ライフサイエンスコーパス: heterostructure

1 e using a halide perovskite/oxide perovskite heterostructure.

2 l magnetization in a ferromagnetic thin film heterostructure.

3 ne electrodes are introduced to an AlGaN/GaN heterostructure.

4 optical excitation of a metal/semiconductor heterostructure.

5 tching in a polycrystalline PtMn/Pt metallic heterostructure.

6 ted V(2)O(3)/PMN-PT [Pb(Mg,Nb)O(3)-PbTiO(3)] heterostructure.

7 metal phase in a BaTiO(3)/SrRuO(3)/BaTiO(3) heterostructure.

8 o(0.4)Fe(0.4)Zr(0.1)Y(0.1)O(3-delta)-ZnO p-n heterostructure.

9 ross section of the BiFeO(3) /TbScO(3) (001) heterostructure.

10 to TiO(2) in a rationally designed Ni-TiO(2) heterostructure.

11 y and promotion of ionic conductivity in the heterostructure.

12 ve capacitance in a ferroelectric-dielectric heterostructure.

13 y and electronic properties of the composite heterostructure.

14 ast excited state dynamics in the 2DP/MoS(2) heterostructure.

15 polylactic acid junctions in the 3D-printed heterostructure.

16 nt growth of other Janus materials and their heterostructures.

17 (4):PEA(2)SnI(4) interfaces in 2D perovskite heterostructures.

18 , metastable crystal structures, and complex heterostructures.

19 ion of components for vertical van der Waals heterostructures.

20 s Hall effect in Cr(2) Ge(2) Te(6) /tantalum heterostructures.

21 ent ferroelectricity in graphene-based moire heterostructures.

22 uantum phenomena in 2DP hybrid van der Waals heterostructures.

23 tch to control ferroelectricity in thin-film heterostructures.

24 date the complex physics of moire engineered heterostructures.

25 -dimensional electron gases in semiconductor heterostructures.

26 covalent triazine frameworks etc.) and their heterostructures.

27 echnological route for up-scalable films and heterostructures.

28 or automating the fabrication process of vdW heterostructures.

29 g-controlled orbital occupancy in perovskite heterostructures.

30 ers, and potentially fabrication of other 2D heterostructures.

31 rying the geometry of Si-Au slanted columnar heterostructures.

32 ies to engineer the device performance of 2D heterostructures.

33 or precise engineering of optimized skyrmion heterostructures.

34 array of novel physical properties in oxide heterostructures.

35 structure of titanate films, substrates, and heterostructures.

36 op of the TMDC templates to realize vertical heterostructures.

37 d layer-by-layer to form van der Waals (vdW) heterostructures.

38 in the strong spin-orbit regime in graphene heterostructures.

39 mergent phenomena at oxide interfaces and in heterostructures.

40 properties of nanoscale materials and their heterostructures.

41 of the highly-porous Si-Au slanted columnar heterostructures.

42 terlayer excitons in vertical MoSe(2)-WSe(2) heterostructures.

43 a potentially scalable synthesis of twisted heterostructures.

44 ter interactions in 2D materials and related heterostructures.

45 in angle-twisted semiconductor van der Waals heterostructures.

46 systems in thin film, and possibly in bulk, heterostructures.

47 irst thickness-dependent study of 2DP/MoS(2) heterostructures.

48 ionic devices based on van der Waals layered heterostructures.

49 face of similar and dissimilar van der Waals heterostructures.

50 citonic(5) and topological phenomena(6-8) in heterostructures.

51 tuning symmetries via strain engineering and heterostructuring.

52 ng, and offer an alternative to conventional heterostructuring.

53 led vertical InSe/black phosphorus (BP)(5-9) heterostructures(10).

54 eport that CTEs can be effectively formed in heterostructured 2D perovskites prepared by mixing PEA(2

55 nd systems realized in twisted van der Waals heterostructures(3-6).

56 he capacitance of a ferroelectric-dielectric heterostructure(4,7,14) or improving the subthreshold sw

57 semiconductor devices based on van der Waals heterostructures(9).

58 exploring proximity effects in van der Waals heterostructures(9-12).

59 thesis of one-dimensional (1D) van der Waals heterostructures, a class of materials where different a

60 Thus, planar heterostructures allow p-n junctions between different t

61 es(12-14) of transition metal dichalcogenide heterostructures allow us to optically create and invest

62 gradient of the bandgap across the monolayer heterostructure allows for the fabrication of heterogene

63 In addition, such heterostructures also exhibited superior activity toward

64 are electrically controlled in such a PE/FM heterostructure and how a back-voltage is generated due

65 remote impurities in the doping layer of the heterostructure and surface roughness and impurity (dang

66 i-, and multimetallic nanoframes, as well as heterostructured and hybrid systems.

67 into how to manipulate topological modes in heterostructures and also provides a basis for recent ex

68 stacking layers of such materials to create heterostructures and can be further boosted by applying

69 In addition, we create artificial heterostructures and hybridize their physical properties

70 erministic fabrication of arbitrary vertical heterostructures and multi-heterostructures of Ruddlesde

71 ) (BZT)/Ba(0.7)Ca(0.3)TiO(3) (BCT) epitaxial heterostructures and studied their structural, dielectri

72 ns are performed for H(x) SmNiO(3) /SrRuO(3) heterostructures, and a Mottronic device is achieved.

73 h high-kappa dielectric gates, van der Waals heterostructures, and metallic interfaces between insula

74 Mo(2)AlB(2) and Mo(2)AlB(2)-AlO(x) nanosheet heterostructures, and opens the door to other previously

75 Through our semiconductor heterostructure approach, our results provide insight in

76 onductor nanostructures and 2D van der Waals heterostructures are also stressed.

77 na in electronically coupled two-dimensional heterostructures are central to next-generation optical,

78 d growing various vertical/lateral TMD-based heterostructures are discussed.

79 properties in ferroelectric oxide films and heterostructures are explored.

80 Spintronic ferromagnetic/non-magnetic heterostructures are novel sources for the generation of

81 diffraction verifies that all shells in the heterostructures are single crystals.

82 Three-dimensional heterostructures are usually created either by assemblin

83 ve FET device, involving the epitaxial oxide heterostructure as an ideal material platform for maximu

84 the potential use of Si-Au slanted columnar heterostructures as a highly porous plasmonic sensor wit

85 onic states in two-dimensional van der Waals heterostructures, as recently demonstrated in the correl

86 henomenon is detected in the Bi(2)Te(3)/FeTe heterostructure associated with the superconducting tran

87 de a large interfacial DMI in TI/ferrimagnet heterostructures at room temperature, resulting in small

88 f the transport properties of SrTiO(3)-based heterostructures at room temperature, while the heterost

89 Herein, a novel heterostructure based on a combination of RuMo nanoalloy

90 (20)B(20)/Pb(Mg(1/3)Nb(2/3))(0.7)Ti(0.3)O(3) heterostructures based on a pseudo-magnetization u = m(x

91 also present results for 2 other foam-based heterostructures based on Kelvin and C15 foams that have

92 Epitaxial heterostructures based on oxide perovskites and III-V, I

93 approach to realise a variety of functional heterostructures based on van der Waals nanocrystal film

94 crystals are of interest for fabricating the heterostructure-based spintronics device.

95 on metal dichalcogenides and graphite/SiO(x) heterostructures beyond the widely accepted van der Waal

96 ensional materials, which exists these days, heterostructures, both vertical (van der Waals) and in-p

97 A van der Waals heterostructure built from atomically thin semiconductin

98 be tailored and probed in spin-orbit coupled heterostructures by engineering subtle structural modula

99 e metal-insulator transitions (MIT) in oxide heterostructures by inducing interfacial oxygen vacancy

100 We systematically studied the TiO(2)/VO(2) heterostructures by structural and transport measurement

101 ation in a heavy metal (HM)/ferromagnet (FM) heterostructure can be regulated to a certain degree usi

102 o-optoelectronic properties of Van der Waals heterostructures can enable unprecedented platforms for

103 emonstrate that epitaxial Mn(3)GaN/permalloy heterostructures can generate unconventional spin-orbit

104 work shows how rational design of colloidal heterostructures can result in materials with significan

105 erfaces and bulk properties of the resulting heterostructures challenge our fundamental understanding

106 Two-dimensional heterostructures combined with vertical geometries are c

107 nificant performance enhancements in abraded heterostructures compared to those fabricated through in

108 We describe here an unconventional heterostructure composed of strongly coupled Ni-deficien

109 Artificial heterostructures composed of dissimilar transition metal

110 are stable black-phase CsPbI(3) by forming a heterostructure comprising 0D Cs(4) PbI(6) and gamma-CsP

111 tretching platform: two dimensional in-plane heterostructure comprising graphene and hexagonal boron

112 c properties, potentially offering unlimited heterostructure configurations for exploration.

113 Here we report Coulomb blockade in a vdW heterostructure consisting of a transition metal dichalc

114 the end of Josephson junctions realized on a heterostructure consisting of aluminium on indium arseni

115 We also report a 5-nanometer-diameter heterostructure consisting of an inner SWCNT, a middle t

116 We use van der Waals heterostructures consisting of a graphene monolayer rota

117 nts were synthesized, and many form triphase heterostructures consisting of either three-interface or

118 improved in hybrid metal semiconductor nano-heterostructures consisting of perovskite semiconductors

119 rts and a plethora of function-designable 1D heterostructures could be realized.

120 Engineered heterostructures create new functionality by integrating

121 inetics and the robust growth of 2D vertical heterostructures, defining a versatile material platform

122 on typical 2D N-doped carbon/RuMo nanoalloys heterostructures demonstrate that introducing N and Mo a

123 ransition metal dichalcogenide van der Waals heterostructures, demonstrate direct exfoliation of the

124 ion of nickelates(5,6), as well as thin-film heterostructures designed to host superconductivity.

125 ties of moire superlattices in van der Waals heterostructure devices is a critically needed diagnosti

126 lar dynamics simulations confirm the reduced heterostructure disorder and larger vacancy formation en

127 The heterostructure domains of 1T-MoS(2) and C(60) NSs exhib

128 nal (2D) layered materials and van der Waals heterostructures due to their intrinsic ultrahigh surfac

129 The 30 % Pt/LiCoO(2) heterostructured electrocatalyst delivers low overpotent

130 , multifunctional active-center-transferable heterostructured electrocatalysts, platinum/lithium coba

131 Initial studies of heterostructured electrodes are compared to state-of-the

132 LaMnO(3) /SrTiO(3) (LMO/STO) polar-nonpolar heterostructures, electronic reconstruction leads to an

133 que mesoporous WS(2) @graphene van der Waals heterostructures ensures the ready access of active site

134 Heterostructures exhibit considerable potential in the f

135 Such rationally designed heterostructures exhibit interesting interlayer properti

136 It is shown that the SnSe/MoS(2) vdW heterostructure exhibits excellent p-n diode rectifying

137 (2)CuO(4)/La(2-x)Sr(x)CuO(4) (LSCO/LCO/LSCO) heterostructures fabricated using atomic layer-by-layer

138 Structurally, these twisted heterostructures feature atomic reconstruction and domai

139 vertical displacement field, the ABC-TLG/hBN heterostructure features an isolated flat valence miniba

140 that graphene-insulator-metal is a promising heterostructure for optically controlled and electricall

141 nts show the topological Hall effect in this heterostructure for temperatures below 100 K.

142 hod for rational fabrication of carbon-metal heterostructures for highly efficient electrocatalysis.

143 icial excitonic crystals using van der Waals heterostructures for nanophotonics and quantum informati

144 providing a new approach to designing oxide heterostructures for novel ionotronics and neuromorphic-

145 lms, and their integration into advanced MTI heterostructures for quantum device applications.

146 for the synthesis of multi-component organic heterostructures for various functions.

147 ures, akin to two-dimensional material-based heterostructures, for enhancing device functionalities(8

148 Van der Waals heterostructures form a unique class of layered artifici

149 lattice mismatch, making them promising for heterostructure formation and semiconductor integration(

150 ly stable self-assembled lead-tin perovskite heterostructures formed between low-bandgap 3D and highe

151 layer-resolved magnetic proximity effect in heterostructures formed by monolayer WSe(2) and bi/trila

152 The proliferation of van der Waals (vdW) heterostructures formed by stacking layered materials ca

153 In van der Waals heterostructures formed by stacking two monolayer semico

154 erials, and pave the way for the creation of heterostructures from 2D Janus layers.

155 A new type of multiferroic heterostructure has been proposed in this work with stro

156 Nanomaterials that form as heterostructures have applications in catalysis, plasmon

157 Interfaces in heterostructures have been a key point of interest in co

158 Although several epitaxial vdW heterostructures have been achieved experimentally, the

159 Fullerene-based low-dimensional (LD) heterostructures have emerged as excellent energy conver

160 Semiconductor heterostructures have enabled a great variety of applica

161 Moire superlattices in van der Waals heterostructures have given rise to a number of emergent

162 Previously, such twisted heterostructures have involved a single planar interface

163 triction effect in piezoelectric/ferromagnet heterostructures holds promise for ultra-low energy info

164 he unconventional interlayer coupling in vdW heterostructures (HSs) by utilizing an emerging 2D mater

165 ition metal dichalcogenides (TMDCs) vertical heterostructures in terms of the nucleation and kinetics

166 eans of a Na (x) CoO(2)/CeO(2) semiconductor heterostructure, in which a field-induced metallic state

167 of new quantum phenomena in two-dimensional heterostructures, in which the interactions between the

168 lution in a variety of twisted van der Waals heterostructures including, but not limited to, conducti

169 tructures and the catalytic functions of the heterostructures, including the role of the fullerenes,

170 onal design of opto-electronic van der Waals heterostructures incorporating 2D semiconductors.

171 ed physical dimension, chemical composition, heterostructure interface, and electronic properties to

172 c field that originates from band bending at heterostructure interfaces induces polar symmetry therei

173 Our study enriches the functionalities of heterostructure interfaces, offering a distinctive appro

174 erostructures at room temperature, while the heterostructure is forming.

175 However, the practical realization of such heterostructures is challenging because of the difficult

176 ical Hall effect) in magnetic thin films and heterostructures is discussed.

177 logical structures in ferroic thin films and heterostructures is explored, including the observation

178 In this way, a family of vertical TMDCs heterostructures is successfully designed.

179 ternative methods that enable preparation of heterostructured materials is desired.

180 hancement mechanism for Ti(3)C(2)T(x)/WSe(2) heterostructured materials is proposed for highly sensit

181 amental control of magnetic coupling through heterostructure morphology is a prerequisite for rationa

182 highly stable and tunable lateral epitaxial heterostructures, multiheterostructures and superlattice

183 Herein, a library of heterostructured, multimetallic (Pt, Pd, Rh, and Au) tet

184 ructural nanocrystals such as core-shell and heterostructured nanocrystals, well-defined multimetalli

185 Strategies to synthesize heterostructured nanoparticles are emerging, but they ar

186 on measurements show that the domains of the heterostructured nanoparticles are epitaxially aligned.

187 Multimetallic heterostructured nanoparticles with high-index facets po

188 xhibit low-index facets, Pt and Au form PtAu heterostructured nanoparticles with high-index facets, i

189 es and under different conditions within the heterostructured nanoparticles.

190 ons, that enable the rational synthesis of a heterostructured nanorod megalibrary.

191 We experimentally observe 113 individual heterostructured nanorods and demonstrate the scalable p

192 Previously unimaginable complexity in heterostructured nanorods is now routinely achievable wi

193 Waals materials and their vertically stacked heterostructures, new mass-scalable production routes wh

194 ional SnSe nanosheets (NSs) and Au/SnSe nano-heterostructure (NHS) prepared by a simple and economica

195 Van der Waals heterostructures obtained via stacking and twisting have

196 udy of the metamagnetic/ferroelectric hybrid heterostructure of a quenched FeRh thin film (25 nm) gro

197 The heterostructure of monolayer transition metal dichalcoge

198 particle is reported, "polaronic trion" in a heterostructure of MoS(2) /SrTiO(3) (STO).

199 euromorphic image sensor array is based on a heterostructure of MoS(2) and poly(1,3,5-trimethyl-1,3,5

200 Vertical van der Waals (vdW) heterostructures of 2D crystals with defined interlayer

201 ly, its superlattice nature may make various heterostructures of [MnBi(2)Te(4)] and [Bi(2)Te(3)] laye

202 Here we report sub-terahertz spin pumping in heterostructures of a uniaxial antiferromagnetic Cr(2)O(

203 refore, introduce Gaussian synapses based on heterostructures of atomically thin two-dimensional (2D)

204 The electronic properties of heterostructures of atomically thin van der Waals crysta

205 exchange bias are demonstrated in all-oxide heterostructures of BiFeO(3) (BFO) and La(0.7) Sr(0.3) M

206 y such embedded topological states (ETSs) in heterostructures of GeTe (normal insulator) and [Formula

207 d demonstrate two-dimensional self-assembled heterostructures of graphene oxide and polyamine macromo

208 owever, epitaxial growth of atomically sharp heterostructures of halide perovskites has not yet been

209 By employing heterostructures of monolayer TMDs, we realize optical a

210 Van der Waals heterostructures of monolayer transition metal dichalcog

211 The crystal phase-based heterostructures of noble metal nanomaterials are of gre

212 eterministic fabrication of arbitrarily long heterostructures of periodically repeating bismuth-nanoc

213 rbitrary vertical heterostructures and multi-heterostructures of Ruddlesden-Popper perovskites with g

214 Here, using van der Waals heterostructures of twisted double bilayer graphene (TDB

215 and enables the synthesis of epitaxial nano-heterostructures of unprecedented complexity.

216 Van der Waals materials and their heterostructures offer a versatile platform for studying

217 Our study shows that ABC-TLG/hBN heterostructures offer attractive model systems in which

218 ational flexibility enabled by van der Waals heterostructures offers significant opportunities for ar

219 iscuss its potential for creating artificial heterostructures or superlattices beyond the reach of ex

220 We report the two-dimensional (2D) natural heterostructure [Pb(3.1)Sb(0.9)S(4)][Au (x)Te(2- x)] ( x

221 with existing atomic resolution sensors, the heterostructure platform paves the way for sequencing DN

222 do physics or isolated quantum bits in a vdW heterostructure platform.

223 magnetization measurements reveal that this heterostructure possesses a metallic phase with high con

224 equilibrium systems, the chemically-specific heterostructures predicted here are lattice-matched, sho

225 magnet-nonmagnet interfaces in van der Waals heterostructures present a unique opportunity to investi

226 lex oxide heterointerfaces and van der Waals heterostructures present two versatile but intrinsically

227 band alignment in this layered ferroelectric heterostructure provide an opportunity to achieve high-p

228 Transition metal dichalcogenide moire heterostructures provide another model system for the st

229 The unique architecture of Pt/LiCoO(2) heterostructure provides abundant interfaces with favora

230 tz microrods@few-layered MoS(2) hierarchical heterostructure (QMSH).

231 kinetics to enable the growth of 2D vertical heterostructure remains a great challenge.

232 of 2DPs that form electronically coupled 2D heterostructures remains an outstanding challenge.

233 to control the components and morphology of heterostructures, respectively.

234 ibbons with well-defined edges; and vertical heterostructures resulted in the observation of supercon

235 oscopy on single block copolymerized organic heterostructures shows energy migration and light-harves

236 sent study has evidently provided a rational heterostructure strategy for improving various field emi

237 onstrate a multitude of different functional heterostructures such as resistors, capacitors and photo

238 condensates in hybrid cavity - van der Waals heterostructure systems.

239 ntheses for monometallic, multimetallic, and heterostructured systems, we showcase how the unique str

240 Advances in van der Waals heterostructure technology(7) have now allowed us to mak

241 Van der Waals materials and heterostructures that manifest strongly bound exciton st

242 as well as the possible van der Waals (vdW) heterostructures that one can create.

243 Like oxide heterostructures, the oxynitride has a superlattice of i

244 Here we show that, in FeSe/SrTiO(3) heterostructures, the superconducting transition tempera

245 structure and emergent functionality of the heterostructure, thereby providing a new approach to des

246 e, we report a strategy for constructing vdW heterostructures through the interface engineering of th

247 between Sn(1-) (x) Pb(x) Te and Pb make the heterostructures to be a promising candidate for topolog

248 multaneous use of in-plane and van der Waals heterostructures to build vertical single electron tunne

249 transition, surface engineering and complex heterostructures to enhance the carrier mobility and pow

250 Here we apply this concept to van der Waals heterostructures using the thickness of exfoliated cryst

251 integration of large-area 2D TMDs and their heterostructure variations onto a variety of unconventio

252 Two-dimensional van der Waals heterostructures (vdWHs) have attracted considerable int

253 Graphene based van der Waals heterostructures (vdWHs) have gained substantial interes

254 s naturally produces two distinct classes of heterostructures, vertical van der Waals (vdW) stacks or

255 structed van der Waals 1T-MoS(2)/C(60) 0D-2D heterostructures via a one-pot synthetic approach for ca

256 d and carrier concentration in van der Waals heterostructures via strain.

257 First, to characterise the heterostructures, we evaluate the GeTe-Sb[Formula: see t

258 The BZT/BCT epitaxial heterostructures were grown on SrRuO(3) (SRO) buffered S

259 ing double-layered PEA(2)PbI(4)/PEA(2)SnI(4) heterostructure when shearing-away PEA(2)SnI(4) film ont

260 red (Pb(0.5)Sn(0.5)Se)(1+delta)(TiSe(2)) (m) heterostructure, where m is the varying number of TiSe(2

261 ling compares well with respect to epitaxial heterostructures, where the epitaxy responsible for stro

262 tion to exciton funneling in a MoSe(2)/WS(2) heterostructure, which manifests itself as the photolumi

263 ed basicity is a significant feature in such heterostructure, which spontaneously split water molecul

264 esonances generate pure spin currents in the heterostructures, which are detected by the heavy metal

265 e behavior in amorphous-crystalline 2D oxide heterostructures, which are synthesized by atomic layer

266 l nonlinearities in graphene-insulator-metal heterostructures, which demonstrate an enhancement by th

267 rk for a better control of the growth of vdW heterostructures, which is critical to their large-scale

268 -covalent synthesis of nascent axial organic heterostructures, which promises to deliver useful appli

269 These novel heterostructures will find use in bottom cells for stabl

270 reation of an artificially layered nickelate heterostructure with a singly occupied [Formula: see tex

271 he graphene interlayer provides a unique vdW heterostructure with a vertical built-in electric field

272 ischarge constructing lithium peroxide-based heterostructure with band discontinuities and a relative

273 y enabled by the combination of an AlGaN/GaN heterostructure with graphene electrodes facilitates the

274 Moreover, through constructing a heterostructure with graphene oxide, ion selectivity of

275 is made by building the hybrid enzyme into a heterostructure with TiO(2) and graphitic carbon nitride

276 The thin-film heterostructures with a completely relaxed NiO buffer la

277 -which are created by stacking van der Waals heterostructures with a controlled twist angle(1-3)-enab

278 ate memory cell based on III-V semiconductor heterostructures with a junctionless channel and non-des

279 Constructing heterostructures with abundant interfaces is essential f

280 s of traditional colloidal syntheses of nano-heterostructures with atomic precision.

281 ate and tune exotic functionalities of oxide heterostructures with atomic precision.

282 that it is possible to construct foam-based heterostructures with complete photonic band gaps.

283 rein, by artificial design of photosensitive heterostructures with desired band alignment, three orde

284 Herein, the synthesis of NiSe(2) /CoSe(2) heterostructures with different interfacial densities vi

285 ropose intrinsically stable 2D semiconductor heterostructures with doubly-indirect overlapping bands

286 sizable DMI and small skyrmions in TI-based heterostructures with great promise for low-energy spint

287 However, the rational preparation of heterostructures with highly active heterosurfaces remai

288 We create heterostructures with incommensurate arrangements of wel

289 ton in WSe(2) monolayers and in WSe(2)/WS(2) heterostructures with large twist angles.

290 c control for the synthesis of axial organic heterostructures with light-harvesting properties.

291 a broad range of TMD/graphene van der Waals heterostructures with novel properties and functionality

292 various semiconductor nanowires and nanowire heterostructures with precisely controlled physical dime

293 of previously inaccessible mesoporous silica heterostructures with separation or catalytic properties

294 Van der Waals heterostructures with small misalignment between adjacen

295 nism leads to the formation of 2D perovskite heterostructures with spatially resolved coherent interf

296 Hybrid metal/semiconductor nano-heterostructures with strong exciton-plasmon coupling ha

297 An emerging class of heterostructures with unprecedented (photo)electrocataly

298 of ferroic functionality into van der Waals heterostructures, with stronger resilience toward detrim

299 Tailoring electronic band gaps in coupled heterostructures would permit control of such phenomena

300 Pt; X = chalcogen, e.g., S, Se, or Te), TMD heterostructure (WS(2) /MoS(2) ), and an atomically thin