ライフサイエンスコーパス: graphene sheet

1 arbon black particles, carbon nanotubes, and graphene sheets).

2 extending up to 30 A from both sides of the graphene sheet.

3 amical screening of charge in a freestanding graphene sheet.

4 confined space between a metal surface and a graphene sheet.

5 ng wire has been embedded in another perfect graphene sheet.

6 ybridized carbon rings embedded in a perfect graphene sheet.

7 , experimental phonon dispersion of a single graphene sheet.

8 ed by nitrogen atoms embedded in an extended graphene sheet.

9 via the resistance of an adjacently stacked graphene sheet.

10 ol the crumpling and unfolding of large-area graphene sheets.

11 shrinkage of giant fullerenes generated from graphene sheets.

12 l % of the solute is present as single-layer graphene sheets.

13 films corroborated the presence of monolayer graphene sheets.

14 nsional capillaries formed by closely spaced graphene sheets.

15 eties sufficient to enable the separation of graphene sheets.

16 ded graphite basal planes to give functional graphene sheets.

17 nd directly produce large, highly conductive graphene sheets.

18 3 J m(-2) for samples containing two to five graphene sheets.

19 rticles and nanowires, carbon nanotubes, and graphene sheets.

20 not ideal for the manufacture of processable graphene sheets.

21 the thermodynamic stability of free-standing graphene sheets.

22 ortions and flexible bending at the edges of graphene sheets.

23 es not readily exfoliate to yield individual graphene sheets.

24 magnified by their structure, intercalating graphene sheets.

25 via AFs complexation and a huge porosity of graphene sheets.

26 n nanotubes (MWCNTs) positioned over stacked graphene sheets.

27 , or Al) nanoparticles encapsulated by large graphene sheets.

28 ied with twist angle in bilayer and trilayer graphene sheets.

29 iform and open-networked array of aggregated graphene sheets.

30 place on the surface of exfoliated few-layer graphene sheets.

31 rier by "locking in" favourable stackings of graphene sheets.

32 high-mobility semiconductor quantum wells or graphene sheets.

33 ut to study the morphology of functionalized graphene sheets.

34 ensions of crystalline single- and few-layer graphene sheets.

35 spaces through folding and rearrangement of graphene sheets.

36 ovide evidence for the presence of monolayer graphene sheets.

37 lvated in a water monolayer confined between graphene sheets.

38 ng adsorption saturation of NaC molecules on graphene sheets.

39 i nanoparticles due to the highly conductive graphene sheets.

40 ween the guest molecules and the polarizable graphene sheets.

41 n, reduction or covalent modification of the graphene sheets.

42 hment of monodisperse Fe3O4 nanoparticles to graphene sheets.

43 e the nature of catalytic sites on ultrathin graphene sheets.

44 TEMPO-assisted exfoliation results in large graphene sheets (5-10 mum on average), which exhibit out

45 Hall insulator, inherently protected by the graphene sheet above and the H-passivated substrate belo

46 rammable photoactuation enabled by graphene: Graphene sheets aligned in liquid crystalline elastomers

47 , we report graphene structures with tunable graphene sheet alignment and orientation, obtained via m

48 lline Ni(OH)(2) nanoplates directly grown on graphene sheets also significantly outperform small Ni(O

49 croscopy imaging of water locked between two graphene sheets, an archetypal example of hydrophobic co

50 n of a nanohybrid by a combination of the 2D graphene sheet and 0D graphene quantum dots (GQDs).

51 e semiconducting channel between a monolayer graphene sheet and a metal thin film.

52 When the particles were sandwiched between a graphene sheet and a proton exchange membrane that is we

53 self-assembly over planar sp(2) carbons of a graphene sheet and furnishes the basis for fabrication o

54 nd AD molecules reduces the voids within the graphene sheet and improves the alignment of graphene pl

55 ond to correlations between electrons in the graphene sheet and ions in the electrolyte.

56 etween the strain energy of curvature of the graphene sheet and the dangling-bond energy of the open

57 from changes in commensurability between the graphene sheet and the substrate when the sheet deforms

58 Ripples are an intrinsic feature of graphene sheets and are expected to strongly influence e

59 ing the preparation and functionalization of graphene sheets and carbon nanotubes to impart oxygen co

60 posing surface morphologies originating from graphene sheets and COF nanofibers or nanospheres, prese

61 ve development of large-scale semiconducting graphene sheets and devices.

62 re effective reduction of chemically derived graphene sheets and graphite oxide than low-temperature

63 Carbon nanotube films, graphene sheets and metal-nanowire meshes can be both st

64 atures below 0 degrees C, due to its aligned graphene sheets and pores.

65 The findings on exfoliation of graphene sheets and related adsorption properties highli

66 of the dual signal amplification strategy of graphene sheets and the multienzyme labeling, the develo

67 formed by depositing alternating wafer-scale graphene sheets and thin insulating layers, then pattern

68 illared graphene (PG) membranes, composed of graphene sheets and vertically aligned carbon nanotubes

69 nar units (unbounded or bounded fragments of graphene sheets), and variable ratios of in-plane to edg

70 poly(acrylonitrile) at 1 wt% functionalized graphene sheet, and with only 0.05 wt% functionalized gr

71 Large fullerenes, fullertubes, graphene sheets, and double- and multiwalled CNTs togeth

72 e recently developed approaches to preparing graphene sheets, and then focus on the methods to assemb

73 erties arising from the nature of individual graphene sheets, and which assemble into monolithic thre

74 Monolayer graphene sheets are employed to preserve and template mo

75 The large voids in the graphene sheets are occupied by chloride ions with an eq

76 The graphene sheets are self-assembled and deeply crumpled i

77 Nanographenes, finite models of graphene sheets, are endowed with intriguing optical, el

78 g, we fabricated Ti(3)C(2)T(x) MXene-bridged graphene sheets at room temperature with isotropic in-pl

79 most of the observed transport properties of graphene sheets at zero magnetic field can be explained

80 constructed by slightly rotating a monolayer graphene sheet atop a thin bulk graphite crystal.

81 ng of such composites requires not only that graphene sheets be produced on a sufficient scale but th

82 band that is primarily localized to a single graphene sheet below the moire interface.

83 rit some of the key properties of individual graphene sheets, but also develop additional functions t

84 ate the solublization/suspension of pristine graphene sheets by an equimolar mixture of benzene and h

85 n selectively remove monolayers in few-layer graphene sheets by means of electron-beam-induced sputte

86 were fabricated from single- and multilayer graphene sheets by mechanically exfoliating thin sheets

87 od for the scalable synthesis of few-layered graphene sheets by the microwave-assisted functionalizat

88 ith horizontally and perpendicularly aligned graphene sheets by tuning the elongational and extension

89 idized sp(3) carbon atoms and vacancies in a graphene sheet can degrade its mechanical strength, they

90 Amyloid protein fibrils and graphene sheets can be combined to make a material that

91 ns of graphene with clean and well-separated graphene sheets can be obtained in both aqueous and orga

92 pproaches, unfunctionalized and non-oxidized graphene sheets can be produced; among them an inexpensi

93 Single-atom-thick graphene sheets can now be produced by chemical vapour d

94 (2)/g, the maximum surface area for infinite graphene sheets, carried mainly by edge sites; we call t

95 raphite flakes to single-layer and few-layer graphene sheets combined with functionalization of the g

96 to ripples in the membrane that stiffen the graphene sheets considerably, to the extent that gamma i

97 The graphene sheets contain extremely small amounts of irons

98 The readily available, super-clean graphene sheets contribute to an enhancement in the opti

99 Moreover, the graphene sheets dampen capillary waves such that rotatio

100 associated with the moire corrugation of the graphene sheet due to local variations in the graphene-s

101 tion sites might be realized across a single graphene sheet, facilitating the development of graphene

102 Interestingly, the graphene sheets favor the Janus-type assembly of COF nan

103 d dispersing small amounts of functionalized graphene sheets (FGSs) in liquid NM.

104 ed arrangement intercalated with small-sized graphene sheets filling the space and microvoids.

105 4.2 A [(12,12) to (3,3)] as well as a C(2)F graphene sheet fluorinated on one side only.

106 Additionally, the impact of the number of graphene sheets for the optimum efficiency of the propos

107 Whereas the graphene sheets formed from the unzipped part of the out

108 nner fiber structure consists of large-sized graphene sheets forming a highly ordered arrangement int

109 ITO) nanocrystals directly on functionalized graphene sheets, forming an ITO-graphene hybrid.

110 of the exfoliated accompanying carboxylated graphene sheet from pristine is achieved via Friedel-Cra

111 the spontaneous twisting and peeling off of graphene sheets from the polymer substrate.

112 synthesized by the controlled reassembly of graphene sheets; from their initial stacked morphology,

113 The existence of layered structures based on graphene sheets gives rise to an electronic structure re

114 Electrical measurements on graphene sheets, graphene nanoribbons, and large graphen

115 ing is opened and attaches covalently to the graphene sheet (Gs) to form exfoliated graphene with gra

116 wth behaviors were observed on low-oxidation graphene sheets (GS) and highly oxidized graphite oxide

117 on lightly oxidized, electrically conducting graphene sheets (GS) exhibit a high specific capacitance

118 eriodic perforation and heteroatom doping of graphene sheets have been developed, patterning closely

119 Bilayer graphene sheets have been found to be superconductive wh

120 nd recent studies have shown that individual graphene sheets have extraordinary electronic transport

121 In-situ TEM shows that graphene sheets help maintain the capacity even in the c

122 supported on N-doped carbon black or N-doped graphene sheets, highlighting the importance of the 3D m

123 on lattice are detected, indicating that the graphene sheets host the ideal charge density wave.

124 oes beyond the traditional model of parallel graphene sheets hosting layers of physisorbed hydrogen i

125 mical functionalization by doping a pristine graphene sheet in a certain pattern with hydrogen atoms

126 sheet, and with only 0.05 wt% functionalized graphene sheet in poly(methyl methacrylate) there is an

127 ies for applications would be to incorporate graphene sheets in a composite material.

128 of the chemical composition of the edges of graphene sheets in both flat and curved sp(2)-hybridized

129 ates, and also holds together the individual graphene sheets in multilayer samples.

130 of stabilization of liquid-phase-exfoliated graphene sheets in N-methylpyrrolidone (NMP), N,N'-dimet

131 orphology that reflects the structure of the graphene sheets in solution.

132 loid aggregation to model the aggregation of graphene sheets in the liquid phase in order to predict

133 enhanced through the excellent dispersion of graphene sheets in the matrix material and the strong gr

134 The highly ordered graphene sheets in the plane of the membrane make organi

135 However, the graphene sheets in these devices have irregular shapes a

136 r since the first isolation of free-standing graphene sheets in year 2004.

137 al reduction removed oxygen and defects from graphene sheets, increased the size of sp(2) domains, an

138 n nitride (hBN)(7,8) used to encapsulate the graphene sheets indicates the importance of the microsco

139 The rolling up of a graphene sheet into a tube is a standard visualization t

140 scalable self-assembly of randomly oriented graphene sheets into additive-free, essentially homogeno

141 port a prompt electrochemical exfoliation of graphene sheets into aqueous solutions of different inor

142 However, the actual processes of rolling up graphene sheets into CNTs in laboratory syntheses have n

143 Processing graphene sheets into nanoribbons with widths of less tha

144 zable approach for fashioning one-atom-thick graphene sheets into resilient and movable parts with mi

145 Here we develop a method to incorporate graphene sheets into vanadium pentoxide nanoribbons via

146 ergy gaps that are sometimes observed when a graphene sheet is placed on a hexagonal boron nitride su

147 The self-assembly of graphene sheets is driven thermodynamically, as graphite

148 Mass production of high-quality graphene sheets is essential for their practical applica

149 The bonding between adjacent graphene sheets is investigated by molecular dynamics si

150 on between two model hydrophobic plates, and graphene sheets, is reduced when urea is added to the so

151 rowth enlarged, over one hour, the nuclei to graphene sheets larger than one hundred nm(2) in area.

152 anus-binding were periodically weaved on the graphene sheet, leading to four different types of zones

153 transfer from the electron beam to few-layer graphene sheets leads to unique structural transformatio

154 d identification of the fluence at which the graphene sheet loses long-range order.

155 ectrical behaviour of both doped and undoped graphene sheets maintain excellent properties, with low

156 graphene surface, the carrier equilibrium in graphene sheet might be altered, and manifested by the c

157 Formula: see text]0.08 can be obtained for a graphene sheet modified with kirigami-inspired cuts when

158 ional (3D) hybrid material of nitrogen-doped graphene sheets (N-RGO) supporting molybdenum disulfide

159 Surfactant-wrapped chemically converted graphene sheets obtained from reduction of graphene oxid

160 lore the non-local correlation dynamics in a Graphene sheet of disordered electrons in a two-dimensio

161 the role of surface mediators on the buckled graphene sheets of acid-microwaved CNTs.

162 Synthesis of large-scale graphene sheets of high quality and at low cost has been

163 and scalable approach produces high-quality graphene sheets of low oxygen content, enabling a broad

164 ousands of tonnes per year, while continuous graphene sheets of tens of metres in length have become

165 o various industries, producing high-quality graphene sheets on a large scale becomes crucial.

166 Graphene sheets--one-atom-thick two-dimensional layers o

167 nd porphyrinic and is located at the edge of graphene sheets or pores.

168 arge MoO(2) film is created/deposited on the graphene sheet, originating and expanding from the origi

169 ctrical-circuit model is established and the graphene-sheet pattern is designed optimally for maximiz

170 R selectivity, we treated partially oxidized graphene sheets (po-Gr) with NR to obtain po-Gr-NR dispe

171 imilar trend, with values for functionalized graphene sheet- poly(methyl methacrylate) rivaling those

172 he molecular migration on a wrinkled/rippled graphene sheet preferentially happens from the valley (p

173 ur bottom-up chemical approach of tuning the graphene sheet properties provides a path to a broad new

174 anchorage, pi-stacking interactions with the graphene sheets provide further pi-delocalization that i

175 ased on our super-tough MXene-functionalized graphene sheets provides a combination of energy and pow

176 cts of graphene-metal contact resistance and graphene sheet resistance, enabling pronounced NDR effec

177 we characterize the hydrophobicity of curved graphene sheets, self-assembled monolayers (SAMs) with c

178 a-fetoprotein (AFP) is described that uses a graphene sheet sensor platform and functionalized carbon

179 Atomically thin graphene sheets serve as folding hinges during a process

180 perating at room temperature, where a single graphene sheet serves simultaneously as the plasmonic me

181 of pre-synthesized Ni(OH)(2) nanoplates and graphene sheets shows lower specific capacitance, highli

182 been observed on all suspended and supported graphene sheets studied so far.

183 However, the finite curvature of the graphene sheet that forms the nanotubes and the broken s

184 At the positively charged graphene sheet, the electrowetting response is amplified

185 With the protection of graphene sheets, the large and freestanding LixM/graphen

186 ain metal atoms are intercalated between its graphene sheets, the same has not been achieved in a sin

187 on-neighboring carbon atoms across an entire graphene sheet, thereby producing only a minimum concent

188 In contrast to the graphene sheet, they are chemically versatile.

189 e may therefore apply ideas from kirigami to graphene sheets to build mechanical metamaterials such a

190 pathways used so far for modification of 2-D graphene sheets to make is three-dimensional.

191 ical concentration of defects, free-standing graphene sheets undergo a dynamic transition from freely

192 Second, functionalized graphene sheets used for the biosensor platform increase

193 discrete electronic domains within a single graphene sheet using scanning transmission X-ray microsc

194 potential of mean force between two solvated graphene sheets using molecular dynamics (MD) simulation

195 wo-dimensional periodic ripples in suspended graphene sheets, using both spontaneously and thermally

196 on of 1,1'-ferrocenedicarboxylic acid on the graphene sheet via the pai-pai stacking.

197 Decorating Fe3O4 nanoparticles on graphene sheets was performed via a facile one-step chem

198 ring descending local curvatures) and a flat graphene sheet, we confirm that adsorption capacity is i

199 y electrically tuning the Fermi level of the graphene sheet, we demonstrate modulation of the guided

200 s and nanotubes tunneling multiple layers of graphene sheets were also observed.

201 m fluorescence property from nanohybrid, the graphene sheets were chemically doped with cadmium sulph

202 The graphene sheets were deposited on 1.00mm thick copper sh

203 With the aid of sonication, multilayer graphene sheets were exfoliated by NaC, leading to bette

204 lectronic properties of molecularly pillared graphene sheets were explored by performing Density Func

205 Graphene sheets were found in the TEM images of the carb

206 Herein, single-layered and few-layered graphene sheets were produced by dispersion and exfoliat

207 id of Ag nanoparticles anchored onto the 2-D graphene sheets were synthesized using a two-step laser

208 Herein, two-dimensional graphene sheets were utilized as the suitable grafter du

209 ext]) at MoO(2) nanowire decorated monolayer graphene sheets, when edge plane like- sites/defects hav

210 on the edge plane like- sites/defects of the graphene sheets, where the basal plane sites remain unal

211 inate from periodic nanoscale ripples in the graphene sheet, which enhance puckering around a sliding

212 Thus, separated graphene sheets, which are referred to as microwave-enab

213 n be obtained by fragmentation/truncation of graphene sheets, which creates surface areas exceeding o

214 f polymer nanocomposites with functionalized graphene sheets, which overcome these obstacles and prov

215 er of confined solvent molecules between the graphene sheets, which results from the strong affinity

216 rbed atoms flipping to the other side of the graphene sheet with a relatively low activation energy o

217 t to directly measure the adhesion energy of graphene sheets with a silicon oxide substrate.

218 (tDBG) comprises two Bernal-stacked bilayer graphene sheets with a twist between them.

219 we find that, counter to standard reasoning, graphene sheets with large-angle tilt boundaries that ha

220 y attaching chemical moieties at the edge of graphene sheets with minimal damage of the carbon basal

221 t an interconnected macroporous framework of graphene sheets with uniform dispersion of Fe(3)O(4) nan

222 Ni(OH)(2) nanocrystals grown on graphene sheets with various degrees of oxidation are in

223 nanoclusters of platinum were supported on a graphene sheet within a catalytic condenser device that

224 ispersion of individual, chemically modified graphene sheets within polymer hosts.

225 nitrogen atoms can be incorporated into the graphene sheet without destroying it.

226 oscopic flattening and in-plane shrinkage of graphene sheets without a complete loss of crystallinity