ライフサイエンスコーパス: electronic property

1 in odd-numbered rings, possess unusual (opto)electronic properties.

2 a detailed understanding of their impact on electronic properties.

3 uch interest due to their largely modifiable electronic properties.

4 and O-nucleophiles with different steric and electronic properties.

5 ve eluded detailed characterization of their electronic properties.

6 composite nanomaterials with precisely tuned electronic properties.

7 e affected at the single atom level than the electronic properties.

8 and connected to its fundamentally different electronic properties.

9 tic design rules to precisely engineer their electronic properties.

10 have rigid, defined conformations and unique electronic properties.

11 ated by bipyridine ligands possessing varied electronic properties.

12 their differing thermodynamic stability and electronic properties.

13 in semiconductors are critical to tune their electronic properties.

14 dividually expressing distinctive and varied electronic properties.

15 es is central for exploiting their different electronic properties.

16 rsal training set on the basis of steric and electronic properties.

17 he 2D layers, which controls the optical and electronic properties.

18 ause of their unique anisotropic optical and electronic properties.

19 cent interest for their tunable chemical and electronic properties.

20 presence of different amines with different electronic properties.

21 e research, due to their unique physical and electronic properties.

22 e stable organized structures with desirable electronic properties.

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

24 the palladium particles and affecting their electronic properties.

25 ome hydrogen-rich structures with intriguing electronic properties.

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

27 amic conditions, toward realizing wholly new electronic properties.

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

29 heir unique nanostructures and extraordinary electronic properties.

30 compounds are of interest for their diverse electronic properties.

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

32 mensional materials because of their unusual electronic properties.

33 a lack of experimental investigation of its electronic properties.

34 g semiconductors with tailorable optical and electronic properties.

35 suppression of surface states dominating the electronic properties.

36 erest owing to their outstanding optical and electronic properties.

37 onjugated functional molecules dictate their electronic properties.

38 and highly anisotropic in-plane optical and electronic properties.

39 scinating due to their unique reactivity and electronic properties.

40 ngle-crystalline form, MoS(2) shows superior electronic properties.

41 e silicon dimers leads to unique optical and electronic properties.

42 te cages affect the structural, optical, and electronic properties.

43 These MXenes show distinctive structural and electronic properties.

44 les (NPs) shows unique optical, thermal, and electronic properties.

45 lled Fe-porphyrins dramatically alters their electronic properties, accelerating the rates of both re

46 hree electrophilic iron complexes of varying electronic properties, affording the desired coupling pr

47 Finally, these specific electronic properties allowed us to prepare a persistent

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

49 terfaces, given (1) their unique optical and electronic properties and (2) their high degree of synth

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

51 s is that dopants and defects can tune their electronic properties and although their impact is well

52 bonds that are nearly identical in terms of electronic properties and bond strengths.

53 Combining the designable electronic properties and controllable assembly approach

54 acterization of their instrinsic optical and electronic properties and demonstration, of metal-free h

55 spacer cations exert influence on desirable electronic properties and device performance of two-dime

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

57 e great stability, ease of modulation of the electronic properties and excellent sigma-donating capac

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

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

60 ising alternatives because they have tunable electronic properties and high water-solubility, but the

61 nection between ultrafast changes in optical-electronic properties and lattice structure.

62 ic substrates strongly screen their designer electronic properties and limit further applications.

63 utadiene (DNBDCs), with orthogonally tunable electronic properties and molecular packing.

64 gn new 3D graphene devices with preserved 2D electronic properties and novel functionalities.

65 The established correlation between MOF electronic properties and photoisomerization kinetics as

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

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

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

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

70 catalysts, due to their unique geometric and electronic properties and their highly efficient use of

71 Next, we review the fundamental electronic properties and various single nanowire transi

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

73 attention due to their exciting optical and electronic properties, and demonstrate immense potential

74 n metal dichalcogenides, their impact on the electronic properties, and how to control them is critic

75 ce structural compatibility has on intrinsic electronic properties, and indicate that the theory prov

76 ect of a glutarimide ring on the structures, electronic properties, and reactivity of fully perpendic

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

78 The structural features, electronic properties, and surface chemistry of 2D nanos

79 with rocksalt crystal structures, remarkable electronic properties, and the general chemical formula

80 en ligands are tunable for steric as well as electronic properties, and their ability to coordinate a

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

82 ion, the stability of these materials, their electronic properties, and their synthesis.

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

84 Their electronic properties are characterized by UV-vis absorp

85 The optical and electronic properties are compared with those of related

86 emistry of complex oxides and the associated electronic properties are equally embraced.

87 These atomistic electronic properties are extraordinarily useful and mot

88 Pentacene's extraordinary photophysical and electronic properties are highly dependent on intermolec

89 by theoretical calculations, indicating the electronic properties are independent of adding a single

90 In complex oxide materials, changes in electronic properties are often associated with changes

91 (3)NH(3))(+) ions and the interplay with the electronic properties are still not fully understood, de

92 The electronic properties are studied via scanning tunneling

93 Overall, the optical and electronic properties are tunable via choice of bridging

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

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

96 d versatile surface modification to tune the electronic properties, are still not applicable to the p

97 for known nanoparticle shapes using the opto-electronic properties as a driver.

98 system that allows for tuning morphology and electronic properties as well as for resolution of trans

99 a-positions alter both the geometric and the electronic properties as well as the crystal packing of

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

101 ic devices are a better understanding of the electronic properties at the individual molecular level

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

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

104 he electronic band structure, including some electronic properties (bandgap and number of electrons),

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

106 towed upon them not only tunability of their electronic properties but also high-performance electron

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

108 in size to hydrogen atoms but have distinct electronic properties, causing C-F bonds to be exception

109 These unique electronic properties controlled by design, makes Mollec

110 This local change in electronic properties correlates with a statistically si

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

112 excess charge carriers, and thus the overall electronic properties, crucial to many technologies.

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

114 y in-plane anisotropic crystal structure and electronic properties for photonic and optoelectronic ap

115 The electronic properties have been investigated by scanning

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

117 nd implication of the strain gradient on the electronic properties in both optoelectronic and photovo

118 en the two regimes, they can also modify the electronic properties in more subtle ways when electron

119 However, while electronic properties in natural materials can show sign

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

121 ysis of the interplay between structural and electronic properties in other emerging 2D Xenes.

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

123 e superlattices(1), enabling new optical and electronic properties in solid-state systems.

124 nic materials can be tailored with on-demand electronic properties in the context of neuromorphic app

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

126 s manifested in the change of mechanical and electronic properties, including exfoliation, blue-shift

127 The control of the V(2)O(3) electronic properties is achieved using the transfer of

128 Such change in structural and electronic properties is confirmed from the nonmonotonic

129 solar energy material, therefore tuning its electronic properties is necessary for optimal performan

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

131 s role of local interactions governing their electronic properties, many of which violate Fermi-liqui

132 t from PBI subunits enables the emergence of electronic properties not evidenced in non-covalent asse

133 ieved through systematic optimization of the electronic properties of 1,6-diene structures.

134 The electronic properties of 3D nanoporous graphene with a c

135 rawings capture only a partial sketch of the electronic properties of a molecule, IMS contour plots p

136 is reveal how the optical field modifies the electronic properties of a solid through combined action

137 Here, we report a systematic studies of electronic properties of a superconducting half-Heusler

138 oth topologically protected and nonprotected electronic properties of a Weyl semimetal.

139 The rich magneto-electronic properties of AA-bottom-top (bt) bilayer sili

140 to predict and investigate the structure and electronic properties of actinides and lanthanides that

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

142 ivity of C-H activation is correlated to the electronic properties of allylic C-H bonds indicated by

143 s to determine both the atomic structure and electronic properties of an abundant chalcogen-site poin

144 ne the atomic-scale structural, chemical and electronic properties of artificial engineered defects i

145 ieved through systematic optimization of the electronic properties of aryl fluorosulfates.

146 The unique electronic properties of Azo-MICs allow for reversible o

147 This retains the electronic properties of Bi(2)O(2)Se while reducing the

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

149 hnology that's been made taking advantage of electronic properties of biological material for address

150 These unique structural characteristics and electronic properties of borophene attract significant s

151 mplexation on conformational preferences and electronic properties of carbonyl group-bearing lithium

152 One of the most effective ways to tune the electronic properties of conjugated polymers is to dope

153 ens a new way for probing local magnetic and electronic properties of correlated materials containing

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

155 Here the magnetic and electronic properties of CrSBr are reported, an air-stab

156 The role of the crystal lattice for the electronic properties of cuprates and other high-tempera

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

158 lent interfacial charge states in tuning the electronic properties of different components to promote

159 in the absorption bands, indicating that the electronic properties of dithia-bis(calix)-sapphyrins we

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

161 ural elements toward tuning the chemical and electronic properties of extended polycyclic aromatic hy

162 t control of the optical properties from the electronic properties of fluorescent organic salts.

163 The electronic properties of heterostructures of atomically

164 Structural and electronic properties of hexagonal (h-) and cubic (c-) p

165 The electronic properties of Ir catalysts ligated by dtbpy o

166 mining the stability, local environment, and electronic properties of isolated atoms and thus providi

167 The remarkable electronic properties of layered semiconducting transiti

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

169 smon qubit(7-9), whose spectrum reflects the electronic properties of massless Dirac fermions travell

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

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

172 Pressure alters the physical, chemical, and electronic properties of matter.

173 surface states provide new insight into the electronic properties of mesoporous NiO films.

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

175 isible transmittance of dielectrics with the electronic properties of metals for plasmonic and meta-m

176 eviously we demonstrated that the steric and electronic properties of Mn(III)-OOR complexes containin

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

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

179 eport detailed measurements of transport and electronic properties of molecular tunnel junctions base

180 The structural and electronic properties of molecularly pillared graphene s

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 We describe the synthesis and electronic properties of new pai-conjugated small molecu

184 Modifying the electronic properties of olefins is the quintessential a

185 Electronic properties of organic semiconductor (OSC) thi

186 However, the electronic properties of oxide heterointerfaces cruciall

187 Controlling the electronic properties of oxides that feature a metal-ins

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

189 Here, the tunability of the electronic properties of perovskite nanocrystal arrays i

190 ching implications for the interpretation of electronic properties of perovskite-related oxides in ge

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

192 provides a new avenue to regulate the (opto)electronic properties of robust nanoscale objects.

193 The optical and electronic properties of semiconducting materials are of

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

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

196 Next, progress in research to understand the electronic properties of single-atom alloys using X-ray

197 ctroscopies to characterize the chemical and electronic properties of such applied interfaces is prov

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

199 This work is highly relevant to tuning the electronic properties of SWCNTs for applications in nano

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

201 The influence of symmetry on the electronic properties of TATBPs was studied by optical s

202 directly map the atomic-scale structural and electronic properties of TBG near the magic angle using

203 Device engineering based on the tunable electronic properties of ternary transition metal dichal

204 razine as an ideal model system to elucidate electronic properties of tetrapyrroles like chlorophyll

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 een the reactivity of such complexes and the electronic properties of the ancillary ligands are unkno

209 that the rate-limiting step varies with the electronic properties of the arene.

210 ized to controllably modify the symmetry and electronic properties of the composite heterostructure.

211 are used to compute the main structural and electronic properties of the compound, taking into consi

212 ical methods like fine-tuning the steric and electronic properties of the coordinating ligands.

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

214 tion/deactivation are determined by both the electronic properties of the Cu catalyst and the ligand-

215 The electronic properties of the cubane are readily tuned by

216 ronegativity of the local environment on the electronic properties of the dopant atom needs to be cla

217 To study the electronic properties of the fabricated devices, current

218 y evolving field, which explores the diverse electronic properties of the ferroelectric domain walls

219 The electronic properties of the five complexes were fully c

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

221 ffold was designed to mimic the geometry and electronic properties of the hPNMT TS.

222 substituents on the structural features and electronic properties of the isomeric borane-functionali

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

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

225 tailored to the central SBA-platform define electronic properties of the materials mimicking the str

226 Persistent luminescence depends on the electronic properties of the molecular components, mainl

227 e, grain boundary engineering determines the electronic properties of the monolayer.

228 of amorphous/nanocrystalline phases, and the electronic properties of the MXene and MAX phases.

229 anning tunneling microscopy to visualize the electronic properties of the prototypical chiral topolog

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

231 oyl)phenyl), which influence the optical and electronic properties of the resulting polythiophenes.

232 The optical and electronic properties of the rr-P3AT can be tuned by con

233 nvestigations, revealing an influence of the electronic properties of the sandwich unit on the lithia

234 The diverse structural and electronic properties of the Si-adsorbed and -substitute

235 nal theory (DFT) calculations to examine the electronic properties of the Sn(1-x)Pb(x)O ternary oxide

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

237 simultaneously measuring the topographic and electronic properties of the superconductor, we find tha

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

239 The electronic properties of these 3R domains, featuring lay

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

241 The electronic properties of these chains have also been cha

242 Here, we investigate the electronic properties of these iron-sulfur clusters and

243 hat must be achieved in order to control the electronic properties of these next generation organic m

244 We also find significant differences in the electronic properties of these two materials, in spite o

245 The optical and electronic properties of this graphitic cone were elucid

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

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

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

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

250 uence of fluorine and chlorine doping on the electronic properties of TiO(2).

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

252 The mechanical and electronic properties of two-dimensional materials make

253 provide a platform for exploring fundamental electronic properties of V(2)O(3).

254 The electronic properties of van der Waals moire superlattic

255 uorophore provides opportunities to tune the electronic properties of water-soluble BODIPY dyes for f

256 ing on morphological, chemical, optical, and electronic properties of WSe(2) is elucidated with detai

257 p a way for studying the quantum effects and electronic properties of zigzag-phosphorene nanobelts.

258 n iodide perovskites through fine-tuning the electronic property of organic ammonium salts, we came t

259 rption on nanoceria support and the tailored electronic property of Pt(1) via the metal-support inter

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

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

262 design of molecular structures for targeting electronic property optimisation and a clear path toward

263 f electrochemical biosensors thanks to their electronic properties, porous structures, and large surf

264 lected by the strong alteration of the SubPz electronic properties produced by phenyl and biphenyl mo

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

266 ng depends on the crystal morphology and the electronic properties simultaneously.

267 Their optical and electronic properties, small singlet-triplet energy spli

268 ch as silicene) fosters a plethora of exotic electronic properties such as a quantum spin Hall effect

269 tron acceptors with fine-tuned adjustment of electronic properties, such as electron affinities, by t

270 ects are highly sensitive to the interfacial electronic properties, such as electron wavefunction ove

271 iosensors, with an emphasis on structure and electronic properties, synthesis, and biofunctionalizati

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

273 materials, with their unique structural and electronic properties that are unavailable in bulk mater

274 ical electronic quantum phases, with valence electronic properties that are well captured by the Su-S

275 exploited to demonstrate dynamic optical and electronic properties that can be processed on-demand, w

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

277 from their unique local atomic structure and electronic properties that facilitate an efficient react

278 valuable quantitative information about the electronic properties that underpin the functions of the

279 In addition to C-H bonds with varied electronic properties, the Co(II)-based metalloradical s

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

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

282 r electronics is in the fine-tuning of their electronic properties through structural modifications,

283 ed 1,4-thiazine paves the way to enhance the electronic properties, thus successfully achieving highe

284 amide ligand with the appropriate steric and electronic properties to afford the desired products in

285 f the ligand synthesis allows the steric and electronic properties to be fine-tuned and hence the app

286 composition, heterostructure interface, and electronic properties to define the material foundation

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

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

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

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

291 crystals (PNCs) possess alluring optical and electronic properties via compositional and structural v

292 They may stimulate further work on tuning electronic properties via disorder/defect nano-engineeri

293 (1,1'-biaceanthrylene), and the optical and electronic properties were compared.

294 lline solids can be used to manipulate their electronic properties, which are fundamentally influence

295 t triggered by mechanical stimuli to control electronic properties, which are ready to deliver new in

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

297 The proposed sensor showed better electronic properties with an improved synergism.

298 and, where possible, compare their redox and electronic properties with their noninterlocked counterp

299 oparticle is demonstrated by its optical and electronic properties, with metal-like electron-phonon r

300 iew covers the most recent understandings of electronic properties within different scale of biologic