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 syntheses generate a heterogeneous mixture of speci

4 SWNT-specific separation was obtained via magnetic separ

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

6 SWNTs also exhibited collector media-dependent transport

7 SWNTs that were grown using conventional arc discharge m

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

23 tronic density transferred between metal and SWNT, both of which increase along the triad W, Re, Os,

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

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

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

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

28 lubilize small-diameter and low chiral angle SWNTs.

29 esults show that repeated applications of AP-SWNTs can affect microbial community structures and indu

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

46 of aligned freestanding single-walled CNTs (SWNTs) makes the technique very attractive.

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

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

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

50 ase of the previously studied large diameter SWNTs.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

67 oscopy is highly sensitive and selective for SWNT and that this technique can be applied to track the

68 applications previously thought reserved for SWNTs.

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

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

71 s (SWNTs), we prepared a well-functionalized SWNT formulation with long blood circulation (half-life

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

73 t-handed helix that enriches the left-handed SWNTs for all suspended (n,m) species.

74 es diameter dilation of only the left-handed SWNTs, whose improved intermolecular interactions with t

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

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

77 n-butyl, diphenylcyclopropyl, and hydrazine SWNT, is presented.

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

79 the optoelectronic properties of individual SWNTs.

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

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

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

83 20,000 SWNTs completely removes all of the m-SWNTs (~7,000) to yield a purity of s-SWNTs that corresp

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

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

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

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

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

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

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

91 are effective in stabilizing and mobilizing SWNTs in environmental media.

92 characterising and regenerating the modified SWNTs.

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

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

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

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

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

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

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

100 rification of single-walled carbon nanotube (SWNT) soot and enrichment in high aspect ratio nanotubes

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

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

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

104 ispersion of single-walled carbon nanotubes (SWNT) and quenching of the near-infrared fluorescence in

105 stability of single-walled carbon nanotubes (SWNTs) and how surfactant-wrapping of SWNTs can impact e

106 Single-walled carbon nanotubes (SWNTs) are a fundamental family of distinct molecules, e

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

123 ve growth of single-walled carbon nanotubes (SWNTs) remains a great challenge that hinders their use

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

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

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

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

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

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

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

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

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

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

134 o solubilize single-walled carbon nanotubes (SWNTs), we prepared a well-functionalized SWNT formulati

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

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

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

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

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

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

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

142 aterials offers the potential enhancement of SWNT applications and potentially simultaneous reduction

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

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

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

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

147 ing 0.03, 0.015, 0.0015, and 0.0003 mg/mL of SWNT, respectively, were determined for planktonic cells

148 othesized that the stability and mobility of SWNT suspensions is directly related to the surface cove

149 cognition using the nIR photoluminescence of SWNT is demonstrated, including selectivity toward pento

150 area processing and electronic properties of SWNT TFTs.

151 here the first detection and quantitation of SWNT in sediment and biota at environmentally relevant c

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

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

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

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

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

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

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

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

160 cy AC iDEP for technological applications of SWNTs.

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

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

163 e first time that the improved dispersion of SWNTs in aqueous solutions in the presence of PVK enhanc

164 of PVK enhances the antimicrobial effects of SWNTs at very low concentrations.

165 Moreover, we show that the ends of SWNTs and the points where two SWNTs cross do not show a

166 umors based on the intrinsic fluorescence of SWNTs in the second near-infrared (NIR-II, 1.1-1.4 mum)

167 The metals released from the raw forms of SWNTs would not play a role in the effects seen in soil

168 onstitute the first study of PECVD growth of SWNTs on the atomic level.

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

173 FD) used to form two-dimensional networks of SWNTs prevented bundle formation during network growth.

174 y is transiently affected by the presence of SWNTs.

175 can be adversely affected by the presence of SWNTs.

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

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

178 reserving intrinsic electrical properties of SWNTs.

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

180 est a route to chiral-selective synthesis of SWNTs through rational synthetic design strategies based

181 Toxicity of the three types of SWNTs was also assessed in liquid cultures using a biolu

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

183 tubes (SWNTs) and how surfactant-wrapping of SWNTs can impact ecological exposures in aqueous systems

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

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

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

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

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

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

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

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

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

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

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

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

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

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

198 r examples of similar semiconducting polymer-SWNT superstructures are reported that demonstrate that

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

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

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

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

203 of semiconducting nanotubes in the produced SWNT arrays.

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

205 advanced, driven by the requirement for pure SWNTs displaying particular features.

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

207 The toxic effects of four different PVK-SWNT (97:3 wt %) nanocomposite concentrations (1, 0.5, 0

208 gnificant reduction of biofilm growth on PVK-SWNT coated surfaces.

209 rules can be applied to the growth of random SWNT networks on silicon wafers.

210 on of pristine, unbundled, high aspect ratio SWNTs over residual impurities, as observed by Raman spe

211 t in unbundled, undamaged, high aspect ratio SWNTs.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

236 Semiconducting SWNTs were imaged during dielectrophoretic manipulation

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

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

239 that can selectively disperse semiconducting SWNTs.

240 isolation of dispersant-free, semiconducting SWNTs.

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

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

243 natural organic matter on chirally separated SWNT aggregation.

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

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

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

247 The chirality sorted SWNTs showed ~5-fold higher photoluminescence intensity

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

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

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

251 Interestingly, suspended SWNTs showed both positive and negative dielectrophoresi

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

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

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

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

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

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

258 ical micelle concentration demonstrated that SWNTs remained suspended for over six weeks in a surface

259 Here we show that SWNTs can target tumours in a two-step approach in which

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

261 The SWNT electrodes are deployed as amperometric (anodic) de

262 The SWNT-chloroplast assemblies also enable higher rates of

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

264 e that relies on exciton dissociation at the SWNT/C(60) interface, as shown in the figure.

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

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

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

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

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

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

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

272 effect of applying an electric field on the SWNT growth process, as one of the effects coming into p

273 elated to the surface coverage of SDS on the SWNT surface that simultaneously increases electrosteric

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

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

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

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

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

279 ns govern the molecular interaction with the SWNT.

280 The SWNTs are shown to enable exceptionally fast transport o

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 orescence spectroscopy demonstrates that the SWNTs exist as well-dispersed tubes that are stable over

287 Then, the SWNTs in the network were decorated with Cu2O nanopartic

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 These SWNTs can assemble into structures featuring aligned nan

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

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

293 t the ends of SWNTs and the points where two SWNTs cross do not show appreciably different HET kineti

294 resonant excitation of 808 nm than unsorted SWNTs on a per-mass basis.

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

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

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

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

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

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

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