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 new high performing crystalline solid proton conductor.

3 ps the most well-known example of an organic conductor.

4 riation of the radiofrequency field within a conductor.

5 ctance when considered as a single-molecular conductor.

6 imultaneously on different parts of a single conductor.

7 ut relying on shared plans or on an external conductor.

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

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

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

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

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

13 ectric and magnetic fields in proximity to a conductor.

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

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

16 sidered for a Goubau line with a rectangular conductor.

17 a 2-pile, 1.03-mm wide, 0.30-mm thick REBCO conductor.

18 nductor, surrounded by a stretchable annular conductor.

19 de so far have been made out of REBCO coated conductor.

20 trategy toward the development of superionic conductors.

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

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

23 ternative to indium tin oxide as transparent conductors.

24 experimental verification is limited to poor conductors.

25 the underlying physical interaction between conductors.

26 nderstanding and designing new organic mixed conductors.

27 nd nonreciprocal carrier transport in chiral conductors.

28 ctronics demands insulators just as it needs conductors.

29 l conduction in a larger class of superionic conductors.

30 trong mobile ion interactions in super-ionic conductors.

31 ossible uses in batteries as solid state ion conductors.

32 is important new class of crystalline porous conductors.

33 xamined relative to other p-type transparent conductors.

34 inside storms, given the absence of physical conductors.

35 domains; a semiconducting glass between two conductors.

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

37 drogels as stretchable and transparent ionic conductors.

38 robotic structures and robust hydrogel-metal conductors.

39 tivation energy across many classes of ionic conductors.

40 iented research on improving solid-state ion conductors.

41 pening up new avenues to develop transparent conductors.

42 sirable structural attributes of good Li-ion conductors.

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

44 al-enabled highly conductive and stretchable conductors.

45 apid electrolocation of fast-moving prey and conductors.

46 h for the materials engineering of solid ion conductors.

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

48 toward mechanosensory cues and later toward conductors.

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

50 ext]) at the room temperature among magnetic conductors.

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

52 mbles the adhesion of bulk Ga drops to solid conductors.

53 o reported layered donor-acceptor electrical conductors.

54 entional inorganic semiconductors or organic conductors.

55 nic conductivities in superionic lithium-ion conductors.

56 to the complex atomic dynamics of superionic conductors.

57 ent with experiments and in contrast to band conductors.

58 re investigated as a novel class of protonic conductors.

59 ement when they are transformed into thermal conductors.

60 ew class of solvent-free, single lithium-ion conductors.

61 and Li sublattice for developing fast Li-ion conductors.

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

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

64 aining the residual resistivity ratio RRR of conductors above 150 to ensure stability of magnets agai

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

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

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

68 sign principles for sulfide and oxide Li-ion conductors, allowing for much greater freedom in structu

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

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

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

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

73 al uniform flow profile imaged in a metallic conductor and also in a low-mobility graphene channel.

74 ts of a highly conductive soft hydrogel as a conductor and an elastic fluorinated photoresist as the

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

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

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

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

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

80 electric field that arises between grounded conductors and charged dielectrics domains.

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

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

83 ies may be important to other spin-polarised conductors and orbitally degenerate materials.

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

85 emergent property in both REBCO and Nb(3)Sn conductors and that for the LTS Nb(3)Sn conductor, the e

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

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

88 asmonic effects), electronic (insulator to a conductor), and chemical parameters (multimetal patterni

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

90 re-Earth)Ba(2)Cu(3)O(7-delta) (REBCO) coated conductor, and a low temperature superconductor (LTS), a

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

92 ng graphene, topological insulators, organic conductors, and magic-angle twisted bilayer graphene.

93 pective applications in sensors, stretchable conductors, and responsive thermal interfaces.

94 ydrogel ionotronics, uses hydrogels as ionic conductors, and uses hydrophobic elastomers as dielectri

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

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

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

98 Strikes initiated in the absence of conductors are aborted.

99 Fast-ion conductors are critical to the development of solid-stat

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

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

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

103 The applications of mixed ionic-electronic conductors are limited due to phase instability under a

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

105 y inert, and electrically insulating thermal conductors are required.

106 When two conductors are separated by a sufficiently thin insulato

107 The two conductors are used as independently addressable electro

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

109 Implementation of the supramolecular ion conductor as a binder material allows for the creation o

110 Using solid-state Li-ion conductors as a model problem, unsupervised materials di

111 c materials, pyro- and ferroelectrics, ionic conductors as well as electrochemical containers.

112 new family of argyrodite lithium superionic conductors, as solid solutions Li(6+x)M(x)Sb(1-x)S(5)I (

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

114 power and hydrogen using solid oxide proton conductors at intermediate temperatures.

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

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

117 limiting the response time of organic mixed-conductor-based devices, and present the first real-time

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

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

120 t a methodology to design an enhanced proton conductor by means of a Na (x) CoO(2)/CeO(2) semiconduct

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

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

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

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

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

126 Transparent conductors combine two generally contradictory physical

127 Nanocarbon electronic conductors combined with pseudocapacitive materials, suc

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

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

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

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

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

133 port that is critical for prototypical mixed conductor devices.

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

135 PON) is an amorphous solid-state lithium ion conductor displaying exemplary cyclability against lithi

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

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

138 *).DMF] has the potential of converting to a conductor due to the selective and fast sorption of cadm

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

140 nanowires), carbon nanotubes/nanofibers, 2D conductors (e.g., graphene, MoS(2) ), metal oxides (e.g.

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

142 (>400%) elastomer tubules filled with liquid conductor (eutectic gallium indium, EGaIn), and fabricat

143 est ionic conductivity of solid-phase Li-ion conductors ever-reported: 5.44 x 10(-2) and 3.62 x 10(-2

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

145 These topological conductors exhibit giant Fermi arcs of maximum length (p

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

147 Organic mixed conductors find use in batteries, bioelectronics technol

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

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

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

151 y of reconciling conflicting requirements on conductors for fabricating magnets.

152 aturated-are not sufficiently good tunneling conductors for their conductivity to have favored them a

153 e as semiconductors for light generation and conductors for transparent electrodes, respectively.

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

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

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

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

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

159 gress has been achieved, polymer-based mixed conductors frequently experience significant volumetric

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

161 Herein, we design an inorganic ionic conductor/gel polymer electrolyte composite, where unifo

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

163 nd packing of organic mixed ionic-electronic conductors have an especially significant effect on tran

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

165 Soft ionic conductors have enabled stretchable and transparent devi

166 Organic mixed conductors have garnered significant attention in applic

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

168 on the atomic scale become excellent proton conductors if native cations are ion-exchanged for proto

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

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

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

172 r potential manipulation for employment as a conductor in medical devices, has gathered substantial i

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

174 strong functionality of the nanofluidic ion conductors in both acidic and basic environments.

175 lysts in heterogeneous reactions, electrical conductors in energy storage and transfer applications,

176 ) is one of the most widely used transparent conductors in optoelectronic device applications.

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

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

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

180 Three new garnet-type Li(+) conductors, including Li(6.5) Nd(3) Zr(1.5) Ta(0.5) O(12

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

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

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

184 The electronic Seebeck response in a conductor involves the energy-dependent mean free path o

185 a semiconductor to function as a fast proton conductor is an emerging strategy in the rapidly develop

186 ic field, the flow of charged particles in a conductor is deflected from the direction of the applied

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

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

189 uctivity ([Formula: see text]) in superionic conductors is of great interest for energy conversion ap

190 erromagnetic Bi(0.9)La(0.1)FeO(3) with ionic conductor KBr, can be relevant.

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

192 curred in the high field regions over a long conductor length.

193 ect in the archetypal superionic lithium-ion conductor Li(10)Ge(1-x)Sn(x)P(2)S(12).

194 Now, a sulfide-based superionic conductor Li(4) Cu(8) Ge(3) S(12) with superior stabilit

195 We report on the novel superionic conductor Li(9) AlP(4) which is easily synthesised from

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

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

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

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

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

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

202 ted polyelectrolyte, is presented as a mixed conductor material that can be used to fabricate high tr

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

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

205 This benchmark may compromise the conductors' mechanical integrity if their epsilon(irr,0)

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

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

208 low tubules made of a mixed ionic-electronic conductor (MIEC).

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

210 Mixed ionic-electronic conductors (MIECs) that display high oxide ion conductiv

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

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

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

214 c conductivity in an archetypical sodium-ion conductor Na(3)PS(4) are not fully understood.

215 solid electrolyte (BASE), sodium superionic conductor (NASICON), and sodium thiophosphate (75Na(2)S.

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

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

218 layered oxide scale function as an efficient conductor of electricity at elevated temperature.

219 he cell surface relies on retromer, a master conductor of endosomal recycling.

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

221 human skin as well as ambient air is a poor conductor of heat, wearable thermoelectric coolers opera

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

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

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

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

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

227 n (PSF)-based deconvolution, where the point conductor plays the same role as the point emitter in op

228 ansient structure of the model organic mixed conductor, poly(3,4-ethylenedioxythiophene) polystyrene

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

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

231 rmining charge-carrier sign and density in a conductor, requires a magnetic field to produce transver

232 stretchable elastomeric materials of rubbery conductors, rubbery semiconductors, and rubbery dielectr

233 rain-induced irreversible degradation of the conductor's critical-current beyond epsilon(irr,0).

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

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

236 great challenges in synthesizing elastomeric conductors, semiconductors and dielectric materials.

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

238 Electronic inks, including conductors, semiconductors, and dielectrics, are drawn o

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

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

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

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

243 The fabricated Zn conductors show excellent electrical conductivity ( appr

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

245 The resulting charge selective conductor shows intriguing features of both high ionic c

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

247 This property is undesirable for stretchable conductors since such composites may become less conduct

248 gn of heterocyclic solid-state organic ionic conductors (SOICs) in flexible energy generation and sto

249 An electrical conductor subjected to a magnetic field exhibits the Hal

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

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

252 aces with a circular transparent stretchable conductor, surrounded by a stretchable annular conductor

253 The magnet uses a conductor tape coated with REBCO (REBa(2)Cu(3)O(x), wher

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

255 ed and experimentally tested with nanoporous conductors that are shown to have a distinctive spectral

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

257 3)Sn conductors and that for the LTS Nb(3)Sn conductor, the emergent behaviour is not consistent with

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

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

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

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

262 on-redox-active proteins are good electronic conductors, though the mechanism of conduction is not ye

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

264 e being adaptable for use with high-strength conductors, thus producing sensors resilient to adverse

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

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

267 istorical development from solid-state ionic conductors to CSSEs, and then summarize the fundamentals

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

269 tetragonal) and electrical (insulator to the conductor) transitions presents a formidable challenge f

270 re among the state-of-the-art in stretchable conductors under large mechanical deformations.

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

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

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

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

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

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

277 The supramolecular lithium ion conductor utilizes orthogonally functional H-bonding dom

278 2.2 mm in diameter with an extended central conductor was switched between a 3-T MR imaging unit and

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

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

281 nd only to that of diamond, the best thermal conductor, which may be of benefit for waste heat manage

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

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

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

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

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

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

288 s a soft, stretchable, and transparent ionic conductor with transmittance of 98.8% and fracture strai

289 unity for various applications as a flexible conductor with unique mechanical and physics properties

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

291 sed learning scheme discovers 16 new fast Li-conductors with conductivities of 10(-4)-10(-1) S cm(-1)

292 les for the preparation of related oxide ion conductors with even better properties.

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

294 Sulfide-based superionic conductors with high ionic conductivity have been explor

295 They are also excellent electrical conductors with metal-like carrier concentrations.

296 for the creation of low-swelling soft mixed conductors with tailored properties and applications in

297 tial importance, a need for developing novel conductors within such devices has evolved over the past

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

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

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