ライフサイエンスコーパス: SWNT

1 SWNT imaging presents lower signal spread ~0.08 x and hi

2 SWNT mobility in the presence of acetic acid was inhibit

3 SWNT-specific separation was obtained via magnetic separ

4 SWNT-TFTs with 5 different channel lengths, namely, 30,

5 SWNTs also exhibited collector media-dependent transport

6 SWNTs that were grown using conventional arc discharge m

7 method on large arrays consisting of ~20,000 SWNTs completely removes all of the m-SWNTs (~7,000) to

8 ; (ii) provide a direct measure of the (6,5) SWNT hole polaron delocalization length (2.75 nm); (iii)

9 that are uniquely associated with the (6,5) SWNT hole polaron state; and (iv) demonstrate that modul

10 ies demonstrate that S-PBN(b)-Ph4 PDI-[(6,5) SWNT] electronic excitation generates PDI(-.) via a phot

11 t unit are reported; S-PBN(b)-Ph4 PDI-[(6,5) SWNT] superstructures feature a PDI electron acceptor un

12 n spectroscopic signatures of oxidized (6,5) SWNTs were probed as a function of the electronic struct

13 The (6,5) SWNTs, i.e., SG65, with relatively lower diameter tubes

14 dified (6,5) chirality enriched SWNTs [(6,5) SWNTs] in which an aryleneethynylene polymer monolayer h

15 ed on (6,5) chirality-enriched SWNTs ([(6,5) SWNTs]) and a chiral n-type polymer (S-PBN(b)-Ph4 PDI) t

16 g favorable interaction tendencies for (7,6) SWNTs-is probed through ab initio molecular modeling.

17 with values as low as 100 meV for the (8,7) SWNT, consistent with a proposed image-charge modified B

18 about whether the electronic structure of a SWNT influences uptake.

19 oal through microwave irradiation of aligned SWNTs grown on quartz substrates.

20 display both tumor-targeting peptides and an SWNT imaging probe, demonstrates excellent tumor-to-back

21 eving high sensitivity and selectivity in an SWNT field-effect transistor (FET) biosensor.

22 both the Aptamer-SWNT and the Aptamer-Anchor-SWNT hybrids formation, facilitating exceptional optical

23 Aptamer-SWNT hybrids and the Aptamer-Anchor-SWNT hybrids with a periodically sequenced single-strand

24 en using the directly wrapped Aptamer-Anchor-SWNT hybrids.

25 g of the interactions between adsorbates and SWNTs is therefore critical to predicting adsorption iso

26 Using normal rat kidney (NRK) cells and SWNTs dispersed with bovine serum albumin (BSA), we demo

27 The specific affinity between DNA and SWNTs was verified and no significant side-interactions

28 pai-pai stacking interaction between PCA and SWNTs.

29 harge transfer between photoexcited TiO2 and SWNTs as well as the mechanism of acetone sensing.

30 gated single-walled carbon nanotube (Aptamer-SWNT) hybrids have demonstrated effective optical biosen

31 lying conjugation nature of both the Aptamer-SWNT and the Aptamer-Anchor-SWNT hybrids formation, faci

32 rived growth factor (PDGF) using the Aptamer-SWNT hybrids and the Aptamer-Anchor-SWNT hybrids with a

33 e increased tube diameter for (7,6) armchair SWNTs likely presented with higher van der Waals interac

34 c soluble derivative of flavin (FC12) around SWNTs and impart effective dispersion and individualizat

35 ) by living cells depends on factors such as SWNT length and surface chemistry.

36 mics involving both an intimately associated SWNT hole polaron and PDI(-.) charge-separated state, an

37 ory, suggesting that the energy gaps between SWNT and the LUMO of acceptor molecules dictate the ET p

38 est strongly that two distinct binaphthalene SWNT binding modes, cisoid-facial and cisoid-side, are p

39 n lysates of cells that had internalized BSA-SWNTs and that the uptake of BSA-SWNTs by NRK cells is n

40 nalized BSA-SWNTs and that the uptake of BSA-SWNTs by NRK cells is not influenced by SWNT electronic

41 BSA-SWNTs by NRK cells is not influenced by SWNT electronic structure.

42 rboxylated single-walled carbon nanotubes (c-SWNTs) in environmental samples using membranes modified

43 method is based on the preconcentration of c-SWNTs and their direct on-filter Raman spectroscopic ana

44 applied to the determination of traces of c-SWNTs in river water samples.

45 The preconcentration of c-SWNTs is performed by microfiltrating the sample through

46 ision, for a 10 mug.L(-1) concentration of c-SWNTs, was 4.74% intramembrane and 6.3% intermembrane.

47 ical parameter to quantify the presence of c-SWNTs, which mainly contribute to the intensity of the G

48 stranded DNA (ssDNA) was employed to capture SWNTs in water.

49 composition not previously known to catalyze SWNT growth, has been identified as the most active comp

50 o produce functionalized single-walled CNTs (SWNTs) with surface chemistries optimized for delivery o

51 Addition of TFA to the copolymer-SWNT dispersion resulted in a rapid conformational chang

52 We demonstrate SWNT trapping at low-frequency alternating current (AC)

53 ed on reversible H(+)/O2 doping to determine SWNT/surfactant thermodynamic stability values with grea

54 ase of the previously studied large diameter SWNTs.

55 copolymer selectively disperses low-diameter SWNTs, as would be expected from its ability to form a t

56 We suggest that sulfur in the small diameter SWNTs exists as a helical polymeric sulfur chain that en

57 of UV and acetone sensitivities of different SWNT-TiO2 hybrid systems, we established a fundamental u

58 Finally, zero-dimensional SWNTs were positively identified using mass spectrometry

59 the simple process of standing arc-discharge SWNTs with I followed by centrifugation.

60 rocess, and the hybridization voyage for DNA-SWNT platforms maneuvers their outcoming optical biosens

61 eport a facile method to controllably n-dope SWNTs using 1H-benzoimidazole derivatives processed via

62 ced charge transfer quenching of the encased SWNTs through the seamless helical encase.

63 The presence of SRHA enhanced SWNT stability in divalent CaCl(2) environment through s

64 olution deposition of semiconductor-enriched SWNT networks has been actively explored for high perfor

65 covalently modified (6,5) chirality enriched SWNTs [(6,5) SWNTs] in which an aryleneethynylene polyme

66 mpositions based on (6,5) chirality-enriched SWNTs ([(6,5) SWNTs]) and a chiral n-type polymer (S-PBN

67 s doping approach, we proceeded to fabricate SWNT complementary inverters by inkjet printing of the d

68 ine helix, and the C60 cage that facilitates SWNT exciton dissociation and electron transfer to the P

69 Finally, SWNT applications, to date, in organic and perovskite ph

70 , at the same time, greatly lowers costs for SWNT separation.

71 rved VOC, from 80 to 440 mV, is observed for SWNT/molecule acceptor pairs that have molecular volume

72 applications previously thought reserved for SWNTs.

73 s within the SWNTs, while the high frequency SWNT bands (nu > 1200 cm(-1)) are decreased in intensity

74 g the material complexity and functionality, SWNTs can probe the interfacial processes in the hybrid

75 NTs) enable the production of functionalized SWNTs that are soluble in organic solvents.

76 timize polyethylenimine (PEI)-functionalized SWNTs and perform plasmid DNA loading.

77 -nanomesh/single-walled carbon nanotube (GNM/SWNT) hybrid membrane with excellent mechanical strength

78 The resulting GNM/SWNT membranes show high water permeance and a high reje

79 Thus, membranes having SWNTs as moisture-conductive pores feature outstanding b

80 Encapsulation of sulfur in HiPCO-SWNTs leads to large changes in the Raman spectra with t

81 e that, high binding energy sites present in SWNT bundles are majorly responsible for their enhanced

82 al understanding of ET transfer processes in SWNT and allow for an accurate calculation of energy gen

83 he constriction sorter were induced for long SWNTs (>=1000 nm) with negative dielectrophoretic proper

84 f electronic materials, but the metallic (m)-SWNTs present in all as-synthesized nanotube samples mus

85 result allows for complete removal of all m-SWNTs, as revealed through systematic experimental and c

86 couple them into only the metallic SWNTs (m-SWNTs).

87 20,000 SWNTs completely removes all of the m-SWNTs (~7,000) to yield a purity of s-SWNTs that corresp

88 enerated from I with ultrasonication) with m-SWNTs is confirmed by changes in the D-band in the Raman

89 functionalized using M13 bacteriophage (M13-SWNT) can distinguish between F'-positive and F'-negativ

90 we attach an anti-bacterial antibody on M13-SWNT, making it easily tunable for sensing specific F'-n

91 This method allows us to manipulate SWNTs with the help of arrays of insulating posts in a m

92 The ability to convert metallic SWNTs to semiconducting without removing them allows for

93 lectively couple them into only the metallic SWNTs (m-SWNTs).

94 eparate the semiconducting from the metallic SWNTs present in the as-synthesized SWNT mixture.

95 he paper surface, which can accommodate more SWNTs.

96 methods to controllably form nanoengineered SWNT networks with controlled nanotube placement are dis

97 ven-chirality single-walled carbon nanotube (SWNT) are crucial for selective enrichment, targeted fun

98 unctionalized single-walled carbon nanotube (SWNT) field-effect transistors (FETs) to use as a fast a

99 th respect to single-walled carbon nanotube (SWNT) growth.

100 t incorporate single-walled carbon nanotube (SWNT) networks experience decreased on-off current ratio

101 cal doping of single-walled carbon nanotube (SWNT) papers is presented.

102 allenges with single-walled carbon nanotube (SWNT) photovoltaics and nanostructured devices is mainta

103 with sub-5 nm single-walled carbon nanotube (SWNT) pores is developed by F.

104 We report a single-walled carbon nanotube (SWNT) transistor technology with an end-bonded contact s

105 Single-walled carbon nanotube (SWNT)-based nanohybrid compositions based on (6,5) chira

106 e threshold voltage of single-wall nanotube (SWNT) thin-film transistors.

107 other hand, single-walled carbon nanotubes (SWNTs) -based chemiresistive biosensors are gaining popu

108 Single-walled carbon nanotubes (SWNTs) are being used in many consumer products and devi

109 tobleaching, single-walled carbon nanotubes (SWNTs) are potentially attractive contrast agents to det

110 iconducting, single-walled carbon nanotubes (SWNTs) are promising candidates for applications in thin

111 -wrapping of single-walled carbon nanotubes (SWNTs) are shown, along with how the resulting nanostruc

112 Here we report carbon nanotubes (SWNTs) as bacterial probes for fluorescence imaging of p

113 ration using single-walled carbon nanotubes (SWNTs) as nanoscale vector templates.

114 toxicity as single-walled carbon nanotubes (SWNTs) by acid treatment and annealing.

115 he uptake of single-walled carbon nanotubes (SWNTs) by living cells depends on factors such as SWNT l

116 Single-walled carbon nanotubes (SWNTs) can deliver imaging agents or drugs to tumours an

117 lically wrap single-walled carbon nanotubes (SWNTs) enable the production of functionalized SWNTs tha

118 Single-walled carbon nanotubes (SWNTs) exhibit high surface areas and precisely defined

119 es on top of single-walled carbon nanotubes (SWNTs) for achieving high sensitivity and selectivity in

120 terials like single-walled carbon nanotubes (SWNTs) in a field-effect transistor (FET)/chemiresistor

121 roperties of single-walled carbon nanotubes (SWNTs) make them ideal building blocks for the construct

122 Single-walled carbon nanotubes (SWNTs) offer unique electrical and optical properties.

123 nctionalized single-walled carbon nanotubes (SWNTs) on fungal and bacterial soil microbial communitie

124 we show that single-walled carbon nanotubes (SWNTs) passively transport and irreversibly localize wit

125 Single-walled carbon nanotubes (SWNTs) possess fascinating electrical properties and off

126 Single-walled carbon nanotubes (SWNTs) possess unique physical, optical, and electrical

127 the field of single-walled carbon nanotubes (SWNTs) significantly enhances the potential for practica

128 ransfer from single-walled carbon nanotubes (SWNTs) to polyoxometalate (POM) clusters results in the

129 he length of single-walled carbon nanotubes (SWNTs) to the same order of magnitude as their diameter

130 miconducting single-walled carbon nanotubes (SWNTs) was systematically studied through time-resolved

131 Single-walled carbon nanotubes (SWNTs) were used as the transducing element.

132 lly modified single-walled carbon nanotubes (SWNTs) with varying degrees of functionalization were ut

133 articles and single-walled carbon nanotubes (SWNTs)) were selected and optimized to enable the realiz

134 rivatives of single-walled carbon nanotubes (SWNTs), and discuss the potential of the mechanical bond

135 tions, using single-walled carbon nanotubes (SWNTs), are only possible with a uniform product.

136 ne, based on single-walled carbon nanotubes (SWNTs), gold electrode and complimentary strand of aptam

137 miconducting single-walled carbon nanotubes (SWNTs), sorted by density-gradient ultracentrifugation,

138 t bundles of single walled carbon nanotubes (SWNTs), synthesized by direct thermal decomposition of f

139 se (BOD) and single walled carbon nanotubes (SWNTs), the AuNC acts as an enhancer of electron transfe

140 n mixed with single-walled carbon nanotubes (SWNTs), this TTFV-fluorene copolymer exhibited strong in

141 of pristine single-walled carbon nanotubes (SWNTs), which covers <1% of the insulating substrate.

142 wrapping of single-walled carbon nanotubes (SWNTs).

143 e supported by single-wall carbon nanotubes (SWNTs).

144 opores using single-walled carbon nanotubes (SWNTs).

145 n mapping of single-walled carbon nanotubes (SWNTs): (i) in a small volume of water-surfactant disper

146 he affinity between single walled nanotubes (SWNTs) and specific single stranded DNA (ssDNA) was empl

147 etic properties compared to short (<=300 nm) SWNTs with positive dielectrophoretic properties.

148 on of divalent cations caused aggregation of SWNT clusters by suppressing the electrostatic repulsive

149 ization were utilized for the fabrication of SWNT thin film catalyst support layers (CSLs) in polymer

150 ng chemical vapor deposition (CVD) growth of SWNT is desirable, and much effort has been made towards

151 egradation of performance and instability of SWNT-FET biosensor devices.

152 Use of the optimum level of SWNT -COOH functionality allowed the construction of a p

153 nd to tackle some of the classic problems of SWNT chemistry.

154 area processing and electronic properties of SWNT TFTs.

155 n (R(2) = 0.90) was obtained with a range of SWNT concentration (0.05-10 mug/mL) against graphene as

156 l energy levels can drive spectral shifts of SWNT hole polaron transitions as well as regulate SWNT v

157 ions, as well as spectroscopic signatures of SWNT hole polaron and PDI radical anion (PDI(-.) ) state

158 , are apparent for three distinct sources of SWNT papers with modes in diameter distributions of 0.95

159 nal theory (DFT) to compute the stability of SWNT fragments of all chiralities in the series represen

160 arget protein, however, the understanding of SWNT hybridization with an aptamer forming a secondary o

161 n the absence of cocaine, a little amount of SWNTs bind to Aptamer-CS-modified electrode, so that the

162 So that, a large amount of SWNTs bind to CS-modified electrode, generating to a str

163 is (PAGE) method for measuring the amount of SWNTs in lysates prepared from cultured cells.

164 Electrical and optical applications of SWNTs often require specific lengths, but the preparatio

165 cy AC iDEP for technological applications of SWNTs.

166 ng as a routine tool for characterization of SWNTs as well as other materials with a pronounced reson

167 s study suggests that high concentrations of SWNTs can have widely varying effects on microbial commu

168 ocol, from the covalent functionalization of SWNTs to expression quantification, can be completed in

169 imate goal of chirality-controlled growth of SWNTs.

170 The major impact of SWNTs on bacterial community was observed after 3 days o

171 d its target and the stronger interaction of SWNTs with single-stranded DNA (ssDNA) than double-stran

172 we characterize the dynamics of migration of SWNTs in the microdevice using a finite element model.

173 onditions for length-based iDEP migration of SWNTs, and we characterize the dynamics of migration of

174 exposed to 0 (control), 250, and 500 mug of SWNTs per gram of soil.

175 ire specific lengths, but the preparation of SWNTs with the desired length is still challenging.

176 y is transiently affected by the presence of SWNTs.

177 can be adversely affected by the presence of SWNTs.

178 rochemical aptasensor inherits properties of SWNTs and gold such as large surface area and high elect

179 Because electronic properties of SWNTs are extremely sensitive to the surface state, dire

180 reserving intrinsic electrical properties of SWNTs.

181 and distinguish the electronic structure of SWNTs internalized by mammalian cells.

182 the lack of methods to measure the uptake of SWNTs by cell populations.

183 entration in landfill-relevant conditions on SWNT transport through a packed-bed of mixed municipal s

184 e influence of individual waste materials on SWNT deposition is also evaluated.

185 o avoid direct attachment of biomaterials on SWNTs, thereby preserving intrinsic electrical propertie

186 rect immobilization of proteins or DNAs onto SWNTs will generate surface defects through chemical rea

187 y delivering poly(acrylic acid)-nanoceria or SWNT-nanoceria complexes.

188 e copolymer were more pure than the original SWNTs that were initially dispersed.

189 oxidized single-walled carbon nanotubes (ox-SWNTs) functionalized with the conductive polymer poly(1

190 PA-SWNTs homoaggregation on the one hand showed no response

191 modified single-walled carbon nanotubes (PA-SWNTs) was systematically studied for a wide range of mo

192 The strategy of using nonaggregating PA-SWNTs is a novel experimental strategy that can be adopt

193 DLCA regime manifested by the presence of PA-SWNTs.

194 ydrophilic channels and the well-defined PCA/SWNTs ink deposition on paper in a facile manner requiri

195 modified single-walled carbon nanotubes (PCA/SWNTs) were deposited by quantitative inkjet printing wi

196 The PCA/SWNTs ink concentration can reach ~4 mg mL(-1) and was s

197 tibodies were then functionalized on the PCA/SWNTs.

198 A high-performance SWNT transistor was fabricated with a sub-10-nanometer c

199 This strategy promises high-performance SWNT transistors, enabling future ultimately scaled devi

200 ical chirality and the population of polymer-SWNT superstructures that feature the unexpected polymer

201 : (i) highlight the utility of these polymer-SWNT superstructures in experiments that establish the p

202 the spontaneous formation of host-guest POM@SWNT redox-active hybrid materials.

203 ges in waste composition influence potential SWNT mobility in landfills.

204 d to enable the realization of fully printed SWNT-based TFTs (SWNT-TFTs) on 150-m-long rolls of 0.25-

205 voltage (VOC) across three types of pristine SWNT papers with varying (n,m) chirality distributions.

206 lity allowed the construction of a prototype SWNT-based PEMFC with total Pt loading of 0.06 mg(Pt)/cm

207 surface, resulting in precipitation of pure SWNTs that were completely free of polymer.

208 hole polaron transitions as well as regulate SWNT valence and conduction band energies.

209 anotube surface, thus controlling rigorously SWNT-electron acceptor stoichiometry and organization.

210 Additionally, robust SWNT complementary metal-oxide-semiconductor inverter (n

211 After s-SWNT separation, the polymer can be depolymerized into m

212 erences in polarizabilities between M- and S-SWNTs have a negligible influence on gas adsorption for

213 energies for molecules adsorbed on M- and S-SWNTs having the same diameter.

214 This approach enables isolation of "clean" s-SWNTs and, at the same time, greatly lowers costs for SW

215 ibits strong dispersion for large-diameter s-SWNTs with high yield (23.7%) and high selectivity (99.7

216 werful and scalable strategy for enriching s-SWNTs, this approach suffers from significant contaminat

217 d acidic conditions, yielding polymer-free s-SWNTs.

218 conducting single-walled carbon nanotubes (s-SWNTs) have emerged as a promising class of electronic m

219 conducting single-walled carbon nanotubes (s-SWNTs) with little contamination are desired for high-pe

220 Blue 71 (I), for high-purity separation of s-SWNTs at high yield.

221 the m-SWNTs (~7,000) to yield a purity of s-SWNTs that corresponds, quantitatively, to at least to 9

222 Highly enriched (~93% purity) s-SWNTs are produced through the simple process of standin

223 verable conjugated polymers for separating s-SWNTs with little polymer contamination.

224 ned arrays of purely semiconducting SWNTs (s-SWNTs).

225 The s-SWNTs total yield is up to 41%, the highest yet reported

226 f transistor devices fabricated with these s-SWNTs exhibited on/off ratios of 10(3) to 10(5) with the

227 show that I preferentially complexes with s-SWNTs and preferentially suspends them.

228 Metallic (M-) and semiconducting (S-) SWNTs have extremely different polarizabilities that mig

229 The PANI coated S/SWNT composite showed a superior specific capacity of 10

230 es, we developed a sulfur-carbon nanotube (S/SWNT) composite coated with polyaniline (PANI) polymer a

231 n the turn-off voltage of the semiconducting SWNT FETs was seen upon incubation with B. burgdorferi f

232 Semiconducting SWNTs of varying length suspended with sodium deoxychola

233 Semiconducting SWNTs were imaged during dielectrophoretic manipulation

234 can detect both metallic and semiconducting SWNTs in lysates of cells that had internalized BSA-SWNT

235 able to selectively disperse semiconducting SWNTs, the subsequent removal of the polymer is challeng

236 that can selectively disperse semiconducting SWNTs.

237 isolation of dispersant-free, semiconducting SWNTs.

238 ctly aligned arrays of purely semiconducting SWNTs (s-SWNTs).

239 er, many applications require semiconducting SWNTs in their pure form.

240 fluidic device has the potential to separate SWNTs by length.

241 natural organic matter on chirally separated SWNT aggregation.

242 is is one manipulation method for separating SWNTs based on dielectric properties and geometry.

243 ics, sorting efficiencies for long and short SWNTs recovered from separate channels of the constricti

244 The demonstrations show SWNTs' immense promise as a low-cost and scalable TFT te

245 reshold voltages of our polythiophene-sorted SWNT thin-film transistors can be tuned accurately and c

246 off) without the need for either specialized SWNT growth methods or post growth processing steps to r

247 Here, targeted M13 virus-stabilized SWNTs are used to visualize deep, disseminated tumors in

248 represents chiralities among the most stable SWNT fragments (within 0.2 eV) from the computations.

249 Interestingly, suspended SWNTs showed both positive and negative dielectrophoresi

250 metallic SWNTs present in the as-synthesized SWNT mixture.

251 findings demonstrate the promise of targeted SWNT nanoprobes for noninvasive disease monitoring and g

252 ealization of fully printed SWNT-based TFTs (SWNT-TFTs) on 150-m-long rolls of 0.25-m-wide poly(ethyl

253 These findings indicate that SWNT materials can be developed as scalable materials fo

254 Results indicate that SWNT transport may be significant in mature waste enviro

255 The results suggest that SWNT stability can be chirality dependent in typical aqu

256 We demonstrate that SWNTs functionalized using M13 bacteriophage (M13-SWNT)

257 Moreover, we show that SWNTs enable near-infrared fluorescence monitoring of ni

258 The SWNT network physically separates the GNM into microsize

259 The SWNT templates control the dimensionality of the wires,

260 The SWNT-chloroplast assemblies also enable higher rates of

261 n site produced via hole migration along the SWNT backbone that occurs over this timescale.

262 lical polymeric sulfur chain that enters the SWNT interior in the form of S2 ((3)Sigma(g)(-)) molecul

263 hange and desorption of the polymer from the SWNT surface, resulting in precipitation of pure SWNTs t

264 utilizing the electrical parameters from the SWNT-TFTs, a Monte Carlo simulation for a 1-bit adder ci

265 Furthermore, the SWNT electrodes can be used as grown, i.e., they do not

266 Furthermore, the SWNT hosts provide a physical barrier, protecting the PO

267 ate changes in the number of carriers in the SWNT channel.

268 The extremely low background signals of the SWNT electrodes, as a consequence of the sparse surface

269 ectroscopic signatures characteristic of the SWNT hole polaron and PDI(-.) states.

270 Our analysis shows that the diameter of the SWNT product is governed by the well-known relation to s

271 ing aptamers (PBA) indirectly wrapped on the SWNT vicinity is influenced by anchoring length for opti

272 spectroscopy measurements confirmed that the SWNT Fermi level shifted to the conduction band edge wit

273 o the analyte for short periods of time, the SWNT electrodes do not foul and can be used repeatedly f

274 ntial facial binding of the polymer with the SWNT and thereby guarantee helically wrapped polymer-nan

275 lymer exhibited strong interactions with the SWNT surface, leading to stable, concentrated nanotube d

276 through the reaction of molybdenum with the SWNT to form carbide, also exhibited no Schottky barrier

277 ns govern the molecular interaction with the SWNT.

278 The SWNTs are shown to enable exceptionally fast transport o

279 The SWNTs can conduct charge to and from the encapsulated gu

280 containing cellulose fibers help connect the SWNTs into an electrical network.

281 Moreover, the SWNTs used are without prepurifications and very low cos

282 onfined sulfur species with the walls of the SWNTs which are not expected to be significant in the ca

283 age and the low intrinsic capacitance of the SWNTs, means that no signal processing is required to me

284 rption on interior and exterior sites of the SWNTs.

285 graphene oxide (GO) membrane covered on the SWNTs as a passivating layer to avoid direct attachment

286 the modulation of the surface charges on the SWNTs caused by the conformational change in SocA upon l

287 ultiple antibodies were immobilized onto the SWNTs surface for highly sensitive and specific field-ef

288 originate from the sulfur species within the SWNTs, while the high frequency SWNT bands (nu > 1200 cm

289 These SWNT-TFTs were characterized, and the obtained electrica

290 d ready dispersivity of MWNTs as compared to SWNTs, there is a significant opportunity to pursue the

291 However, traditional SWNT-based chemiresistors need to be more affordable for

292 persed, actively targeted, modularly tunable SWNT probes offer new avenues for exploration of deeply

293 ication of novel FET biosensor devices using SWNTs as semiconducting channels, and a monolayer of gra

294 ors by a gynecological surgeon improved with SWNT image guidance and led to the identification of sub

295 In this work, SWNT-TiO2 core/shell hybrid nanostructures were found to

296 signatures of semiconducting polymer-wrapped SWNT assemblies with the structural properties of the ch

297 HRTEM and AFM images of single-chain-wrapped SWNTs that reveal significant preferences for the antici

298 f surfactant and single-stranded DNA-wrapped SWNTs suspended in aqueous solutions manipulated by insu

299 Common synthesis procedures yield SWNTs with large length polydispersity and varying chira

300 Common synthesis processes yield SWNTs with large length polydispersity (several tens of