ライフサイエンスコーパス: electronic property

1 ne quaterthiophene-derived COFs with tunable electronic properties.

2 ome hydrogen-rich structures with intriguing electronic properties.

3 dimensionally reduced structures with novel electronic properties.

4 chains and/or organic groups, limiting their electronic properties.

5 ral changes are necessary for fine-tuning of electronic properties.

6 r specific binding, catalytic, nucleating or electronic properties.

7 ene, due to their unique physicochemical and electronic properties.

8 ifficulty to independently control ionic and electronic properties.

9 sights into their outstanding structural and electronic properties.

10 aterials with novel mechanical, optical, and electronic properties.

11 n an accurate knowledge of their fundamental electronic properties.

12 a semiconductor is one of its most important electronic properties.

13 -member heterocycle affect photophysical and electronic properties.

14 te redox switching of optical, magnetic, and electronic properties.

15 ficant attention due to their promising opto-electronic properties.

16 eir crystal orientation, film morphology and electronic properties.

17 ecular recognition and unique biological and electronic properties.

18 ractions have important roles in determining electronic properties.

19 e stable organized structures with desirable electronic properties.

20 k solids with diverse crystal structures and electronic properties.

21 grow single or multilayer graphene with good electronic properties.

22 lysis because of their unique structural and electronic properties.

23 ogy, providing tunability of the optical and electronic properties.

24 elatively low but significantly affect their electronic properties.

25 the tailoring of their chemical, optical and electronic properties.

26 ronics due to their distinctive physical and electronic properties.

27 hey have active sites with unique steric and electronic properties.

28 s with atomically thin geometries and unique electronic properties.

29 3 ) monolayer, is predicted to possess novel electronic properties.

30 oncrystalline materials with well-controlled electronic properties.

31 c strains, which significantly affects their electronic properties.

32 n extended pi-conjugated materials and their electronic properties.

33 ns with other materials to engineer targeted electronic properties.

34 fundamental role in determining the material electronic properties.

35 e can possess a wide range of structural and electronic properties.

36 a monolayer platform to investigate emerging electronic properties.

37 talled within pi-systems to tune optical and electronic properties.

38 als can markedly influence their macroscopic electronic properties.

39 e size, controllable thickness and excellent electronic properties.

40 onductors to improve the intrinsic materials electronic properties.

41 amic conditions, toward realizing wholly new electronic properties.

42 e to its outstanding mechanical, thermal and electronic properties.

43 heir unique nanostructures and extraordinary electronic properties.

44 compounds are of interest for their diverse electronic properties.

45 e impact of common defects on structural and electronic properties.

46 mensional materials because of their unusual electronic properties.

47 re dynamic materials possessing unique (opto)electronic properties.

48 tures and can possess unusual mechanical and electronic properties.

49 the palladium particles and affecting their electronic properties.

50 rials has grown, displaying a broad range of electronic properties.

51 on methods and their subsequent influence on electronic properties, a comprehensive review of the mod

52 ture, characterized by distinct chemical and electronic properties along the edges.

53 quantum sized nanoparticles exhibit specific electronic properties and also expand the working surfac

54 eed with minimal dependence on the substrate electronic properties and at electrode potentials 0.5-1.

55 ng of the relationship between its intrinsic electronic properties and atomic bonding configurations.

56 doping opens possibilities for tailoring the electronic properties and band gap of graphene toward it

57 dine (ppyH) or related compunds with diverse electronic properties and C^N is the corresponding cyclo

58 Elucidating the correlations between electronic properties and catalytic activity is crucial

59 r reliable interpretation of its optical and electronic properties and enables controlled processing

60 lized nanomaterials due to their unique opto-electronic properties and enhanced surface to volume rat

61 rinsic and/or extrinsic defects can tune the electronic properties and extend applications to gas sen

62 ls with unprecedented physical, optical, and electronic properties and have also found many applicati

63 The exotic electronic properties and high specific surface areas of

64 The altered electronic properties and implications for redox catalys

65 ntalum, show strong interactions between the electronic properties and lattice dynamics.

66 Despite graphene's long list of exceptional electronic properties and many theoretical predictions r

67 has proven to be effective in modulating the electronic properties and molecular geometries of the pi

68 d to demonstrate the local modulation of the electronic properties and possible benefits in potential

69 The fine-tuning of the electronic properties and redox potentials of the photoc

70 synthetic chemical route for controlling the electronic properties and stability within the tradition

71 understand the effect of cyclization on the electronic properties and structure.

72 We evaluate the optical and electronic properties and the solid-state packing of the

73 ing to engineer their chemical, physical and electronic properties and thus achieve good performance

74 es, where its inherent transparency, tunable electronic properties, and accessible nanostructures can

75 eteroaromatics, focusing on their synthesis, electronic properties, and applications in materials sci

76 ew single-ion/CNT heterostructure with novel electronic properties, and demonstrate that as electroni

77 ng with the role of defects in governing its electronic properties, and methods employed to modulate

78 The structure, electronic properties, and redox behavior were investiga

79 f their unique cyclic architectures, tunable electronic properties, and supramolecular chemistries, c

80 mong the materials synthesis, structural and electronic properties, and their major applications.

81 n this work, we report the atomic structure, electronic properties, and vibrational modes of few-laye

82 However, the observed electronic properties are blurred by the concomitant eff

83 Their electronic properties are characterized by UV-vis absorp

84 Correlated vibrational (chemical), and electronic properties are obtained simultaneously with t

85 y defects are ubiquitous their structure and electronic properties are very poorly understood since i

86 fields, whereas applications based on their electronic properties are virtually unexplored.

87 esolved electron microscopy, and their local electronic properties, as measured by single-atom electr

88 These results suggest that different electronic properties at domain walls are not necessary

89 re, fundamental gaps remain in understanding electronic properties at the nanoscale.

90 t of an enhanced electric field and distinct electronic properties at the step edges.

91 Molecular solids with cooperative electronic properties based purely on pi electrons from

92 opological insulators give rise to exquisite electronic properties because of their spin-momentum loc

93 jugated cycloparaphenylene rings have unique electronic properties being the smallest segments of car

94 Carbon nanotubes feature excellent electronic properties but narrow absorption bands limit

95 access to a variety of topologies with tuned electronic properties, but also in the ability of a fami

96 oexist, enable manipulation of magnetism and electronic properties by external electric fields throug

97 d may provide a basis for rational design of electronic properties by variation of molecular structur

98 t, we demonstrated that the tailoring of MOF electronic properties could be performed as a function o

99 nic devices due to their tunable optical and electronic properties depending on their functional grou

100 mologs exhibit very different structural and electronic properties, despite differing by only a singl

101 aries in condensed-matter systems often have electronic properties distinct from the bulk material an

102 The key to the functional electronic properties exhibited by perovskites is often

103 Furthermore, to demonstrate preservation of electronic properties following solution processing, the

104 e nanoribbon heterostructures have promising electronic properties for high-performance field-effect

105 Given that all other structural and electronic properties for the series are held at parity,

106 ntrinsic characteristics (e.g., diameter and electronic properties), has been investigated under envi

107 Their unique electronic properties have been exploited in Pt(II) cata

108 other ultrathin materials with unprecedented electronic properties have been explored, with particula

109 While changes in single-particle electronic properties have been investigated extensively

110 alow trap densities, exceptional optical and electronic properties have been reported for lead halide

111 ctionalized 3D nanographenes with controlled electronic properties have been synthesized through a mu

112 been studied for decades, its structure and electronic properties have only recently been correctly

113 imer superstructures with unique optical and electronic properties have recently been described.

114 The confinement-enabled control over electronic properties, however, requires nanoparticles t

115 e review is on photoinduced processes and on electronic properties important for optoelectronic appli

116 has been hypothesized to possess intriguing electronic properties in an atom-thick hexagonal form.

117 A novel approach to on-demand improvement of electronic properties in complex-oxide ferroelectrics is

118 date the effect of structural defects on the electronic properties in order to develop an application

119 ing is an essential tool for modifying local electronic properties in silicon-based electronics.

120 at exhibit unique size-dependent optical and electronic properties; in particular, they are strongly

121 new clathrate-like structures and remarkable electronic properties including room-temperature superco

122 interesting interplay between structural and electronic properties, including electronic many-body ex

123 dom, dramatically affecting their low-energy electronic properties, including superconductivity.

124 These nanowires have band-like electronic properties, low effective carrier masses and

125 Its excellent electronic properties make it attractive for application

126 merous strategies that allow tuning of their electronic properties make these materials very attracti

127 this Pentagon Carbon leads to extraordinary electronic properties, making it a cornucopia of emergen

128 nic systems with abundant and easily tunable electronic properties, namely La(1-x)Sr(x)BO3 perovskite

129 ructure allows us to describe all low-energy electronic properties obtained in our experiments with r

130 unctionalization has been used to adjust the electronic properties of 2D materials.

131 phasizing the novel structural, optical, and electronic properties of [5]-[12]CPPs.

132 The structural and electronic properties of a series of manganese complexes

133 er than being determined by the structure or electronic properties of active sites, the enhanced oxid

134 nt absorbance spectra, despite the identical electronic properties of all PMI amphiphiles.

135 class of matter characterized by the unique electronic properties of an insulating bulk and metallic

136 ance band of the AuNP, indicating that other electronic properties of AuNPs are also affected by the

137 The different electronic properties of BICAACs as compared to CAACs al

138 These preferences are consistent with the electronic properties of both the carbohydrate C-H bonds

139 tions are highly dependent on the steric and electronic properties of coupling partners; thus, carboh

140 a nanosize Cu lattice is known to alter the electronic properties of Cu, improving catalytic perform

141 play between the mechanical response and the electronic properties of CVD-grown structures.

142 c devices in which function derives from the electronic properties of discrete single molecules, and

143 stability, synthesis routes, mechanical and electronic properties of diverse ruthenium nitrides.

144 Despite this recognition, the electronic properties of domain walls under illumination

145 to accurate, predictive calculations of the electronic properties of electrolytes, of interest to a

146 he aryl diazonium substituent and alters the electronic properties of exfoliated BP, ultimately yield

147 dielectric, piezoelectric, pyroelectric and electronic properties of ferroelectric materials.

148 cking orders with spin-orbit coupling on the electronic properties of few-layer 3R-type MoS2 by first

149 urface chemistry can be used to modulate the electronic properties of gold nanoparticles.

150 The Dirac cone underlies many unique electronic properties of graphene and topological insula

151 The electronic properties of graphene are described by a Dir

152 ctronic nanoscopy to measure the optical and electronic properties of graphene devices locally.

153 The extraordinary optical and electronic properties of graphene make it a promising co

154 The remarkable mechanical and electronic properties of graphene make it an ideal candi

155 The unique optical and electronic properties of graphene make possible the fabr

156 The exceptional electronic properties of graphene stem from linear dispe

157 Interfacial interactions allow the electronic properties of graphene to be modified, as rec

158 s, which promises to combine the outstanding electronic properties of graphene with a bandgap that is

159 Control over the architectural and electronic properties of heterogeneous catalysts poses a

160 physical mechanisms that determine the (opto)electronic properties of high-performance organic materi

161 croscopic morphology is vital to develop the electronic properties of hybrid perovskites.

162 The electronic properties of individual layers are studied u

163 The ability to understand and control the electronic properties of individual molecules in a devic

164 rol device functions through the fundamental electronic properties of individual molecules, but reali

165 Due to the different electronic properties of its carbonyl oxygen atoms, a di

166 The remarkable electronic properties of layered semiconducting transiti

167 which significantly reshapes the fundamental electronic properties of Li2CuO2.

168 re of graphene gives rise to its exceptional electronic properties of linear dispersion relation and

169 venient, contactless approach to probing the electronic properties of low-dimensional charge carrier

170 udies show that differences in structure and electronic properties of LS-3DCHIm and LS-4DCHIm lead to

171 Here, inspired by the electronic properties of materials, we introduce and dem

172 uctures and can influence the mechanical and electronic properties of materials.

173 We modify the fundamental electronic properties of metallic (1T phase) nanosheets

174 ciated with conventional polymers and unique electronic properties of metals or semiconductors.

175 is work provides a new method to enhance the electronic properties of Mn2O3 using high-pressure treat

176 ble to identify the essential structural and electronic properties of MnCats.

177 tive, the understanding and tailoring of the electronic properties of MOFs are key fundamental challe

178 l the possible pathways for transforming the electronic properties of MOFs from insulating to semicon

179 ng of stereoelectronics to establish how the electronic properties of molecules relate to their confo

180 cuss self-consistently obtained ground-state electronic properties of monolayers of graphene and a nu

181 scopy (PEEM) and mu-ARPES we investigate the electronic properties of MoS2 as a function of the numbe

182 hich gives new insight into the variation of electronic properties of MoS2 films with thickness bears

183 an be an effective tool for manipulating the electronic properties of multi-orbital systems, where el

184 n great progress in our understanding of the electronic properties of nanomaterials in which at least

185 ostered a surge of computational research on electronic properties of organic molecular solids.

186 ificant step forward in our understanding of electronic properties of organic semiconductors.

187 The structures and electronic properties of partial C, Si and Ge decorated

188 ng and exploiting the remarkable optical and electronic properties of phosphorene require mass produc

189 In this paper, the structural and electronic properties of polythiophene and polyprrrole-b

190 Herein, we used this feature to measure electronic properties of provitamin A, vitamin E, and vi

191 Here we combine the outstanding optical and electronic properties of purified, solution-processed se

192 Ultrafast light pulses can modify electronic properties of quantum materials by perturbing

193 king example of this complexity, whereby the electronic properties of reactive ferryl intermediates a

194 out to determine the relative stability and electronic properties of ruthenium doped germanium clust

195 The optical and electronic properties of semiconducting materials are of

196 f considerable importance in determining the electronic properties of semiconductors, especially in p

197 et underexplored, approach for tuning of the electronic properties of semiconductors.

198 ons can be used to tailor the structural and electronic properties of single crystal films.

199 The electronic properties of small molecule organic crystals

200 An extremely sensitive dependence of the electronic properties of SnOx film on sputtering deposit

201 exploration on the chemical, structural, and electronic properties of such conjugated systems contain

202 The ability to fine-tune the electronic properties of synthetic bacteriochlorins is i

203 may open up new possibilities to tailor the electronic properties of TAPP-based materials for certai

204 The electronic properties of the 13-ring N-heteroarene allow

205 charge carriers is strongly dependent on the electronic properties of the 2D MoS2 with metallic MoS2

206 method was used to modify the morphology and electronic properties of the absorber and it clearly imp

207 ptimization of the denticity, and steric and electronic properties of the ancillary ligand (initially

208 ds are not affected by varying the steric or electronic properties of the aromatic imines.

209 ncreasing the range of functional groups and electronic properties of the aryl groups that are tolera

210 The steric/electronic properties of the boryl fragment employed ena

211 shows that encapsulation does not change the electronic properties of the catalyst nor its first coor

212 It is argued that the optimization of the electronic properties of the chromophore, which affects

213 peripheral ferrocenes noticeably impacts the electronic properties of the corresponding ZnPc and RuPc

214 Designing a data set in which the steric and electronic properties of the Cp(X)Rh(III) catalysts were

215 The electronic properties of the cubane are readily tuned by

216 A study on the electronic properties of the dilute-P GaN(1-x)P(x)alloy

217 processing parameters on the structural and electronic properties of the films.

218 mical studies reveal that the structural and electronic properties of the GNR composite matrix increa

219 n science and technology, where the emergent electronic properties of the gold core are valued for us

220 the alkyl tail exerts clear control over the electronic properties of the gold core, as determined by

221 aser initiation was achieved by altering the electronic properties of the ligand scaffold to tune the

222 ic applications, the ability to modulate the electronic properties of the ligand with facility may be

223 e ligand substituent fundamentally alter the electronic properties of the luminophore itself.

224 ularities dramatically affect the low-energy electronic properties of the material, including superco

225 anic semiconductor, and, in turn, affect the electronic properties of the material.

226 uper-acid treated MoS2, and suggest that the electronic properties of the MoS2 are also superior.

227 he degree of fusion and thus the optical and electronic properties of the resulting GNRs can be contr

228 y and the identity of the cation perturb the electronic properties of the SAM-chelated iron-sulfur cl

229 The electronic properties of the Si horizontal lineO bond we

230 les with low to good yields depending on the electronic properties of the substituents on the borodie

231 be achieved, and a strong dependency on the electronic properties of the substituents was observed.

232 of different types of C-H bonds based on the electronic properties of the substrate.

233 We also show that the electronic properties of the superlattices are highly tu

234 dynamic equilibrium that is modulated by the electronic properties of the supporting ligands.

235 er and using it investigate the magnetic and electronic properties of the system.

236 re either probabilistic or pre-determined by electronic properties of the system.

237 lator to metal transition through tuning the electronic properties of the target perovskite families

238 shown to stem from a combination of inherent electronic properties of the thioacyl substituent and en

239 d by QM calculations giving a picture of the electronic properties of the transition state (TS) for n

240 Significant differences were found in the electronic properties of the two structures, and the met

241 ulations, we investigated the mechanical and electronic properties of the two Zr polymorphs.

242 Our results allow many electronic properties of the underdoped cuprates to be u

243 Yet, the electronic properties of these broken symmetry phases ar

244 ation, can have significant influence on the electronic properties of these composite materials.

245 Furthermore, physical, structural, and electronic properties of these compounds were explored c

246 e possibility of novel applications in which electronic properties of these materials can be locally

247 ctural similarities, we demonstrate that the electronic properties of these MOFs are markedly differe

248 n discussed as a way in which to control the electronic properties of these nanoparticles, we show th

249 Moreover, the electronic properties of these pigment-proteins result f

250 atter strongly influences the mechanical and electronic properties of this material that are importan

251 s-conjugated side-chains on the physical and electronic properties of this new class of boron-contain

252 e may be electrochemically generated and the electronic properties of this unique high-valent state m

253 the fundamental insights responsible for the electronic properties of three distinct classes of bimet

254 Studies of mechanical and electronic properties of TmB4 suggest that these tetrabo

255 Here, we investigate the electronic properties of TMDs and transition metal oxide

256 ulations, we investigated the structural and electronic properties of tungsten trioxide (WO3) surface

257 Electronic properties of two-dimensional (2D) MoS2 semic

258 When combined with the unique electronic properties of two-dimensional crystals, they

259 esults motivate future studies tailoring the electronic properties of van der Waals heterostructures

260 The electronic properties of ZnO nanosheets and AILE of othe

261 Here, we investigate the electronic property of SrRu2O6 using density functional

262 ue planar structures and various fascinating electronic properties offers great potential for batch f

263 pact of P-Pd-P coordination angle and ligand electronic properties on catalysis.

264 design Floquet states of matter with tunable electronic properties on ultrafast timescales.

265 The band structures, electronic properties, optical absorption, and interfaci

266 ectronic applications based on their diverse electronic properties, ranging from insulating to superc

267 of an electromagnetic wave based on tunable electronic properties (rather than geometric structure)

268 hough much work has been done to improve its electronic properties, relatively little is known of its

269 ir interesting structural chemistry, unusual electronic properties, rich intercalation chemistry and

270 Their electronic properties strongly depend on the number of l

271 on electronic applications due to its unique electronic properties such as large carrier Fermi veloci

272 nd bond length are used to explain trends in electronic properties such as the magnitude and temperat

273 Electronic properties, such as conductivity and supercon

274 ons of small molecules for fine-tuning their electronic properties, such as ionization potentials and

275 orted compounds with peculiar structural and electronic properties, such as the N4H, N3H, N2H and NH

276 atomic crystals, (ii) it demonstrated unique electronic properties, thanks to charge carriers which m

277 atomic crystals, (ii) it demonstrated unique electronic properties, thanks to charge carriers which m

278 tices, which can lead to unique physical and electronic properties that are not available in the pare

279 macrocycles, have size-dependent optical and electronic properties that are the most dynamic at the s

280 ing effect of the layer-stacking sequence on electronic properties that are typically expected to be

281 create electronic interface systems with new electronic properties that do not exist in bulk.

282 es were conducted to evaluate the steric and electronic properties that govern the reactivity of iodo

283 oromethyl groups possess specific steric and electronic properties that invite their use as chemicall

284 metal dichalcogenide (TMD) with physical and electronic properties that make it attractive for a vari

285 ls possess unique structural, mechanical and electronic properties that make them highly attractive i

286 ults introduce a concept for the domain wall electronic property, the walls own internal degrees of f

287 elated to the controllability of domain wall electronic properties.The electronic states within domai

288 th the fact that the ligands impart distinct electronic properties to a metal, will support the inven

289 also revealed that periodic sequences allow electronic properties to be tuned while retaining nanofi

290 ands that are able to modify their steric or electronic properties to fulfill the requirements of a d

291 Tin-based perovskites have very comparable electronic properties to lead-based perovskites and are

292 have been involved in the transfer of these electronic properties to new Fe/Co coordination networks

293 hat these heterodimers feature complementary electronic properties to tetrathiafulvalenes (TTFs).

294 nthesis of silicene and investigation of its electronic properties, to date there has been no report

295 parameters to quantify phosphine steric and electronic properties together with regression statistic

296 generating stable radicals with fascinating electronic properties useful for a large variety of appl

297 tial factor for their functionality is their electronic properties, which can be modified by quantum

298 amolecular assemblies with new geometric and electronic properties whose more representative examples

299 s (TMDs) have unique mechanical, optical and electronic properties with promising applications in fle

300 Monolayer graphene exhibits many spectacular electronic properties, with superconductivity being argu