ライフサイエンスコーパス: ultrathin

1 that measure the electrical impedance of an ultrathin (~ 150-200 nm), two-layer polymeric channel.

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

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

4 ct states by reduced dielectric screening in ultrathin 2D films.

5 precisely tailoring the growth temperature, ultrathin 2D layered tetragonal CoSe nanoplates and nonl

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

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

8 can be used to exfoliate samples and produce ultrathin 2D nanosheets.

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

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

11 ide insight into changes in the structure of ultrathin a-C films during deposition and annealing.

12 ure and, in turn, the physical properties of ultrathin a-C films used as protective overcoats.

13 onstrating low-threshold lasing even with an ultrathin (about three QD monolayers) active layer.

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

15 e consisting of a n(+)p-Si wafer coated with ultrathin Al(2)O(3) and AgP(2) NCs achieves an onset pot

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

17 Six experimentally observed Raman modes from ultrathin alpha-Mo(2) C crystal are first assigned with

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

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

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

21 Despite widespread interest, ultrathin and highly flexible light-emitting devices tha

22 omparable to liquid electrolyte-based cells, ultrathin and lightweight solid electrolytes with high i

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

24 Lightweight, ultrathin, and flexible electromagnetic interference (EM

25 The as-obtained ultrathin antimony oxide single crystals exhibit high di

26 ere, we successfully synthesize high-quality ultrathin antimony oxide single crystals via a substrate

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

28 -controlled outer-sphere electrochemistry on ultrathin back-gated ZnO working electrodes (i.e., 5 nm

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

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

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

32 Possibility to obtain ultrathin Bi(2)Se(3) thin films on these substrates is e

33 e of cobalt single atoms and two-dimensional ultrathin Bi(3)O(4)Br atomic layers, the optimized catal

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

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

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

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

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

39 mly establish the potential for lightweight, ultrathin, broadband lenses for high-quality imaging in

40 er mechanism formed by the dimension-matched ultrathin (ca. 8 nm) heterojunction nanostructure.

41 trate a direct pattern method to manufacture ultrathin carbides (MoC(x), WC(x), and CoC(x)) on versat

42 ctive, and precursor-free methods to prepare ultrathin carbides are lacking.

43 rces and displacements, we used low-density, ultrathin carbon nanotube electrodes which can sustain a

44 is commonly pictured as a parallel array of ultrathin carbonated hydroxyapatite (HAp) platelets dist

45 new insight for the design and synthesis of ultrathin catalysts with high activity.

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

47 Ultrathin ceramic coatings are of high interest as prote

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

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

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

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

52 rtion of Mg within the CoFeB gave rise to an ultrathin CoFeB layer with large anisotropy, high satura

53 However, the difficulty in attaining PMA in ultrathin CoFeB layers has imposed the use of thicker Co

54 resistance-area product MgO tunnel barrier, ultrathin CoFeB magnetic tunnel junctions (MTJs) demonst

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

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

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

58 Herein, a chemical vapor deposition route to ultrathin CoSe nanoplates with tunable structure phases

59 tunneling current in nanoscale junctions of ultrathin CrI(3) , a natural layer antiferromagnet, is r

60 It is found that the metallicity of an ultrathin CrN film recovers from insulating behavior upo

61 an spectroscopy analysis of hydrogenation in ultrathin crystalline MoSe(2) deposits.

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

63 and temperature effect on the growth rate of ultrathin CsPbBr(3) single-crystal film.

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

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

66 onal boron nitride (h-BN) is exploited as an ultrathin decorating layer to form a metal-insulator-sem

67 , composite Janus MD membranes comprising an ultrathin dense hydrophilic layer are developed by layer

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

69 ear optical effects over broad bandwidths in ultrathin devices.

70 TD calculations are used to confirm that the ultrathin dielectric cladding has negligible influence o

71 nement of green emission (540 nm) by such an ultrathin dielectric cladding is directly observed.

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

73 Here we report ferroelectricity in ultrathin doped hafnium oxide (HfO(2)), a fluorite-struc

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

75 on long-term clinical outcomes with a novel ultrathin drug-eluting stent, to date, are limited.

76 total HOA (P <= 0.001) in DMEK compared with ultrathin DSAEK (4.0- and 6.0-mm OZ).

77 HOA after ultrathin DSAEK and DMEK were compared; correlation was

78 posterior HOA was increased (P <= 0.036) in ultrathin DSAEK at 3, 6, and 12 months, in contrast to D

79 trafoil (P <= 0.045) were lower in DMEK than ultrathin DSAEK at 3, 6, or 12 months (either 4.0- or 6.

80 ces in anterior surface HOA between DMEK and ultrathin DSAEK at any post-surgical time.

81 brane endothelial keratoplasty decreases and ultrathin DSAEK increases posterior corneal HOA compared

82 in less posterior corneal HOA compared with ultrathin DSAEK.

83 topathy who were good candidates for DMEK or ultrathin DSAEK.

84 e excellent morphology of the SURMOF-derived ultrathin electrocatalyst coating led to a high exposure

85 n transfer in achieving optimum activity for ultrathin electrocatalysts.

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

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

88 etoelectric devices were made by integrating ultrathin FDTO with multiferroic BiFeO(3).

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

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

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

92 Ultrathin ferroelectric materials could potentially enab

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

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

95 results demonstrate a strategy for creating ultrathin ferromagnetic oxides by exploiting atomic hete

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

97 onstrated to be excellent semiconductors for ultrathin field-effect transistors(4,5).

98 -property relation of SAMs for the design of ultrathin film dielectrics as well as the understanding

99 The TaS(x) ultrathin film is industry-friendly, BEOL-compatible, an

100 an atomic force microscope tip polarizes an ultrathin film of an archetypal dielectric SrTiO(3) via

101 icroscope tip, we systematically polarise an ultrathin film of otherwise nonpolar SrTiO(3), and simul

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

103 tural wood can be directly converted into an ultrathin film with a record-small thickness of less tha

104 nd the object waves, we demonstrated that an ultrathin film, being an X-ray waveguide, can also gener

105 MF process comprises two steps: (1) applying ultrathin-film metal deposition, with a typical thicknes

106 Epitaxial ultrathin films are of utmost importance for state-of-th

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

108 ability to achieve highly conductive nitride ultrathin films by harnessing strain-control over compet

109 ynthesize freestanding SrTiO(3) and BiFeO(3) ultrathin films by reactive molecular beam epitaxy and t

110 Ultrathin films exhibit 2 additional electronic effects

111 Pb ultrathin films exhibit a Moire superstructure due to th

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

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

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

115 Controlled synthesis of nanostructure ultrathin films is critical for applications in nanoelec

116 y surface termination conversion in SrRuO(3) ultrathin films is reported.

117 control of the ferroelectric polarization in ultrathin films of ferroelectric perovskites needs to be

118 Ultrathin films of inorganic materials serve as an ideal

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

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

121 um self-assembly of ferroelectric domains in ultrathin films of Pb(Zr(0.4)Ti(0.6))O(3) results in a m

122 rmits us to determine the composition of the ultrathin films to be 38% Ni and 62% Si.

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

124 tigate the interface effect of hafnium oxide ultrathin films.

125 understanding of morphology and dynamics in ultrathin films.

126 ic morphology of embedding nanostructures in ultrathin films.

127 t promising for many applications, including ultrathin flexible materials, solar cells, touch-screen

128 es, and can advance emerging applications on ultrathin flexible memory, printed electronics, neuromor

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

130 and they can be used as the active layer in ultrathin flexible solar cells.

131 a lower-density origin of replication and an ultrathin flexible string of DNA at the terminus of repl

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

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

134 % at 550 nm, 84% over visible range), and an ultrathin form factor ( approximately 2.7 microm thickne

135 Soft, ultrathin frameworks nonlinearly organized in tandem are

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

137 ategy is developed to yield silver-decorated ultrathin g-C(3) N(4) nanosheets (Ag@U-g-C(3) N(4) -NS).

138 We report the synthesis of centimeter sized ultrathin GaN and InN.

139 The potential of ultrathin GO laminates for organic solvent nanofiltratio

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

141 suitably chosen single molecules between an ultrathin gold film supporting surface plasmon polariton

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

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

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

145 The membrane with an ultrathin hydrophilic multilayer of 48 nm has a sufficie

146 3-nm inorganic cores and approximately 1-nm ultrathin hydrophilic shell.

147 Experimentally, a class of ultrathin In(2) O(3) -ZnIn(2) Se(4) (denoted as In(2) O(

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

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

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

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

152 th-substituted iron-garnet nanopillars on an ultrathin iron-garnet slab forms a metasurface supportin

153 s of perfect absorption resonances within an ultrathin (lambda/165) metasurface to develop broadband

154 lica nanoparticles, which are shielded by an ultrathin layer of a potassium-permeable membrane, which

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

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

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

158 is approach to enhancing ferroelectricity in ultrathin layers could provide a route towards polarizat

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

160 synthesis method for chromium-sulfide-based ultrathin layers.

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

162 The ultrathin, lightweight, all-in-one device captures the c

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

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

165 Because the ultrathin limit cannot be reached for traditional semico

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

167 tegrated flexible sensors and circuits in an ultrathin, low-modulus elastomer.

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

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

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

171 The hybrid device employs an ultrathin (<3 um) LED structure conformed on a surface-w

172 Here we demonstrate an ultrathin (<=100 nm) lithium-ion ionomer membrane consis

173 cal aberrations in gradient index lens-based ultrathin (<=500 um) microendoscopes using aspheric micr

174 heranostic paradigm based on small-sized and ultrathin M-NSs, which will broaden the application of 2

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

176 ition-temperature superconductors, proteins, ultrathin magnetic films, liquid crystals and metallic a

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

178 as opened new opportunities to explore these ultrathin magnets for such applications.

179 These ultrathin materials have good interface attachment with

180 Ultrathin materials often require high temperatures for

181 gies can support these use cases in soft and ultrathin materials that conformally interface with the

182 ique can be extended to fabrication of other ultrathin materials, e.g. graphene, as well as final sub

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

184 y proportional to the thickness of the pore, ultrathin membranes have the advantage of providing rela

185 ally, we demonstrate thermal dewetting of Au ultrathin metal films and growth of MoS(2) on NaCl at 75

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

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

188 e several of the limitations of single-layer ultrathin metastructures, and extend their feasibility i

189 nique by designing, realizing and testing an ultrathin MetaSurface cloak for surface waves.

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

194 The uniform mesopores and ultrathin MnO(2) enable fast electron/ion transport comp

195 Facile fabrication of ultrathin monolayer PDMS nanobrush on an underlying subs

196 hlighting the important surface-to-volume of ultrathin MoS(2) structure, which enhances the overall p

197 Interestingly, our analysis indicates that ultrathin MoSe(2) deposits with exposed edges show a blu

198 fabrications, high dielectric materials and ultrathin multilayers have been selected to improve the

199 In addition to their use in DNA sequencing, ultrathin nanopore membranes have potential applications

200 Here, we overcome this challenge using an ultrathin nanoporous membrane in a pure vapour ambient.

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

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

203 Once exfoliated, ultrathin nanosheets of g-C(3) N(4) attain much intrigui

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

205 ifferent substrates is crucial for obtaining ultrathin nanostructures and films of this material by p

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

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

208 ransmission of 98.8% when passing through an ultrathin NaYF(4) /NaGdF(4) superlattice cladding (thick

209 ierarchical nanoarchitectures, consisting of ultrathin Ni-Fe layered-double-hydroxide (Ni-Fe LDH) nan

210 itu characterization of phase transitions of ultrathin nickel silicides using 3D medium-energy ion sc

211 resistance of 220 +/- 50 ohm micrometres on ultrathin niobium disulfide (NbS(2)) and near-ideal band

212 the combined OSDAs work in tandem to produce ultrathin, nonfaulted HOU-4 crystals that exhibit improv

213 s up a wide range of novel possibilities for ultrathin OLEDs.

214 nanophotonic devices and applications, from ultrathin optical elements to metal-free sub-diffraction

215 plications of polaritons in metasurfaces and ultrathin optical elements.

216 Microscopy during growth of ultrathin orthorhombic SnS on trigonal SnS(2) shows that

217 ng the crystalline order in the freestanding ultrathin oxide films.

218 primary approaches toward the preparation of ultrathin oxides are only applicable to amorphous or pol

219 Ultrathin oxides have been reported to possess excellent

220 an avenue in broadening the applicaitons of ultrathin oxides in many emerging fields.

221 tegy can also be utilized to fabricate other ultrathin oxides, opening up an avenue in broadening the

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

223 The result demonstrates that ultrathin PDMS nanobrush can either promote or inhibit c

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

225 mework, we demonstrate the design of various ultrathin planar THz optical elements, namely (i) a high

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

227 Here, we show that ultrathin plasmonic nanogaps support complete mode sets

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

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

230 dothelialized fibrin grafts with an external ultrathin poly(epsilon-caprolactone) sheath as an interp

231 to design liquid crystals (LCs) supported on ultrathin polycrystalline gold films (predominant crysta

232 Herein, an ultrathin polymer film of "polyurea" as an artificial SE

233 uced by the impact of a solid sphere onto an ultrathin polymer sheet floating on water.

234 a general approach is reported for preparing ultrathin PtNiM (M = Rh, Os, and Ir) nanowires (NWs) wit

235 ture and optimal electronic interaction, the ultrathin PtNiM NWs show enhanced electrocatalytic perfo

236 ead halide perovskites, with unprecedentedly ultrathin quantum barriers that screen interlayer intera

237 rintuitively stabilize polar symmetry in the ultrathin regime.

238 tal nanoframes consisting of interconnected, ultrathin ridges have received considerable attention in

239 Ultrathin sagittal sections of maxillary incisors from 8

240 Serial ultrathin section analysis and 3D reconstructions reveal

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

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

243 The non-destructive collection of ultrathin sections on silicon wafers for post-embedding

244 Ultrathin sections scanned with super-resolution STED mi

245 h transmission electron microscopy on serial ultrathin sections.

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

247 , we report on a novel nonlinear material-an ultrathin semiconductor metasurface-that exhibits effici

248 s devised through large-scale integration of ultrathin sensors and stimulator arrays in multiple laye

249 ssed for immunocytochemistry and prepared by ultrathin series sectioning for transmission electron mi

250 toluminescence by two orders of magnitude in ultrathin sheets and an unexpected thickness-dependent m

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

252 Here, 2D ultrathin single-crystal molybdenum oxide (MoO(2) ) flak

253 Two materials are studied as model systems: ultrathin SiO(2) and Pt.

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

255 rior catalysts because of their engineerable ultrathin/small dimensions and large surface areas and h

256 finding unambiguously bridges experiments on ultrathin SnTe films with predictions of robust ferroele

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

258 We introduce a pair of ultrathin, soft, skin-like electronic devices whose coor

259 upt increase in the tunneling conductance of ultrathin SrTiO(3) under strain gradients.

260 ificantly enhanced flexocoupling strength in ultrathin SrTiO(3), compared to that in bulk, rendering

261 all frequencies used by bats with light and ultrathin structures that meet aerodynamic constraints o

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

263 BioFreedom stent is noninferior to a modern ultrathin strut biodegradable polymer cobalt-chromium si

264 We sought to assess the long-term effect of ultrathin-strut (60 mum) BP-SES versus thin-strut (81 mu

265 385279), allocating in a 1:1 ratio to either ultrathin-strut biodegradable polymer MiStent sirolimus-

266 s (cumulative incidence, 22.3%) treated with ultrathin-strut BP-SES and 109 patients (18.3%) treated

267 years were similar in patients treated with ultrathin-strut BP-SES and thin-strut DP-EES.

268 ients with small vessel disease treated with ultrathin-strut BP-SES versus thin-strut DP-EES.

269 sel size and failed to specify the impact of ultrathin-strut thickness on long-term clinical outcomes

270 a surrogate to compare patients treated with ultrathin-strut versus thin-strut drug-eluting stent.

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

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

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

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

275 Ultrathin tantalum carbide, nitride, and boride are grow

276 of intense light measured at the rear of an ultrathin target foil irradiated by a relativistically i

277 Here, we demonstrated ultrathin thermal emitters that violate this one-to-one

278 The material's ultrathin thickness and exceptional mechanical strength

279 are enzymatic nanosheets with small size and ultrathin thickness by current synthetic protocols.

280 nt g-C(3)N(4) NS with laminar morphology and ultrathin thickness were fabricated.

281 Over 26,500 ultrathin tissue sections from the same block were image

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

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

284 Ultrathin transition metal carbides with high capacity,

285 The physical properties of ultrathin transition metal dichalcogenides (2D-TMDCs) ma

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

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

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

289 Ultrathin two-dimensional (2D) semiconducting layered ma

290 The micellar brushes can also be grown on ultrathin two-dimensional materials such as graphene oxi

291 harness valley excitons for applications in ultrathin valleytronic devices.

292 Ultrathin van der Waals semiconductors have shown extrao

293 philic graphene grid allows the formation of ultrathin vitrified ice layer embedded most protein part

294 llary length reduces analysis time while the ultrathin wall (15 mum) efficiently dissipates heat from

295 Highly integrated, flexible, and ultrathin wireless communication components are in signi

296 nalysis, suggesting that the aspect ratio of ultrathin WO(3-x) NPLs is the key to producing an unprec

297 As a proof-of-concept, we directly use the ultrathin wood film as a diaphragm in a real speaker tha

298 om this aligned and laminated structure, the ultrathin wood film exhibits excellent mechanical proper

299 The ultrathin wood film with excellent mechanical property a

300 The ultrathin ZnO QD-nanocellulose composite is obtained by