ライフサイエンスコーパス: conductor

1 , the La and Pr complexes would be the worst conductors).

2 riation of the radiofrequency field within a conductor.

3 temperature solid-state Na-S cell using this conductor.

4 cades as a stable, solution-processable hole conductor.

5 ns and holes, which are scattered inside the conductor.

6 /lithiation process in this promising Li-ion conductor.

7 ions in 4-12% doped CeO2 as a model fast ion conductor.

8 ectric and magnetic fields in proximity to a conductor.

9 ized zirconia (YSZ), an emblematic oxide ion conductor.

10 ks can serve as a template for a transparent conductor.

11 rom any lengths of cuprate-based HTS wire or conductor.

12 e membrane (ISM) and the underlying electron conductor.

13 ctron conductor and also a very good thermal conductor.

14 ed with few-layer graphene-an excellent heat conductor.

15 carrier, while graphene is an excellent hole conductor.

16 egrated blocking layer or an integrated hole-conductor.

17 MtrF is a nearly reversible two-dimensional conductor.

18 ctance when considered as a single-molecular conductor.

19 imultaneously on different parts of a single conductor.

20 ith arbitrary B 1 field distributions in non-conductors.

21 pening up new avenues to develop transparent conductors.

22 ternative to indium tin oxide as transparent conductors.

23 sirable structural attributes of good Li-ion conductors.

24 t Li-conducting materials and other fast ion conductors.

25 al-enabled highly conductive and stretchable conductors.

26 apid electrolocation of fast-moving prey and conductors.

27 h for the materials engineering of solid ion conductors.

28 in and charge is a crucial issue in magnetic conductors.

29 toward mechanosensory cues and later toward conductors.

30 as Sr2 FeMoO6 , are important spin-polarized conductors.

31 experimental verification is limited to poor conductors.

32 rt in plastic crystals and other solid-state conductors.

33 on strategy for high performance transparent conductors.

34 those of carbon nanotubes and other organic conductors.

35 the underlying physical interaction between conductors.

36 ighly stretchable and transparent electrical conductors.

37 hat is central to many organic and inorganic conductors.

38 transparent conductors are mostly electronic conductors.

39 heet resistance than all existing electronic conductors.

40 nderstanding and designing new organic mixed conductors.

41 lectronic correlations exist between the two conductors.

42 dates for novel oxonitridosilicate based ion conductors.

43 nd nonreciprocal carrier transport in chiral conductors.

44 value reported to date for molecular n-type conductors.

45 ctronics demands insulators just as it needs conductors.

46 l conduction in a larger class of superionic conductors.

47 trong mobile ion interactions in super-ionic conductors.

48 ossible uses in batteries as solid state ion conductors.

49 is important new class of crystalline porous conductors.

50 d heating with as few as three conveyor belt conductors.

51 xamined relative to other p-type transparent conductors.

52 inside storms, given the absence of physical conductors.

53 domains; a semiconducting glass between two conductors.

54 be used to guide the design of organic mixed conductors.

55 drogels as stretchable and transparent ionic conductors.

56 robotic structures and robust hydrogel-metal conductors.

57 tivation energy across many classes of ionic conductors.

58 iented research on improving solid-state ion conductors.

59 Of the 147 leads with externalized conductors, 10.9% had abnormal electrical parameters vs

60 It is also a good thermal conductor (35 Wm(-1)K(-1) at 26 degrees C).

61 benzene-bridged 1,2,3-bisdithiazolyl radical conductor 3a are strongly dependent on pressure.

62 alide perovskites are mixed ionic-electronic conductors, a finding that has major implications for so

63 point, the interaction is maximized, and the conductor absorbs strongly.

64 ple applications, including as a transparent conductor, active material in thin film transistors for

65 d Si-Hx seed layer for gate oxide or contact conductor ALD has been deposited via two separate self-l

66 arge quantization in small, weakly connected conductors allows for circuits in which single electrons

67 he majority of the radiation to pass; a good conductor also does not absorb, reflecting the wave almo

68 r the interfacial field at the junction of a conductor and a dielectric.

69 ise to two problems: the leaching-out of the conductor and a percolation-limited membrane conductivit

70 ene is a room temperature ballistic electron conductor and also a very good thermal conductor.

71 oxide matrix serves as an effective electron conductor and current collector with a stable mechanical

72 ed monolayers (SAMs) can be formed on (semi-)conductor and dielectric surfaces, and have been used in

73 st of four concentric, alternating layers of conductor and dielectric, respectively.

74 g cases such as engineering perfect magnetic conductor and epsilon-and-mu-near-zero media with nonmag

75 hene and hexagonal boron nitride are typical conductor and insulator, respectively, while their hybri

76 s are of significant interest as transparent conductors and as active components in power electronics

77 the area of nanomaterial-enabled stretchable conductors and devices are discussed.

78 to determine the prevalence of externalized conductors and electrical abnormalities in Riata ICD lea

79 (HIB = hexaiminobenzene) are bulk electrical conductors and exhibit ultraviolet-photoelectron spectro

80 y, the carbon nanotubes act as both electric conductors and ion-to-electron transducers of the potent

81 orted for state-of-the-art artificial proton conductors and make it possible to use reflectin in prot

82 e understanding of ionic transport in Li-ion conductors and serve as design principles for future dis

83 ility islands in high-mobility inhomogeneous conductors and that this process is only weakly affected

84 e realization of other magnesium solid ionic conductors and the eventual development of an all-solid-

85 idely applied to study ion pathways in ionic conductors and to provide useful insights for developing

86 re used to fabricate a stretchable composite conductor, and a fully printed and intrinsically stretch

87 are reviewed systematically: semiconductors, conductors, and dielectrics.

88 impedes REBa2Cu3Ox (RE = rare earth) coated conductor applications is the low engineering critical c

89 lms are a desirable material for transparent conductor applications; in particular when application-s

90 ted safety concerns associated with multiple conductor approaches were avoided.

91 Strikes initiated in the absence of conductors are aborted.

92 umps and adsorbent-based chillers and proton conductors are also reviewed.

93 Not only the bulk properties of the conductors are explored, but the concept of tuning the c

94 , optical and thermal properties, that oxide conductors are ideal candidates for plasmonic devices an

95 Oxide ion conductors are important materials with a range of techn

96 Existing stretchable, transparent conductors are mostly electronic conductors.

97 The majority of externalized conductors are not detectable with standard ICD interrog

98 he first examples of chiral single component conductors are reported.

99 When two conductors are separated by a sufficiently thin insulato

100 Here, ionic conductors are used to create a new type of sensory shee

101 Mixed ionic-electronic conductors are widely used in devices for energy convers

102 Using a solid-state ionic conductor as a gate dielectric, we generate unprecedente

103 f hard copper dendrites by the composite ion conductor at extreme discharge conditions is demonstrate

104 t proton-conducting perovskites or oxide ion conductors at this temperature.

105 llization of a subsitutionally doped organic conductor based on a host lattice composed of spiro-bis(

106 Finally, transparent conductors based on Al-doped Ag possess both a high and

107 ing this manufacturing strategy, stretchable conductors based on aligned carbon nanotubes are demonst

108 Transparent conductors based on few-layer graphene (FLG) intercalate

109 om the outset of the study of MOFs as proton conductors, both conductivity and hydrolytic robustness

110 trate can be an insulating material or (semi)conductor, but herein, we focus mainly on conducting sub

111 materials are a nontraditional route to ion conductors, but their crystallinity can give insight int

112 sm, SAMs of oligo(ethylene glycol)s are good conductors (by hole tunneling) but good insulators (by e

113 e-out abrasion results in externalization of conductor cables, with a higher risk of electrical failu

114 abrasion characterized by externalization of conductor cables.

115 reviously observed for this "supramolecular" conductor can be readily understood with our 2:2 complex

116 of K or THz respectively, a wide variety of conductors can be used like Quantum Point Contacts (this

117 e we show that monolayer graphene, a tunable conductor, can be electrically modified to reach this tr

118 de that analysis of the currents these ionic conductors carry has become a standard technique.

119 iometry and the attendant mixed ion-electron conductor character so important for intermediate temper

120 Transparent conductors combine two generally contradictory physical

121 onducting filaments across solid state ionic conductors commonly attribute the observed polarity of t

122 ansport properties in mixed ionic-electronic conductor composites through processing induced modifica

123 quick recovery: A semitransparent composite conductor comprising a layer of silver nanowire percolat

124 tons in the paraelectric phase of the proton conductor CsH2PO4.

125 g of an electromagnetic plane wave to a thin conductor depends on the sheet conductance of the materi

126 ability, a Li(7)P(2)S(8)I solid-state Li-ion conductor derived from beta-Li(3)PS(4) and LiI demonstra

127 port that is critical for prototypical mixed conductor devices.

128 ferent context, plasmonic metasurfaces (thin conductor-dielectric composite materials) have been prop

129 conductivity in the iodine-bonded molecular conductor (DIETSe)2 FeBr2 Cl2 [DIETSe=diiodo(ethylenedit

130 vely control particles similar to electrical conductors, diodes and capacitors.

131 he phosphor powders luminesce, but the ionic conductors do not electrolyze.

132 e we show that fast diffusion in super-ionic conductors does not occur through isolated ion hopping a

133 domain of the unique transmembrane reductant conductor DsbD as a model for an in-depth analysis of th

134 ion electrons of non-magnetic metals or semi-conductors due to the Rashba spin-orbit coupling.

135 mbranes is often carried out by dispensing a conductor (e.g., carbon nanotubes, or CNTs) in the membr

136 ics of an inorganic Conductor/WO3/LiNbO3/NiO/Conductor EC cell isaccompanied by the modulation of its

137 ons between electrons in spatially separated conductors enable a current flowing in one of the conduc

138 (>400%) elastomer tubules filled with liquid conductor (eutectic gallium indium, EGaIn), and fabricat

139 The P-doped Ba-122 coated conductor exceeds a transport Jc of 10(5) A/cm(2) at 15

140 These helical conductors exhibit strong non-local transport signals an

141 Oxide ion conductors find important technical applications in elec

142 ypical solids or how one can design fast ion conductors following simple principles.

143 n silicon-integrated lasers, and a plasmonic conductor for bio-sensing.

144 d with a conducting polymer film as the sole conductor for both the electrodes and the leads.

145 s FeCl(3)-FLG materials the best transparent conductor for optoelectronic devices.

146 ersal application of graphene as transparent conductors for both the anode and cathode.

147 shes the essential role of REBa2Cu3Ox coated conductors for very high field magnet applications.

148 pic conductors realized in a two-dimensional conductor form the hot source and the cold converter of

149 heet constructed from an artificial magnetic conductor - formed from non-magnetic, conducting, metama

150 ristics on x-ray correlate with risk of lead conductor fracture.

151 hest x-ray that correlate with risk for lead conductor fracture.

152 riate shocks for rapid oversensing caused by conductor fractures and reported for Medtronic Fidelis c

153 fractures and reported for Medtronic Fidelis conductor fractures.

154 photovoltaic performance of the derived hole-conductor-free device to 15.9%, outperforming the value

155 We report for the first time on a hole conductor-free mesoscopic methylammonium lead iodide (CH

156 erformance and stability of the derived hole-conductor-free printable mesoscopic PVSCs.

157 It can originate in an inhomogeneous conductor from distortions in the current paths induced

158 Within this context, bulk proton conductors from naturally occurring proteins have receiv

159 ices are designed by integrating stretchable conductors, functional chips, drug-delivery channels, an

160 which electrons collide with the atoms of a conductor, generating heat locally and only in regions o

161 The large potential of the conductor has been demonstrated by building a small coil

162 cal conductance of one-dimensional ballistic conductors has long been experimentally established, dem

163 r solid-state batteries, thiophosphate ionic conductors have been in recent focus owing to their high

164 Organic mixed conductors have garnered significant attention in applic

165 The ionic conductors have higher resistivity than many electronic

166 d high transmittance are required, the ionic conductors have lower sheet resistance than all existing

167 ove the performance of graphitic transparent conductors; however, none has demonstrated an increase o

168 have higher resistivity than many electronic conductors; however, when large stretchability and high

169 hierarchically wrinkled elastic transparent conductor (HWETC) is fabricated.

170 ed to PEDOT: PSS as a mixed ionic/electronic conductor in applications including bioelectronics, ener

171 ictates that the net electric field inside a conductor in electrostatic equilibrium is zero by effect

172 akes this material an attractive transparent conductor in future flexible electronic applications.

173 entary structure of Conductor/WO3/LiNbO3/NiO/Conductor in the frequency range from 1 GHz to 20 GHz.

174 opens up a new direction to design oxide ion conductors in perovskite oxides.

175 The prevalence of externalized conductors in Riata leads is significantly high (14.3%)

176 eries, improved thermoelectrics and fast-ion conductors in super-capacitors and fuel cells.

177 ns the way to future searches of transparent conductors in unexpected chemical groups.

178 t the anomaly affects the transport of clean conductors, in particular near the quantum limit.

179 ps substantially reduce the work function of conductors including metals, transparent conductive meta

180 suggests that in many other low-dimensional conductors, incoherent interlayer transport also arises

181 drive to replace the most common transparent conductor, indium tin oxide (ITO), with a material that

182 ionic motion, which are built from a simple conductor/insulator/conductor thin-film stack.

183 he sheet conductance of the material: a poor conductor interacts weakly with the incoming light, allo

184 he neutral polymer, which turns the modified conductors into efficient electron-selective electrodes

185 If the second conductor is part of a closed circuit, a net current wil

186 rent, self-healing, highly stretchable ionic conductor is presented that autonomously heals after exp

187 An appealing attribute of this Bi-2212 conductor is that, being without macroscopic texture, it

188 ting complex insulators, semiconductors, and conductors is discussed, along with its use in novel str

189 Research in stretchable conductors is fuelled by diverse technological needs.

190 nt of SOECs based on conventional oxygen-ion conductors is limited by several issues, such as high op

191 nd optical frequency ranges reveals that the conductor kinetic inductance creates an ultra-broadband

192 he best intermediate-temperature oxide-ionic conductor known.

193 The quasi-one-dimensional conductor Li0.9Mo6O17 has been of great interest because

194 A fluorine-doped antiperovskite Li-ion conductor Li2 (OH)X (X=Cl, Br) is shown to be a promisin

195 ence map (BVS-DM) analysis, the novel Li-ion conductor Li2Mg2P3O9N was synthesized by ion exchange fr

196 cluster ions, we report a lithium superionic conductor, Li3SBF4, that has an estimated 3D RT conducti

197 Utilizing the conductor-like polarizable continuum model of implicit s

198 The COnductor-like Screening MOdel for Realistic Solvents (C

199 adults, family carers are conceptualised as 'conductors'; making strong contributions to maintaining

200 -diameter carbon nanotube porins as a proton conductor material and suggest that strong spatial confi

201 and the free-carrier scattering rate of the conductor material.

202 Super-ionic conductor materials have great potential to enable novel

203 ce attack, for example, electrodeposition of conductors (metals) and non conductive, phosphate, anodi

204 ical and chemical environments of electronic conductors (metals, semiconductors) and biosystems.

205 s, similar studies of mixed ionic-electronic conductors (MIECs) have been hampered by the paramagneti

206 materials for SOFCs, mixed ionic-electronic conductors (MIECs), He-ion implantation, and superconduc

207 recordings using experiment-specific volume conductor models constructed from magnetic resonance ima

208 results demonstrate that homogeneous volume conductor models introduce substantial spatial inaccurac

209 II) redox couples in these sodium superionic conductor (NASICON) compounds.

210 A special case is sodium super ion conductor (NASICON)-based electrode materials as they ex

211 A deeper conductor observed east of the ridge at a depth of more

212 nting to the transmembrane form as the major conductor of collagen XIII effects.

213 and stiffest known material and an excellent conductor of heat and electricity.

214 Here we review how the liver is the central conductor of systemic iron balance and show that this ce

215 Here we demonstrate stretchable conductors of polyurethane containing spherical nanopart

216 re single-channel room-temperature ballistic conductors on a length scale greater than ten micrometre

217 ost manufacturing approach for bioresorbable conductors on bioresorbable polymer substrates by evapor

218 ate that the generation of excellent Nb:TiO2 conductors on glass (without breaking vacuum) only occur

219 pplication, nanomaterial-enabled stretchable conductors (one of the most important components for str

220 low for the targeted design of better proton conductors operating over a wide variety of temperatures

221 t for superconductors, but making attractive conductors out of the high-temperature cuprate supercond

222 w-layer graphene are perfect one-dimensional conductors owing to a set of gapless states that are top

223 grain coupling make iron-chalcogenide-coated conductors particularly attractive for high-field applic

224 ntrast gratings (HCGs) on a perfect electric conductor plane.

225 igh-frequency radiation emitted by a quantum conductor presents a rising interest in quantum physics

226 g that melanin is an electronic-ionic hybrid conductor rather than an amorphous organic semiconductor

227 Two capacitively coupled mesoscopic conductors realized in a two-dimensional conductor form

228 y the roles of both light harvester and hole conductor, rendering superfluous the use of an additiona

229 the distance of the graphene layers from the conductor's surface, the energy band gap between valence

230 Interacting electrical conductors self-assemble to form tree like networks in t

231 The substrate can be an electrical conductor, semiconductor, or insulator.

232 nic structure of individual point defects in conductors, semiconductors and ultrathin films, but such

233 nt classes of materials range from compliant conductors, semiconductors, to dielectrics, all of which

234 in future such as stretchable capacitors or conductors, sensors and oil/water separators and so on.

235 great potential in applications of flexible conductors, shock/vibration absorbers, thermal shock bar

236 Our P-doped Ba-122 coated conductors show a superior in-field Jc over MgB2 and NbT

237 The fabricated Zn conductors show excellent electrical conductivity ( appr

238 lenafulvalene], which is the first molecular conductor showing a large hysteresis in both magnetic mo

239 fy the local structure and dynamics of ionic conductors, similar studies of mixed ionic-electronic co

240 films grown on single-crystalline and coated conductor substrates.

241 outperform the current limit of transparent conductors such as indium tin oxide, carbon-nanotube fil

242 minimize such grain boundary obstacles, HTS conductors such as REBa2Cu3O(7-x) and (Bi, Pb)2Sr2Ca2Cu3

243 devices based on mixed ionic and electronic conductors, such as lithium-ion batteries, solid-oxide f

244 s and could be compared with the best proton conductors, such as Nafion.

245 fabrication of dense membranes, making this conductor suitable for industrial adoption.

246 ene terephthalate, glass, and quartz, and to conductor supports, such as indium tin oxide, aluminum,

247 hexanethiol monolayer as underlying electron conductor suppresses the formation of a water layer and

248 anically robust, and inexpensive transparent conductors (TCs) for optoelectronic device integration.

249 e membrane and the underlying solid electron conductor that is designed to reduce the irreproducibili

250 Hydrated BaSn(1-x)Y(x)O(3-x/2) is a protonic conductor that, unlike many other related perovskites, s

251 describe a class of devices enabled by ionic conductors that are highly stretchable, fully transparen

252 Among the superionic conductors that show a Faraday transition - the continuo

253 ver, in marked contrast to other stretchable conductors, the electrical conductance of the stretchabl

254 has been recent progress towards stretchable conductors, the realization of stretchable semiconductor

255 missing compounds are potential transparent conductors, thermoelectric materials and topological sem

256 In addition to forming excellent conductors, these metals can be used actively to form me

257 When charges are injected into organic conductors, they get trapped and influence single molecu

258 are built from a simple conductor/insulator/conductor thin-film stack.

259 point for high-temperature, anhydrous proton conductors through inclusion of guests other than water

260 ting extracellular potentials in a 3D volume conductor to a one-dimensional problem.

261 the unforseen stability of this transparent conductor to a relative humidity up to 100% at room temp

262 pths in a warm damp mantle, we interpret the conductor to be a partially molten layer capped by an im

263 -type Li6.4La3Zr2Al0.2O12 (LLZO) lithium-ion conductor to provide continuous Li(+) transfer channels

264 aps of these atomic layers can be tuned from conductor to semiconductor to insulator.

265 ensitivity of these neutral single-component conductors to external pressure, as compared with "class

266 ctors enable a current flowing in one of the conductors to induce a voltage drop in the other.

267 nductivity when employed in a 3D stretchable conductor, together with a high conductivity at low CNT

268 The best-known stretchable conductors use polymer matrices containing percolated ne

269 nt on the nature and geometry of the quantum conductor used for the detection, up to a Fano factor, c

270 s presented to determine optimal currents in conductors used for the transportation.

271 damental challenge for designing transparent conductors used in photovoltaics, displays and solid-sta

272 dopant layers coalesce into a homogeneous 3D conductor using anisotropic quantum interference measure

273 ew guidance for preparing good ion-selective conductors using electrochemical approaches.

274 tates in quasi-one dimensional (Q1D) organic conductors, using an extended Su-Schrieffer-Heeger (SSH)

275 2.2 mm in diameter with an extended central conductor was switched between a 3-T MR imaging unit and

276 thin phase-change materials and transparent conductors, we demonstrate electrically induced stable c

277 In contrast with classical conductors, we find that increasing the number of parall

278 The estimated rates of externalized conductors were 6.9% and 36.6% at 5 and 8 years after im

279 g this approach, we engineer helical 1D edge conductors where the counterpropagating modes are locali

280 aining a very low quantity (1.8%) of organic conductor, which self-organizes to provide z conduction

281 bricated neural probes utilize hard metallic conductors, which hinder their long-term performance bec

282 e eel presses its chin against a threatening conductor while discharging high-voltage volleys.

283 e demonstrate that the chain is a mechanical conductor, whose carriers are nonlinear solitary waves,

284 odule characterized by brief openings into a conductor with a prolonged lifetime in the open state.

285 ted crystal structure and p-type transparent conductor with a strong optical absorption peak at 3.36

286 ing this the prototype of a new class of ion conductor with applications in a range of energy generat

287 Herein, we report a novel sodium superionic conductor with NASICON structure, Na3.1Zr1.95Mg0.05Si2PO

288 onding interactions, we tailored a molecular conductor with random exchange interactions exhibiting u

289 and printed electronics technologies require conductors with a work function that is sufficiently low

290 the availability of flexible and transparent conductors with at least a similar workfunction to that

291 iralities, paving the way towards 1D helical conductors with fractional quantum statistics.

292 role as a completely new family of oxide ion conductors with potential applications in intermediate-t

293 second compound of this class of superionic conductors with very high values of 7 mS/cm for the grai

294 rt electrolyte functions solely as the ionic conductor without contribution to the cell capacity.

295 the optical characteristics of an inorganic Conductor/WO3/LiNbO3/NiO/Conductor EC cell isaccompanied

296 (EC) cell with a complimentary structure of Conductor/WO3/LiNbO3/NiO/Conductor in the frequency rang

297 tor, we show that it behaves like a metallic conductor would under photocathodic H(2) evolution condi

298 phene as an alternative flexible transparent conductor, yielding white organic light-emitting diodes

299 SnS4], a recently discovered, good Li(+) ion conductor, yields Li10SnP2S12, the thiostannate analogue

300 erconductivity emerges upon Se doping in CDW conductor ZrTe3 when the long range CDW order is gradual