ライフサイエンスコーパス: polycrystalline

1 Photoexcitation of vapor-deposited polycrystalline 188 nm thick films of 1 results in a 140

2 NMR spectra show that the Fe(CO)3 moiety in polycrystalline 4c (but not 4a) undergoes rapid rotation

3 on process can aid in rational design of the polycrystalline absorber films, leading to their enhance

4 nted thin films, and for CO and HCOO(-) over polycrystalline Ag and Sn.

5 nm amorphous-phase Co nanocrystals and 4 nm polycrystalline Ag nanocrystals at 25 degrees C, triangl

6 genated cis-azobenzene single crystal into a polycrystalline aggregate of its trans-isomer in a photo

7 can be expediently obtained in high yield as polycrystalline aggregates from solution.

8 thod to unravel microstructural evolution of polycrystalline Al microstructures at the mesoscales.

9 Our findings have shown that for polycrystalline alumina ceramics, an average grain size

10 ic circuitry and ultra-broadband imaging but polycrystalline and amorphous thin films have shown infe

11 made with scalable fabrication techniques is polycrystalline and contains inherent nanoscale line and

12 The gradient FeNi nanowires exhibit polycrystalline and crystal twinning at different areas

13 Excitons in polycrystalline and disordered films of organic semicond

14 hotogenerated via singlet exciton fission in polycrystalline and single-crystalline pentacene is repo

15 means of chemical vapor deposition (CVD) are polycrystalline and thus contain grain boundaries that c

16 oduced by chemical vapor deposition (CVD) is polycrystalline, and scattering of charge carriers at gr

17 teamine self assembled monolayers on a clean polycrystalline Au electrode surface.

18 Under identical conditions, polycrystalline Au electrodes and several other nanostru

19 l CO2 reduction catalysis mediated by planar polycrystalline Au surfaces.

20 concerted proton-electron transfer (CPET) to polycrystalline Au was probed indirectly by studying the

21 ion of the polymer-coated nanowires afforded polycrystalline Au-Co(3)O(4) nanowires that were determi

22 uch more positive result in which untextured polycrystalline (Ba(0.6)K(0.4))Fe(2)As(2) bulks and roun

23 rate, followed by overgrowth of high quality polycrystalline BDD (pBDD) and polishing to reveal appro

24 regions of sp(2) carbon into a high quality polycrystalline BDD electrode.

25 in transport properties of single elemental polycrystalline Bi via spark plasma sintering results in

26 of heterogeneous electron transfer (HET) at polycrystalline boron-doped diamond (pBDD) electrodes ha

27 rodes: glassy carbon (GC), oxygen-terminated polycrystalline boron-doped diamond (pBDD), edge plane p

28 Past studies of polycrystalline BPs were challenged by the existence of

29 single crystal synthesis yield a phase-pure polycrystalline bulk material of an additional forth sol

30 Polycrystalline Ca3-xTbxCo4O9 (x = 0.0-0.7) samples were

31 ation of enhanced thermoelectric response in polycrystalline Ca3Co4O9 on doping Tb ions in the materi

32 two industrially important binary tellurides-polycrystalline cadmium and bismuth tellurides- were stu

33 of tubule-delineating cells, and consist of polycrystalline calcium phosphate similar to the mineral

34 have in low temperature carrier transport in polycrystalline CdTe by revealing their propensity to ac

35 tomography, carrier lifetimes are mapped in polycrystalline CdTe photovoltaic devices.

36 carriers through and across defect states in polycrystalline CdTe thin films.

37 Recent experiments in polycrystalline, centrosymmetric perovskites (for exampl

38 rmed that the (In + Nb) co-doped rutile TiO2 polycrystalline ceramic had semiconductor grains and ins

39 ctric behavior and impedance spectrum of the polycrystalline ceramic sample indicated that the intern

40 ved in a lead-free (Bi1/2 Na1/2 )TiO3 -based polycrystalline ceramic.

41 e that the high translucency and strength of polycrystalline ceramics can be achieved through microst

42 iented specimen relative to the conventional polycrystalline ceramics.

43 Nb) co-doped rutile TiO2 single crystal and polycrystalline ceramics.

44 ation of single-crystal calcite (CaCO3) into polycrystalline cerussite (PbCO3) through reaction with

45 mately 220 nm in 2 ns for solution-processed polycrystalline CH3NH3PbI3 thin films.

46 nd Na(+) at pH 6 formed dendritic growth and polycrystalline circular assemblies on air-water interfa

47 in superdense nonmagnetic cobalt layers in a polycrystalline cobalt thin film.

48 our of some species of birds are examples of polycrystalline colloidal structures found in nature.

49 calcium phosphate, brushite), and 20 were of polycrystalline composition.

50 an organic matrix that arrange in fibre-like polycrystalline configurations.

51 Blue-phase specimens, however, are generally polycrystalline, consisting of randomly oriented domains

52 ts seem to be the dominant crystal facets in polycrystalline copper, opening up new routes to afforda

53 ut the electrochemical reduction of CO2 over polycrystalline copper.

54 s, current) over 3,000 times higher than its polycrystalline counterpart under moderate overpotential

55 ls of the hydrate (III) can be dehydrated to polycrystalline CsAgCu(CN)(3) (II) on heating at 100 deg

56 over the course of several hours, whereas a polycrystalline Cu electrode exhibited deactivation with

57 from the terraces and stepped sites found on polycrystalline Cu foil.

58 ) surface can be readily achieved on stacked polycrystalline Cu foils via simple oxygen chemisorption

59 Polycrystalline Cu surfaces were gradually oxidized in O

60 s and required 0.5 V less overpotential than polycrystalline Cu to reduce CO(2) at a higher rate than

61 zed by ambient chemical vapour deposition on polycrystalline Cu, and show how individual boundaries b

62 ivities were indistinguishable from those of polycrystalline Cu.

63 ately 200 to approximately 17,000 MOmega(-1) Polycrystalline CuI thin films were deposited at room te

64 Polycrystalline CuRhO2 is investigated as a photocathode

65 l diode), compared with a value of 3.1 for a polycrystalline deposit.

66 ducting (heavily boron doped), and intrinsic polycrystalline diamond are grown to create a sandwich s

67 we introduce a direct approach to transform polycrystalline diamond into high-quality graphene layer

68 Cantilevers based on polycrystalline diamond surfaces are very promising as c

69 ated for chemically grafting porcine OBPs on polycrystalline diamond surfaces for biosensor developme

70 ious similar devices fabricated on (100) and polycrystalline diamond, where the device is shown to op

71 lucidate the mechanism of graphene growth on polycrystalline diamond.

72 The long-range order is disrupted by polycrystalline disorder and the variations in electrost

73 nometres, and the realization so far of only polycrystalline DNA-interconnected nanoparticle superlat

74 ew characterization method for understanding polycrystalline domain structure and transport in plasti

75 films grown by vapour deposition tend to be polycrystalline due to the nucleation and growth of isla

76 ted CO reduction on Cu(100), Cu(111), and Cu(polycrystalline) electrodes in 0.1 M alkaline hydroxide

77 Using Li3OCl as a model polycrystalline electrolyte, we apply large-scale molecu

78 and hence they can affect the performance of polycrystalline engineering alloys.

79 oscillations in linear birefringence of many polycrystalline ensembles is accompanied by oscillations

80 cate that the inhomogeneous deformation in a polycrystalline environment results in significant resid

81 O states at relatively high temperature in a polycrystalline Er0.1Yb0.9Fe2O4 using Raman scattering.

82 t 2,600~3,000 degrees C and exhibits a micro-polycrystalline feature.

83 ielectric, and specific heat measurements on polycrystalline FeCr2S4 in external magnetic fields.

84 By using polycrystalline ferroelectric capacitors as a model syst

85 n size effects on the physical properties of polycrystalline ferroelectrics have been extensively stu

86 For example, it was shown in polycrystalline ferroelectrics that residual strains are

87 onstrated for BaTiO3-BiZn0.5Ti0.5O3 (BT-BZT) polycrystalline ferroelectrics, a prototypical lead-free

88 and cluster glasses, phase-separated oxides, polycrystalline ferroelectrics, and ferromagnets alike.

89 n electric-field-induced residual strains in polycrystalline ferroelectrics.

90 We report on SF in thin polycrystalline films of two terrylene-3,4:11,12-bis(dic

91 Unlike tetracene, which tends to form polycrystalline films when vapor deposited, DPT's pendan

92 substrates by different deposition methods, polycrystalline films with excess Ge were frequently obt

93 In fact, in the case of polycrystalline films, depending on the synthetic route,

94 ering chloride-capped CdTe nanocrystals into polycrystalline films, where Cl selectively segregates i

95 manner the proton-withdrawing conditions of polycrystalline films, where excess basic precursors are

96 up to 8 x 10(-4) cm/(V s) were obtained for polycrystalline films.

97 exchange bias phenomenon is not possible in polycrystalline films.

98 In polycrystalline form, Ca3Co4O9 is known to exhibit much

99 om a disordered amorphous form to an ordered polycrystalline form.

100 s with auxetic homogenous Poisson's ratio in polycrystalline form.

101 ver, most nanotwinned metals are produced in polycrystalline forms and therefore contain randomly ori

102 2-ylidene (Ir-NHC-Me2) complex adsorbed on a polycrystalline gold electrode.

103 A), and Ricinus communis agglutinin (RCA) on polycrystalline gold electrodes was optimized and charac

104 ptimised antibody immobilization on standard polycrystalline gold electrodes.

105 fied, polyethylene glycol monolayer modified polycrystalline gold surfaces, respond in a highly speci

106 Using a polycrystalline gold thin film subjected to heating, we

107 line materials is a single crystal; however, polycrystalline grain growth almost always stops before

108 e is known about the mechanical roles of the polycrystalline grains that constitute the ferritic matr

109 nto controlling the mechanical properties of polycrystalline graphene and provides guidelines for the

110 r dynamics simulations of nanoindentation on polycrystalline graphene at different sites including gr

111 Consequently, the failure behavior of polycrystalline graphene by nanoindentation is criticall

112 simulations to study the failure behavior of polycrystalline graphene by varying both grain size and

113 eristics at and near the indentation site in polycrystalline graphene during nanoindentation.

114 We show that polycrystalline graphene fails in a brittle mode and gra

115 hene biosensors reported so far are based on polycrystalline graphene flakes which are anchored on su

116 provides guidelines for the applications of polycrystalline graphene in flexible electronics and nan

117 Polycrystalline graphene is characterized using advanced

118 the grain size-dependent failure behavior of polycrystalline graphene is important for its applicatio

119 Our study suggests that polycrystalline graphene with good stitching may allow f

120 the first statistical theory of toughness in polycrystalline graphene, and elucidate the nanoscale or

121 f research reported in the past few years on polycrystalline graphene.

122 rmal, mechanical and optical properties of a polycrystalline graphene.

123 ons of grain boundaries, and applications of polycrystalline graphene.

124 used to measure the mechanical properties of polycrystalline graphene.

125 between the indenter tip and the defects in polycrystalline graphene.

126 by shock compression of pyrolytic as well as polycrystalline graphite to pressures from 19 GPa up to

127 nd starting at 50 GPa for both pyrolytic and polycrystalline graphite, we also record the direct form

128 bed by defects, leading to a rich variety of polycrystalline growth forms.

129 ced face-centered cubic titanium (fcc-Ti) in polycrystalline hexagonal close packed titanium (hcp-Ti)

130 monstrate that the superconductivity in bulk polycrystalline hexagonal epsilon-NbN is below approxima

131 rt the new discovery of superconductivity in polycrystalline hexagonal epsilon-NbN synthesized at hig

132 incompressibility and high shear rigidity of polycrystalline hexagonal epsilon-NbN using ultrasonic i

133 s) are comparable to reference devices using polycrystalline indium tin oxide (ITO) electrodes.

134 ition at approximately 3.2 K was observed in polycrystalline ingots.

135 and shear moduli (K and G, respectively) for polycrystalline inorganic compounds, using 1,940 compoun

136 interfacial regions show a thin region with polycrystalline Ir nanocrystals.

137 more complete Li-storage occurring in porous polycrystalline iron fluoride, and further, incomplete c

138 In polycrystalline islands, certain grain boundary types ar

139 phene films synthesized so far are typically polycrystalline, it is important to characterize and con

140 Amorphous and polycrystalline IYO films were grown via a low-temperatu

141 k-etched polymers to synthesize (i) vertical polycrystalline La0.7Sr0.3MnO3 nanorods on top of single

142 acitance may result from LIG's unusual ultra-polycrystalline lattice of pentagon-heptagon structures.

143 Light scattering by the polycrystalline lenses is minimized by the use of relati

144 0(5) are fabricated by depositing a layer of polycrystalline lithium niobate on the flat top surfaces

145 on the fabrication of such solar cells from polycrystalline, low purity (99.98%) p-type silicon star

146 tes remain obscured by extensive disorder in polycrystalline MAPbX3 films.

147 dynamics of ubiquitin to be even more like a polycrystalline material in which the alpha-helix and be

148 Polycrystalline material properties depend on the distri

149 These results pave the way for understanding polycrystalline material response under external stimuli

150 The properties of polycrystalline materials are often dominated by the siz

151 g and predicting the macroscopic rheology of polycrystalline materials based on single-crystal elasti

152 Grain boundaries create strained regions in polycrystalline materials by stabilizing dislocations an

153 The physical properties of polycrystalline materials depend on their microstructure

154 This is in direct contrast with the polycrystalline materials generally observed when magnes

155 e plastic deformation when the grain size of polycrystalline materials goes small.

156 Recent investigations in thin film polycrystalline materials have shown the formation of co

157 on behavior of rocks and other heterogeneous polycrystalline materials is proposed, based on understa

158 Polycrystalline materials synthesized by an iodine-catal

159 odels, I show that stress percolates through polycrystalline materials that have heterogeneous elasti

160 oundly important determinant of character in polycrystalline materials that is not well understood.

161 als changes in the local atomic structure in polycrystalline materials under fields.

162 Nano-grained polycrystalline materials were found to be strong but br

163 s have only been reported for crystalline or polycrystalline materials, suggesting that molecular dis

164 urity or phonon-impurity scattering in these polycrystalline materials, which supports high charge-ca

165 l length scales for both single crystals and polycrystalline materials.

166 ated to damage and deformation mechanisms in polycrystalline materials.

167 s general implications for the properties of polycrystalline materials.

168 erature deformation and recrystallization of polycrystalline materials.

169 le junctions are a key structural element in polycrystalline materials.

170 t co-orientation of the nanoparticles in the polycrystalline matrix occurs via solid-state secondary

171 The pure-phase Zr-MOF (i.e., UiO-66) polycrystalline membranes were fabricated on alumina hol

172 Polycrystalline metal oxides find diverse applications i

173 organic semiconductor molecule, polymer, and polycrystalline metal, respectively.

174 plication of dipole engineering to versatile polycrystalline metal/binary oxide functional interfaces

175 odel, predictions for bending and torsion in polycrystalline metals show excellent agreement with exp

176 e temperature ductility minimum" observed in polycrystalline metals.

177 Here we turn to polycrystalline methylammonium lead iodide perovskite, w

178 e report the preparation of highly textured, polycrystalline Mn3Ge films on amorphous substrates, wit

179 Using our results, we propose a polycrystalline model to quantify the impact of grain bo

180 aterials properties as well as supporting 3D polycrystalline modelling of materials performance.

181 Furthermore, the performance of polycrystalline MOF membranes strongly depends on the me

182 rain-growth models, validated by large-scale polycrystalline molecular dynamics simulations, show tha

183 gy of the grains and their boundaries in the polycrystalline molybdenum disulphide atomic layers are

184 yrmion bubbles in perpendicularly magnetised polycrystalline multilayers patterned into 1 microm diam

185 Observations revealed growth of winding polycrystalline nanoparticle chains by shape-directed na

186 the formation of an alpha-MoO3 phase with a polycrystalline nature.

187 PL was performed in both single-crystal and polycrystalline NGO (substrates and pellets) respectivel

188 rature is discovered, where a porous, rough, polycrystalline NH4 PbI3 non-perovskite thin film conver

189 geometric effect which enables large MFIS in polycrystalline Ni-Mn-Ga by matching grain and sample si

190 deformation experiments at high pressure on polycrystalline nickel suggest that dislocation activity

191 In bismuth-doped polycrystalline nickel, we found that ordered, segregati

192 and dissolution (e.g., crevice corrosion) of polycrystalline nonnoble metals, alloys, and inorganic m

193 ve to the orientation of grain boundaries in polycrystalline OIPCs.

194 of the viscous anisotropy of highly deformed polycrystalline olivine, we demonstrate a significant di

195 nsor to have superior uniformity compared to polycrystalline ones.

196 space and 3D reciprocal space for almost any polycrystalline or multi-phase material.

197 emperature under uniaxial stress can convert polycrystalline or single-crystal benzene monomer into s

198 By exposing a polycrystalline organic material, consisting of a XB-acc

199 d crystallization can yield solution-printed polycrystalline organic semiconductor films with transpo

200 ing on charge transport in the most relevant polycrystalline organic semiconductors is reviewed, and

201 n lengths greater than 100 nanometers in the polycrystalline organolead trihalide compound CH3NH3PbI3

202 In order to produce polycrystalline oxygen-terminated boron-doped diamond (B

203 ualitatively distinct from commonly observed polycrystalline packings contradicts conventional wisdom

204 n the MRJ state and the typical hyperstatic, polycrystalline packings with [Formula: see text] that a

205 oxygen reduction reaction (ORR) activity of polycrystalline palladium, platinum, ruthenium, gold, an

206 hydrothermal approach is used to synthesize polycrystalline particles with sizes ranging from <200 n

207 pography and trapped charge are acquired for polycrystalline pentacene thin-film transistors using el

208 However, the mobility and trap densities of polycrystalline perovskite films are still significantly

209 efforts on preparing uniform and large-grain polycrystalline perovskite films have led to enhanced ca

210 fect of large morphological heterogeneity of polycrystalline perovskite films on their device perform

211 and diffusivities, in neat CH3 NH3 PbI3 (Cl) polycrystalline perovskite films, the local (intra-grain

212 arrays that are distinguishable from general polycrystalline perovskite materials in terms of their c

213 vapor-assisted solution process to construct polycrystalline perovskite thin films with full surface

214 ear response under strong light, superior to polycrystalline photodetectors.

215 ivity and stability of Ni3S2 exceeds that of polycrystalline platinum and manganese, nickel, and coba

216 mical measurements at individual grains of a polycrystalline platinum electrode, while also allowing

217 entally measured hydrogen binding energy for polycrystalline platinum examined in several buffer solu

218 mm-sized, single-crystal graphene by coating polycrystalline platinum foils with a silicon-containing

219 techniques to study hydrazine oxidation on a polycrystalline platinum substrate both in air and in a

220 Hypochlorite oxidation on polycrystalline platinum yields ClO. radicals, which ini

221 ntification of adsorbed hydrogen, H(ads), at polycrystalline platinum.

222 7, which was synthesized in the form of bulk polycrystalline powder via high-temperature solid-state

223 exceeds the highest value reported for bulk polycrystalline Pt bimetallic alloys, and is 20-fold mor

224 bes (PtNT (Cu)), a 5% Cu monolayer on a bulk polycrystalline Pt electrode (5% ML Cu/BPPt), BPPt, and

225 ure the vibrational mode of CO adsorbed on a polycrystalline Pt surface.

226 Sputter-cleaned, polycrystalline Pt(5)Gd shows a 5-fold increase in ORR a

227 smooth surface mainly composed of thin-film polycrystalline Pt, with some apparent nanoscale roughne

228 The materials are among the most active polycrystalline Pt-based catalysts reported, presenting

229 single crystal pyrite and nanocrystalline or polycrystalline pyrite films for successful solar applic

230 port on phase-pure, large-grain, and uniform polycrystalline pyrite films that are fabricated by solu

231 le with field and laboratory observations of polycrystalline rocks), coupled to an idealized model of

232 re synthesized by wet chemistry methods, and polycrystalline rods, which are synthesized by templated

233 A polycrystalline sample of 1 displays three sextets in th

234 Ac measurements conducted on a polycrystalline sample of the complex (NBu4)2[ReCl4(ox)]

235 the highest value observed till date in any polycrystalline sample of this system.

236 Indentation testing on a well-sintered polycrystalline sample yielded the hardness of 11.8(4) G

237 rved low-field magnetoresistance effect in a polycrystalline sample.

238 ystal x-ray diffraction studies in nominally polycrystalline samples at ultrahigh pressures, as demon

239 Although previous studies on polycrystalline samples have identified a 105-K phase tr

240 nd -field electron paramagnetic resonance on polycrystalline samples of 1 and 2 and on single crystal

241 field-dependent magnetization experiments on polycrystalline samples of 1 reveal the occurrence of hi

242 the possibility of efficient DNP transfer in polycrystalline samples of [Co(en)3Cl3]2.NaCl.6H2O (en =

243 terizing the mechanical behavior of tungsten polycrystalline samples with ion-irradiated surfaces.

244 wth, and a coreactant for the synthesis of a polycrystalline semiconductor.

245 Thin-film polycrystalline semiconductors are currently at the fore

246 In polycrystalline semiconductors, grain boundaries are oft

247 ostic and applicable to other disordered and polycrystalline semiconductors.

248 The presence of the Ni layer as a polycrystalline shell completely hindered the light emis

249 iven core-shell morphology that emerges when polycrystalline shells of ZIF-8 (zeolitic imidazolate fr

250 probe the real-time interfacial dynamics of polycrystalline Si particles growing from an Al-Si-Cu li

251 d on the character of the twin boundaries in polycrystalline Si photovoltaic cells.

252 raphitic domains ( approximately 2.5 nm) and polycrystalline silicon ( approximately 5 nm).

253 While usually based on either amorphous or polycrystalline silicon (alpha-Si and poly-Si, respectiv

254 Here, we demonstrate wavelength-scale polycrystalline silicon (pSi) PhC microresonators with Q

255 t electronic immunoassay that uses a pair of polycrystalline silicon interdigitated electrodes for th

256 e propose innovative devices using step-gate polycrystalline silicon nanowire FET (poly-Si NW FETs),

257 diagnosis of bladder cancer, using an n-type polycrystalline silicon nanowire field-effect transistor

258 In this research, we used a polycrystalline silicon nanowire field-effect transistor

259 rmance demonstrated is comparable to that of polycrystalline-silicon backplane transistor-driven disp

260 Intrinsic nonuniformity in the polycrystalline-silicon backplane transistors of active

261 t room temperature; however, the traditional polycrystalline silver electrocatalyst requires a large

262 Measurements of polycrystalline silver films over a range of distances (

263 g time, it has not been directly observed on polycrystalline silver films which suffer from significa

264 approximately 20 times higher) compared with polycrystalline silver.

265 e and interparticle electrostatic repulsion, polycrystalline, single-crystalline and quasi-amorphous

266 ermolecular quintet at room temperature as a polycrystalline solid is studied.

267 e, orientation, and defects of inhomogeneous polycrystalline solids by raster scanning them under a m

268 Much like energy transport in polycrystalline solids, hydraulic transport in semi-orde

269 anic materials that exhibit this behavior as polycrystalline solids.

270 The protocol is applied to polycrystalline specimens of two different dipeptide nan

271 it from high-density "random-close packing" polycrystalline states and hence provides a stringent te

272 uctor thin films exist in semicrystalline or polycrystalline states, incorporating a high degree of l

273 The activity trend found on the polycrystalline surfaces was in good agreement with the

274 y for industrial applications, are typically polycrystalline - that is, composed of single-crystallin

275 it is essential to develop high-performance polycrystalline thermoelectric materials.

276 ological evolution of a chemically deposited polycrystalline thin film.

277 sample temperature and excitation fluence on polycrystalline thin films composed of two polymorphs.

278 Singlet fission (SF) in polycrystalline thin films of four 3,6-bis(thiophen-2-yl

279 ctly probe the process of exciton fission in polycrystalline thin films of pentacene.

280 roscopic approaches, Wenger et al. show that polycrystalline thin films possess similar optoelectroni

281 ld an efficiency enhancement 44-fold that of polycrystalline thin films, due to the much longer carri

282 erovskite photodetectors are mainly based on polycrystalline thin films, which have some undesired pr

283 rap densities in the single crystals than in polycrystalline thin films.

284 of TSCs are 10-100 folds lower than that of polycrystalline thin films.

285 ely studied in two forms: single-crystals or polycrystalline thin films.

286 le crystals are almost identical to those of polycrystalline thin films.

287 he manufacturing process involves doping the polycrystalline thin-film CdTe with CdCl2.

288 Large-aspect-ratio grains are needed in polycrystalline thin-film solar cells for reduced charge

289 820 nm, 20 nm broader than the corresponding polycrystalline thin-film solar cells.

290 , with average value similar to results from polycrystalline thin-film studies.

291 best-performing, extrinsically doped p-type polycrystalline tin selenides.

292 terahertz spectroscopy, that low mobility in polycrystalline TiO(2) nanotubes is not due to scatterin

293 red to sintered nanoparticle films, oriented polycrystalline titania nanotubes offer the advantage of

294 ells over the ZnO NRs gradually changed from polycrystalline to single crystalline.

295 Lastly, defect structures in monolayer polycrystalline transition metal dichalcogenides grown b

296 y contributes to the possible application of polycrystalline W under irradiation in advanced nuclear

297 graphene films produced so far are typically polycrystalline, with point and line defects that can st

298 the sacrificial template and then a layer of polycrystalline ZIF-8.

299 Headed for a membrane: Continuous, polycrystalline ZIF-90 membranes (picture, left) can be

300 We demonstrate that UV-light activation of polycrystalline ZnO films on flexible polyimide (Kapton)