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1 a 20 um diameter capacitor in a 100-nm-thick film).
2 tive readings of the bio (sensing) imprinted film.
3 applied to the epitaxial alpha-FAPbI(3) thin film.
4 ive field of 30 mT at 5 K for a 125-nm-thick film.
5 e soft layers, fabricated on a piezoelectric film.
6 droplet and a smooth solid or a liquid thin film.
7 ) and a neighboring ferroelectric oxide thin film.
8 ubstrate are broken to create a freestanding film.
9 itude improvement over that of the monomeric film.
10 V does not affect the osmolarity of the tear film.
11 the (100) film, followed by (110) and (111) films.
12 lting in the formation of lead and iodine in films.
13 es of surfactant-templated mesoporous silica films.
14 stinctly different from the undoped BiFeO(3) films.
15 ductive meanders encapsulated by stretchable films.
16 igh-quality synthesis of the above-mentioned films.
17 y systems including mucoadhesive tablets and films.
18 desired mechanical property of the chitosan films.
19 based on amorphous [Formula: see text] thin films.
20 LED behavior on the pre-deposited insulating films.
21 of etoricoxib was calculated in each of the films.
22 ature dependence observed in thicker organic films.
23 ower than the bulk IL, even for the thickest films.
24 of glass-forming materials confined to thin films.
25 process emitting materials into uniform thin films.
26 to previously reported pure Ti(3) C(2) T(x) films.
27 opy nitrides have only been produced as thin films.
28 agreement with reported works on dry protein films.
29 nanopillar regions in perovskite oxide thin films.
30 angstroms to nanometers thick adsorbed H(2)O films.
31 d topological order in topological insulator films.
32 e and negative ion mode for a series protein films.
33 ferromagnetism was induced in the composite films.
34 harge leached at the slowest rate from CNT/E films.
35 , increasing doses of apomorphine sublingual film (10-35 mg) were administered until a tolerable full
36 ized thickness and optical properties of ITO film, a lossy-mode resonance (LMR) could be observed in
37 membrane, smooth thickness variations in the film act as a correlated disordered potential, focusing
38 ce render repeated and fast actuation of the films (actuation within 5 s and recovery in 2 s) when ex
39 tion spectroscopy) study of a sputtered thin film Ag cathode on a Ge ATR crystal in CO(2)-saturated 0
40 s onto methylammonium lead iodide (MAPbI(3)) films, age them under accelerated conditions, and determ
41 e orientation of graphitic planes within the film aligns preferentially with the silicon substrate.
42 l domain, where electrical properties of the film allowed for application of the sensor as a working
43 with improved PLQY of 36%, for a 60 nm thick film, among the highest reported for lead-free low-dimen
44 near the bandgap edge, the Se(0.32) Te(0.68) film (an optical bandgap of ~0.8 eV)-based photoconducto
45 e strength up to ~570 MPa for a 940 nm thick film and electrical conductivity of ~15 100 S cm(-1) for
46 thermodesorbed pollutants on a polymer thin film and then, their quantification by ATR-FTIR using a
48 e mismatch of the mixed "A" site composition films and devices leads to a steric effect to impede the
49 oscopy to measure the ion permeability of GO films and evaluate its relationship with the measured ca
52 oping in green solvent-processed metal oxide films and the promise of high-performance, ultra-stable
53 s were performed on single crystals and thin films, and theoretical predictions were made using molec
55 c structure, and charge transport of IGO:PVA film are investigated by a battery of experimental and t
56 similar topographical features of the liquid film are produced during the standard technique used to
57 nducting molecularly imprinted polymer (MIP) films are deposited by electropolymerization at relative
58 n walls in single-crystal complex oxide thin films are found to be orders of magnitude slower when th
60 operties of organic semiconductor (OSC) thin films are largely determined by their morphologies and c
61 no acid fragments from such hydrated protein films are observed and identified in the positive ion mo
64 afety and efficacy of apomorphine sublingual film as an on-demand therapy for off episodes in patient
69 osslinking imbues chemical stability to thin films at the expense of lower molecular transportation r
72 he deposition and physical properties of a-C films, basic understanding of the structure evolution du
74 ar Surface Disease Index questionnaire, Tear film break-up time, Ocular Protection Index, Ocular Surf
75 a microhole array patterned onto the PS thin film by laser dewetting was sprayed with dyed PVP in the
76 asses of 3D-inorganic nanofiber network (FN) films by a blow-spinning technique, including semiconduc
77 roperties in strain-released epitaxial oxide films by using electroactive substrates to impart strain
80 -excited coherent spin waves in a V(TCNE)(x) film can be transferred into an adjacent Pt layer via sp
81 shown that the bandgaps of Se(x) Te(1-) (x) films can be tuned continuously from 0.31 eV (Te) to 1.8
82 robust thermoplastic polyurethane fibers and films capable of autonomous self-healing under ambient c
84 PCL Film is prepared using a combination of film casting and sacrificial material leaching with a po
85 ring enhancement on chiral nanostructured Au films (CNAFs) equipped in the normal Raman scattering Sp
87 utegravir pharmacokinetics within-subject on film-coated tablet doses of 25 mg or 35 mg once daily, w
89 those 30 kg to less than 40 kg taking 35 mg film-coated tablets the GM C(trough) was 0.46 mg/L (63%)
90 ighing 20 kg to less than 25 kg taking 25 mg film-coated tablets, the geometric mean (GM) C(trough) (
91 ighing 25 kg to less than 30 kg taking 25 mg film-coated tablets, the GM C(trough) was 0.39 mg/L (48%
96 tural defects in the metal-organic framework film comprising uncoupled Cu(II) centres homogenously di
98 resent a facile technique, which uses a thin film contact thermometer based on the phase change mater
100 singly, thermal annealing does not alter the film crystallinity, R-SoXS characteristic size scale, re
101 ely low water vapor transmission rate of the films, decreasing the fruits' mass loss, and, consequent
102 in colloidal quantum dot solar cells due to film defects, physical damage, and contaminants across n
104 e-step generated 0D-2D bio-composite sensing film demonstrates synergetic effects from both the soft
108 enabled by epitaxial Fe(0.52) Rh(0.48) thin films designed so that both ferromagnetic and antiferrom
111 egrated with the diffusive gradients in thin films (DGT) technique for the direct determination of aq
112 pling technique, diffusive gradients in thin films (DGT), confronts many of the challenges associated
114 n of the structure of amorphous carbon (a-C) films during deposition and thermal annealing is of sign
115 ducted site-directed mutagenesis and protein film electrochemistry to determine how efficient catalys
116 of Cr(2)O(3) on isostructural V(2)O(3) thin film electrodes helps eliminate the existence of twin do
117 tal-organic frameworks (MOFs) as drop-casted film electrodes that facilitate voltammetric detection o
118 esigned and fabricated Pd/Au bimetallic thin film electrodes with isolated Pd nanoparticles via under
119 nterlayer slips and wrinkles of the graphene film endow the robust protective skin with high stretcha
121 st antimicrobial effect was obtained with MC films enriched with 2% (w/w) RE against to Listeria mono
122 t into the fundamental mechanisms underlying film evolution at pressures between one and hundreds of
123 that gold electrodes prepared on polyolefin films exhibit a low charge transfer resistance of about
129 ication of PSMNs to the skin, implanted thin films facilitated sustained and temporal release of indi
131 al sensor with a biomimetic plastic antibody film for carcinoembryonic antigen (CEA, an important bio
132 ms to utilize diamond-like carbon (DLC) thin films for bioreceptor immobilization and amperometric bi
134 ic devices, yet fundamental understanding of film formation, key to optimizing these devices, is lack
135 erous iodine vacancies at the surface of the film formed by their evaporation during the thermal anne
137 (GenX, ADONA, 9Cl-PF3ONS), and three aqueous film-forming foam (AFFF)-related zwitterionic PFASs (AmP
140 del is employed to discern the signal of the film from the signal of the seed layer and the data are
141 hin-film transistor based on this irradiated film gave a highest mobility of 1.5 cm(2) V(-1) s(-1) al
142 cillations and Kiessig thickness fringes for films grown at 200 degrees C under 15 mTorr Ar, indicati
143 N, studied by comparative analysis of GaN:Mg films grown by MOCVD on high and low hillock density GaN
144 ructure evolution due to phase change during film growth and heating is fairly sparse and empirical,
145 orce microscopy to yield nearly pinhole-free film growth while maintaining epitaxy and high crystal q
147 Optical measurements show as-deposited FAPI films have absorption onsets in the near infra-red with
148 on chiral pai-conjugated systems whose thin films have been characterized by ECD and/or CPL, as well
149 ansport properties of MoS(2,) and WS(2) thin films have been investigated systematically to fabricate
150 er, water clusters from the hydrated protein films have been observed and identified in both the posi
151 increase in the oxygen diffusion through the films (i) faded the black color of the olives, (ii) soft
156 ovide a promising approach to transform flat films into 3D complex structures that are difficult to a
158 magnification SEM images show that the thin film is comprised of a network of intimately connected F
159 angle of ~90 in the modulation-doped Cr-BST film is demonstrated at 2.5 K, and the spin Hall angle d
160 ules, indicating that the hydrogel waveguide film is highly porous to both sizes of molecule, thus po
161 he materials studied, an anthocyanin-agarose film is nominated as the optimum materials with the best
164 fabrication of epitaxial beta-Ga(2)O(3) thin films is challenging on flexible substrates due to high-
165 anomalous Hall conductivity in Mn(3)Sn thin films is investigated by polarization-resolved spectrosc
166 methylammonium concentration in mixed cation films is reduced or when NMPT is used as an additive, an
167 n of unreacted PbI(2) crystals in perovskite films is very important to improve device operational st
169 the bulk mobility transition, while in thin films it is a variant of the bulk result shifted toward
170 sample is available, for example, polyolefin film layers or the fractions from polyolefin separation
171 ding of supranano liquid metal in perovskite films leads to a cesium-based ternary perovskite solar c
172 h allows measurement of device-relevant thin films (<200 nm thickness), is exploited to deduce the pr
173 I(3) nanocrystal (NC)-polymer composite thin-film luminescent solar concentrators (LSCs) featuring hi
174 ovskites along the out-of-plane direction in films made by both spin-coating and scalable blading pro
177 sted that the prepared biocomposite chitosan films may be considered for active food packaging applic
178 e vision loss and macular disturbance, blood film microscopy to detect vacuolated lymphocytes is a ra
179 ribe the preparation and use of a thin metal film modified Indium Tin Oxide (ITO) electrode as a high
181 order by modulating the oxidation state of a film of a conducting polymer, such as poly(3-octylthioph
182 force microscope tip polarizes an ultrathin film of an archetypal dielectric SrTiO(3) via flexoelect
183 es a glassy carbon electrode modified with a film of conductive MOF (M(3)HXTP(2); M = Ni, Cu; and X =
186 Here, using 3D straining in nanocomposite films of (SmMnO(3))(0.5)((Bi,Sm)(2)O(3))(0.5), we demons
187 one to four layers), uniform, and continuous films of both defective gallium(II) sulfide (GaS): GaS(0
189 n emerging technique for rapid deposition of films of materials including micrometer-size and sub-mic
190 led the growth of centimeter-scale monolayer films of MoSi(2)N(4) This monolayer was built up by sept
193 roscopy on molecular beam epitaxy-grown thin films of YbRh(2)Si(2), a model strange-metal compound.
194 mmobilizing tyrosinase enzyme on spin-coated films of ZnO-rGO nanocomposite prepared via self-assembl
196 comprised of a vanadium dioxide (VO(2)) thin film on a silicon substrate with a gold back reflector.
202 m of our study was to assess changes of tear film osmolarity after micro-incision 25G+ pars plana vit
205 havior of 2D Ti(3) C(2) T(x) MXene assembled films over a broad range of film thicknesses, monolayer
208 g calcium carbonate nanoparticles to enhance film porosity leading to increased surface area of color
213 t the incorporation of ZnO@gal into chitosan films remarkably enhanced the desired mechanical propert
215 Molecular structure analysis of the product films revealed that C-H functionalization by [B(12)X(11)
217 address these gaps in understanding, organic film samples in an apartment unit were collected over th
219 le transistors based on the Dif-TES-ADT thin films show a mobility as high as 16.1 cm(2) V(-1) s(-1)
220 ransistors fabricated from the full-coverage films show high mobility (33 and 49 cm(2) V(-1) s(-1) fo
221 ort studies further demonstrated that MoS(2) films show p-type thermoelectric characteristics, while
222 nanoscopic picture of switching in molecular films show random current spikes, just opposite to the e
225 ed TONs as high as 175 when prepared as thin films, showing the beneficial influence of the POM.
226 anding the drainage dynamics of the thin air film squeezed by gravity between a millimetric droplet a
227 tivity modulation of a perovskite oxide thin film, SrTiO(3), that is well known to serve as the subst
231 ons at controlled positions in the modifying film, strong CO(2) adsorption and hydrogenation reactivi
232 er the optimum design of a multilayered thin film structure made out of transparent conducting oxide
233 on in 2D/three-dimensional (3D) hierarchical film structures broke new ground toward high device perf
234 ey physical properties of complex-oxide thin films, such as piezoelectricity and magnetostriction, ar
235 al hot-wall CVD system, CVD-derived graphene films suffer from surface contamination originating from
236 nd 3-nitrotyrosine (3-NT)) at the Pd/Au thin film surfaces affect the nature and reactivity of Pd/Au
237 ry layer on top of the primary 3D perovskite film that results in significant improvements in the pho
240 ion mechanism, providing mechanically robust films that can be easily separated from their substrates
241 use of bio-resorbable poly(ester urea) (PEU) films that controllably deliver a non-opioid COX-2 inhib
245 e the existence of twin domains in Cr(2)O(3) films, therefore significantly reducing leakage current
247 kness but also enhanced polar distortions as film thickness is reduced, unlike in perovskite ferroele
251 observed for the conversion of amorphous PET film to monomers across all nonzero MHETase concentratio
252 e SLED with a pre-existing patterned polymer film to study SLED's fundamental behavior in a bilayer g
253 nt to control the morphology of the quasi-2D films to achieve efficient energy transfer, which is a c
254 t rather facilitates Y6 migration to the BHJ film top surface, changes the PBDB-TF/Y6 vertical phase
255 h-resolved crystallography shows that the Ni films transform from an as-deposited disordered layer to
258 the realization of complementary oxide thin film transistors technology, transparent flexible circui
261 rication of these materials as wires, coils, films, tubes, cones, unimorphs, bimorphs, and printed el
262 ontrolling the temperature of the perovskite film under both dark and illuminated conditions, the mec
263 to our knowledge, AFM imaging of adsorbed PS films under physiologically relevant conditions using a
264 bout 100 micrometres), area (continuous thin films up to about 5.5 centimetres by 5.5 centimetres), a
266 eading to solid-state nanostructured colored films upon solvent evaporation, even in the presence of
270 nanocrystalline (NC) free-standing gold thin-film via in situ ion irradiation studied using atomic-re
271 2,4-triazole-3-thiol) (poly(T3T)) conductive film was coated successfully on the gold electrode (Au).
272 We discovered that the permittivity of the film was non-uniform with respect to the growth directio
274 Previous investigators concluded that the film weight is responsible for both the film collapse an
276 water vapor permeability (WVP) values of the films were found to have decreased significantly in para
277 ium-tin-oxide (ITO, In(2)O(3):Sn) mesoporous films were functionalized with 4-[N,N-di(p-tolyl)-amino]
278 conductive and transparent Ga doped ZnO thin films were grown via aerosol assisted chemical vapor dep
281 ivity of ~15 100 S cm(-1) for a 214 nm thick film, which are both the highest values compared to prev
282 the adsorption-induced squeeze-out of the PS film, which likely results in an interfacial monolayer e
283 ctrons at the grain boundaries of perovskite films, which are of significance to influence the carrie
284 erform experiments on vanadium dioxide VO(2) films, which exhibit a first-order PIPT accompanied by a
285 mbination of mechanical properties of GO/Mfp films will be attractive for a range of applications.
287 n, a 2D titanium carbide (Ti(3) C(2) ) MXene film with transparent conducting electrode (TCE) propert
288 ch for the industrial production of graphene films with appealing controllability and uniformity.
289 odifying the defective surface of perovskite films with cadmium iodide (CdI(2)) effectively reduces t
290 of single crystal Mn(x) Fe(3-) (x) O(4) thin films with controlled stoichiometry, 0 <= x <= 2.3, and
291 ithiophene (Dif-TES-ADT) as an example, thin films with millimeter-sized single-crystal domains and p
292 solvent leads to high-quality 2D perovskite films with sandwich-type structures and vertical phase s
294 in highly crystalline antiferromagnetic CrN films with strain and reduced dimensionality is reported
296 of the polymers allows the formation of thin films with uniaxially aligned polymer chains by using a
297 patient treated with apomorphine sublingual film (with known cardiac risk factors) had a fatal cardi
298 around 0.5 volts across a 7-micrometre-thick film, with a current density of around 17 microamperes p