ライフサイエンスコーパス: ultrathin

1 fter correction, only 17 of the 114 remained ultrathin.

2 igh-resolution confocal microscopy employing ultrathin (120 nm) sections of mouse liver, improving z-

3 e Co3O4 surface and embedded in a dense, yet ultrathin (2 nm), silica layer that separates light abso

4 We observe an ultrathin (2-3 unit cells) interlayer best described as

5 ructures, where top layer is chosen to be an ultrathin (20 nm) VO2 film, we demonstrate broadband IR

6 collective plasmonic responses in SNL, these ultrathin 2D films display rapid and reversible red-blue

7 modulating the intrinsic valley carriers in ultrathin 2D materials and potentially open new paths fo

8 o tissue and efficient ROS diffusion through ultrathin 2D MOLs (ca. 1.2 nm) enable highly effective X

9 ess in the utilization of solution-processed ultrathin 2D nanomaterials for fabrication of non-volati

10 n-volatile resistive memory devices based on ultrathin 2D nanomaterials have been emerging as promisi

11 rogress in high-yield, massive production of ultrathin 2D nanomaterials via various solution-based me

12 epitaxial growth of nanostructures based on ultrathin 2D nanosheets or in situ growth of lateral or

13 ial growth of hetero-nanostructures based on ultrathin 2D nanosheets.

14 ting in the easy exfoliation of TPA-COF into ultrathin 2D NSs.

15 In addition, an ultrathin (800-nm) biodegradable cellulose substrate wit

16 Frequent water exchange occurs even for an ultrathin adsorbed water film persisting on the surface

17 cond, hyperbolic metamaterials consisting of ultrathin Al-doped Ag films are attained having a homoge

18 r-induced dewetting of initially continuous, ultrathin alloy films through a combination of morpholog

19 tes are formed by atomic layer deposition of ultrathin alumina films on a lithographically patterned

20 The ETLs, ZnO nanoparticle assemblies with ultrathin alumina overlayers, dramatically enhance durab

21 metal anode and the garnet electrolyte using ultrathin aluminium oxide (Al2O3) by atomic layer deposi

22 e-selected in the gas phase, deposited on an ultrathin amorphous alumina support, and tested as catal

23 l photonic devices, to achieve, for example, ultrathin and efficient optical elements, and realize th

24 ould bring wide benefits for applications in ultrathin and flexible electronics, photovoltaics and di

25 cement of conventional optical elements with ultrathin and planar photonic structures.

26 Graphene can serve as an ultrathin and transparent diffusion barrier in solar cel

27 magnetic sub-layers, exchange-coupled via an ultrathin antiferromagnetic-coupling spacer layer.

28 Specifically, we have probed ultrathin ( approximately 2 nm) core-shell Pt approximat

29 relaxed phase matching condition due to the ultrathin area lead to a giant FWM efficiency, which is

30 the basis for the robust formation of these ultrathin assemblies.

31 ied to >1.00 mm included 96% of the original ultrathin-associated deaths and 100% of the original pos

32 te that amine-modified ZnO nanorods on which ultrathin Au nanowires are grown act as an excellent cat

33 of approximately 100 nm via the assembly of ultrathin AuAg nanowires in the presence of the triblock

34 The proposed ultrathin back-to-back quarter-wave plates cavity can be

35 Here, taking ultrathin BaTiO3 films as a model system, an intrinsic t

36 The films considered here are ultrathin because their interior regions are not truly b

37 leys, offer new opportunities for developing ultrathin biexciton lasers and polarization-entangled ph

38 ce induced giant spontaneous polarization in ultrathin BiFeO3 ferroelectric films is reported.

39 the spontaneous polarization in a 2 nm-thick ultrathin BiFeO3 film is abnormally increased up to appr

40 INTERPRETATION: The outperformance of the ultrathin, bioresorbable polymer sirolimus-eluting stent

41 Ultrathin black phosphorus is a two-dimensional semicond

42 boron nitride can be used for passivation of ultrathin black phosphorus.

43 analysis of many three-terminal devices with ultrathin body channels.

44 on because of their great potential to be an ultrathin body for efficient electrostatic modulation, w

45 r superb electrical properties and intrinsic ultrathin body, but problems such as limited semiconduct

46 -wave plates, which are integrated within an ultrathin cavity.

47 Ultrathin ceramic coatings are of high interest as prote

48 ent ECCs, showing great potential for wiring ultrathin circuits for high performance flexible electro

49 Here we developed the stacked ultrathin Co3 O4 nanosheets with surface functionalizati

50 icity" to "super-lithiophilicity" through an ultrathin coating of amorphous Si deposited by plasma-en

51 a proof-of-concept application, the obtained ultrathin COF NSs are used as a novel fluorescence sensi

52 red to pristine CoFe LDHs, the as-exfoliated ultrathin CoFe LDHs nanosheets exhibit excellent catalyt

53 For the first time, this study prepares ultrathin CoFe LDHs nanosheets with multivacancies as OE

54 ferromagnets formed from a repeated motif of ultrathin CoFeB/Pt layers.

55 Here, we fabricate ultrathin, coherently strained films of CeO2-delta betwe

56 Such broadband absorber designs are ultrathin compared to carbon nanotube based black materi

57 Here we introduce an ultrathin, compliant skin-like, or 'epidermal', photonic

58 The design of an ultrathin, conformal electronic device that integrates e

59 The design of an ultrathin, conformal electronic device that integrates e

60 at uses heat driven benzoin radicals to grow ultrathin copper nanowires with tunable diameters.

61 ined peroxisomal membrane remnants, which in ultrathin cross sections generally appeared as double me

62 tals which facilitates the growth of smooth, ultrathin crystalline films.

63 imize combined electron-photon harvesting in ultrathin crystalline silicon solar cells.

64 The ultrathin crystals are found on the copper surface (oppo

65 Highly uniform single crystal ultrathin CsPbBr3 nanowires (NWs) with diameter of 2.2 +

66 We go on to show that insertion of an ultrathin CTE buffer layer mitigates this problem and ca

67 Here, we develop the synthesis of ultrathin Cu@Au core-shell nanowires using trioctylphosp

68 validity of the proposed soft materials and ultrathin device designs through theoretical modeling an

69 optoelectronic properties for high-density, ultrathin devices.

70 ear optical effects over broad bandwidths in ultrathin devices.

71 d a plethora of emerging functions within an ultrathin dimension, paving way towards flat and highly

72 mon resonances is experimentally verified in ultrathin disks.

73 sion-based photon upconversion capsules with ultrathin double shells are developed through a single d

74 Here we demonstrate that the use of ultrathin electron transparent graphene membranes, which

75 The bubble domains appear in ultrathin epitaxial PbZr0.2 Ti0.8 O3 /SrTiO3 /PbZr0.2 Ti

76 Furthermore, an ultrathin Fe-ion-containing polydopamine layer has been

77 ty of Pb(II) and As(V) in waste water by the ultrathin FeOOH nanosheets.

78 ructure calculations reveal that the VCMA of ultrathin FeRh/MgO bilayers exhibits distinct linear or

79 ic La0.7Sr0.3MnO3 electrodes separated by an ultrathin ferroelectric BaTiO3 tunnel barrier, where a h

80 the richness of polar topologies possible in ultrathin ferroelectric structures and bring forward the

81 terfaces in improving large polarizations in ultrathin ferroelectrics and are meaningful for the deve

82 owave voltage to a nanosized VCMA gate in an ultrathin ferromagnetic nanowire results in the parametr

83 nance in multiferroic bilayers consisting of ultrathin ferromagnetic NiFe and ferroelectric Pb0.92La0

84 An ultrathin (few nanometer) polymer spacer layer is soften

85 cs or cellular in vivo biosensing when using ultrathin fiber optic probes for research purposes.

86 ent optical absorbers based on a three-layer ultrathin film composed of subwavelength chromium (Cr) a

87 Coating a conformal, conductive and optimal ultrathin film on cathode particles has significantly in

88 of spin structures in an in-plane magnetized ultrathin film system where out-of-plane spin orientatio

89 ed molecularly imprinted polymer (MIP)-based ultrathin film using R(+)-atenolol (ATNL) as a template

90 can act as nanopores, making rGO a promising ultrathin-film membrane candidate for separations.

91 ose of graphene, enabling the realization of ultrathin-film photovoltaic devices or systems for hydro

92 can provide useful insights to guide future ultrathin-film solar cell designs incorporating nanostru

93 Light trapping in planar ultrathin-film solar cells is limited due to a small num

94 e very smooth, homogeneous, highly oriented, ultrathin films across millimeter-scale areas that displ

95 of lateral electronic structures of various ultrathin films by extra interfacial potentials due not

96 Pb ultrathin films exhibit a Moire superstructure due to th

97 High-mobility semiconducting ultrathin films form the basis of modern electronics, an

98 gnificantly improve the infrared analysis of ultrathin films in aqueous environments by employing in

99 icrophase-separated sub-10-nm nanostructured ultrathin films in the form of alternating CB and aPP la

100 ectronic structure computations of growth of ultrathin films of compounds of group III (B, Al, In, Ga

101 Metasurfaces can also be created by using ultrathin films of materials with large optical losses.

102 d as a probe to measure surface diffusion of ultrathin films of N,N'-Bis(3-methylphenyl)-N,N'-dipheny

103 Here, we report ultrathin films of non-encapsulated layered Bi2O2Se, gro

104 Control over the properties of ultrathin films plays a crucial role in many fields of s

105 used to measure the surface stress of other ultrathin films supported on soft substrates.

106 t higher energy conversion efficiencies with ultrathin films than conventional thin-film solar cells

107 nt defects in conductors, semiconductors and ultrathin films, but such single-defect electronic chara

108 erits of high efficiency, at visible regime, ultrathin films, good tolerance to the incidence angle a

109 Chiral spin textures in ultrathin films, such as skyrmions or chiral domain wall

110 structure of n-type Pr2-xCexCuO4 (x = 0.15) ultrathin films, via the electric double layer transisto

111 Unlike unpatterned ultrathin films, which tend to warp or even roll up beca

112 d for tailoring the adsorption properties of ultrathin films.

113 forming continuous corrugated plates out of ultrathin films.

114 esign of innovative optical elements such as ultrathin flat lenses, directional couplers for surface

115 e light is experimentally demonstrated in an ultrathin flexible dispersion-free metadevice.

116 Tsukruk and co-workers develop self-powered ultrathin flexible films for bio-tactile detection.

117 h-performance MgO-barrier MTJs directly onto ultrathin flexible silicon membrane with a thickness of

118 on and technical procedures for implementing ultrathin, flexible optofluidic neural probe systems tha

119 pressure sensing architectures, allowing an ultrathin, flexible, and imperceptible packaging with co

120 are promising candidates for next-generation ultrathin, flexible, and transparent electronics.

121 % at 550 nm, 84% over visible range), and an ultrathin form factor ( approximately 2.7 microm thickne

122 electronic sensors in a mechanically robust, ultrathin format comparable in size to a credit card.

123 are layered materials that are available in ultrathin forms such as mono-, bi- and multilayers, whic

124 Soft, ultrathin frameworks nonlinearly organized in tandem are

125 Herein we demonstrate an ultrathin freestanding ZnO quantum dot (QD) active layer

126 for the topological surface electrons in the ultrathin gapped-Dirac-cone limit.

127 The potential of ultrathin GO laminates for organic solvent nanofiltratio

128 ing process to facilitate the development of ultrathin GO-based membranes for CO2 capture.

129 This paper describes ultrathin gold nanowires (NWs) and nanoparticles (NPs) p

130 Our study shows that ultrathin gold nanowires and nanoparticles prepared by o

131 s inducing petal-like rutile TiO2 wrapped by ultrathin graphene-rich layers are proposed to fabricate

132 iques to directly grow on a continuous basis ultrathin graphite (uG) on uneven nanoscale surfaces.

133 The unconventional modification of ultrathin graphite optoelectronic properties is explaine

134 ation and growth of large-area, uniform, and ultrathin h-BN directly on oxidized substrates (B/N atom

135 spintronic devices, currently accessible in ultrathin heavy metal/ferromagnetic bilayers and multila

136 Then, we propose the ultrathin hemispherically curved image sensor array as a

137 the use of abortive or newborn animals with ultrathin hides, but could equally well reflect a produc

138 ovel type of Ni3V2O8 nanowires, organized by ultrathin hierarchical nanosheets (less than 5 nm) on Ti

139 ms consisting of nitrogen-doped graphene and ultrathin honeycomb-like MoS2 nanosheets.

140 3-nm inorganic cores and approximately 1-nm ultrathin hydrophilic shell.

141 In SEER, 21% of thin melanomas were ultrathin; in other registries, they comprised 5.8-15%.

142 Ultrathin inorganic piezoelectric and semiconductor mate

143 tum mechanical tunneling of electrons across ultrathin insulating oxide barriers has been studied ext

144 d in a hysteretic manner in bilayers made of ultrathin insulators whose electric polarization cannot

145 Semiconductor surfaces and ultrathin interfaces exhibit an interesting variety of t

146 The electrochemical interface is an ultrathin interfacial region between the electrode surfa

147 esulfonate) (PEDOT:PSS) by over 1 eV, and an ultrathin interlayer of PSBMA reduced the electron injec

148 Here, we demonstrate experimentally an ultrathin invisibility skin cloak wrapped over an object

149 the orthogonal state upon reflection from an ultrathin (lambda/25) cavity array.

150 positing of wide band gap Ga2O3 layer and Fe ultrathin layer due to inter diffusion between two layer

151 Electrodes modified with an ultrathin layer of ALD Al2O3 and an overlayer of Pt dend

152 ilotriacetic acid (NTA) using graphene as an ultrathin layer.

153 o/nanofabrication process was used to create ultrathin-layer cells (UTLCs) with a critical dimension

154 Herein, this study demonstrates that ultrathin layered-double-hydroxide (LDH) photocatalysts,

155 n important role in many compounds for which ultrathin layers can behave very differently from the bu

156 ure of the effective dielectric screening in ultrathin layers of transition-metal dichalcogenides (TM

157 produce multivacancies in the as-exfoliated ultrathin LDHs nanosheets.

158 A rigorous method for ultrathin lens design, and the trade-off between high ef

159 scoding of thickness that is concentrated in ultrathin lesions is present in SEER and results in misc

160 ties of FCVA-deposited carbon films, even at ultrathin levels (1.2 nm).

161 We crafted ultrathin light sheets from two-dimensional optical latt

162 ion techniques has led to the realization of ultrathin, lightweight, and flat lenses (metalenses) wit

163 trolling electric dipoles is hindered in the ultrathin limit by the finite screening length of surfac

164 Because the ultrathin limit cannot be reached for traditional semico

165 Bringing this concept to the ultrathin limit would substantially broaden the range of

166 hem promising candidates for next-generation ultrathin, low-power, high-speed electronics.

167 tases among patients with thin (</=1 mm) and ultrathin (</=0.25 mm) melanomas have been reported.

168 These flexible circuits are ultrathin (<1 mum) and ultralightweight ( approximately

169 By limiting contaminants and defects, ultrathin (<10 nm) CVD polymeric device layers have been

170 t capacitive contribution, is governed by an ultrathin (<3 nm) oxide layer.

171 Here, we synthesize and characterize ultrathin (<5 nm) Cu9S5 nanosheets that are formed by so

172 Multifunctional materials composed of ultrathin magnetic films with perpendicular magnetic ani

173 he physical origin of the Gilbert damping in ultrathin magnetic films.

174 These ultrathin materials have good interface attachment with

175 experimental realization of graphene, other ultrathin materials with unprecedented electronic proper

176 ss in one SEER site revealed that 114 of 447 ultrathin melanomas had errors; after correction, only 1

177 melanoma-related death rate of patients with ultrathin melanomas was higher in SEER (2.8%) compared w

178 A novel hyper-cross-linked ultrathin membrane is presented, consisting of a giant m

179 tructure tunnel diodes, and millimetre-scale ultrathin membranes and windows.

180 o-dimensional materials offer a new class of ultrathin membranes that can have atomically defined nan

181 counterintuitively, anisotropic ultrathin (meta)materials can be made sensitive or insen

182 sional materials such as graphene, MoS2, and ultrathin metal films.

183 Localized resonances in ultrathin metal nano-strip optical resonators consisting

184 Ultrathin metal oxides exhibit unique chemical propertie

185 the long-lived terahertz magnons excited in ultrathin metallic alloy films.

186 An interconnected framework of ultrathin metallic copper formed provides a high conduct

187 cture of these new waveguides consists of an ultrathin metallic strip with periodic subwavelength sta

188 as indium tin oxide ( approximately 80%) and ultrathin metals ( approximately 60%).

189 We experimentally demonstrate such an ultrathin metasurface lens that can function either as a

190 ward and backward scattering by single layer ultrathin metasurfaces, and they lead to confinement of

191 s of a general class of non-magnetic passive ultrathin metasurfaces.

192 the performance limitations of single layer ultrathin metasurfaces.

193 enerating large temperature gradients across ultrathin MgO tunnel barriers that considerably affect t

194 mical transistor (sensing component) with an ultrathin microbial nanocellulose wicking membrane (samp

195 e of plasmonic nanoshells, embedded within a ultrathin microcrystalline silicon solar cell, in enhanc

196 Ultrathin molybdenum disulphide (MoS2) has emerged as an

197 es, vertical p-n junctions are fabricated in ultrathin MoS(2) by introducing AuCl(3) and benzyl violo

198 The ultrathin MoS(2) p-n junctions present a significant pot

199 This work enriches the investigation of ultrathin MoS2 and has potential application in the mech

200 D assembled hierarchical architecture of the ultrathin MoS2 nanosheets and the interconnection of 3D

201 In this paper, a new kind of oil-soluble ultrathin MoS2 nanosheets is prepared through a one-pot

202 By adding 1 wt% ultrathin MoS2 nanosheets, at the temperature of 120 deg

203 clear and practical guidelines for designing ultrathin multilayer composite membranes to achieve high

204 We show that all these ultrathin nanomasks can be used for high-contrast quantu

205 Two-dimensional (2D) nanomaterials are ultrathin nanomaterials with a high degree of anisotropy

206 Herein, we report that ultrathin nanoplates of cobalt-manganese layered double

207 content up to 5.9% was on the surface of the ultrathin nanoribbon.

208 spheres assembled from N-doped carbon-coated ultrathin nanosheets are synthesized.

209 nospheres which facilitates the formation of ultrathin nanosheets by the oxidation of the metal and t

210 The ability to exfoliate LDHs into ultrathin nanosheets enables a range of new opportunitie

211 the sheet-on-sheet sandwich-like structure, ultrathin nanosheets with abundant nanopores, large surf

212 materials is also proceeding as new types of ultrathin nanostructures are constantly being created, s

213 Moreover, the resultant PdCu aerogel with ultrathin nanowire networks exhibits excellent electroca

214 insights gained into the performance of our ultrathin nanowires from our demonstrated approach will

215 ocaloric temperature change in ferroelectric ultrathin nanowires.

216 rst step, Te grows one-dimensionally to form ultrathin nanowires; in the second step, these nanowires

217 d from an electromagnetic perspective, their ultrathin nature may also provide novel and useful mecha

218 The ultrathin nature of Tr-QLEDs allows their conformal inte

219 ace area of the sheets associated with their ultrathin nature promises a wide range of applications.

220 S) pattern shows the periodic packing of the ultrathin NWs along the radial direction, demonstrates t

221 These bright ultrathin NWs may be used as a model system to study str

222 Despite the extreme aspect ratios of the ultrathin NWs, their composition and the resulting optic

223 cy acoustic wave sensing in combination with ultrathin, oligoethylene glycol-based mixed surface chem

224 fibers based on the self-assembly of various ultrathin one-dimensional and two-dimensional nanomateri

225 view focuses on recent developments on flat, ultrathin optical components dubbed 'metasurfaces' that

226 Ultrathin optical metasurface lenses have been demonstra

227 ngly enhancing the interaction and realizing ultrathin optoelectronic devices.

228 Epitaxially grown ultrathin organic semiconductors on graphene show great

229 All of these ultrathin oxide film thicknesses completely passivated t

230 e iron started participating in formation of ultrathin oxide films on LMNO particle surface.

231 At this interface, an ultrathin oxidized iron layer exists, whose magnetizatio

232 We report on a study of epitaxially grown ultrathin Pb films that are only a few atoms thick and h

233 on sustainability is reported in a series of ultrathin PbTiO3 films scaled down to three unit cells g

234 -pot synthesis of atomically dispersed Ru on ultrathin Pd nanoribbons.

235 Furthermore, the ultrathin Pd/Ru nanoribbons could remarkably prohibited

236 ures are employed for making high-performing ultrathin photodetectors.

237 gnetic and mechanical resonances in a single ultrathin piezoelectric nanoplate.

238 Our work introduces an ultrathin, planarized nanophotonic interface to sense ch

239 Ultrathin plasmonic metasurfaces have proven their abili

240 rations is demonstrated on suitably designed ultrathin plasmonic metasurfaces with only 2D planar chi

241 Surfaces covered by ultrathin plasmonic structures--so-called metasurfaces--

242 The inorganic piezoelectric sensor on an ultrathin plastic achieves conformal contact with the co

243 Therefore, the interface of ultrathin PMMA films on native aluminum oxide, deposited

244 Ultrathin polyarylate nanofilms with thickness down to 2

245 The development of an ultrathin polymer coating is described to sustain the de

246 To demonstrate this potential, here ultrathin reflection metasurfaces (also called metamirro

247 Serial ultrathin section analysis and 3D reconstructions reveal

248 graphy, a microscopy technique that combines ultrathin sectioning of tissue with immunofluorescence a

249 icroscopy, or electron micrographs of single ultrathin sections imaged by transmission electron micro

250 However, air-stable ultrathin semiconducting materials with superior perform

251 the field of optical metamaterials to create ultrathin semiconductor metafilms with designer absorpti

252 is believed that the good dispersion and the ultrathin shape of the nanosheets ensure that they can e

253 dability that brings three major advantages: ultrathin sheets automatically achieve optimally efficie

254 Conformal deposition of platinum as ultrathin shells on facet-controlled palladium nanocryst

255 n the surfaces of Ag nanocubes as conformal, ultrathin shells.

256 electrochemical process was used to grow an ultrathin silica film ( approximately 100 nm) consisting

257 red quantum dots (QDs) as dual fluorophores, ultrathin silica shell as spacer, and meso-tetra(4-sulfo

258 lar cells constructed on highly flexible and ultrathin silver-mesh/conducting polymer substrates.

259 nd universal approach for the preparation of ultrathin single- or multiple-component transition-metal

260 f tiny Pt nuclei which directs the growth of ultrathin single-crystal Pt nanowire (2.5-3 nm in diamet

261 rate smart prosthetic skin instrumented with ultrathin, single crystalline silicon nanoribbon strain,

262 were extracted directly from the surface of ultrathin slices of liver tissue prior to detection by h

263 ver, advances in nanophotonics have produced ultrathin, so-called 'flat' optical components that bege

264 eless optofluidic neural probes that combine ultrathin, soft microfluidic drug delivery with cellular

265 When transported through ultrathin solid-state nanopores, short DNA fragments con

266 s of crystal violet molecules embedded in an ultrathin spin-on-glass detection "hot zone", which is a

267 itanite (SrTiO3) single crystals capped with ultrathin SrTiO3/LaAlO3 bilayers.

268 ts were randomly assigned (2:1) to either an ultrathin strut (60 mum) bioresorbable polymer sirolimus

269 rmed a prespecified subgroup analysis of the Ultrathin Strut Biodegradable Polymer Sirolimus-Eluting

270 Ultrathin strut biodegradable polymer sirolimus-eluting

271 We assessed noninferiority of a novel ultrathin strut drug-eluting stent releasing sirolimus f

272 loit localized surface plasmon resonances in ultrathin subwavelength plasmonic nanoresonators are dem

273 ation-sensitive light-matter interactions in ultrathin (subwavelength thickness) media.

274 - ranging from high-temperature cuprates to ultrathin superconducting films - that experience superc

275 Surface-structural modulation of the ultrathin superconducting NbSe2 by polar reductive hydra

276 We have discovered the existence of ultrathin superdense nonmagnetic cobalt layers in a poly

277 Ultrathin tantalum carbide, nitride, and boride are grow

278 The single-crystalline nature and ultrathin thickness of these 2D nanosheets make them ide

279 -EDTA and one-dimensional (1D) ultralong and ultrathin TiO2 nanofibers.

280 nduced optical permittivity modulation of an ultrathin titanium nitride (TiN) film, which is incorpor

281 e a better understanding of the chemistry of ultrathin TMDCs crystals, introduce an effective method

282 spin-texture behaviour of boundary modes in ultrathin topological insulator films is critically esse

283 le magnetic skyrmions at room temperature in ultrathin transition metal ferromagnets with magnetic tr

284 Here, a generic approach of making scalable ultrathin transition metal-carbide/boride/nitride using

285 ssisted phosphorus doping is demonstrated on ultrathin transition-metal dichalcogenides (TMDCs) inclu

286 The ability to prepare ultrathin two-dimensional (2D) covalent organic framewor

287 Ultrathin two-dimensional (2D) nanomaterials, such as gr

288 ds with homogeneous interfacial contacts and ultrathin two-dimensional (2D) nanosheet subunits.

289 Ultrathin two-dimensional (2D) nanosheets of layered tra

290 Ultrathin two-dimensional (2D) nanosheets, such as graph

291 Metasurfaces are ultrathin, two-dimensional arrays of subwavelength reson

292 Metasurfaces, as the ultrathin version of metamaterials, have caught growing

293 CNS and metal carbide@CNS structures possess ultrathin walls, good electrical conductivity, strong ad

294 dented electronic structure arising from its ultrathin walls.

295 Triple emulsion drops with an ultrathin water layer are developed to achieve high enca

296 Interestingly, the gas transport through ultrathin water membranes at nanobubble interface is fre

297 Defect-rich ultrathin ZnAl-layered double hydroxide nanosheets are s

298 We find that ultrathin ZnO behaves like a 2D semiconductor, in which

299 cular dopants/formulations directly onto the ultrathin ZnO channels.

300 The ultrathin ZnO QD-nanocellulose composite is obtained by