ライフサイエンスコーパス: semiconducting

1 2D c-COFs) are emerging as a unique class of semiconducting 2D conjugated polymers for (opto)electron

2 Here, the magnetization of a semiconducting 2D ferromagnet, i.e., Cr(2) Ge(2) Te(6) ,

3 stance between the consecutive layers of the semiconducting 2D material and dynamically reduces its b

4 aspects of graphene and the new families of semiconducting 2D materials, like transition metal dicha

5 ptimized synthesis of electronically coupled semiconducting 2DP/2D transition metal dichalcogenide va

6 The 1T' phase is fully convertible into the semiconducting 2H phase upon thermal annealing at 400 de

7 c properties of purified, solution-processed semiconducting (6,5) single-walled carbon nanotubes (SWC

8 y results that range from insulating(5-8) or semiconducting(9,10) to metallic-like behaviour(11).

9 LG) stacks in either a semimetallic ABA or a semiconducting ABC configuration with a gate-tunable ban

10 Semiconducting absorbers in high-performance short-wave

11 ics of the defect chemistry and processes in semiconducting alloys is both technologically and theore

12 The knowledge of diffusion processes in semiconducting alloys is very important both technologic

13 ilm exhibit metallic along [100], but remain semiconducting along [010] under application of a magnet

14 on methods, which are predominantly used for semiconducting and hybrid photocatalytic materials will

15 activated electronic transport properties of semiconducting and insulating perovskite oxides.

16 These mechanisms are facilitated by semiconducting and insulating substrates that modify the

17 essure range of 28.2-61.7 GPa, where a mixed semiconducting and metallic feature is observed due to t

18 sively explain why tetragonal FeS shows both semiconducting and metallic responses in contrast to tet

19 is of metallic, ferroelectric, upconversion, semiconducting, and thermoelectric 1D nanocrystals, amon

20 tronic properties of MOFs from insulating to semiconducting, as well as provide a blueprint for the d

21 All contain AuH2(-) molecular units and are semiconducting at P = 1 atm, and some form metallic and

22 This material exhibited semiconducting behavior (bandgap ~1.94 electron volts),

23 ngle crystal transport measurements indicate semiconducting behavior for the anionic radical Ni compl

24 This work provides evidence for intrinsic semiconducting behavior of TaGeIr and serves as an examp

25 ts of single crystals of the MV salts show a semiconducting behavior with a remarkably high conductiv

26 y(0.24)Tb(0.1))(3)O(7-x) (FDTO), which shows semiconducting behavior with reasonable electrical condu

27 ases with decreasing temperature, suggesting semiconducting behavior.

28 anisotropic properties and shows interesting semiconducting behavior.

29 free carriers, while the finite- or zero-gap semiconducting behaviors are revealed in various Si-subs

30 te excellent air stability and high-mobility semiconducting behaviour.

31 of Sb(2)O(3) flakes can be transformed into semiconducting beta-phase under heat and electron-beam i

32 race oxygen sensor based on 2D high-mobility semiconducting Bi(2) O(2) Se nanoplates.

33 holes (or electrons) at the interface of the semiconducting Bi(3.33)(VO(4))(2)O(2) and Bi(46)V(8)O(89

34 2 to a mixture of superconducting Bi2212 and semiconducting Bi2Sr2CuO6+delta (Bi2201) during the shoc

35 ecently, alpha-MoO(3) has been reported as a semiconducting biaxial vdW material capable of sustainin

36 Such interplay is particularly intriguing in semiconducting black phosphorus (BP) due to the highly a

37 A ternary organic semiconducting blend composed of a small-molecule, a con

38 nsequently the optical properties-of organic semiconducting building blocks that are incorporated bet

39 hermally-activated carrier absorption in the semiconducting bulk states.

40 Metallic silver and semiconducting cadmium selenide nanocrystals are deposit

41 esistance end-bonded contacts, a high-purity semiconducting carbon nanotube source, and self-assembly

42 Built on one semiconducting carbon nanotube, it occupies less than ha

43 The combination of the short channel and semiconducting carbon nanotubes (CNT) allows for an exce

44 Precise fabrication of semiconducting carbon nanotubes (CNTs) into densely alig

45 e measurements on individual polymer wrapped semiconducting carbon nanotubes.

46 Controlling the charge transfer between a semiconducting catalyst carrier and the supported transi

47 odetector efficiency by uniformly decorating semiconducting CdSe quantum dots on Si channel (Si-QD).

48 nsition metal dichalcogenides (TMDCs) as the semiconducting channel is motivated by their potential t

49 day relies on the electric-field effect in a semiconducting channel to tune its conductivity from the

50 As the dimensions of the semiconducting channels in field-effect transistors decr

51 symmetry, low coordination numbers, and even semiconducting character with increasing density.

52 erve a 25% reduction in the transport gap of semiconducting CNTs, and a 32% reduction in the band gap

53 nd ultrahigh purity (99.997%) polymer-sorted semiconducting CNTs.

54 for the development of synthetic microporous semiconducting composites, as well as new strategies for

55 c regimes are almost symmetric, those of the semiconducting compound with x = 0.34 in close proximity

56 nt functional shell, Tube(wedge)2 allows the semiconducting conduction pathway to be modulated solely

57 ge rearrangement with the adjacent metal and semiconducting contacts.

58 on the case of the two most studied systems-semiconducting CrI(3) and metallic Fe(3)GeTe(2)-and illu

59 ectivity from atomically thin conducting and semiconducting crystals enables us to exploit these hete

60 rporate rather thick two-dimensional layered semiconducting crystals for reliable vertical diodes sho

61 Ultra-thin two-dimensional semiconducting crystals in their monolayer and few-layer

62 ased on a deeply depleted graphene-insulator-semiconducting (D(2)GIS) junction, which offers the poss

63 le were chemically assembled on H-terminated semiconducting degenerate-doped n-type Si(111) substrate

64 lusters as a solution-processed material for semiconducting devices.

65 nsistors as powerfully as they have in other semiconducting devices.

66 nologies, doping plays a crucial role in all semiconducting devices.

67 selective transformation of the cylindrical semiconducting domain into discrete spheres while keepin

68 Dielectric, semiconducting, electrically conducting, and ionically c

69 f a probe, and with the simple design of one semiconducting electrode, one electrical lead and a sing

70 Combining the semiconducting energy gap, the 100% spin polarized valen

71 on and solid state reduction of metallic and semiconducting enriched HiPco SWCNTs.

72 to conductive behaviour at charged walls in semiconducting ErMnO3.

73 r films can electronically couple and become semiconducting, exhibiting electric field effect and pho

74 s a material with combined ferroelectric and semiconducting features could be a promising solution fo

75 A sol-gel method for the synthesis of semiconducting FeCrAl oxide photocathodes for solar-driv

76 rons and holes, a possibility if MAPbI3 is a semiconducting ferroelectric, which, however, requires c

77 Semiconducting ferromagnet-nonmagnet interfaces in van d

78 es featuring stripes of metallic TaTe(2) and semiconducting FeTe(2), alpha-TaFeTe(4) and beta-TaFeTe(

79 As a result, our fabricated semiconducting film can be stretched up to 100% strain w

80 by ultrasonication produces a gold-coloured, semiconducting fluoropolymer.

81 t the nanoscale, comprising metallic (Au) or semiconducting ([Formula: see text]) nanostructures and

82 entional clathrates with unprecedented III-V semiconducting frameworks have been synthesized: Cs(8)In

83 with quasiparticles injection across a rigid semiconducting gap.

84 trate, we produce large area two-dimensional semiconducting GaS of unit cell thickness ( approximatel

85 nternal non-contacting continuous domains; a semiconducting glass between two conductors.

86 rlattice of zero-energy modes into otherwise semiconducting GNRs.

87 ay for potential applications in spintronics.Semiconducting graphene nanoribbon provides a platform f

88 Unlike graphene, semiconducting graphene nanoribbons do not have free ele

89 s to be an ordered composite of uniform-size semiconducting graphene quantum dots laterally integrate

90 The energy band gaps of 2D semiconducting Group 15 monolayers cover a wide range fr

91 bandgaps, represents an important target for semiconducting halide perovskites, but has so far proven

92 ed diblock polymer (PEG-Py) to encapsulate a semiconducting, heavy-atom-free pyrrolopyrrolidone-tetra

93 nd alignment of vertically stacked WS2 /MoS2 semiconducting heterobilayers and finite density of stat

94 Here, using semiconducting heterostructures assembled from incommens

95 ot perturb the ordered microstructure of the semiconducting host.

96 minescence was observed thanks to the use of semiconducting hybrid IOPCs material even at 0 V.

97 nd the field into a more diverse subgroup of semiconducting hybrids that possesses even higher tunabi

98 d gap transforming graphene from metallic to semiconducting in a continuous way.

99 ilms by a blow-spinning technique, including semiconducting indium-gallium-zinc oxide (IGZO) and copp

100 his effect may be explained by deposition of semiconducting iron oxide particles within LSLs.

101 n transistor comprises a small conducting or semiconducting island separated from two metallic reserv

102 Analogous to a depleted metal-oxide-semiconducting junction, photo-generated charge collects

103 ic tubes generate a high density of metallic-semiconducting junctions but cannot form a percolated me

104 Here, we show that metallic-semiconducting junctions in aptasensors are sensing hots

105 vice response occurs when gating at metallic-semiconducting junctions.

106 Ultrathin two-dimensional (2D) semiconducting layered materials offer great potential f

107 rical transport property measurements of the semiconducting layers in complete Si solar cells.

108 ower generation from nanoscale conducting or semiconducting layers in contact with moving aqueous dro

109 o study the photo-response of photosensitive semiconducting layers or patterns in an environment imit

110 en photonic and electronic performance of 2D semiconducting layers, and demonstrates that they are no

111 is argued that in the observed high-pressure semiconducting Li phase (oC40, Aba2), an example of such

112 eld the quantum wells show a transition from semiconducting-like to metallic behaviour with decreasin

113 ctivity and could lead to the realization of semiconducting, magnetic, and topologically insulating M

114 Schottky barrier diode (SBD) prepared from a semiconducting material poly-(9,9-dioctylfluorene) (F8).

115 ock modulation of semimetallic graphene to a semiconducting material with controllable bandgap has th

116 a crucial feature for two-dimensional (2-D) semiconducting material-based image sensor applications.

117 ing interactions, which render this series a semiconducting material.

118 ine the best features of metals or inorganic semiconducting materials (excellent electrical and optic

119 Organic semiconducting materials (OSMs) composed of pai-conjugat

120 The optical and electronic properties of semiconducting materials are of great importance to a va

121 High-performance organic semiconducting materials are reliant upon subtle changes

122 ghly desirable trait, opening ways to design semiconducting materials based on tunable III-V clathrat

123 block in the syntheses of efficient organic semiconducting materials during the past decade.

124 rid) perovskites have emerged as competitive semiconducting materials for photovoltaic devices due to

125 Two-dimensional semiconducting materials of the transition-metal-dichalc

126 or a new family of organic, microporous, and semiconducting materials with high surface areas and hig

127 stors demonstrating that SBT can enable good semiconducting materials with hole mobilities ranging fr

128 However, air-stable ultrathin semiconducting materials with superior performances rema

129 with functional materials such as graphene, semiconducting materials, and piezoelectric polymers.

130 alize the solid-state laser refrigeration of semiconducting materials, are discussed.

131 ion demonstrate their promising potential as semiconducting materials, exhibiting high current on/off

132 y pseudospin via magnetic dopants in layered semiconducting materials, paving the way toward magneto-

133 enide takes advantage of the high quality of semiconducting materials, reliability in fabricating arr

134 particularly problematic for lone-pair-rich, semiconducting materials, such as phase-change materials

135 in lead-halide perovskites-cheap, versatile semiconducting materials-it is critical to examine their

136 s attest the potential of these materials as semiconducting materials.

137 cs in light-harvesting protein complexes and semiconducting materials.

138 ing in the rational design of small molecule semiconducting materials.

139 cenes comprise an important class of organic semiconducting materials.

140 nsely enrich property-tuning capabilities of semiconducting materials.

141 While the chemical composition of semiconducting metal halide perovskites can be precisely

142 forming atomically precise GNRs directly on semiconducting metal oxide surfaces.

143 aterials, including graphene, boron nitride, semiconducting metal oxides, and transition metal chalco

144 and surface-supported synthesis of metallic, semiconducting, metal oxide, and carbon-based nanomateri

145 ique sensor design with an array of nanofilm semiconducting/metal electrode interface, functionalized

146 eal "hidden" spectral features, connected to semiconducting, metallic and magnetic properties of soli

147 thin and flexible rectenna based on a MoS(2) semiconducting-metallic-phase heterojunction with a cuto

148 sulfurization process that directly converts semiconducting molten stibnite (Sb2S3) into pure (99.9%)

149 sis of heterostructures made of single-layer semiconducting molybdenum disulfide contacting conductiv

150 s of multiple split-gates with nanogaps on a semiconducting MoS(2) channel connected to the source/dr

151 en the 1T'-MoTe(2) (semimetallic) phase to a semiconducting MoTe(2) phase in a field-effect transisto

152 d digital electronics using ZnO and/or other semiconducting nanomaterial.

153 from a broad spectrum of materials spanning semiconducting nanomaterials to organic molecular dyes,

154 the chemical and photophysical properties of semiconducting nanoparticles (NPs).

155 nt experiments and calculations suggest that semiconducting nanoparticles could act as efficient volt

156 m-confined Stark effect in membrane-embedded semiconducting nanoparticles, examines their possible ut

157 to switch from an impermeable semimetal to a semiconducting nanosieve.

158 Semiconducting nanostructures are one of the potential c

159 Well-ordered and highly interconnected 3D semiconducting nanostructures of bismuth sulphide were p

160 o a full superconducting shell surrounding a semiconducting nanowire core.

161 m trans-configuration and self-assemble into semiconducting nanowires.

162 a temperature dependence consistent with the semiconducting nature of the TI film and freeze-out of b

163 tion is stable and preserves the monolayer's semiconducting nature, along with other attractive chara

164 P-type semiconducting NiO thin film was deposited by RF sputter

165 aggregation-induced emission (AIE) dyes and semiconducting oligomer/polymer nanoparticles (SONs/SPNs

166 This is often accompanied by semiconducting or insulating behavior.

167 nic/molecular conductivity in conducting and semiconducting organic polymers and small molecules, the

168 ermolecular electron transfer, parallel to a semiconducting oxide electrode, was shown to be more rap

169 Interaction of molecular oxygen with semiconducting oxide surfaces plays a key role in many t

170 oach to passivate the surface of a versatile semiconducting oxide, zinc oxide (ZnO), evoking a self-a

171 of multishell nanotubes combining different semiconducting oxides and metal nanoparticles is as well

172 to surface passivation will allow the use of semiconducting oxides in a variety of different electron

173 allic MoS2 showing high responsivity and the semiconducting phase exhibiting high on/off ratios.

174 norganic hybrid perovskites with metallic or semiconducting phases of 2D MoS2 nanosheets via solution

175 Semiconducting photocatalytic solar-hydrogen conversion

176 electrochemical reaction on the surface of a semiconducting photoelectrode.

177 echnologically advanced systems are based on semiconducting photoelectrodes.

178 ation and mechanochemical unzipping to yield semiconducting polyacetylene-based block copolymers.

179 ent in response to mechanical force to yield semiconducting polyacetylene.

180 nescent nanoprobe, composed of a fluorescent semiconducting polymer and palladium complex, for quanti

181 A thin layer of nondoped semiconducting polymer at the perovskite/HTL interface i

182 We herein report an all-in-one fluorescent semiconducting polymer based far-red to near-infrared (N

183 Melt-processing of complementary semiconducting polymer blends provides an average charge

184 y is reported based on a rationally designed semiconducting polymer brush (SPPF).

185 Bright long-wavelength-excitable semiconducting polymer dots (LWE-Pdots) are highly desir

186 Semiconducting polymer dots (Pdots) and conjugated-polym

187 Semiconducting polymer dots (Pdots) have recently been p

188 pe of fluorometric ICTS based on ultrabright semiconducting polymer dots (Pdots) in which the traffic

189 we report a probe of lanthanide-coordinated semiconducting polymer dots (Pdots), which possess fluor

190 ese phenomena, we developed a novel class of semiconducting polymer dots that can operate in two supe

191 ene glycol-based side chains, as a promising semiconducting polymer for accumulation-mode organic ele

192 e integration of photochromic molecules into semiconducting polymer matrices via blending has recentl

193 Here we present semiconducting polymer nanoparticles (SPNs) <40 nm in di

194 Semiconducting polymer nanoparticles (SPNs) emerge as at

195 Additionally, we used highly fluorescent semiconducting polymer nanoparticles to visually assess

196 nic imaging agents, small organic molecules, semiconducting polymer nanoparticles, and nonlinear PA-i

197 Herein, we report the synthesis of a semiconducting polymer nanoprodrug (SPNpd) that not only

198 PDs) by doping tributyl phosphate (TBP) in a semiconducting polymer poly[9,9-dioctylfluorenyl-2,7-diy

199 tructure-property relationships required for semiconducting polymer repeat units to ensure optimal ba

200 However, controlling the chain dynamics of semiconducting polymer thin films and understanding the

201 Thienoisoindigo-based semiconducting polymer with a strong near-infrared absor

202 ment encoded in the spectral response of the semiconducting polymer, and correlate chain packing with

203 xceeds other known materials such as organic semiconducting polymers (<1 cm(2) V(-1) s(-1) ), amorpho

204 eractions between photochromic molecules and semiconducting polymers are far from being fully underst

205 Semiconducting polymers are versatile materials for sola

206 It has been demonstrated that LBG semiconducting polymers based on electron-donor units co

207 effects of disorder on the TE properties of semiconducting polymers based on the Gaussian disorder m

208 Here, we present a series of semiconducting polymers designed to elucidate important

209 e of totally disintegrable and biocompatible semiconducting polymers for thin-film transistors.

210 Solution processable semiconducting polymers have been under intense investig

211 otential applications of these disintegrable semiconducting polymers in low-cost, biocompatible, and

212 The charge-carrier mobility of organic semiconducting polymers is known to be enhanced when the

213 dox-active materials based on conducting and semiconducting polymers represent an exciting class of m

214 behaviors are also observed in other common semiconducting polymers such as poly(3-hexyl thiophene)

215 Molecular dopants are often added to semiconducting polymers to improve electrical conductivi

216 Three n-type fused lactam semiconducting polymers were synthesized for thermoelect

217 IDT-type units, guiding the design of novel semiconducting polymers with extended fused backbones fo

218 e effective design rules for approaching LBG semiconducting polymers with high molar absorptivity, su

219 we present a design concept for stretchable semiconducting polymers, which involves introducing chem

220 severely limited by the hole mobility of LBG semiconducting polymers, which is significantly lower th

221 bility control is a patterning technique for semiconducting polymers, which utilizes the reduction in

222 s an attractive strategy to high performance semiconducting polymers.

223 rs of diketopyrrolopyrrole-based (DPP-based) semiconducting polymers.

224 study reports the development of an organic semiconducting pro-nanoenzyme (OSPE) with a photoactivat

225 The interplay between semiconducting properties and ferroelectricity in this t

226 icate nanographenes with a broad spectrum of semiconducting properties and high charge mobilities.

227 technologically useful manner.Integration of semiconducting properties into the basic topological mot

228 rmining the surface electronic structure and semiconducting properties of hybrid perovskites.

229 (1-x)N as a class of materials combining the semiconducting properties of main-group wurtzite nitride

230 n opportunity to integrate ferromagnetic and semiconducting properties through the Rasbha effect for

231 lms of the macrocycle show that they exhibit semiconducting properties with a redox-conductivity of u

232 Such materials combine semiconducting properties with tailored surface chemistr

233 However, the routine integration of semiconducting properties, particularly long-range elect

234 g mode, in combination with the demonstrated semiconducting property of octabenzo[8]circulene, sugges

235 talline morphology formation for spin-coated semiconducting PTB7 (poly[[4,8-bis[(2-ethylhexyl)oxy]ben

236 in texture in monolayer, centrosymmetric and semiconducting PtSe2 film without the characteristic spi

237 ultrathin body, but problems such as limited semiconducting purity and non-ideal assembly still need

238 mbled carbon nanotube arrays with over 99.9% semiconducting purity, and the complementary feature was

239 ha-CsPbI(3) QDs) as a newly emerging type of semiconducting QDs hold tremendous promise for fundament

240 The well-studied physics of semiconducting QDs suggests that the dimer coherences ca

241 Semiconducting quantum dots (QDs) and magnetic nanoparti

242 ging light-harvesting nanomaterials, such as semiconducting quantum dots (QDs), metal nanoparticles,

243 Compared to common semiconducting quantum dots, C-Dots have good physicoche

244 ccess to single spins, demonstrated in III-V semiconducting quantum dots, has fueled research aimed a

245 Similar to quantum-confined, semiconducting quantum dots, the electrical coupling in

246 hyperbolic metasurfaces, wherein distributed semiconducting quantum wells display extreme absorption

247 n intensity enhancement relative to the bare semiconducting quantum wells.

248 However, robust implementations of semiconducting qubits must overcome the effects of charg

249 a wire-like material that can also integrate semiconducting sequences into the framework of DNA mater

250 straightforward method by which to integrate semiconducting sequences, site-specifically, into the fr

251 was developed and used to uniformly deposit semiconducting single-wall carbon nanotube (SWCNT)-based

252 k leverages the unique optical properties of semiconducting single-wall carbon nanotubes (SWCNTs) to

253 thographic generation of OCCs on solid-state semiconducting single-walled carbon nanotube films at sp

254 larly tunable fluorescent quantum defects in semiconducting single-walled carbon nanotube hosts throu

255 Composed of a semiconducting single-walled carbon nanotube nested in a

256 in the molarity of any structurally enriched semiconducting single-walled carbon nanotube preparation

257 High-purity semiconducting single-walled carbon nanotubes (s-SWNTs)

258 Chirality-selective functionalization of semiconducting single-walled carbon nanotubes (SWCNTs) h

259 Semiconducting single-walled carbon nanotubes are one-di

260 molybdenum disulfide and solution-processed semiconducting single-walled carbon nanotubes to emulate

261 e show that optical excitation of individual semiconducting single-walled carbon nanotubes triggers s

262 ty organic single crystals, based on various semiconducting small molecules on virtually any substrat

263 , including models of realistic metallic and semiconducting solids.

264 rmi level crosses a van Hove singularity for semiconducting species.

265 g conversion to the thermodynamically stable semiconducting state (2H) when mildly annealed in a nitr

266 Full device relaxation back to a semiconducting state is accomplished by annealing in vac

267 s and nanoribbons directly on insulating and semiconducting surfaces.

268 t thin-film transistors fabricated from long semiconducting SWCNTs exhibit a carrier mobility as high

269 Semiconducting SWNTs of varying length suspended with so

270 Semiconducting SWNTs were imaged during dielectrophoreti

271 graphene transferred onto polystyrene (PS), semiconducting thienoazacoronene (EH-TAC), gold, and als

272 This strategy is universally valid for other semiconducting TMD materials, either p-doped or n-doped,

273 ransition-metal dichalcogenides (m-TMDs) and semiconducting TMDs (s-TMDs).

274 n switch continuously from a low-conductance semiconducting to a high-conductance metallic state.

275 sistivity studies reveal a transition from a semiconducting to a metallic phase with decreasing tempe

276 monitored at doping level spanning from the semiconducting to the metallic limit.

277 In addition, a single-step integration of semiconducting/transducer polymer poly(3-octylthiophene)

278 ons of charged excitons (trions) observed in semiconducting transition metal dichalcogenides (TMDCs).

279 s heterostructure built from atomically thin semiconducting transition metal dichalcogenides (TMDs) e

280 remarkable electronic properties of layered semiconducting transition metal dichalcogenides (TMDs) m

281 roperties of atomically thin two-dimensional semiconducting transition metal dichalcogenides enable i

282 cate that bulk ReS(2) and ReSe(2) are unique semiconducting transition metal dichalcogenides having s

283 Charge carriers in semiconducting transition metal dichalcogenides possess

284 cting graphene, insulating boron nitride and semiconducting transition metal dichalcogenides.

285 -achieved via a van der Waals contact with a semiconducting transition-metal dichalcogenide(8-21)-to

286 the majority of related research focuses on semiconducting transition-metal dichalcogenides (for exa

287 Two-dimensional (2D) layered semiconducting transition-metal dichalcogenides (TMDCs)

288 Monolayer semiconducting transition-metal dichalcogenides (TMDs) r

289 titution doping for chemical-vapor-deposited semiconducting transition-metal-dichalcogenide monolayer

290 Monolayer semiconducting transitional metal dichalcogenides have e

291 Unlike quantum dots, however, semiconducting transport has not been reported in Au nan

292 current formulations providing at least 99% semiconducting tube content.

293 However, it usually suffers from low semiconducting tube purity, low device yield, and the mi

294 Miniaturized photonic sources based on semiconducting two-dimensional (2D) materials offer new

295 For semiconducting two-dimensional transition-metal dichalco

296 van der Waals (vdW) heterojunctions between semiconducting two-dimensional transition-metal dichalco

297 High-mobility semiconducting ultrathin films form the basis of modern

298 Films with R = 0.6 were semiconducting with visible light transmission due to a

299 These results revealed that semiconducting WS2 thin film works as a metallic conduct

300 l detection of strongly correlated phases in semiconducting WSe(2)/WS(2) moire superlattices.