ライフサイエンスコーパス: thin film

1 t presents the liquid to the laser beam as a thin film.

2 bs to the air-water surface of the lung as a thin film.

3 it has yet to be deposited and studied as a thin film.

4 eters thanks to the continuous nature of the thin film.

5 in the highly strain sensitive quenched FeRh thin film.

6 ins are dried onto the ATR crystal forming a thin film.

7 t is applied to the epitaxial alpha-FAPbI(3) thin film.

8 etric droplet and a smooth solid or a liquid thin film.

9 MoS(2) and a neighboring ferroelectric oxide thin film.

10 nanoparticles buried under a 50 nm thick Cu thin film.

11 nctions via selective chemical doping of TMD thin films.

12 crystals and anthradithiophene (diF-TES-ADT) thin films.

13 urity binding energy of ~1 eV for dielectric thin films.

14 anced atomic layer deposition of metal oxide thin films.

15 -entropy nitrides have only been produced as thin films.

16 on rate is obtained in organic semiconductor thin films.

17 rming nanopillar regions in perovskite oxide thin films.

18 d comparing the transition behaviour of FeRh thin films.

19 port properties of lithium-decorated ZrTe(5) thin films.

20 tching experiments in PbZr(0.2) Ti(0.8) O(3) thin films.

21 ray-coating ink to produce large-area 2D COF thin films.

22 rm structural and chemical properties of our thin films.

23 not been explored for surface doping of OSC thin films.

24 storage performance of relaxor ferroelectric thin films.

25 easurements on the superconducting nickelate thin films.

26 sts in molecular single crystals but also in thin films.

27 t magnetization (NRM) of the above-mentioned thin films.

28 films to 77.2 degrees for QA coated MAPbI(3) thin films.

29 vices based on amorphous [Formula: see text] thin films.

30 amics of glass-forming materials confined to thin films.

31 d to process emitting materials into uniform thin films.

32 s with well-defined sizes and geometries, in thin films.

33 PV performance in comparison to nanocrystal thin-films.

34 single-crystal hBN monolayers on a Cu (111) thin film across a two-inch c-plane sapphire wafer.

35 Combining our experiments with thin film active chiral fluid theory we identify a mecha

36 bsorption spectroscopy) study of a sputtered thin film Ag cathode on a Ge ATR crystal in CO(2)-satura

37 in-plane strain that transfers to the CoFeB thin film and changes its magnetic anisotropy H(k).

38 on of thermodesorbed pollutants on a polymer thin film and then, their quantification by ATR-FTIR usi

39 l pending groups affect molecular packing in thin films and affect the long-term performance of PSCs.

40 overs the recent design and synthesis of COF thin films and covalent monolayers as well as their prop

41 The synthesis of COF thin films and covalent monolayers mainly utilizes dynam

42 f internal fields, deep inside semiconductor thin films and heterojunctions.

43 (e.g., topological Hall effect) in magnetic thin films and heterostructures is discussed.

44 e study of topological structures in ferroic thin films and heterostructures is explored, including t

45 Mid-infrared (IR) ellipsometry of thin films and molecule layers at solid-liquid interface

46 ability of QA passivated MAPbI(3) perovskite thin films and PSCs were significantly enhanced, retaini

47 discovered to exist in both CH(3)NH(3)PbI(3) thin films and single crystals.

48 so examine the strategies to process them as thin films and stress the importance of analysing the ef

49 microscopy study of nominal 50 nm thick FeRh thin films and subtractively patterned wires of width 0.

50 In ferroelectric thin films and superlattices, the polarization is intric

51 their reduced domain spacing when cast into thin films and their reduced micellar size in solution.

52 c 1d periodic texture previously observed in thin films and under applied electric fields.

53 following: three-dimensional (3D) printing, thin-film and multilayered structures, and integrated ma

54 nano-spectroscopic characterization for MOF thin-films and explore the potential of MOFs as model sy

55 sensitive metamagnetic materials systems in thin film, and possibly in bulk, heterostructures.

56 calculations, the synthesis of high-quality thin films, and the characterization of their emergent p

57 ements were performed on single crystals and thin films, and theoretical predictions were made using

58 optoelectronic properties suggest CuPbSbS(3) thin films are excellent candidates for solar absorbers.

59 domain walls in single-crystal complex oxide thin films are found to be orders of magnitude slower wh

60 e attributes of 2D COFs, spray-coated 2D COF thin films are incorporated as the active material in ac

61 ic properties of organic semiconductor (OSC) thin films are largely determined by their morphologies

62 These results suggest that PbPdT thin films are multiferroic (ferroelectric-ferromagnetic

63 We experimentally demonstrate that such thin films are promising candidates to tune and control

64 um oxide (TiO(2)) and tungsten oxide (WO(3)) thin films, as examples.

65 d molecular excitons in a disordered organic thin film at room temperature is demonstrated, where the

66 e investigated the optical properties of ITO thin films at high temperatures up to 800 degrees C usin

67 and reduction potential energies of the ITO thin films at high temperatures.

68 er crosslinking imbues chemical stability to thin films at the expense of lower molecular transportat

69 Among various candidates, thin films based on relaxor ferroelectrics, a special ki

70 rigorous dynamical scattering theories, the thin-film-based X-ray waveguide fluorescence holography

71 The thin-film bioelectronic system avoids the use of bulky,

72 For structures consisting of a thin film bonded to a compliant substrate, wrinkling of

73 nnovative approach to produce anchored smart thin films both thermo- and electro-responsive, with the

74 ray, a microhole array patterned onto the PS thin film by laser dewetting was sprayed with dyed PVP i

75 ed [Formula: see text] preferred-oriented Au thin films by DC plating at 5 mA/cm(2).

76 a TiO(2) capping layer on an epitaxial VO(2) thin film can effectively reduce the resistance of the i

77 rs, CAR-T-cell-loaded micropatterned nitinol thin films can improve the effects of cell-based therapi

78 asy-plane insulating AFM, an alpha-Fe(2)O(3) thin film, can efficiently transmit spins over micrometr

79 Direct synthesis of thin-film carbon nanomaterials on oxide-coated silicon s

80 wo-pronged strategy for producing engineered thin-film carbon nanomaterials that have a nano-graphiti

81 ltaT(EC) , have been achieved in traditional thin-film ceramics and polymer ferroelectrics, they requ

82 With halide perovskite thin films coated by QA, PSCs based on methylammonium le

83 Our study shows that thin-film-coated ITO electrodes are simple to make and c

84 The novel thin film coating method significantly improved extracti

85 is work, it is demonstrated that a plasmonic thin film composed of Au nanoparticles embedded in a CuO

86 membrane surface in the form of a relatively thin film composed of connected submicrometer silica par

87 water recovery, and metal rejection, using a thin-film composite (TFC) membrane.

88 Scanning electron microscope images of the thin-film composite membrane after long-term assays were

89 lopment of a pervaporation (PV) desalination thin-film composite membrane with water fluxes reaching

90 y are being used to guide the development of thin-film composite membrane-based detection methods for

91 Conventional polyamide thin-film composite membranes with a ridge-and-valley st

92 ces were enabled by the advent of mesoporous thin films, comprised of anatase TiO(2) nanocrystallites

93 The perovskite-molecule composite thin films consist of in-situ formed high-quality perovs

94 we present a facile technique, which uses a thin film contact thermometer based on the phase change

95 al sclerosis, we show that the piezoelectric thin films, coupled with algorithms for the real-time de

96 Improvement of thin film crystal quality and removal of void and pinhol

97 r-to-electric power conversion efficiency in thin film crystalline silicon solar cell architectures r

98 es of both polycrystalline and epitaxial ITO thin films decrease with increasing temperature due to e

99 e perform theoretical modeling to understand thin film delamination from an indium tin oxide (ITO) cu

100 graphene on SiC by sulfurization of WO(3-x) thin films deposited directly onto the substrate.

101 due to the difficulties in fabrication, GaP thin films deposited on transparent substrates have neve

102 solar photovoltaic devices, Cu(3)VSe(4) NSs thin-films deposited on FTO were subjected to photoelect

103 uasi-2D sulvanite nanosheets are amenable to thin-film deposition and could show superior PV performa

104 gy is enabled by epitaxial Fe(0.52) Rh(0.48) thin films designed so that both ferromagnetic and antif

105 that enables the integration of 2D COFs into thin-film device architectures.

106 imits its further applications in large-area thin-film devices and integrated circuits.

107 ents a critical step toward functional ultra-thin-film devices for future thermoelectric and molecula

108 Here we show that thin-film devices made from nanometre-scale protein wire

109 a promising alternative to ILs for advanced thin-film devices.

110 The diffusive gradients in thin films (DGT) passive sampling technique has been inc

111 s integrated with the diffusive gradients in thin films (DGT) technique for the direct determination

112 e sampling technique, diffusive gradients in thin films (DGT), confronts many of the challenges assoc

113 rine conditions using diffusive gradients in thin-films (DGT) coupled to regionally specific ecotoxic

114 The 17-AAG liposomes was prepared by thin film dispersion methods.

115 tion on locations of defects relative to the thin film edge of the qubit circuit.

116 Recently, epitaxial V(2)O(3) thin film electrodes have been used to eliminate twin bo

117 rowth of Cr(2)O(3) on isostructural V(2)O(3) thin film electrodes helps eliminate the existence of tw

118 RF-PECVD method was employed to prepare DLC thin film electrodes with desirable surface and bulk pro

119 we designed and fabricated Pd/Au bimetallic thin film electrodes with isolated Pd nanoparticles via

120 e, we present a combinatorial study of Pd-Cu thin-film electrodes with well-defined composition and s

121 the first demonstration of a wireless, soft, thin-film electronics for a real-time, reliable assessme

122 nt a step forward in the characterization of thin films experiencing buckling-induced out-of-plane sh

123 tile titanium oxide (TiO(2)) nanoparticulate thin films fabricated on silica and Indium Tin Oxide (IT

124 application of PSMNs to the skin, implanted thin films facilitated sustained and temporal release of

125 creation and erasure of arbitrary shapes of thin-film ferromagnetic structures is reported.

126 rk aims to utilize diamond-like carbon (DLC) thin films for bioreceptor immobilization and amperometr

127 re, we develop perovskite-molecule composite thin films for efficient and stable PeLEDs.

128 ss-manufacturable, conformable piezoelectric thin films for strain mapping; multiphysics modelling fo

129 e COF powders, eliminating the need for both thin-film formation and conductive polymer guests, would

130 Thin films grown at 150 mTorr exhibits the highest magne

131 ing niobium-titanium-nitride (Nb(1-x)Ti(x)N) thin films grown by the atomic layer deposition (ALD) wi

132 ed by focusing on the properties of BaTiO(3) thin films grown on very thin layers of PbTiO(3) using x

133 erties of electrodeposited bismuth telluride thin films, grown on indium tin oxide.

134 By exploiting the thin-film growth mechanisms of aluminum during ultrahigh

135 hile both compounds show pai-pai stacking in thin films, H-tpPDI is more slip-stacked than octyl-tpPD

136 h of polycrystalline CdMnTe ternary compound thin films has been carried out using cathodic electrode

137 ature on chiral pai-conjugated systems whose thin films have been characterized by ECD and/or CPL, as

138 inium lead iodide (CH(NH(2))(2)PbI(3), FAPI) thin films have been deposited on glass substrates at 15

139 ic transport properties of MoS(2,) and WS(2) thin films have been investigated systematically to fabr

140 electrical conductivity) of electrodeposited thin films have been measured down to 100 K.

141 dimensional magnetization in a ferromagnetic thin film heterostructure.

142 tice mismatch to control ferroelectricity in thin-film heterostructures.

143 ent of small size Pd nanoparticles in the Pd thin film in the presence of gold exhibits unusual prope

144 perties of poly(3,4-propylenedioxythiophene) thin films in-situ using customized environmental nanoin

145 ding a layer of air (an air bridge) within a thin-film In(0.53)Ga(0.47)As cell.

146 Dynamic thin film interferometry is a technique used to non-inva

147 d to a compliant substrate, wrinkling of the thin film is commonly observed as a result of mechanical

148 High magnification SEM images show that the thin film is comprised of a network of intimately connec

149 the top surface and bottom interface of the thin film is crucial toward this aim.

150 Mass transport at the PB thin film is shown not to be rate-limiting.

151 The fabrication of epitaxial beta-Ga(2)O(3) thin films is challenging on flexible substrates due to

152 gap states in metal halide perovskite (MHP) thin films is crucial to the further improvement of the

153 e THz anomalous Hall conductivity in Mn(3)Sn thin films is investigated by polarization-resolved spec

154 in gas or liquid state, the investigation of thin films is of high interest in the field of optoelect

155 than the bulk mobility transition, while in thin films it is a variant of the bulk result shifted to

156 ambient) model with two-dynamic (metal oxide thin film layer thickness and surface ligand layer void

157 e and roughness interface layer, metal oxide thin film layer, surface ligand layer, ambient) model wi

158 Recently, thin-film lithium niobate (LN) emerges as a promising pl

159 which allows measurement of device-relevant thin films (<200 nm thickness), is exploited to deduce t

160 ites has limited COF-based devices either to thin films (<250 nm) grown on conductive substrates or t

161 CsPbI(3) nanocrystal (NC)-polymer composite thin-film luminescent solar concentrators (LSCs) featuri

162 uced as a new hard magnet with potential for thin-film magnetic recording.

163 l in biorelevant applications as a versatile thin film material, e.g., as adhesive coating for cell i

164 hly attractive, and to be effective, demands thin film materials with large Seebeck coefficients.

165 h a broad tunability inaccessible to bulk or thin-film materials.

166 gs pave the way for lithium oxides to enable thin-film memristive devices with adjustable symmetry an

167 employed liquid chromatography (LC)-amenable thin-film microextraction (TFME) devices to further eluc

168 nus stresses, as measured using the Muscular Thin Film (MTF) assay.

169 ring system was constructed using a flexible thin-film multiplexed electrodes with b2LOxS and a DET-t

170 Compared to thin films, nanowires exhibit a higher surface-to-volume

171 ould positively impact the research on VO(2) thin films, not only as smart windows but also for numer

172 hthalene by local probe chemistry on a ultra-thin film of NaCl formed on a Cu(111) surface at 4.3 K i

173 sensing device constructed from an oriented thin film of the COF responded quickly to water vapor an

174 lly investigate the infrared emission from a thin film of vanadium dioxide (VO(2)).

175 ere, we investigate SB-CS in polycrystalline thin films of 1,6,7,12-tetra(phenoxy)perylene-3,4:9,10-b

176 The structural dynamics of planar thin films of an ionic liquid (IL) 1-butyl-3-methylimida

177 ely remove nanoparticles on centimeter-scale thin films of colloidal crystals, allowing them to be ph

178 l multilayer sample composed of 100 nm thick thin films of Cu, Zr, and ZrCuAg alloy in a fluorine gas

179 ight stoichiometric ratios yields phase-pure thin films of CuPbSbS(3) upon solution deposition and an

180 or doping beyond the superconducting dome in thin films of electron-doped La(2-) (x) Ce (x) CuO(4) (L

181 Thin films of four discotic liquid-crystalline hexa-peri

182 Since thin films of MoS(2) and MoSe(2) are typically more resi

183 verage of chiroptical properties measured on thin films of organic pai-conjugated molecules.

184 The successful realization of thin films of Sr(3) SnO opens opportunities to manipulat

185 n irradiation in a photooxidation microcosm, thin films of the asphalt binder produce abundant oil- a

186 Thin films of the compound readily fabricated from solut

187 nsfer from a Xe(+) focused ion beam (FIB) to thin films of the group IV dopants pre-deposited onto a

188 We explore the properties of thin films of the prototypical ferroelectric lead titana

189 or of electronic anisotropy, in high-quality thin films of the unconventional superconductor Sr(2)RuO

190 The structure is based on thin films of tungsten-doped vanadium dioxide where the

191 tudy, polystyrene (PS), Parylene C, and SU-8 thin films of varying thickness on silicon are utilized

192 spectroscopy on molecular beam epitaxy-grown thin films of YbRh(2)Si(2), a model strange-metal compou

193 d on [Formula: see text] crystals, amorphous thin-films of [Formula: see text] are potentially import

194 Thin-film OFETs fabricated with 1 and 2 both exhibited h

195 ice, comprised of a vanadium dioxide (VO(2)) thin film on a silicon substrate with a gold back reflec

196 pitaxy of (0001)-oriented CuCrO(2) epitaxial thin films on Al(2)O(3) substrates.

197 l growth of halide perovskite single-crystal thin films on lattice-mismatched halide perovskite subst

198 on in optimal-doped La(1.85) Sr(0.15) CuO(4) thin-film on SrTiO(3) substrate (LSCO/STO) is investigat

199 ive provides an overview of the emergence of thin film optical waveguides used for evanescent field s

200 ible reactions suitable for the synthesis of thin films or monolayers are still very limited.

201 arrangements of nanoparticles are needed for thin-film or membrane applications of GO, dispersed nano

202 is mediated by weighted stimuli through the thin film oxide leading to responses that resemble excit

203 Separately, lattice strain between thin film oxides and a substrate induces improved functi

204 s hydrogen absorption and HER activity for a thin film palladium electrocatalyst.

205 Submicron-scale EGaIn thin-film patterning with feature sizes as small as 180

206 A thin film placed on the surface of the fiber end-face ca

207 The resulting semiconductor thin films possess a direct optical band gap of 1.24 eV,

208 est magnetization with T(C) = 340 K as these thin films possess the lowest roughness and might exhibi

209 ere carried out in nanocrystalline pentacene thin films possessing spatial inversion symmetry that pr

210 e surface and film-center transitions, while thin films practically have a single transition througho

211 nificance of these results in the 30 nm LSMO thin films prepared at different oxygen growth pressures

212 resistance of large area MoS(2) and MoSe(2) thin film, prepared via low pressure chalcogenation of m

213 TMD thin-films present uniquely difficult challenges to effe

214 difference measurements are conducted on MHP thin films processed from dimethylformamide (DMF)-based

215 per cent, respectively(3)) is surprising in thin films processed from solution at low-temperature, a

216 In thin films, processes such as charge conduction, light a

217 With developments in materials, thin-film processing, fine-tuning of morphology, and opt

218 ion of inorganic semiconductors with organic thin films promises new strategies for the realization o

219 structure and symmetry of single-crystal and thin-film samples.

220 eestanding N -doped porous carbon nanofibers thin film (Se@NPCFs) as cathode.

221 lexible transistors based on the Dif-TES-ADT thin films show a mobility as high as 16.1 cm(2) V(-1) s

222 reached TONs as high as 175 when prepared as thin films, showing the beneficial influence of the POM.

223 The preformed lithium sulfate thin film significantly suppresses the generation of LiO

224 ew-layered nanosheets, nano- or microplates, thin films, single crystals, and polycrystalline bulks),

225 ersion efficiency of metal halide perovskite thin film solar cells.

226 acing state-of-the-art CdS in Cu(In,Ga)Se(2) thin-film solar cells, alternatives rarely exceed refere

227 with a hydrophilic-lipophilic balance (HLB), thin-film solid-phase microextraction (TF-SPME) sampler

228 al composition, and electronic uniformity of thin-film solution-processed optoelectronics are believe

229 polyacrylonitrile (PAN)-based biocompatible thin film sorbent coatings are used, since such material

230 able ovarian cancer, the cell-loaded nitinol thin films spatially conformed to the implantation site,

231 onductivity modulation of a perovskite oxide thin film, SrTiO(3), that is well known to serve as the

232 uggests that the electronic structure of ITO thin films strongly depends on temperature and oxygen pa

233 e after the optimum design of a multilayered thin film structure made out of transparent conducting o

234 er, key physical properties of complex-oxide thin films, such as piezoelectricity and magnetostrictio

235 It is observed that the TiO(2) thin films surface are predominated with nanoparticulate

236 (2) and 3-nitrotyrosine (3-NT)) at the Pd/Au thin film surfaces affect the nature and reactivity of P

237 s contact line, and the wetting state of the thin film surrounding the droplet.

238 A thin film synthesis of high-hardness (up to 37 GPa) B(50

239 ilms are very smooth with low roughness, the thin films synthesized at 150 mTorr having the lowest av

240 The results showed that the Au:CuO thin film system is a RI sensitive platform able to dete

241 Polymer thin films that emit and absorb circularly polarised lig

242 We have also succeeded in fabricating thin films that exhibit a large ANE at zero field, which

243 erials, leading to oscillations of the metal thin film thickness with small but positive growth per c

244 n their ensemble behaviour (as monolayers or thin films), this potential remains largely unexplored.

245 Here, we report the realization of tellurium thin films through thermal evaporation at cryogenic temp

246 l for the growth of various high-quality OSC thin films, thus opening up opportunities for high-perfo

247 A memristor paired with a metal-thin film titanium oxide microelectrode connects a silic

248 from 35.6 degrees for the pristine MAPbI(3) thin films to 77.2 degrees for QA coated MAPbI(3) thin f

249 ng of a magnesium zinc oxide (MZO) dual gate thin-film transistor (DGTFT) as the actuator and an MZO

250 d, vertically integrated stretchable organic thin-film transistor active-matrix, which is enabled by

251 A thin-film transistor based on this irradiated film gave

252 man mapping from a device in custom-designed thin-film-transistor-like geometry to track and actually

253 Among organic thin film transistors (OTFTs), Organic Electrochemical T

254 l for the realization of complementary oxide thin film transistors technology, transparent flexible c

255 as a dielectric material for use in organic thin film transistors was reported.

256 Bottom-gate bottom-contact organic thin film transistors were fabricated using PSBBB as die

257 amorphous indium-gallium-zinc oxide (a-IGZO) thin-film transistors (TFTs) and integrated circuits.

258 olution-processed indium gallium oxide (IGO) thin-film transistors (TFTs) is significantly enhanced b

259 become necessary to produce high-performance thin-film transistors (TFTs) that enable faster switchin

260 Specifically, thin-film transistors based on IGZO FN exhibit negligibl

261 reveals that the photoresponsive behavior of thin-film transistors including polymer/diarylethenes bl

262 oughly studied for its use in p-type organic thin-film transistors over the course of the past decade

263 igh-performance optically switchable organic thin-film transistors were fabricated.

264 y, this technique has been shown to work for thin films under aqueous environments but is limited to

265 As temperature increases, amorphous ITO thin films undergo a phase transition at ~ 200 degrees C

266 to about 100 micrometres), area (continuous thin films up to about 5.5 centimetres by 5.5 centimetre

267 tion-processed conjugated small-molecule OSC thin films usually exhibit abundant grain boundaries and

268 as studied using DGT (diffusive gradients in thin films): vertical one-dimensional (1D) profiles of C

269 hick nanocrystalline (NC) free-standing gold thin-film via in situ ion irradiation studied using atom

270 The Pd/Au thin film was demonstrated as an extremely sensitive and

271 A mixed-phase (anatase/rutile) TiO(2) thin film was produced at a substrate temperature of 400

272 us energy, the direct band gap E(g) of PbPdT thin films was calculated as 3 eV.

273 metal oxide semiconductor (CMOS) compatible thin film waveguides and microfluidics shows great promi

274 Highly oriented PbPdT thin films were deposited on {(LaAlO(3))(0.3)(Sr(2)AlTaO

275 The CdMnTe thin films were electroplated from electrolyte containin

276 The optical energy bandgaps of the thin films were found to be varying between ~ 1.90 and ~

277 Polymer multilayer thin films were generated to co-deliver a model combinat

278 ghly conductive and transparent Ga doped ZnO thin films were grown via aerosol assisted chemical vapo

279 Thin films were obtained by spin coating of colloidal so

280 ical and electrical properties of the CdMnTe thin films were studied using X-ray diffraction (XRD), S

281 rge area highly crystalline MoS(2) and WS(2) thin films were successfully grown on different substrat

282 Unlike MoS(2) ultra-thin films, where solution-based single source precursor

283 fs-PLD process parameters to prepare TiO(2) thin films, which are suitable for applications in photo

284 thiophene) polystyrene sulfonate (PEDOT:PSS) thin films, whose optical absorption can be modulated by

285 tive mechanistic insight into chiral polymer thin films will offer new approaches towards chiroptical

286 OER kinetics on PBSCF thin films with (100), (110), and (111) orientation, dep

287 midinium lead triiodide [CH(NH(2))(2)PbI(3)] thin films with a low dose of electron irradiation.

288 nickel titanium (commonly known as nitinol) thin films with complex designs, high structural resolut

289 ries of single crystal Mn(x) Fe(3-) (x) O(4) thin films with controlled stoichiometry, 0 <= x <= 2.3,

290 e sublimation to obtain high-quality compact thin films with favourable crystallographic orientation.

291 s demonstrated to fabricate high-quality OSC thin films with greatly enhanced charge transport proper

292 Our systematic study reveals that VO(2) thin films with just one layer 80 nm thick has the poten

293 e topological surface states in Bi(2)Te(2)Se thin films with large tunability using varied gate volta

294 thradithiophene (Dif-TES-ADT) as an example, thin films with millimeter-sized single-crystal domains

295 ontacts on monocrystalline halide perovskite thin films with minimum interfacial damage and an atomic

296 thermally evaporated Se(x) Te(1-) (x) alloy thin films with tunable bandgaps for the fabrication of

297 ture of the polymers allows the formation of thin films with uniaxially aligned polymer chains by usi

298 P behavior in LNO is manifested in epitaxial thin films with unprecedented high purities.

299 Here, we report [Formula: see text] thin-films with a thickness in the 5-200 nm range, depos

300 oducible superconducting state in Cd(3)As(2) thin films without any external stimuli.