
99 eference data obtained from state-of-the-art electronic structure calculations and experimental measu
100  scale Density Functional Theory (DFT) based electronic structure calculations are highly time consum
101                                              Electronic structure calculations are playing an increas
102      Here, we report results from high-level electronic structure calculations as well as both classi
103                 First-principles theoretical electronic structure calculations confirm the experiment
104                                              Electronic structure calculations correlated to experime
105                                              Electronic structure calculations indicate that beta-GeS
106 ation, structure-property relationships, and electronic structure calculations on two new DUV NLO mat
107 of exohedral fullerenes without the need for electronic structure calculations or geometry optimizati
108 erimental spectra are in good agreement with electronic structure calculations performed with Dynamic
109                                    Ab initio electronic structure calculations reveal that the VCMA o
110  approximately 2.30 A) reported to date, and electronic structure calculations show some degree of mu
111                                              Electronic structure calculations suggest that the O2 ad
112 ic molecular systems.Machine learning allows electronic structure calculations to access larger syste
113 edge X-ray absorption spectroscopy (XAS) and electronic structure calculations to quantify the extent
114             The findings are rationalized by electronic structure calculations using density function
115                       Green's function based electronic structure calculations were carried out in or
116 Ca(+) These methods, augmented by high-level electronic structure calculations, permit detailed inves
117 scopy, electrical transport measurements and electronic structure calculations, we demonstrate that t
118 spectroscopy and highly correlated ab initio electronic structure calculations, we demonstrate that t
119            In this work, employing ab initio electronic structure calculations, we show that epitaxia
120 nds in the dark state, which is supported by electronic structure calculations.
121 ution x-ray Compton scattering combined with electronic structure calculations.
122 -situ STEM, in-situ synchrotron XRD, and DFT electronic structure calculations.
123 f Naph(+*)(Pyr) isomers are characterized by electronic structure calculations.
124 t-principles density functional theory-based electronic structure calculations.
125 roduce an energy functional for ground-state electronic structure calculations.
126 ood agreement with recent predictions by DFT electronic structure calculations.
127                                              Electronic-structure calculations further predict that b
128  The multiple-bond character is confirmed by electronic-structure calculations, and an upfield (6)Li
129                                From advanced electronic-structure calculations, we find that the Kita
130                                          The electronic structure can be tuned, for example, by chang
131 standing the role of topology in determining electronic structure can lead to the discovery, or appre
132                           Interestingly, the electronic structures can be further engineered in multi
133 ion spectroscopy for following the intricate electronic structure changes accompanying the non-adiaba
134  reaction valley approach that registers all electronic structure changes of the target molecule alon
135  Fe(IV)(O) units in 1 and A undergo the same electronic-structure changes during HAT.
136                             Its experimental electronic structure characterization via UV-PES, cyclic
137 s with respect to materials design concepts, electronic structure, charge transport mechanisms, defec
138 tructures (M = redox-inactive metal) defines electronic structure contributions to Co(IV) formation.
139 nium is predicted utilizing first-principles electronic structure coupled with a self-consistent phon
140 died by quantum chemical calculations at the electronic structure density functional theory and MP2 l
141 igand, and iron nitrosyls can have different electronic structure descriptions depending on their spi
142                   This results in archetypal electronic structures, determined with CASSCF-SO calcula
143  caused by removing local-lattice strain and electronic-structure disorder by thermal annealing.
144 pulses, and find that the new phase exhibits electronic structures entirely different from that of th
145 lso as to the degree of its influence on the electronic structure even in the simplest representative
146 ion resonances, which reveals the underlying electronic structure evolution and serves as its infrare
147                   In this communication, the electronic structure evolution of SrFeOx epitaxial thin
148 oretical methods to provide insight into the electronic structure, formation, and N-H insertion react
149               The formation of 3-5 and their electronic structures have been elucidated with DFT calc
150 ock) chains to better understand fundamental electronic structure in the f-block.
151 he calculations illustrate the complexity of electronic structure in this strongly delocalized superc
152                     The growth mechanism and electronic structure in zone I are further discussed in
153 roscopy (sXAS) results reveal differences in electronic structures in the bulk and at the surface of
154 iginating from fairly compensated multi-band electronic structure, in full accordance with our first-
155      We performed a full mapping of the bulk electronic structure including the Fermi surface and Fer
156 on-layered nanomaterials, study their exotic electronic structures, introduce electronic-structure ma
157                         This work details an electronic-structure investigation of [Fe(IV)(O)(L(NHC))
158 llow electrochemical characterization of the electronic structure, investigation of charge transport
159        The analysis shows that the {FeNO}(6) electronic structure is best described as Fe(III)-NO(neu
160                                          The electronic structure is computed using the WIEN2k code a
161                                          The electronic structure is corroborated by DFT and TD-DFT c
162  impact of this change on the momentum-space electronic structure is essential for understanding thei
163 nd experimental approach that looks into the electronic structure is proposed to improve accuracy of
164 heir exotic electronic structures, introduce electronic-structure manipulation strategies, and provid
165                                   Mean-field electronic structure methods like Hartree-Fock, semiloca
166 approach that uses accurate first-principles electronic structure methods to compute unique model par
167 -Plesset perturbation theory, fragment-based electronic structure methods, and diffusion Monte Carlo.
168 f the transverse ligands on the magnetic and electronic structure of 1-Dy were investigated through a
169  unambiguous assignment of the geometric and electronic structure of 1.
170                                The contested electronic structure of [Cu(CF3)4](1-) is investigated w
171                                          The electronic structure of a charge density wave (CDW) syst
172  properties, and theoretical analysis of the electronic structure of a family of expanded bacteriochl
173 s regardless of the chemical composition and electronic structure of a material.
174 ce topology in mixed valence systems.How the electronic structure of a mixed-valence system changes w
175 challenge though is that key features of the electronic structure of an insulator (and its evolution)
176                                          The electronic structure of an insulator encodes essential s
177   Following this idea, here we report on the electronic structure of an ordered array of poly(para-ph
178                      The high magnetic field electronic structure of bilayer graphene is enhanced by
179                                          The electronic structure of Bk(IO3)3 and Bk(IO3)4 were exami
180  cobalt phosphoselenide favorably change the electronic structure of cobalt selenide, assuring a rapi
181 the article discusses (i) measurement of the electronic structure of colloidal QDs and the influence
182 111} nanofacets, which favourably affect the electronic structure of CoO, assuring a rapid charge tra
183 ted herein is a comprehensive account of the electronic structure of corrole derivatives.
184 ions are used to determine the geometric and electronic structure of CuZ degrees , an intermediate fo
185  Just as in the original IrAl2.75 phase, the electronic structure of Fe14 Pd17 Al69 exhibits a pseudo
186 dy the influence of the nematic order on the electronic structure of FeSe and determine its exact ene
187        Here we report the ARPES study of the electronic structure of FeSe/STO(110).
188 onvenient and effective approach to tune the electronic structure of few-layer black phosphorus.
189  Here we experimentally demonstrate that the electronic structure of few-layer phosphorene varies sig
190  a p-n diode, to investigate the fundamental electronic structure of individual, partially supported
191                                 Based on the electronic structure of M and S, we classify the M.S com
192 efit from a 'bottom-up' approach whereby the electronic structure of magnetic molecules is chemically
193            Understanding and controlling the electronic structure of molecules is crucial when design
194              Here, we directly visualize the electronic structure of MoTe2, a recently proposed type-
195 ductivity in the cuprates.Exploration of the electronic structure of nickelates with similar crystal
196                    A critical feature of the electronic structure of oxobenzene-bridged bisdithiazoly
197 ease from 0.7 to 7 nm because changes in the electronic structure of Pd surface atoms decrease their
198                 The strongly layer-dependent electronic structure of phosphorene, in combination with
199 -ray absorption studies of the geometric and electronic structure of primarily heterogeneous Co, Ni,
200  are efficient nanocrystal emitters with the electronic structure of quantum wells, coupled to a phot
201  to resolve important aspects of the complex electronic structure of rare-earth nickelates, taking Nd
202 igh-resolution data provide insight into the electronic structure of SmB6, which reconciles many curr
203  currently no consensus for the band gap and electronic structure of ST12-Ge (tP12, P43212) due to ex
204 this phenomenon to repetitive changes in the electronic structure of superlattices such that charge c
205                        The unusual intrinsic electronic structure of the [B12X12](2-) MCAs provides t
206  rutile IrO2 have provided insight about the electronic structure of the active X-ray amorphous phase
207 rcent of N atoms has a drastic effect on the electronic structure of the alloys.
208 hat is dependent on duplex integrity and the electronic structure of the analogue.
209 ure analyses illuminate the architecture and electronic structure of the BTSA unit versus other accep
210  is demonstrated at room temperature and the electronic structure of the C60-metal probe complex with
211  spectroscopy measurements indicate that the electronic structure of the Ca2IrO4 thin-films is simila
212 sents an elite strategy for fine turning the electronic structure of the catalytic centers, hence the
213 allows for parallels to be drawn between the electronic structure of the Co4O4 cubane model system an
214 uence of the trifluoroethoxide ligand on the electronic structure of the complex.
215 nd Hubbard model, which represents the local electronic structure of the copper-oxygen plane.
216 properties, which are only determined by the electronic structure of the cyanine-type backbone (appro
217 y states associated with the local intrinsic electronic structure of the edges of the perovskite laye
218 k that senses and responds to changes in the electronic structure of the flavin on the ultrafast time
219 theoretical framework, we show here that the electronic structure of the molecular crystals determine
220  approach has enabled the fine-tuning of the electronic structure of the organoboron species by modif
221 t is shown that accurate predictions for the electronic structure of the para-quinonimide anion requi
222  an unexpected reaction pathway in which the electronic structure of the phosphoramidite dramatically
223                        The modulation of the electronic structure of the Pt shell by the nitride core
224  to the Pt, and thus favorable tuning of the electronic structure of the Pt.
225 lysis, which exploits the combination of the electronic structure of the QD core and the chemistry at
226  model, to directly experimentally probe the electronic structure of the S = 0 {FeNO}(6) compound [Fe
227 or these intermediates, we characterized the electronic structure of the stable compound Tp(tBu)Cu(II
228 ecause these choices dramatically impact the electronic structure of the system and, in turn, catalys
229 sent a significant step toward tailoring the electronic structure of these and other semiconductor pa
230   Despite numerous experimental reports, the electronic structure of these materials is still challen
231 stitution and organic functionalization, the electronic structure of these materials is systematicall
232                                          The electronic structure of these species therefore involves
233 g with an isoelectronic oxo, we quantify the electronic structure of this 5f(1) family by magnetometr
234 top apparatus to directly reveal the valence electronic structure of this transient intermediate stat
235 rong resemblances and key differences of the electronic structure of trilayer nickelate La4Ni3O10 com
236                                  Crystal and electronic structures of 380 nm BiFeO3 film grown on La
237  with different rotational angles change the electronic structures of bilayer MoS2 and produce two ne
238 ed two guiding principles for predicting the electronic structures of BN acene compounds: (1) Orienta
239 ight binding calculations to investigate the electronic structures of bulk 2H-MX2.
240 ermanium, tin, and lead homologues uniformly electronic structures of carbene analogues that are stab
241 the SCAN functional for accurate modeling of electronic structures of layered materials in high-throu
242          The definition of the geometric and electronic structures of metallozeolites has advanced to
243                                          The electronic structures of Mo carbide and carbyne species
244                           The geometries and electronic structures of molecular ions featuring He ato
245 S and HR-XANES to gain new insights into the electronic structures of the actinide elements.
246                                          The electronic structures of the antifluorite-type compound
247                            The molecular and electronic structures of these compounds were clearly el
248 scopic, and DFT studies reveal geometric and electronic structures of these Cu(II) organometallic com
249                                          The electronic structures of these mixed-valent complexes ha
250 ituent incorporation perturbs geometries and electronic structures of these nonplanar aromatics.
251 quantum chemistry to determine molecular and electronic structures of unligated (deoxy), CO-inhibited
252 ults indicate the controllability of lateral electronic structures of various ultrathin films by extr
253                                              Electronic structures of Zn2NF as well as ZnO0.2N0.5F0.3
254 e transition metal complex and metal surface electronic structure opens the possibility to control th
255 d from predicted crystal structures, such as electronic structure or mechanical properties.
256 t defects in TMDs and their influence on the electronic structure, photoluminescence, and electric tr
257                                 The emergent electronic structure picture reveals that Cu coordinatio
258 ysics, with the differences from the cuprate electronic structure potentially shedding light on the o
259 scheme of density functional theory to solve electronic structure problems in a wide variety of scien
260     Quantum computers can be used to address electronic-structure problems and problems in materials
261 onal methods have made solving even few-atom electronic-structure problems interesting for implementa
262  tensile strain strongly couples the atomic, electronic structure properties and the activity of the
263 e iron-carbon multiply bonded species reveal electronic structure properties indicative of a conforma
264  This review aims to give an overview of how electronic structure properties obtained from quantum ch
265                                              Electronic structure properties such as ballistic transm
266  understand the evolution of the optical and electronic structure properties with degree of functiona
267  of how a robust understanding of perovskite electronic structure provides fundamental insights into
268                                        Their electronic structure ranges from trivial insulators, to
269 study the changes in the local geometric and electronic structure related to these intrinsic point de
270 ture was clarified, while its reactivity and electronic structure remain under debate.
271 ia catalysts and their effect on the surface electronic structure remains unclear.
272 llic Ni(OH)2 nanosheets by engineering their electronic structure, representing a first metallic conf
273 nd is highly inefficient for high-throughput electronic structure screening calculations.
274 calculations confirm the method's impressive electronic structure sensitivity for excited-state inves
275                                              Electronic structure simulations corroborated structural
276 ported by density functional theory computed electronic structures, single crystal structures, and ex
277 +)), are quantitatively assessed in terms of electronic structure, solvation structure, and dynamics.
278                               Studies of the electronic structure support open-shell intermediates, a
279 ensity functional theory calculations of the electronic-structure supporting the complex metallic con
280                         This article reviews electronic structure techniques used to model molecular
281 favorable local coordination environment and electronic structure that enhance the energetics for OER
282    This can reveal much about the materials' electronic structure that is invisible in standard probe
283 n, the technologies of chemical dynamics and electronic structure theory are coupled so that the pote
284                                         From electronic structure theory we find that the theoretical
285               These fundamental questions in electronic structure theory, which have not been address
286 he simulation are obtained directly from the electronic structure theory.
287 ed explicitly with computationally demanding electronic structure theory.
288 uation of the potential energy surface using electronic structure theory.
289 e correct classical dynamics predicted by an electronic structure theory; (4) determine a deeper unde
290 absorption spectroscopy and first-principles electronic-structure theory.
291 roperties stemming from their characteristic electronic structure to highly efficient real-life techn
292 itate water dissociation, and fine tunes the electronic structure to weaken hydrogen adsorption towar
293                            The triplet-state electronic structure was characteristic of the expected
294 ction analysis and local measurements of the electronic structure, we identify key structural motifs
295 congener were fully characterized, and their electronic structures were elucidated in a combined expe
296 roscopy was used to map the occupied valence electronic structure, while absorption and fluorescence
297 cal withC(C6H4)CH3)DPFN](NTf2)2, revealed an electronic structure with an unexpected partially deloca
298     However, many oxides have a more complex electronic structure, with charge, orbital and/or spin o
299  more significant quasi two-dimensional (2D) electronic structure, with the out-of-plane transport sh
300 nd a highly anisotropic in- and out-of-plane electronic structure, with the valence band maxima locat

WebLSDに未収録の専門用語(用法)は "新規対訳" から投稿できます。
 
Page Top