ライフサイエンスコーパス: graphene

1 gue of what electrons experience in strained graphene.

2 th a Fermi velocity of comparable to that of graphene.

3 suggested to serve as models for defects in graphene.

4 emergent properties approaching single-layer graphene.

5 sizes and shapes, and to different types of graphene.

6 technique opens up enormous applications of graphene.

7 o the mobility values reported for suspended graphene.

8 sound thermoacoustically by Joule heating in graphene.

9 surfactants or chemical modification of the graphene.

10 n to the model interface formed by water and graphene.

11 fion composites based on carbon nanotube and graphene.

12 examples of two-dimensional materials beyond graphene.

13 large plasmonic field concentration in doped graphene.

14 sion from individual atomic-scale defects in graphene.

15 rahigh vacuum to an inert substrate, such as graphene.

16 nomenon is also prevalent in nanocrystalline graphene.

17 A membrane based on 30 m(2) of graphene, a readily accessible amount, could provide a h

18 Here we show that monolayer graphene, a tunable conductor, can be electrically modif

19 s the sulfur host, the quinonoid imine-doped graphene affords a very tiny shuttle current of 2.60 x 1

20 n this effort we propose a new laser wrapped graphene-Ag array as a highly sensitive Surface-enhanced

21 imaging of strongly confined THz plasmons in graphene and 2DEGs has been elusive so far-only GPs with

22 applied potential on the interaction between graphene and a silicon tip in an ionic liquid and descri

23 As both the graphene and device principles are transferrable to arbi

24 ndium oxide, dysprosium-doped cadmium oxide, graphene and diffused semiconductors, but also for 'opaq

25 Two-dimensional (2D) graphene and graphene oxide (GO) offer great potential a

26 haracterize the complex interactions between graphene and immune cells, we propose an integrative ana

27 face conformity of 2D capping layers such as graphene and MoS2 substantially suppress surface fluctua

28 ctivated carbon), and related materials like graphene and nanotubes.

29 ctrochemical sensors and biosensors based on graphene and on graphene-like 2D materials for biomarker

30 We show that graphene and other membrane-like monolayers support a sp

31 ry, where an electron is transferred between graphene and other species, encompasses many important p

32 or example, many applications based on using graphene and peptides require peptides to interact with

33 recent developments in organo-functionalized graphene and printed biosensor technologies are comprehe

34 studied two-dimensional materials: zero-gap graphene and visible/near-infrared gap transition metal

35 attractive Coulomb potential of vacancies in graphene, and further envision its universality for dive

36 oupling of GPs with the metal gate below the graphene, and that plasmon damping at positive carrier d

37 ll-cell battery that contains a lithiated Si/graphene anode paired with a selenium disulfide (SeS2) c

38 0 and 100% of the deep valence-band holes in graphene are filled via an Auger transition.

39 The zigzag edges of single- or few-layer graphene are perfect one-dimensional conductors owing to

40 Atomically thin materials such as graphene are uniquely responsive to charge transfer from

41 g intersection of these materials wherein 2D graphenes are hybridized with 3D hydrogels to develop th

42 n, carbon nanotubes and crosslinked or holey graphenes are used exclusively as the active electrode m

43 igh reversibility by using B,N-codoped holey graphene as a highly efficient catalyst for CO2 reductio

44 Our results establish graphene as a pristine and tunable experimental platform

45 ectra of electrons emitted from single layer graphene as a result of the decay of deep holes in the v

46 and ionic screening of ions adsorbed on the graphene as well as charged amino acids associated with

47 quantum numbers.The phase diagram of bilayer graphene at high magnetic fields has been an outstanding

48 interact with (e.g., noncovalently bind to) graphene at one end, while simultaneously exposing the o

49 The proposed graphene based electrical biosensor provided advantages

50 5.50 mA cm(-2) on the quinonoid imine-doped graphene based electrode with a high sulfur loading of 3

51 creating highly collimated electron beams in graphene based on collinear pairs of slits, with absorpt

52 Among most reports, only a few printed graphene-based biosensors including screen-printed oxida

53 Biosensors comprising of graphene-based conductive nanomaterials offer the advant

54 In this work, we developed an aptamer/graphene-based electrochemical biosensor for on-step, se

55 ive strategy with which to engineer advanced graphene-based functional nanocomposites with rationally

56 Graphene-based materials (GBMs), with graphene, their mo

57 The modification of graphene-based materials is an important topic in the fi

58 ar and chlorine resistance of these scalable graphene-based membranes are promising for use in practi

59 eoxycholate enhances NaCl rejection in these graphene-based membranes.

60 ce/chemiluminescence-quenching properties of graphene-based nanocomposites are exploited in various d

61 Herein, a graphene-based polylactic acid filament (graphene/PLA) h

62 detection of folic acid protein (FAP) using graphene-based SPR chips.

63 y exploits the pH dependency of liquid-gated graphene-based transistors and the change in the local p

64 er a polymer, metal, or even atomically thin graphene, between the substrate and the brittle thin fil

65 The integration of the novel aptamer in the graphene biosensor allows a promising way for cost-effec

66 luding screen-printed oxidase-functionalized graphene biosensor have been demonstrated.

67 Taken together, the graphene biosensors provide an effective tool for clinic

68 applicable to all layered materials such as graphene, black phosphorous and transition metal dichalc

69 eport the observation of excitons in bilayer graphene (BLG) using photocurrent spectroscopy of high-q

70 e film exfoliated from In2 Se3 crystals on a graphene bottom electrode, it is shown that SET/RESET pr

71 ' method and can be readily transformed into graphene by chemical reduction.

72 phene layers without noticeably damaging the graphene by using a controlled low energy oxygen (O2(+)/

73 as SiO2, the addition of each extra layer of graphene can drastically alter their electronic and stru

74 s with a direct covalent linkage between the graphene carbon network and the functional porphyrin uni

75 site film consisting of the Au nanoparticles/graphene-chitosan has been designed to construct an impe

76 receptor molecules onto our high-sensitivity graphene-coated IDE-arrays with identical sensor charact

77 a new electrical biosensor platform based on graphene-coated interdigitated electrode arrays (IDE-arr

78 The temperature dependence of the silicon-graphene conductive photodetector is studied for the fir

79 We find that the triple junctions in graphene consist mostly of five-fold and seven-fold carb

80 With a systematic investigation, a novel graphene/cotton-carbon cathode is presented here that en

81 sing a trilayer graphene, mono- and bi-layer graphene could be successfully fabricated after one- and

82 asma infiltrating sintering of copper-coated graphene (Cu@Gr) composite powders.

83 s that contributes to the molecular basis of graphene cytotoxicity.

84 The approach reveals that graphene derivatives at the nanoscale assemble into vari

85 Covalently functionalized graphene derivatives were synthesized via benchmark redu

86 A hybrid metamaterial/graphene device is implemented into an external cavity s

87 by electrostatic gating of the metamaterial/graphene device, demonstrating a modulation depth of 100

88 intrinsic 2D Dirac plasmons in 3D nanoporous graphene disclosing strong plasmonic absorptions tunable

89 of the electronic heat energy deposited on a graphene disk can be transferred to a neighboring nanois

90 icotine sensor having coatings of silver and graphene doped ZnO nanostructure onto the unclad core of

91 ic residues, whereas MSI-78(C1) lies down on graphene due to an even distribution of Phe residues and

92 icated that part of cecropin P1 stands up on graphene due to an unbalanced distribution of planar and

93 ered towards entities predominantly fused to graphene edges through two pyrrole rings by thermal anne

94 In graphene, electrically tunable and highly confined plasm

95 he electrochemical sensing activities of the graphene-electrode was explored as a model for bioelectr

96 (vdW) heterostructure sandwiched between two graphene electrodes, to achieve high energy conversion e

97 terobilayers and finite density of states of graphene electrodes.

98 rallel and sandwiched between top and bottom graphene electrodes.

99 ocity, to probe the nonlocal response of the graphene electron liquid.

100 have developed a cost-effective and portable graphene-enabled biosensor to detect Zika virus with a h

101 the phonon Kohn anomaly near the K point for graphene encapsulated in hBN, and shifts the dominant in

102 of van der Waals heterostructures of In2Se3/graphene, exhibiting a tunable Schottky barrier, and In2

103 The expansion of the graphene family by adding silicene, germanene and stanen

104 of standardization in the production of the graphene family members.

105 this issue, we fabricated protein-decorated graphene FETs and measured their electrical properties,

106 The "graphene fever" has certainly provided a number of funda

107 ion, development and typical applications of graphene fibers.

108 High mobility graphene field-effect devices, fabricated on the complex

109 This work presents a fully integrated graphene field-effect transistor (GFET) biosensor for th

110 uces charges of opposite polarity within the graphene film modifying its conductivity.

111 observed for a single buffer layer on SiC or graphene films thicker than three to five layers.

112 ductive alkylation reaction in monolayer CVD graphene films.

113 Aligned graphene flakes exhibit emergent properties approaching

114 In few-layer graphene (FLG) systems on a dielectric substrate such as

115 microfluidic chamber with three-dimensional graphene foam as anode, allowing nutritional medium to f

116 The graphene foam enabled microfluidic flow-through approach

117 onsidering the very facile synthesis of this graphene foam/TiO2 nanosheet hybrid, and its excellent w

118 Herein, we designed a graphene foam/TiO2 nanosheet hybrid, which is able to ef

119 ex-doped carbon grown on flexible exfoliated graphene foil is designed and constructed for both elect

120 t the suggested pull and release approach to graphene folding may find applications in the theoretica

121 emerged as promising materials to complement graphene for advanced optoelectronics.

122 makes them a more attractive candidate than graphene for several applications, for example, as mecha

123 pproach, the interactions between avidin and graphene for the development of a sensing platform that

124 ing tungsten, silicon, graphite, diamond and graphene, for point defects such as vacancies, interstit

125 Rich, porous graphene frameworks decorated with uniformly dispersed a

126 search interest for the development of III-V/graphene functional hybrid heterostructures.

127 derstanding of basic principles of reductive graphene functionalization and will serve as a guide in

128 d will serve as a guide in the design of new graphene functionalization concepts.

129 Graphene (G) modified with magnetite (Fe3O4) and sol-gel

130 We find that the resistance across graphene GBs vary over a wide range depending on misorie

131 approach was utilised for the development of graphene-gold (G-Au) nanocomposite.

132 irus was accomplished by functionalizing the graphene-gold nanoparticles composite modified carbon el

133 cid oxidase (FAO) immobilized nitrogen-doped graphene/gold nanoparticles (AuNPs)/fluorine doped tin o

134 bon nanostructures such as carbon nanotubes, graphene, graphene oxide and nanodiamonds.

135 layer is used to transfer single crystalline graphene grown on silicon carbide substrates to flexible

136 We also map the local Hall voltage in graphene Hall nanosensors induced by the probes in diffe

137 are active material or component in hybrids, graphene has been the subject of numerous studies in rec

138 Recently, high-mobility graphene has emerged as an ideal two-dimensional semimet

139 Since its discovery, graphene has held great promise as a two-dimensional (2D

140 ct of nitrogen on the magnetic properties of graphene has so far only been addressed theoretically, a

141 aterials, the carbonaceous material such as 'graphene' has attracted the tremendous attention of rese

142 Applications of graphene have extended into areas of nanobio-technology

143 Stoichiometric derivatives of graphene, having well-defined chemical structure and wel

144 the thermoelectric transport across Au/h-BN/graphene heterostructures.

145 e realized GFETs offer the prospect of using graphene in a much wider range of electronic application

146 e factors still hindering the application of graphene in commercial batteries.

147 The participation of graphene in electron transfer chemistry, where an electr

148 The volume fraction (f) of graphene in ZnO was optimized using simulation of electr

149 We provide a detailed study of the light-graphene interactions by investigating the optical absor

150 Graphene is a 2D material that has been extensively used

151 Graphene is a highly promising material for biosensors d

152 Graphene is ideally suited for optoelectronic applicatio

153 demonstrating that the high conductivity of graphene is not lost when transferred to textile fibres.

154 f near total optical absorption in monolayer graphene is reported.

155 tion state (unmodified graphene vs. oxidized graphenes) is essential for the translation of this mate

156 Together with the optical qualities of graphene, its acoustic capabilities should inspire the d

157 the finite thermal resistance induced by the graphene layer.

158 is study, we demonstrated the ALE process of graphene layers without noticeably damaging the graphene

159 the van der Waals coupling between adjacent graphene layers, and the ability of reactants to diffuse

160 low diffusion within commensurately-stacked graphene layers.

161 red beta-W films with and without sandwiched graphene layers.

162 nd the range of properties for laser-induced graphene (LIG), specifically to tune the hydrophobicity

163 sors and biosensors based on graphene and on graphene-like 2D materials for biomarkers detection.

164 rch in the synthesis and characterization of graphene-like 2D materials, single and few-atom-thick la

165 their bulk counterparts and also from their graphene-like analogues.

166 The graphene-like B layer is highly active, whereas the phos

167 lk MoB2 (which contains only the more active graphene-like boron layers) by a 5-times increase of its

168 des, the working electrode was modified with graphene materials, and an enhancement of electroactive

169 g the transfer, the intactness of large-area graphene membranes can be as high as 95%, prominently la

170 tanding transparency to electron beam endows graphene membranes great potential as a candidate for sp

171 ricate large-area and high-quality suspended graphene membranes has been achieved.

172 In addition, using a trilayer graphene, mono- and bi-layer graphene could be successfu

173 The recent discovery of flexible graphene monolayers has triggered extensive research int

174 Tungsten-graphene multilayer composites are fabricated using a st

175 A doping effect is directly observed in graphene multilayer system as well as vHSs in bilayer gr

176 splacements greater than nanotube-Nafion and graphene-Nafion actuators and continuous operation for m

177 structure-switching biosensing principle in graphene nanoelectronics.

178 al bottom-up synthesis of atomically defined graphene nanoribbon (GNR) heterojunctions represents an

179 (AuNPs) embedded in a bottom-up synthesized graphene nanoribbon (GNR) matrix for the electrocatalyti

180 ness in carbon-based Dirac materials, namely graphene nanoribbons and nanotubes, thus showing the val

181 cient synthesis of donor-acceptor, cove-edge graphene nanoribbons and their properties in solar cells

182 is molecule-gold substrate separation if the graphene nanoribbons are absent.

183 We synthesized these new graphene nanoribbons in solution and found that the late

184 c molecules separated from a gold surface by graphene nanoribbons in vertically stacked heterostructu

185 As graphene nanoribbons of ultimate width, they are valuabl

186 bon nanotubes create magnetic fields through graphene nanoribbons, cascading logic gates through inco

187 ized Pd particles are uniformly dispersed on graphene nanosheets (GNSs) using a supercritical-fluid-a

188 ar dynamics simulations reveal that multiple graphene nanosheets can cooperate to extract large numbe

189 Such processes combined with graphene-nanostructure synthesis has the potential to cr

190 polycyclic aromatic hydrocarbons (PAHs) and graphene nanostructures demand methods that are capable

191 weakly interacting incommensurately-stacked graphene network, followed by a further flexible rearran

192 les encapsulated in few-layer nitrogen-doped graphene (Ni@NC) are synthesized by using a Ni-based met

193 tive succinimide ester group, interacts with graphene non-covalently via pi-stacking.

194 ier type, density, and mobility in epitaxial graphene on silicon-face silicon carbide.

195 Also, the graphene on the SiN membrane reveals not only the fastes

196 The properties of graphene open new opportunities for the fabrication of c

197 its atomic thickness and unique properties, graphene opens up new paradigms to realize this concept,

198 hly conductive nanocarbon framework (such as graphene or carbon nanotubes) is an attractive avenue to

199 physics in two-dimensional materials such as graphene or transition metal dichalcogenides.

200 multilayer system as well as vHSs in bilayer graphene over a wide range of twist angles (from 5 degre

201 IL) immobilized on electrochemically reduced graphene oxide (ERGO) for the detection of glucose via a

202 was immobilized on electrochemically reduced graphene oxide (ERGO) through the pi-pi stacking of hydr

203 ell mass cytometry to dissect the effects of graphene oxide (GO) and GO functionalized with amino gro

204 ed perylenediimide (PDI-HIS), copper ion and graphene oxide (GO) and that could be utilized as a high

205 lirubin oxidase (BOD)-based biocathode using graphene oxide (GO) could be prepared in 2 steps.

206 Recently, graphene oxide (GO) has been suggested as an adsorbent;

207 he aerogel is prepared through incorporating graphene oxide (GO) into alginate (ALG) matrix by using

208 One emerging example consists of graphene oxide (GO) membranes for separation processes.

209 We explore graphene oxide (GO) nanosheets functionalized dual-peak

210 tibacterial prickly Zn-CuO nanoparticles and graphene oxide (GO) nanosheets on a Ni porous electrode.

211 Two-dimensional (2D) graphene and graphene oxide (GO) offer great potential as a new type

212 of poly(3,4-ethylene dioxythiophene) (PEDOT)/graphene oxide (GO) onto the CFE surface is shown to inc

213 We combined graphene oxide (GO) sheets with a specific peptide aptam

214 flow system comprised of two functionalized graphene oxide (GO) surfaces that allow the capture of d

215 of a nature-inspired synthetic leaf made of graphene oxide (GO) thin film material, which exhibited

216 for reduction and simultaneous derivation of graphene oxide (GO) to form a biocompatible polymeric ma

217 isotropic orientation of GBNs, most notably graphene oxide (GO), in previous experimental studies ob

218 mical oxidation routes for the production of graphene oxide (GO), such as the Hummers' method, suffer

219 In this study, sub-20-nm thick, layered graphene oxide (GO)-based hollow fiber membranes with gr

220 coccus lysodeikticus whole cells adsorbed on graphene oxide (GO)-coated Surface Plasmon Resonance (SP

221 tum dots (QDs), carbon nanotubes (CNTs), and graphene oxide (GO).

222 tify the adsorption of U(VI) to multilayered graphene oxide (MLGO), we tested whether three different

223 er mesoporous Co3 O4 /nitrogen-doped reduced graphene oxide (N-rGO) nanosheets.

224 f redox active and bioengineering of reduced graphene oxide (RGO) for the development of versatile bi

225 d on the controllable integration of reduced graphene oxide (rGO), amorphous carbon, and MgO nanocrys

226 en developed using nanomaterials; Exfoliated Graphene Oxide and Gold Nano-Urchins for modification of

227 ructures such as carbon nanotubes, graphene, graphene oxide and nanodiamonds.

228 Besides, graphene oxide is water soluble and thus easy to process

229 exhibit better chlorine resistance than pure graphene oxide membranes.

230 Reduced graphene oxide modified by pulsed laser ablation causes

231 vel and highly sensitive biosensor employing graphene oxide nano-sheets (GO), multiwalled carbon nano

232 in the same RNA family using two-dimensional graphene oxide nanoassemblies.

233 urface of Ag-ZnO bimetallic nanoparticle and graphene oxide nanocomposite.

234 (FET) biosensor utilizing solution-processed graphene oxide nanoribbon (GONR) for methylene blue (MB)

235 s and an oxygen-functional-group gradient in graphene oxide nanoribbon network assemblies.

236 ne oxide-carbon nanotube composite (GO-CNT), Graphene oxide nanosheets (GO) and Iron oxide nanopartic

237 y(N-isopropylacrylamide) covalently bound to graphene oxide via free-radical polymerization.

238 lved the simultaneous reduction of RhCl3 and graphene oxide with NaBH4 and the in situ deposition of

239 pared by one pot synthesis from a mixture of graphene oxide, copper nitrate and uric acid, followed b

240 The gallery spaces in multilayer graphene oxide, for example, can intercalate hydrated me

241 (bamyl) from peanut (Arachis hypogaea) onto Graphene oxide-carbon nanotube composite (GO-CNT), Graph

242 To develop the method, a graphene oxide-silica composite reinforced hollow fiber

243 This biosensor was constructed by coating graphene oxide/ssDNA (GO-ssDNA) on an Au-electrode for V

244 pproach to assemble copper-nanowires/reduced-graphene-oxide hybrid coatings onto inorganic and organi

245 articles as a model system, we implemented a graphene-oxide layer as a substrate to significantly red

246 The GKTFET consists of a sequence of angled graphene p-n junctions (GPNJs).

247 tivity ( approximately 10 Omega per square), graphene patterned on wood surfaces can be readily fabri

248 e enhanced responsivity compared to pristine graphene photodetectors.

249 , a graphene-based polylactic acid filament (graphene/PLA) has been 3D printed to fabricate a range o

250 Here, we use graphene plasmons, propagating at extremely slow velocit

251 Further, the graphene platform can simultaneously provide the advance

252 ment with a model that accounts for both the graphene polarization charge and ionic screening of ions

253 Graphene-porphyrin nanohybrid materials with a direct co

254 sites are prepared by using polyaniline as a graphene precursor and introducing phenanthroline as a p

255 Graphene quantum dots embedded silica molecular imprinte

256 hotoluminescence quenching capabilities of a graphene-related hybrid material, is truly new and may h

257 after one- and two-cycle ALE of the trilayer graphene, respectively.

258 mer in the outer layer of unmodified reduced graphene (rGO; sensing layer) micromotors.

259 Graphene's success has stimulated great interest and res

260 chanical stability compared to the suspended graphene sensor.

261 capacity retention of the lithiated silicon/graphene-SeS2 full cell is 81% after 1,500 cycles at 268

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

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

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

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

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

267 The structural and binding analysis of graphene show that lithium atoms highly intercalate with

268 -free clean transfer of sub-centimeter-sized graphene single crystals onto TEM grids to fabricate lar

269 erconductivity was predicted in single-layer graphene (SLG), with the electrons pairing with a p-wave

270 l merits, this series hydrophilic multilayer graphene stack is showcased as suitable model cathode ho

271 The remarkable properties of graphene stem from its two-dimensional (2D) structure, w

272 ge of poorly understood experiments in gated graphene structures at low doping.Two-dimensional Dirac

273 The many unique properties of graphene, such as the tunable optical, electrical, and p

274 e to the change in the local pH close to the graphene surface.

275 give rise to a magnetic writing board using graphene suspension and a bar magnet as a pen.

276 during thermal oxidation of the sacrificial graphene template.

277 Graphene-templated growth of Mo2 C produces well-faceted

278 In bilayer graphene, the resistance exhibits a monotonic decrease w

279 Graphene-based materials (GBMs), with graphene, their most known member, at the head, constitu

280 We report on the fabrication of a graphene/titanium dioxide nanocomposite (TiO2-G) and its

281 have also incorporated the conversion of 2-D graphene to their various other dimensions like zero-, o

282 g experiments are performed for single-layer graphene transferred onto polystyrene (PS), semiconducti

283 film in the centimeter range can be grown on graphene using a Mo-Cu alloy catalyst.

284 ucture and energetics of triple junctions in graphene using a multiscale modelling approach based on

285 uding magnetic ones, carbon-based nanotubes, graphene variants, luminescent carbon dots, nanocrystals

286 trolled by modulating the carrier density of graphene via electrical gating.

287 few layers) and oxidation state (unmodified graphene vs. oxidized graphenes) is essential for the tr

288 ring-shaped nanostructures with surrounding graphene walls are stable under ambient conditions.

289 Chemical vapor deposition grown multilayer graphene was transferred onto nano/microIDE-arrays and u

290 ent the formation of WC after sintering, and graphene was uniformly distributed on the surfaces of ne

291 The exceptional properties of CVD graphene were exploited to construct a highly sensitive

292 protein complexes on ultraclean freestanding graphene were prepared by soft-landing electrospray ion

293 attractive Coulomb potential as realized in graphene.When the continuous scale symmetry of a quantum

294 ts four different plasmonic structures using Graphene which yielded an efficient plasmonic mode with

295 proximately three times higher than that for graphene, which was reported to have a large chi ((3)).

296 In striking contrast to graphene, whose strength decreases by more than 30% when

297 s development of magnetically active N-doped graphene with spin-polarized conductive behavior.

298 eractions between Cu and the pi electrons of graphene without the need of chelator conjugation, provi

299 Here, atomically thin graphene-WS2 heterostructure photodetectors encapsulated

300 nsing platform has been constructed based on graphene/zinc oxide nanocomposite produced via a facile