ライフサイエンスコーパス: flake

1 he stability of a representative phosphorene flake.

2 ized and graphitic domains across the entire flake.

3 ements of frictional domains within a single flake.

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

5 er graphene sandwiched between boron nitride flakes.

6 ally settle to form dome-shaped nanographene flakes.

7 are obtained on the underlying chalcogenide flakes.

8 yrolysis of polysilazane functionalized MoS2 flakes.

9 nd spelt were compared with commercial wheat flakes.

10 uring the spectral measurements in thin GaSe flakes.

11 ercial flakes and muesli produced from these flakes.

12 ditions starting from aqueous graphene oxide flakes.

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

14 as a surface charge transfer donor for MoS2 flakes.

15 ic nanostructures, such as circular graphene flakes.

16 uring methods and the production of tools on flakes.

17 e interactions between the substrates in the flakes.

18 (2D) capillaries made from large (10-20 mum) flakes.

19 ns when graphene monolayers are grown on hBN flakes.

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

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

22 ssion peak around 0.75 eV in exfoliated MoS2 flakes.

23 eding on both types of pellets compared with flakes.

24 lupin protein isolates compared to the lupin flakes.

25 tive requirements for the emergence of stone flaking.

26 Oat (1.39 g/serving) and barley flakes (1.30 g/serving) can be recommended as the best s

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

28 2/HT-2 concentrations were determined in oat flakes (89.4mug/kg) and calf feed (129.3mug/kg).

29 erythema (27%), scabbing or crusting (21%), flaking (9%), erosion (6%), edema (4%), and weeping (3%)

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

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

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

33 We found the aluminium flakes align within 15 degrees of the coating surface in

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

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

36 ctionalized graphenes starting from graphite flakes and a reactive monomer, styrene.

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

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

39 by nanocarbon fillers consisting of graphene flakes and fullerenes.

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

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

42 Flakes and muesli made from Dickkopf wheat and red wheat

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

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

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

46 m more stable C-H bonds, separating graphene flakes and promoting the binding with the matrix materia

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

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

49 genomic sequences revealed highly divergent flaking and intron sequences, whereas they encoded nearl

50 es were characterized by visible presence of flaking and thickened skin, loss of the granular cell la

51 rs for the Maillard reaction at the cooking, flaking and toasting stages of cornflake production proc

52 s include a hearth, lithic cutting tools and flakes, and abundant processed marine fauna, primarily s

53 the most significant fibre fractions in rye flakes, and beta-glucan in oat flakes, cellulose and res

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

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

56 been observed on single crystals, nanowires, flakes, and powders.

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

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

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

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

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

62 MoS2 flakes are predominantly monolayers with high material q

63 2D Nb2CTx MXene flakes are produced using an amine-assisted delamination

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

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

66 Moreover, the electronic properties of the flakes are superior to those achieved with other solutio

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

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

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

70 The flakes are transferred from their growth substrate using

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

72 tradition, characterized by a large (>10 cm) flake-based component, represents a significant technolo

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

74 bifaces/unifaces made predominantly on large flake blanks.

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

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

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

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

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

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

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

82 ctions in rye flakes, and beta-glucan in oat flakes, cellulose and resistant starch were present in s

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

84 ard a nanoscale realization of the selective flake concept first proposed by Cussler.

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

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

87 rostructure composed of a monolayer graphene flake coupled to a rotationally aligned hexagonal boron

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

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

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

91 The soy flour and full-fat soy flake diets contained 0.049% genistein derivatives (prim

92 The GaTe flakes display multiple sharp photoluminescence emission

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

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

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

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

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

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

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

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

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

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

103 Aligned graphene flakes exhibit emergent properties approaching single-la

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

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

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

107 The mixtures containing GO flakes exhibited varying dielectric relaxation processes

108 flake (flk), an N-ethyl-N-nitrosourea-induced recessive

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

110 ar cataract, vacuoles, waterclefts, coronary flakes, focal dots, retrodots, fiber folds), with refrac

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

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

113 Fibers extruded from large flake graphene oxide dope without drawing show unconvent

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

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

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

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

118 flake homozygotes show reduced sebum production and are

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

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

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

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

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

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

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

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

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

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

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

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

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

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

133 del limit, which describes ideal behavior of flake-like fillers uniformly imbedded in a polymer.

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

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

136 The flakes made from non-traditional wheat were sensorially

137 , yielded a stratified assemblage with small flakes, microblades, and retouched crescentic and trapez

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

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

140 s, nonuniform conductivity patterns across a flake of graphene, one can have this material as a one-a

141 s" with different conductivities on a single flake of graphene.

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

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

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

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

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

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

148 ning prospect: piles of information but only flakes of knowledge.

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

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

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

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

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

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

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

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

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

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

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

160 al characteristics of psoriasis is excessive flaking of the skin.

161 rther degrade the tissue, causing sloughing (flaking) of lesional epidermis, but rapid wound healing

162 In Mode 3A, keratinocytes cornified and flaked off to free skin appendages (feather sheath, pulp

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

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

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

166 buffer but may also be due to the additional flaking peptide bonds of the pentapeptides.

167 . aureus-infected mice partially rescues the flake phenotype, which indicates that an additional comp

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

169 ts and a stone tool assemblage of bifacially flaked points, simple flake tools, and numerous handston

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

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

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

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

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

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

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

177 An increase in the number of flake scars was observed within the Konso Formation hand

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

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

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

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

182 nal semiconductors continue to be limited by flake size.

183 promise the properties of graphene or reduce flake size.

184 orest of Cote d'Ivoire produce unintentional flaked stone assemblages at nut-cracking sites, leaving

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

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

187 0-250 nm, composed of ~50-nm aluminosilicate flakes studded with Fe and Ti-rich clusters (<10 nm) tha

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

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

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

191 For rye flakes, the pattern of these benzoxazinoids was differen

192 After flaking, the samples appeared lighter, while the pigment

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

194 ndirect band gap semiconductor when the InSe flake thickness is reduced to a few nanometers.

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

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

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

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

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

200 the mechanochemical exfoliation of graphite flakes to single-layer and few-layer graphene sheets com

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

202 semblage of bifacially flaked points, simple flake tools, and numerous handstones and milling stone b

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

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

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

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

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

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

209 c-Out-of-plane oriented MCM-22 flakes were chosen because of the expected H(2)-selectiv

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

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

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

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

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

215 For log breaking, small flakes were rotated drill-like or used as scrapers, wher

216 or used as scrapers, whereas thick cortical flakes were used as axes or wedges, leaving consistent w

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

218 iscarded, such as flour from oat cutting and flaking, were 1.5- to 2.5-fold higher than in native gra

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

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

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

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

223 h substituted for sucrose), 98 [full-fat soy flakes (whole soybeans)], 87 (defatted soy flour), 77 (0

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

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

226 t outputs, whereas no output is observed for flakes with an even number of layers.

227 cyclic stretching and releasing of thin MoS2 flakes with an odd number of atomic layers produces osci

228 s only mild sonication, it produces graphene flakes with areas as large as 50 microm(2).

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

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

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

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

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

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

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

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

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

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

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