ライフサイエンスコーパス: flake

1 ements of frictional domains within a single flake.

2 he stability of a representative phosphorene flake.

3 ized and graphitic domains across the entire flake.

4 birch tar, encompassing one-third of a flint flake.

5 cond-harmonic generation maps of the PdSe(2) flakes.

6 films containing highly aligned large MXene flakes.

7 e interactions between the substrates in the flakes.

8 (2D) capillaries made from large (10-20 mum) flakes.

9 ns when graphene monolayers are grown on hBN flakes.

10 e as nanoscale-confined volume modes in thin flakes.

11 flakes is similar to that of tape-exfoliated flakes.

12 -optimal responsivity for a wide range of 2D flakes.

13 ssion peak around 0.75 eV in exfoliated MoS2 flakes.

14 eding on both types of pellets compared with flakes.

15 lupin protein isolates compared to the lupin flakes.

16 Pellets, and one flaked diet, Tetramin Fish-Flakes.

17 er graphene sandwiched between boron nitride flakes.

18 ally settle to form dome-shaped nanographene flakes.

19 are obtained on the underlying chalcogenide flakes.

20 yrolysis of polysilazane functionalized MoS2 flakes.

21 nd spelt were compared with commercial wheat flakes.

22 uring the spectral measurements in thin GaSe flakes.

23 ercial flakes and muesli produced from these flakes.

24 ditions starting from aqueous graphene oxide flakes.

25 knots, with 'frozen' orientational order of flakes.

26 as a surface charge transfer donor for MoS2 flakes.

27 ic nanostructures, such as circular graphene flakes.

28 a-glucan) and viscosities of oat kernels and flakes.

29 ting temperatures in kernels, thin and thick flakes.

30 opy investigations in thin (8-35 nm) CrCl(3) flakes.

31 ply decrease the size of as-exfoliated FL-BP flakes.

32 chemically unstable delaminated single-layer flakes.

33 n and bending of the interconnected graphene flakes.

34 tive requirements for the emergence of stone flaking.

35 PL signals for 32 out of 35 many-layer MoS2 flakes (2-15 layers) tested, indicating that this method

36 2/HT-2 concentrations were determined in oat flakes (89.4mug/kg) and calf feed (129.3mug/kg).

37 to manipulate the magnetization in such thin flakes, a combination of an in-plane magnetic field and

38 We examined these flakes according to nine measures of morphology.

39 ry cell made using pristine natural graphite flakes achieves a specific capacity of approximately 110

40 graphitic domains were observed for the same flake after a step-by-step chemical reduction process us

41 of an extended fiber assembly into discrete flakes after incorporation of Pt-DA.

42 of the small flake size and relatively poor flake alignment that occurs during solution-based proces

43 Large-area flakes allow manufacturing of large-area mono-layer tran

44 A plasma-induced p-type MoS2 flake and n-type ZnO film diode, which exhibits an excel

45 Both single crystalline individual flakes and continuous films of 1 L MoS2 were successfull

46 current, conchoidally fractured, sharp-edged flakes and cores that have the characteristics and morph

47 revent the usual restacking of the Ti(3)C(2) flakes and create fast ion transport pathways.

48 However, the total content was increased in flakes and extruded products made only from brown teff g

49 range of foodstuffs, especially gluten-free flakes and extruded products.

50 treatments (industrial milling, formation of flakes and extrusion) on the phenolic composition of two

51 by nanocarbon fillers consisting of graphene flakes and fullerenes.

52 ncrease, thus filling in voids among the hBN flakes and highly densifying the hBN bulks.

53 The AC of rapeseed, white flakes and meal varied from 10.0 to 86.7mumolsinapicacid

54 nt capacity (AC) of Brassica oilseeds, white flakes and meal was determined by a new spectrophotometr

55 Flakes and muesli made from Dickkopf wheat and red wheat

56 idant activity were determined in commercial flakes and muesli produced from these flakes.

57 Wheat flakes and muesli were assessed for basic analyses (dry

58 beam epitaxy (MBE) of graphene layers on hBN flakes and on sapphire wafers at substrate growth temper

59 ucture, while the starch with lime exhibited flakes and porous network.

60 the vacancies in the hydrophilic exfoliated flakes and subsequently bonding with water, not possible

61 cavitation preferentially exfoliates larger flakes and that the graphene exfoliation rate and flake

62 tion processes, depending on the size of the flakes and the elastic properties of the dispersant flui

63 causes for the long-range cross-talk between flakes and the formation of a single-grain graphene laye

64 res, and electrical properties of 2D PtSe(2) flakes and thus alters their catalytic performance for H

65 The industrial processes, mainly flaking and extrusion, caused marked changes in the phen

66 s located in the internal part of the hybrid flakes, and more precisely at the BN/graphene intersecti

67 ixed human epithelial cells, corneocyte skin flakes, and polymers used for bioimplants.

68 largely limited to exfoliated and restacked flakes, and the controlled growth of such heterostructur

69 e tailored from compact triangles to fractal flakes, and the pattern formation can be explained by th

70 d meat, other cereals [e.g., corn or frosted flakes], and full cream milk), increased temperature of

71 Charge carriers of MoTe2 flakes annealed via RTA at various vacuum levels are tun

72 Thus, with flakes approaching typical experimental sizes (~0.1-1 mu

73 Flakes are an assortment of grain products mainly consum

74 These flakes are characterized by superconducting quantum inte

75 2D Ti(3) C(2) T(x) flakes are ideal candidates for making conductive films

76 As the monolayer flakes are isolated at predetermined locations, transist

77 MoS2 flakes are predominantly monolayers with high material q

78 2D Nb2CTx MXene flakes are produced using an amine-assisted delamination

79 Here, single-crystalline MoS2 flakes are reported with regular trigonal symmetric patt

80 t time (up to 500 s), (ii) only small sample flakes are required for the measurements, which are anal

81 The 2D flakes are stable in a nitrogen atmosphere or in select

82 ve metal-oxide nanoparticle-decorated carbon flakes are synthesized via a facile biotemplating method

83 Atomically thin quasi-2D GaSe flakes are synthesized via van der Waals (vdW) epitaxy o

84 y of this process, the resulting phosphorene flakes are thinner than anhydrous organic solvent disper

85 The flakes are transferred from their growth substrate using

86 ocessing, the aqueous-exfoliated phosphorene flakes are used in field-effect transistors with high dr

87 ucture in which the nanometer-thick graphite flakes are wrapped by negatively charged nanofibrillated

88 le-walled carbon nanotubes (SWCNT), graphene flakes, biological particles, SERS-active metal nanopart

89 modified bones, European Lower Palaeolithic flaked bone tools, along with Middle and Late Pleistocen

90 TAEA expands the interlayer spacing of MXene flakes by only ~ 1 angstrom and reinforces the interconn

91 The restacking and densification of these flakes by SPS promoted the formation of charged grain bo

92 of many-layer, mechanically exfoliated MoS2 flakes by up to 20 times, without reducing the layer thi

93 In this study, we propose to evaluate the flaking by automatically analyzing hyperspectral images

94 The interactions between flakes can be also controlled by varying the oil-to-wate

95 In addition, it is predicted that graphene flakes can be efficiently used as a new-generation stabi

96 Here we report that vanadium disulfide flakes can be rendered stable in the electrochemical env

97 that the insulating alpha-phase of Sb(2)O(3) flakes can be transformed into semiconducting beta-phase

98 Owing to a large diamagnetism, graphene flakes can respond and be aligned to magnetic field like

99 t PMMA passivated black phosphorus thin film flakes can stay pristine for a period of 19 days when le

100 e femtosecond carrier dynamics in individual flakes can thus give much insight into light-matter inte

101 nts performed in a solution of graphene nano-flakes clearly highlight this remarkable transition.

102 ed on flexible substrate using graphene nano-flakes conductive ink through stencil printing method.

103 TEM analyses of GO flakes confirm the size decrease of ordered sp(2) domain

104 tion suggests that most of the alpha-Mo(2) C flakes contain multiple domains and the c-axes of neighb

105 ials from metals (e.g., Au nanoparticles, Ag flakes, Cu nanowires), carbon nanotubes/nanofibers, 2D c

106 nding the duplicate entries in the published flake dataset.

107 mistakenly included duplicate entries in the flake datasets for the new Pech de l'Aze IV and Warwasi

108 now repeated this analysis with the correct flake datasets.

109 ne tools, such as handaxes, by tools made on flakes detached from Levallois cores documents the most

110 emonstrated the possibility of label-free 2D flake detection via selective enhancement of the Stokes

111 l Pellets and Nishikoi Fish Pellets, and one flaked diet, Tetramin Fish-Flakes.

112 s and that the graphene exfoliation rate and flake dimensions are strongly correlated with, and there

113 The GaTe flakes display multiple sharp photoluminescence emission

114 rent density than mechanically exfoliated ML flakes due to the reduced contact resistance which mainl

115 ire surface of the individual graphene oxide flake during the chemical reduction process.

116 ct unexpected condensation of large graphene flakes during high-temperature oxidation of nSiC.

117 ch stem from nonuniform deposition of 2-D NM flakes during layer build-up, has been almost entirely o

118 aman spectroscopy monitoring of 2D dispersed flakes during the device operation.

119 MD stacking sequence, chalcogen/metal ratio, flake edge diffusion and vacancy diffusion.

120 , surface-confined modes can be found at the flake edges.

121 ture-dependence of resistance) through inter-flake effects.

122 ntally characterized a printed graphene nano-flakes enabled flexible and conformable wideband radar a

123 The flexibility of the printed graphene nano-flakes enables the absorber conformably bending and atta

124 detect them from multivitamin tablets, corn flakes, energy drinks, cerebrospinal fluid (CSF) and blo

125 nd biological functionalization of 2D MoS(2) flakes, epitaxially grown on sapphire, to develop an opt

126 d to confirm the number of quintuples in all flakes examined in this study.

127 e report spin potentiometric measurements in flakes exfoliated from bulk insulating Bi2Te2Se crystals

128 Aligned graphene flakes exhibit emergent properties approaching single-la

129 In addition, the 2D flakes exhibit metallic character and an optical respons

130 These CVD-grown ML MoS2 flakes exhibit much higher mobility and current density

131 nd sintered at 1400 degrees C, the resulting flakes exhibited an optimal combination of hardness (534

132 The mixtures containing GO flakes exhibited varying dielectric relaxation processes

133 noparticles decorated reduced graphene oxide flakes, exhibits a LOD of 0.088 mg L(-1).

134 Fully nanodimensional GO flakes floating in nitrogen gas were incorporated with A

135 r soft matters and a hexagonal boron nitride flake for two-dimensional materials.

136 ant effect on major morphological aspects of flake form.

137 The graphene flakes form a percolating network to render the resultan

138 om 19,000 to 18,000: "Using more than 18,000 flakes from 81 assemblages spanning two million years...

139 ically tested these hypotheses by generating flakes from cores exposed to three different temperature

140 Twenty commercial flakes from different raw materials were included in thi

141 rt here the results in exfoliated ZrTe5 thin flakes from the studies of aberration-corrected scanning

142 nsional (1D) nanowires (NWs) and 2D graphene flakes grown out-of-plane for highly controlled photothe

143 etworks made of large reduced graphene oxide flakes (>20 mum) are superelastic and exhibit high energ

144 n the following two sentences, the number of flakes has been changed from 19,000 to 18,000: "Using mo

145 but to date, growth of isolated crystalline flakes has been demonstrated at random locations only.

146 We discovered that wheat bran flakes have a 'rough' and 'smooth' surface with substant

147 ReS2 is prepared in the form of flakes having thicknesses of 60-450 nm by micromechanica

148 The thinner the flakes, hysteresis and remanence in the magnetization lo

149 d multiple internal reflections from Ti3C2Tx flakes in free-standing films.

150 ing the HER catalytic activity of individual flakes in micro electrochemical cells, we investigated t

151 Orientational ordering of graphene oxide flakes in self-assembled liquid-crystalline phases enabl

152 frequencies decreased as the size of the GO flakes in the isotropic solvent was increased.

153 .on more that 18,000 complete and unmodified flakes." In addition, in Figs.

154 ce of the reflectance of exfoliated graphene flakes, including monolayer, bilayer and trilayer graphe

155 In contrast, two-dimensional graphene flakes induce a strongly size-dependent response: we fin

156 age capability, here, processing of 2D MXene flakes into hollow spheres and 3D architectures via a te

157 The oxidized flake is then submerged into water for selective oxide r

158 true amphipathic nature of pristine graphene flakes is demonstrated through wet-chemistry testing, op

159 in solutions to obtain high-quality graphene flakes is desirable for printable electronics, catalysis

160 erties of hybrid boron nitride (BN) graphene flakes is opened up.

161 cess for transition metal dichalcogenide WS2 flakes is reported and the effect of the underlying subs

162 ) from the mechanically exfoliated thin GeAs flakes is reported.

163 show that the quality of the gold-exfoliated flakes is similar to that of tape-exfoliated flakes.

164 uction of archaeologically visible cores and flakes is therefore no longer unique to the human lineag

165 ng to thin down thick-exfoliated phosphorene flakes, layer by layer with atomic precision.

166 occur frequently in nature as flowers, snow-flakes, leaves and so on.

167 rmined to be 86.25~131.2 Wm(-1) K(-1) with a flake length of 5~100 mum.

168 i and thereby modifying the eutectic Si from flake-like to fibrous is a key factor in improving the p

169 mechanical properties than those with small flakes (<2 mum).

170 The flakes made from non-traditional wheat were sensorially

171 A second is that it also alters flake morphological properties.

172 aphene nanoplatelets, molybdenum(IV) sulfide flakes, neodymium(III) oxide nanoparticles, two sizes of

173 Here, graphene flakes, nucleated over a polycrystalline graphene film,

174 ermal in-plane anisotropy of a flexible thin flake of black-phosphorus (BP), we devise plasma-wave, t

175 quency nanodetector exploiting a 10 nm thick flake of exfoliated crystalline black phosphorus as an a

176 flectance spectra acquired on a single thick flake of this material.

177 covered that the degradation of few-layer BP flakes of <10 nm can be suppressed for months by using i

178 ar-field optical microscopy (s-SNOM) on thin flakes of alpha-MoO(3) , with analytical and transfer-ma

179 ormed ultrafast optical microscopy on single flakes of atomically thin CVD-grown molybdenum disulfide

180 on mechanism in a transistor channel made of flakes of black-phosphorus or InAs nanowires.

181 Graphene oxide (GO) flakes of different sizes were prepared and dispersed in

182 rtant is the recent capability to grow large flakes of few-layered structures using chemical vapor de

183 iety of substrates, as well as on exfoliated flakes of hexagonal boron nitride.

184 seeds of molybdenum source material to grow flakes of MoS2 at predetermined locations with micrometr

185 tematic micro-Raman study of two-dimensional flakes of n-type Bi2Te2.7Se0.3 produced by the C/ME proc

186 n non-contact AFM imaging reveal rectangular flakes of nanographene featuring parallel pairs of zig-z

187 r of layers showed that more than 90% of the flakes of T-GR had less than two layers and about 84% of

188 Such rotation is macroscopic (for graphene flakes of tens of micrometres the tangential movement ca

189 r Waals interface between freshly exfoliated flakes of the high-T c superconductor, Bi-2212, and the

190 a uniaxial tensile strain is applied to thin flakes of the vdW magnet Fe(3) GeTe(2) (FGT), and a dram

191 haviors (hardness, roughness and density) of flakes of the ZrO2 nanoparticles.

192 hifts of the 2D Raman phonons of rectangular flakes of various sizes under load, the critical strain

193 g and blistering of TD MPs and shredding and flaking of LS MPs.

194 eloped to effectively evaluate the degree of flaking of the murals.

195 Hulling and flaking of the seeds resulted in a 15% increase of LOX a

196 n and steaming; FSF: fermentation, steaming, flaking) of whole grain sorghum on the proximate composi

197 rowth, the stability of nanoscale cluster or flake on a substrate is crucial.

198 By suspending WSe2 flakes onto sub-20-nm-wide trenches in gold substrate, w

199 eaction, large mono/bilayer (1.1 mm/200 mum) flakes or full-coverage films (with a record-high averag

200 le micrometer-scale objects such as graphene flakes or living cells, and besides for achieving intens

201 The NR-treated po-Gr flakes (po-Gr-NR) were characterized by UV-vis, FT-IR, a

202 nation of FB1 in corn meal, corn flour, corn flakes, polenta, canned corn and popcorn collected from

203 sed graphene oxide flakes, pristine graphene flakes possess well-defined hydrophobic and hydrophilic

204 nitride particles incorporated into the hBN flake powders transform into BN onions with a significan

205 In contrast to commonly used graphene oxide flakes, pristine graphene flakes possess well-defined hy

206 Graphene flake production capability has reached thousands of ton

207 t treatment does reduce the force needed for flake propagation, they also demonstrate that such treat

208 hat it merely reduces the force required for flake propagation.

209 he effect of the underlying substrate on the flake properties is investigated using Raman spectroscop

210 MXene films with aligned flakes provide an effective route for producing large-ar

211 ent in stiffness, which scales linearly with flake radius.

212 al colloidal properties of pristine graphene flakes remain incompletely understood, with conflicting

213 rkup was adapted to lupin seeds, kernels and flakes, respectively.

214 py and elemental analysis reveal that the 2D flakes retain the crystal structure and stoichiometry of

215 effects of production methods for red pepper flakes (RPF) and traditional (TRI) and industrial (INI)

216 ds and volatile compounds (VC) of red pepper flakes (RPF), traditional (TRI), and industrial (INI) is

217 nstrate an excess of sulfur vacancies at the flake's edges by means of cathodoluminescence mapping, a

218 oduces a series of phase transitions in thin-flake samples with reduced dimensionality.

219 on, and cyclic compression and release of BP flakes show an intrinsic current output as large as 4 pA

220 The measurement of few-layer graphene flakes shows the variation of work function between grap

221 to macroscale films as a result of the small flake size and relatively poor flake alignment that occu

222 several GO fractions differing in an average flake size and zeta-potential were prepared using centri

223 irst failure were found to be independent of flake size at a mean value of -0.60% corresponding to a

224 at the cost of limited exfoliation yield and flake size distribution.

225 oliation rates, low material yields and wide flake size distributions, making the graphene dispersion

226 action that appears to be independent of the flake size when the thickness is tens of nanometers.

227 , a thin nanosheet architecture, and a small flake size, which endow it with superior efficiency in l

228 nal semiconductors continue to be limited by flake size.

229 As a result, at lower flake sizes GO rapidly internalizes into HeLa cells with

230 ures such as contrast, color, edges, shapes, flake sizes, and their distributions, based on which an

231 The manufacture of flaked stone artifacts represents a major milestone in t

232 etween behavioral adaptations-in the form of flaked stone artifacts-and the biological evolution of o

233 e a substantial assemblage of systematically flaked stone tools excavated in situ from a stratigraphi

234 A single monolayer flake strained by 0.53% generates a peak output of 15 mV

235 Sharp-edged stone flakes, struck from larger cores, are the primary eviden

236 However, because of its flake structure and general inertness, it is currently i

237 Tungsten (W) based non-periodic chalcogenide flakes (sulfides and selenides) were considered.

238 trodes fabricated using assembled V(2) CT(x) flakes surpasses Ti(3) C(2) T(x) in various aqueous elec

239 of ab-initio calculations, that layered InSe flakes sustain luminescent excitons with an intrinsic ou

240 d in the right section of the right graphene flake, systems of giant quadratic NLO octupolar and/or d

241 ly depend on the engineering of the graphene flake that controls the property of the cell walls.

242 from electric field to electrically neutral flakes that are suspended in a higher electrical conduct

243 in single-crystal molybdenum oxide (MoO(2) ) flakes that exhibit unexpected piezoelectric-like respon

244 microscopy and Raman spectra reveal that the flake thickness actually increases as a result of the pl

245 Furthermore, the effect of the flake thickness on the THG conversion efficiency is show

246 ed by the C/ME process, as a function of the flake thickness.

247 r the synthesis of boron-containing graphene flakes through reductive B-B coupling.

248 far- and near-field properties for multiple flakes, thus providing strong verification of the accura

249 simply capping the edges of individual MXene flakes, Ti(3) C(2) T(z) and V(2) CT(z) , by polyanions s

250 care was taken for the examined area of the flake to be free of residual stresses.

251 a wet etch to allow the user to transfer the flakes to a final substrate using a microscope and micro

252 y and Raman spectroscopy show the exfoliated flakes to be unoxidized and free of basal-plane defects.

253 ctively, the interplay of which allows small flakes to be utilized as stabilizers with an amphipathic

254 those outstanding properties of single MXene flakes to macroscale films as a result of the small flak

255 firm the material quality of the transferred flakes to the substrates and subsequently to analyze and

256 nthesized at 500 degrees C were pressed into flakes under 6 MPa and sintered at 1400 degrees C, the r

257 nanodimensional gold-graphene oxide (Au@GO) flakes under visible light and the potential of the resu

258 d mica and highly ordered pyrolytic graphite flakes used as reference substrates.

259 he transistors fabricated on the same WSe(2) flake using conventional deposited Au contacts with pron

260 and n-type FETs on the same intrinsic MoS(2) flake using Pd and low-work-function molybdenum (Mo) con

261 pic nematic liquid crystal of graphene oxide flakes using a pulsed near-infrared laser.

262 of this physical phenomenon, studied on MoS2 flakes using ex-situ AFM imaging, Raman mapping, and pho

263 determination of cadmium and iron in cereal flakes using high-resolution continuum source graphite f

264 enic molecules, which are anchored to the GO flakes via dispersion interactions.

265 availability from the gluten and gluten-free flakes was evaluated and compared.

266 To predict the degree of flaking, we adopted four algorithms: deep belief network

267 he experimental results showed that the ZrO2 flakes were comparable to human bones with a higher dens

268 Monolayer SCG flakes were derived from low pressure chemical vapor dep

269 Exfoliated monolayer graphene flakes were embedded in a polymer matrix and loaded unde

270 The MoS(2) flakes were modified with a thiolated DNA probe compleme

271 magnitude is altered by heat treatment, the flakes were not.

272 hird-harmonic generation from few-layer GaSe flakes were observed.

273 of muesli composed of non-traditional wheat flakes were prepared and analysed.

274 Murals with various degrees of flaking were scanned in the 126th cave using a near-infr

275 were determined in different kinds of cereal flakes, where both elements are of great interest.

276 so far are based on polycrystalline graphene flakes which are anchored on supporting substrates.

277 to preferentially exfoliate larger graphene flakes which causes the exfoliation rate to decrease as

278 e edges before appearing in the bulk of MoS2 flakes, which can be explained by our first-principles c

279 ate lateral homo-junctions in few layer WSe2 flakes, which constitutes an important advance towards t

280 of precursor to render large single-crystal flakes, which usually causes low coverage of the materia

281 esulting from the relaxation modes of the GO flakes while the fast relaxation frequencies (~100 kHz)

282 uent encapsulation of the ion exposed MoS(2) flake with high-quality hBN reveals spectrally narrow em

283 inction and fluorescence taken from the same flake with the cavity.

284 SFBRCN, containing a 3D spirobifluorene core flaked with a 2,1,3-benzothiadiazole (BT) and end-capped

285 Polarizing microscopy showed that GO flakes with a mean diameter of 10 mum, dispersed in wate

286 In graphene flakes with both stacking configurations, the region bet

287 nthesis of high-quality multilayer (ML) MoS2 flakes with gradually shrinking basal planes by chemical

288 Roasting resulted in oat flakes with improved sensory properties.

289 Here we study twisted multilayer graphene flakes with multi-wavelength Raman spectroscopy.

290 rongly size-dependent response: we find that flakes with radii in the 2-4 nm range provide appreciabl

291 olygonal and plate-like to a mixture of fine flakes with round corners, feathery and fibrous, or a co

292 wed indicating amaranth and teff products as flakes with the highest impact on the realization of dai

293 gnetism of micromechanically cleaved CrCl(3) flakes with thickness >10 nm is performed.

294 ent atomically thin rhenium disulfide (ReS2) flakes with unique distorted 1T structure, which exhibit

295 at incorporating fully nanodimensional Au@GO flakes with ZC is a suitable technique for ambient photo

296 We found Raman evidence for flakes with: (i) integer number of quintuples which exhi

297 from Mott-insulator to metal in 1T-TaS2 thin flakes, with five orders of magnitude modulation in resi

298 products are composed of multi-layers of C/S flakes, with predominantly amorphous and some graphene-l

299 ignal sensitivity to the xyz alignment of 2D flakes within the optofluidic waveguide.

300 the growth of GaN on mechanically-exfoliated flakes WS2 and MoS2 by metalorganic vapour phase epitaxy