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1 interface as well as in the solid phase (dry film).
2 al diaphragm materials (e.g., silica, silver films).
3 pport a metallic transport across the entire film.
4 n of the optical axis along the plane of the film.
5 ncreasing the overall resistance of the thin film.
6 areas is prevented via a surface-passivating film.
7 s of magnitude over that of a reference TiO2 film.
8 lubility than the native high amylose starch film.
9 , between the substrate and the brittle thin film.
10 particles in this 3.2 mum thick REBa2Cu3Ox film.
11 nic-inorganic trihalide lead perovskite thin films.
12 lkylation reaction in monolayer CVD graphene films.
13 f nearly planar copper nanocrystalline (111) films.
14 y)cyanoterephthalylidene) conjugated polymer films.
15 cles compared to the compact MWCNT electrode films.
16 d allow for efficient charge transport in QD films.
17 trical conductivity of nanoribbon-based thin films.
18 nd allow for the growth of thick ( 3.44 mum) films.
19 thick galvanostatically deposited PEDOT(PSS) films.
20 and electronic properties of single crystal films.
21 r the increase in the elastic modulus of the films.
22 ophanes as well as the hydrophobicity of the films.
23 odes, tin-doped indium oxide and silver nano-films.
24 structural changes in the fully strained SFO films.
25 ctrochemical and chemical stability of these films.
26 tion than traditional Hg sphere-caps or thin-films.
27 licated in the macroscopic, centimeter-scale films.
28 rable quantum yields in solution and viscous films (10(-5)-10(-4) in the case of 4-nitrophenol) and o
31 he proposed System on-Glass hosts thin metal films acting as heating sources; hydrogenated amorphous
33 as used to define fluorescent patterns on QD films, allowing for further applications in biosensing.
34 ing sol-gel films, and even drying colloidal films, along with this study, share the same physical or
36 ems: a music-playing flag, a sound recording film and a flexible microphone for security applications
37 ows a low optical bandgap of 1.49 eV in thin film and a high molar extinction coefficient of 1.90 x 1
40 of arbitrarily shaped structures of released film and locally specified thickness for each region.
42 in both the superconducting behaviour of the film and the three-dimensional (3D) magnetic structure o
43 ch as particles, 1D nanowires and fibres, 2D films and coated surfaces, and 3D patterned surfaces suc
44 elate with the increased permeability of the films and electrochemically active surface area of elect
45 at interest in releasing single crystal thin films and fabricating flexible electronics with these co
48 vated temperatures when compared to neat PEI films and other high-temperature polymer and nanocomposi
49 current photovoltaics, ferroelectric polymer films and single-layer orthorhombic monochalcogenides su
50 eps, the deposition temperatures of the thin films and the parameters of the photolithographic proces
51 t, these materials were fabricated into thin films and their specific binding ability was tested.
52 cracks in SiN films, self-de-bonding sol-gel films, and even drying colloidal films, along with this
53 process was used to grow an ultrathin silica film ( approximately 100 nm) consisting of highly ordere
57 composition of the gate dielectric and CuPc films are analyzed by atomic force microscopy, grazing i
58 aterials consisting of ultrathin Al-doped Ag films are attained having a homogeneous and low-loss res
62 vertical composition and properties of these films are designed at the atomic scale using layer-by-la
64 Moreover, while domain walls in in-plane films are generally expected to be non-chiral, we show t
65 y, high-quality mixed-cation perovskite thin films are normally made by use of antisolvent protocols.
67 ar processes of creep in metallic glass thin films are simulated at experimental timescales using a m
73 uper-fast vortices into a superconducting Pb film at rates of tens of GHz and velocities up to tens o
74 ed in the PEI sandwiched with CVD-grown h-BN films at elevated temperatures when compared to neat PEI
76 rength and lower elongation when compared to films based on native and single acid modified starches.
79 on optical properties and composition of the films, but negligible impact on TiOx surface silanizatio
80 evaluate the hero-villain skin dichotomy in film by (1) identifying dermatologic findings of the all
82 methylammonium lead iodide (CH3NH3PbI3) thin films by ultrafast transient absorption microscopy, demo
83 ere, we describe micro-patterned all-polymer films called micro-rolls that we use for encapsulating,
84 ecanethiol layer, the stability of the Ag-NW film can be greatly improved by 150-times compared with
85 -wavelength fs laser-based dewetting of thin films can be an effective means for the scalable manufac
86 perature of the substrate and thus conformal films can be coated on a range of substrates, including
87 he coloration intensities of these nanoscale films can be tuned by the number of deposition steps.
88 % for monolayer films to 130% for multilayer films, causing the adhesion toughness G c to decrease fr
92 t is commonly assumed that thinning of water films controls solute diffusion at low water contents, t
94 pproximately 100 nm linewidths by patterning film-coupled nanocubes in pixels using a fusion of botto
95 Cs of larger areas because of the incomplete film coverage caused by the dewetting of the hydrophilic
101 coated and passivated with an aluminum oxide film deposited by atomic layer deposition (ALD) with opt
103 on the use of ED-XRF spectrometry after thin film deposition on special sample retainers and a subseq
104 By using conformal oblique incidence thin film deposition onto an optical grating substrate, it is
105 rting electrolyte, the conditions of bismuth film deposition, an accumulation potential and time, the
107 ed here, using Diffusive Equilibrium in Thin-film (DET) gels as high-spatial-resolution passive-sampl
110 asmonic responses in SNL, these ultrathin 2D films display rapid and reversible red-blue color change
111 ed metal ions that assemble into metal oxide films during thermal oxidation of the sacrificial graphe
112 see text] decreases rapidly and the average film dynamics are enhanced by 6-14 orders of magnitude.
114 l microfabricated optically transparent thin-film electrode chip for fluorescence and absorption spec
115 lectropolymerization as a thin film on an Au film electrode in an electrochemical miniaturized microf
117 10microM to 50nM] in comparison to ta-C thin film electrodes and (ii) the coating method significantl
118 noncontinuous, nanostructured plasmonic gold film, enabling quantitative fluorescent detection of ant
119 ncies and grain boundaries of the perovskite film, enhancing the crystallization of perovskites and a
122 nodes for sodium-ion storage, these 3D MXene films exhibit much improved performances compared to mul
123 Here we report H c2 data for epitaxial thin films extracted from the electrical resistance measured
124 ) process to grow highly oriented perovskite films, featuring strong uniaxial-crystallographic textur
125 e study of the crystal structure of the thin-film, ferromagnetic topological insulator (Bi, Sb)2-x V
127 is investigated in situ, revealing that thin-film formation is mediated by solid-state precursor solv
128 olid-supported biofilms, elastic interfacial film formation occurs in the absence of flagella, pili,
131 ated with the use of PFAS-containing aqueous film-forming foams (AFFF) in firefighting activities.
134 large superconducting gaps observed in FeSe films grown on different STO surface terminations are li
135 epitaxial topological insulator Bi2Se3 thin films grown on superconducting NbSe2 single crystals.
136 ion at the surfaces of bulk Fe1+yTe and thin films grown on the topological insulator Bi2Te3 is cante
140 ack of low-damping, magnetostrictive ferrite films has hindered the development of power-efficient ma
141 aging but polycrystalline and amorphous thin films have shown inferior performance compared to inorga
142 gic findings to the all-time top 10 American film heroes quantitatively and qualitatively, and (3) an
144 ansport is investigated for solution-sheared films in field-effect transistors demonstrating that SBT
146 surements on an ultra-thin (001) BiFeO3 thin film, in combination with phase-field simulations, we sh
149 uced spontaneous partitioning of PbTiO3 thin films into nearly energetically degenerate, hierarchical
152 structure evolution of SrFeOx epitaxial thin films is identified in real-time, during the progress of
155 arent electrodes, the use of multilayer thin-films is steadily increasing throughout high-tech indust
157 eneration over many coherent lengths in thin film lithium niobate waveguides patterned with the gradi
160 thetic leaf made of graphene oxide (GO) thin film material, which exhibited broadband light absorptio
161 a new class of low-loss, magnetoelastic thin film materials that are promising for spin-mechanical de
163 ein, we deposit a 200 nm-thick Zr-based thin-film metallic glass (TFMG), which acts as an effective d
166 r understanding and optimization of the thin-film morphology and charge-transport properties of conju
167 ypical of nanoparticles, nanowires, and thin films, nanolattices redefine the limits of the accessibl
168 families and staff, and the impact of using filmed narrative interviews to enhance the 'voice' of se
169 ector-encoded chiral shape actuation in thin-film nematic polymer networks under external stimulus.
172 ctric ultracapacitors based on ferroelectric films of Ba(Zr0.2,Ti0.8)O3 which display high-energy den
173 roximately 200 nm) ionophore-based polymeric films of defined ion-exchange capacity have recently eme
174 of the films is shown to produce crystalline films of high chemical purity Li2S for the first time.
176 usion coefficients of these sites within PEC films of poly(diallyldimethylammonium), PDADMA, and poly
179 Using detailed structural analyses of FeRh films of varying crystalline quality and chemical order,
181 lithiation kinetics in epitaxial Fe3 O4 thin film on a Nb-doped SrTiO3 substrate is investigated.
182 entiodynamic electropolymerization as a thin film on an Au film electrode in an electrochemical minia
183 molecular beam epitaxy (MBE) grown NiO(001) film on Mg(001) substrate as the defect free NiO prototy
187 olution-processable, can be produced as thin films on electrodes by oxidative polymerizations, are pi
188 t UV-light activation of polycrystalline ZnO films on flexible polyimide (Kapton) substrates can be u
189 report physical vapor deposition of Cu thin films on large-format ( approximately 6 cm(2)) single-cr
191 Deposition of epitaxial germanium (Ge) thin films on silicon (Si) wafers has been achieved over larg
192 emically grow and transfer mesoporous silica films onto other substrates makes them an attractive mat
194 notable new diagnostic tests in DED are tear film osmolarity, inflammatory biomarkers, and meibomian
196 ommercial inkjet printer to fabricate a thin-film paper-based biophotovoltaic cell consisting of a la
198 (CIGS) is presently the most efficient thin-film photovoltaic technology with efficiencies exceeding
200 perties of soybean protein concentrate (SPC) films, plasticized with varying levels of glycerol and p
201 on, highly ordered and textured crystals for films prepared from solutions with lower colloidal conce
202 uniform from 2-12 wk, whereas flexible thin-film probes yield a marked accumulation of astrocytes an
203 PS characterization of the same FA-PVSK thin films provide complementary near-surface measurements of
205 s transport from the solution to the sensing film, resulting in an increase of peak current with ion
209 t previous studies of periodic cracks in SiN films, self-de-bonding sol-gel films, and even drying co
211 onductor architecture, in which an insulator film serves as a protection layer, can prevent corrosion
212 l studies on B-site doping of Nb ions in BFO films showed change in the domain structures due to dopi
213 n aqueous media by tamoxifen and BAY 11-7082 films shows similar behavior to drugs pre-dissolved in d
214 ulk aqueous solutions and in viscous aqueous films, simulating the conditions of a high-solute-streng
215 sing these insights, it is demonstrated that films simultaneously harvest energy and information from
216 laying the further commercialization of thin-film solar cells based on hybrid organohalide lead perov
220 ted average (TWA) passive sampling with thin film solid phase microextraction (TF-SPME) and liquid ch
222 At the same time, the coherently strained film structure suppresses extrinsic damping, enables sof
223 In this work, 4-layered SiO2/Bi2Te3/SiO2/Cu film structures were designed and fabricated and the opt
225 P-dependent cellular degradation of collagen film, suggesting that cell-surface collagen degradation
226 dispersion in a 300 nm thick silicon nitride film, suitable for semiconductor manufacturing but previ
227 alize epitaxial (SrFeO2.5)1/(CaFeO2.5)1 thin film superlattices possessing both anion-vacancy order a
228 Novel techniques of MIP deposition as thin films, surface development, and introduction of addition
229 n a single glass substrate of different thin film technologies in order to develop a multifunctional
231 general approach to remote-controlled, smart films that undergo simultaneous changes of surface color
232 rature cuprates to ultrathin superconducting films - that experience superconductor-to-insulator tran
235 ography process, and the surface profile and film thickness of each layer were measured by two differ
236 e the effect of doping, substrate choice and film thickness on the (Bi, Sb)2Te3 unit cell using high-
237 o many limitations, such as material choice, film thickness, and spectral ranges where combs can be g
238 ed the diffusion length to always exceed the film thickness, leading to full exponential growth over
239 d this mobile SEF system by tuning the metal-film thickness, spacer distance, excitation angle and po
240 Specifically, these steps cause increased film thickness, which diminishes performance by mass ove
243 mage through as-deposited, ultra-thin silver films, this technique requires no nanofabrication beyond
244 the behaviour of single-crystal La2-xSrxCuO4 films through which an electrical current is being passe
245 ll-time top 10 American villains are used in film to highlight the dichotomy of good and evil, which
246 ode mixity decreases from 232% for monolayer films to 130% for multilayer films, causing the adhesion
249 processed as semiconductors in organic thin-film transistors (TFTs) that show ambipolar behavior.
250 r based on copper phthalocyanine (CuPc) thin film transistors (TFTs) with a simple, low-cost UV-ozone
253 g porous multiwalled carbon nanotube (MWCNT) films using cultured, harmless bacteria as porogens, and
254 ing high-resolution e-beam lithography, thin film vacuum deposition and reactive-ion etching processe
255 anopores into the organic semiconductor thin films via a simple and robust templated meniscus-guided
256 soporous metal-organic framework (mMOF) thin films via the electrochemically assisted self-assembly (
258 gic findings of the all-time top 10 American film villains, (2) comparing these dermatologic findings
262 lass of site-specifically metal-modified DNA films was characterized by UV, circular dichroism (CD),
263 ed method, the sample specimen of multilayer films was fabricated via photolithography process, and t
264 hat by using functionalized NDs on ta-C thin films we can significantly improve sensitivity towards d
265 y-induced bonding; where amorphous polymeric films were bonded together in a period of time on the or
268 on-withdrawing conditions of polycrystalline films, where excess basic precursors are found between g
269 ilm amplifies the ethanol sensitivity of the film, whereby the GN/BCN sensor has 12400% sensitivity f
270 directly observed on polycrystalline silver films which suffer from significant plasmonic losses due
271 A prominent instance is the Tp-Bpy thin film, which displays an unprecedented acetonitrile perme
272 ation of an ultrathin titanium nitride (TiN) film, which is incorporated in a gated TiN/SiO2/Ag plasm
273 to produce different oxygen contents in the films, which has resulted in significant structural chan
274 that, by decorating the as-formed Ag-NW thin film with a dense, hydrophobic dodecanethiol layer, the
280 al conditions for thin-layer ionophore-based films with cation-exchange capacity read out with cyclic
284 the past 2-3 years, direct lithography on NC films with e-beams and X-rays has gone through an import
286 By tuning the solution-state structure, films with high crystallinity and good interdomain conne
288 nge bias (EB) in single-phase manganite thin films with nominallyuniform chemical composition across
289 of 3 kOe, indicating that the epitaxial BaM films with strong self-biased behaviors have good electr
290 UV-Vis spectrophotometry reveals that DNA films with surface densities up to 0.031 mg/mm(2) can re
292 gation, the quarternary TiSiCN nanocomposite films with the different C and Si contents are synthesiz
294 ately approximate the dye absorption on TiO2 films with up to a 250 nm blue-shift of the dye absorpti
295 transport study of the codoped (Bi,Sb)2 Te3 films with varied Cr/V ratios reveals that magnetic codo
298 er, centrosymmetric and semiconducting PtSe2 film without the characteristic spin splitting in conven
299 oltaic devices from optimized ACI perovskite films yield a power-conversion-efficiency of 7.26% with
300 d magnetic properties of single crystal thin-film YIG where the temperature dependence of the magneti
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