ライフサイエンスコーパス: conductivity

1 evated surface area and excellent electrical conductivity.

2 thosphere-asthenosphere boundary, and mantle conductivity.

3 arity within the graphene film modifying its conductivity.

4 intensity correlates strongly with the film conductivity.

5 superior specific surface area and ballistic conductivity.

6 the additional reduction of lattice thermal conductivity.

7 material quality and showing good electrical conductivity.

8 bserved MOF that exhibits band-like metallic conductivity.

9 seasonal variation in 50% loss of hydraulic conductivity.

10 nsport with little degradation of electrical conductivity.

11 Mn2O3 is limited due to its poor electrical conductivity.

12 amellar Ag-CoSe2 nanobelts with controllable conductivity.

13 alloying often significantly decrease their conductivity.

14 ng the precise Li-ion migration barriers and conductivity.

15 at the individual fibres exhibit appreciable conductivity.

16 , yielding 3.5 x 10(4) S m(-1) in electrical conductivity.

17 -doped conductive polymer with this level of conductivity.

18 ral stability, and enhanced electronic/ionic conductivity.

19 centrate TNT into the GPE and provided ionic conductivity.

20 ditional separators at minimal cost to ionic conductivity.

21 and mid-infrared ranges, with lower metallic conductivity.

22 ields necessary to change graphene's optical conductivity.

23 on-coated structure can increase the overall conductivity.

24 o connected networks that support electrical conductivity.

25 g a high amount of oxygen and thus decreased conductivity.

26 n developed to establish the reduced thermal conductivity.

27 tering temperature and increased lithium ion conductivity.

28 cific surface area, and excellent electrical conductivity.

29 on of active sites as shown by the excellent conductivity.

30 smotic gradients, or the integrity of phloem conductivity.

31 finitely deformable while retaining metallic conductivity.

32 rees with recently published correlations to conductivity.

33 lenges in characterizing anisotropic thermal conductivity.

34 odeling significantly affect TATS electrical conductivity.

35 d for different channel heights and solution conductivities.

36 rdered metal divacancies and high electrical conductivities.

37 lysts through finely tuning their electrical conductivities.

38 iscretely distributed fractures with dynamic conductivities.

39 lus (dry condition), 160% increase in proton conductivity, 300% increase in water uptake, cyclic stra

40 An unprecedented combination of high proton conductivity (326 mS cm(-1) at 80 degrees C) and superio

41 ieve a approximately 25x increase in thermal conductivity (4.7 +/- 0.2 Wm(-1)K(-1)) over the base pol

42 he large cages results in a very low thermal conductivity, a unique feature of the clathrate family o

43 oper balance between activity, stability and conductivity-a challenging mission of great importance f

44 lues of nontransient Seebeck coefficient and conductivity agree with empirical modeling for materials

45 In this work, we show that the local thermal conductivity along a single Si nanowire can be tuned to

46 350 S cm(-1), the highest reported nonionic conductivity among films made from dopant-polymer soluti

47 recedented combination of metal-like thermal conductivity, an elastic compliance similar to soft biol

48 perovskite oxides with high room temperature conductivities and structural compatibility with a diver

49 -bandgap semiconductors with incipient ionic conductivity and a host of ferroic properties are review

50 s are, however, an inherently low electrical conductivity and a limited hole diffusion length that si

51 electrodiffusion with renormalized electric conductivity and a nonzero cation-anion diffusion coeffi

52 insulating BaBiO3 we observed an increase in conductivity and a subsequent relaxation, which are cons

53 Owing to the outstanding conductivity and biocompatibility as well as numerous ot

54 ata set allows for constraining both thermal conductivity and equation-of-state models.

55 The disposable devices show excellent conductivity and fast electron transfer kinetics.

56 The combination of low thermal conductivity and good transport properties results in a

57 In addition, the activation energies for the conductivity and Hall effect measurements indicated that

58 perties of zinc oxide thereby increasing the conductivity and hence the sensitivity of the sensor.

59 gold nanoparticles, which demonstrated good conductivity and high localized surface plasmon resonanc

60 ribbons, thus achieving increased electrical conductivity and improved chemical sensing capabilities.

61 The thermal conductivity and interface thermal conductance of ReS2 a

62 atorio model or Sesame S27314 for Al thermal conductivity and LEOS for Au/Al release equation-of-stat

63 hat require materials with both high thermal conductivity and low mechanical stiffness.

64 With the high electrical conductivity and low thermal conductivity, the screen-pr

65 ases fuel cell performance due to the proton conductivity and macroporosity characteristics of the po

66 he optimal conditions, i.e., maximum thermal conductivity and minimum nanofluid viscosity, based on t

67 thermoelectric materials of high electrical conductivity and of 1D electronic structure.

68 Electrical conductivity and partial pressure of CO2 (PCO2) indicate

69 n innate milk properties, such as electrical conductivity and pH, upon addition of adulterants as a t

70 by monitoring the changes in milk electrical conductivity and pH.

71 ing on the mechanical properties, electrical conductivity and piezoresistive behavior was explored.

72 We demonstrate p-type electrical conductivity and remarkable electrochemical properties o

73 y dilute solutions the renormalized electric conductivity and renormalized diffusion coefficients are

74 Here we analyse the electrical conductivity and Seebeck coefficient together and determ

75 improves electron delocalization, electrical conductivity and sodium uptake capacity.

76 injection efficiency due to their electrical conductivity and strong electronic coupling to the metal

77 Ion conductivity and the gating characteristics of tetrameri

78 Both the enhanced conductivity and the retained active sites contributed t

79 , apparent diffusion is linked to electrical conductivity and used to evaluate the efficiency of the

80 d multiobjective optimization of the thermal conductivity and viscosity of water-based spinel-type Mn

81 Canada, by quantifying three BTs, electrical conductivity, and delta(18)O in high-frequency streamwat

82 ignificantly impact fabrication, patterning, conductivity, and electrochemical performance.

83 ty, high fatigue resistance, high electrical conductivity, and excellent thermal-insulation/flame-ret

84 reveals the topological-in-origin nonlinear conductivity, and it leads to a universal scaling functi

85 fectively improve the intrinsic activity and conductivity, and the disordered structure from a lower

86 ondrial modifications that alter cytoplasmic conductivity, and these changes are benchmarked against

87 tion of antigorite is believed to cause high-conductivity anomalies.

88 c and polymer semiconductors have shown high conductivity approaching that of metals, the transport m

89 extensive attention due to their high ionic conductivity, approaching 1 mS cm(-1), excellent environ

90 Because of its high electrical conductivity ( approximately 10 Omega per square), graph

91 The conductivities are stable in air without extrinsic ion c

92 f the interlayer magnetoresistivity and Hall conductivity arising from the lowest Landau level under

93 to an acceptor stream causing an increase in conductivity as detected by a detector and recorded as a

94 This leads to a lattice thermal conductivity as low as 0.4 Wm(-1) K(-1) and a high therm

95 at grain boundaries is enabling the observed conductivity as proton conduction dominated by extrinsic

96 osited on nonconducting substrates and their conductivity as well as their ability to generate electr

97 e report that remarkably enhanced mobilities/conductivities, as high as 5.7x/3.9x, are achieved by co

98 ermal (>65 W/m-K) and electrical ( 700 S/cm) conductivities, as well as high thermoelectric power (22

99 same time, the small electrical and thermal conductivities at high temperatures imply that neither w

100 concentrations and the temporal dynamics of conductivity at a range of stream sites in watersheds wi

101 n a "universal" density-independent (scaled) conductivity at high densities.

102 stretchable conductor, together with a high conductivity at low CNT concentrations.

103 bulk length-scales, engineering the thermal conductivity at micro- and nano-scale dimensions is cons

104 ransport and to derive the intrinsic thermal conductivity at the thermal equilibrium limit.

105 It was found that the calculated thermal conductivity at two temperatures, 40 and 730 degrees C,

106 athin metallic copper formed provides a high conductivity backbone and cohesive support to accommodat

107 The electrical conductivity behavior of different dry matter samples of

108 n microfluidic devices, where a single, high-conductivity buffer expedites the transition from cell l

109 n while measuring impedance spectrum in high conductivity buffers and at low RF spectrum.

110 Here we move beyond thermal conductivity calculations and provide a rigorous and com

111 e)2 (Ni3(HITP)2), a MOF with high electrical conductivity, can serve as the sole electrode material i

112 The conductivity, carrier mobility, dielectric, and luminesc

113 ission based THz-TDS and are able to resolve conductivity changes in response to induced back-gate vo

114 charge carrier concentration and electronic conductivity character, which consequently affects their

115 sport pointed to a role for reduced membrane conductivity consistent with published data for cells an

116 ay contents, bulk density, and soil electric conductivity- cover a large area of Southern Taiwan.

117 The conductivity data of the metallic compound show the sign

118 ship between moisture content and electrical conductivity data was developed for the soil zone, and a

119 At very high pressure, the electrical conductivity decreases on compression, opposite to the b

120 rine, using capacitively coupled contactless conductivity detection (C(4)D), at pH 2.7.

121 oresis with capacitively coupled contactless conductivity detection (CE-C(4)D) electropherograms and

122 lectrochemical preprocessing and contactless conductivity detection (hybrid EC-CE-C(4)D) is herein de

123 Two electrophoretic methods with contactless conductivity detection have been developed for determina

124 a valve that transfers the H2S to a thermal conductivity detector (TCD), enables a precise heart cut

125 ochemical window, their electronic and ionic conductivities determine the electrochemical performance

126 At lower densities, the conductivity deviates from this universal curve, pointin

127 ertz regime, which arise from a reduction in conductivity due to carrier heating, have only recently

128 transfer rate and nearly three times higher conductivity due to the nanojunction architecture.

129 faces, electron velocities, hole or electron conductivity, effective mass and inner potential by simp

130 the solution matrix like current, potential, conductivity, electrochemical impedance, and electrochem

131 These e-textiles display reliable conductivity, enhanced porosity, flexibility, and stabil

132 ange materials relies on adding high thermal-conductivity fillers to improve the thermal-diffusion-ba

133 the same average pitch, and reduced thermal conductivities for nanomeshes with smaller pitches.

134 re identical (within 6% uncertainty) thermal conductivities for periodic and aperiodic nanomeshes of

135 The proton conductivities for the La and Pr complexes were roughly

136 We first compute the thermal conductivity for the case with aligned circular pores, c

137 ign crystalline solids with ultralow thermal conductivity for various applications including thermoel

138 can be identified for a well near a dynamic-conductivity fracture.

139 of salinity and temperature, and the thermal conductivity greatly affected pore water signals.

140 oundary scattering and its effect on thermal conductivity has impeded efforts to improve the thermoel

141 ihilation of planar walls, which show robust conductivity, has not been easy to achieve.

142 With addition of LiBF4, the Li(+) conductivity improves to 4.8 x 10(-4) S/cm.

143 menon, which may help explain the high ionic conductivity in doped fluorite-structured oxides such as

144 mall vessels, while promoting high hydraulic conductivity in large vessels.

145 The water potential at 50% loss of hydraulic conductivity in P. abies and P. mugo was -3.35 and -3.86

146 We exploit the fact that conductivity in semiconductors provides a modulation ind

147 ce confinement to the abnormal lower thermal conductivity in the MIM metamaterial with Ag layer thick

148 ring centers, leading to low lattice thermal conductivity in the printed n-type material.

149 as linearly correlated to change in electric conductivity in the soil zone; (b) vegetation cover type

150 To minimize the lattice thermal conductivity in thermoelectrics, strategies typically fo

151 Tunable conductivity in these systems is therefore key to their

152 s that likely causes the low lattice thermal conductivity in TlInTe2.

153 thermoreflectance (FDTR), we measure thermal conductivity in two series of SACs: the unary compounds

154 sing air-stable molecular dopants to improve conductivity in, and provide ohmic contacts to, organic

155 rcentage of 71 +/- 8% carbon particles), the conductivity increases dramatically and a maximum conduc

156 Whereas the electrical conductivity increases uniformly with increasing tempera

157 The traditional ratio of optical-to-DC conductivities is alone not an adequate figure of merit,

158 anes (AEMs) with high alkaline stability and conductivity is a considerable challenge in materials ch

159 evidence that geometric frustration-induced conductivity is a general phenomenon, which may help exp

160 The in-plane thermal conductivity is higher along the Re-chains, (70 +/- 18)

161 rain boundaries and clearly show that Li-ion conductivity is severely hindered through the grain boun

162 nterlayer bonding, the through-plane thermal conductivity is the lowest observed to date for 2D mater

163 ed conductivity, whereas s = 1 and itinerant conductivity is typically found in crystalline semicondu

164 Ionic conductivity is ubiquitous to many industrially importan

165 of phonon transport, which constrain thermal conductivity (k) to decrease monotonically with decreasi

166 nons and thereby reduces the lattice thermal conductivity kappa l .

167 We investigate lattice thermal conductivity kappa of MgSiO3 perovskite (pv) by ab initi

168 quantities, with high porosity, low thermal conductivity (kappa) and excellent figure of merit (z T)

169 4Cu1.7Se2.7Cl0.3: a room-temperature thermal conductivity (kappa) of 0.4(1) W/mK was measured on a pe

170 he order of 10(11) , and anisotropic thermal conductivity (kappa|| /kappa perpendicular ) of 18.

171 strategy for minimizing the lattice thermal conductivity (kappaL ) in thermoelectric materials.

172 formance of GeTe is the high lattice thermal conductivity (kappalat).

173 e is vital for limiting parasitic electrical conductivity losses in future electronic applications.

174 alloys are typically used due to their high conductivity, low viscosity, negligible nontoxicity, and

175 The films exhibit very low conductivity (<6 x 10(3) S m(-1)) for low particle loadi

176 ggest an opportunity to discover low thermal conductivity materials among unexplored inorganic crysta

177 Cryogenic conductivity measurements indicate intrinsic transport e

178 High pressure conductivity measurements indicate that the charge gap b

179 Here we present the first thermal conductivity measurements of aluminum at 0.5-2.7 g/cc an

180 fficient, electrical resistivity and thermal conductivity measurements were performed.

181 IR reflectivity and variable-temperature dc conductivity measurements.

182 However, the conductivity mechanisms remain in debate, particularly a

183 or liquid states and processes such as ionic conductivity, melting, and crystallization.

184 enabling new avenues for systematic thermal conductivity minimization and potentially accelerating t

185 o the limiting, comparatively low electronic conductivity, nano-structuring is a prerequisite for ach

186 However, the poor conductivity obtained through this process hindered the

187 Sharp increases in the electrical conductivity occurred at approximately 848 and 898 K fol

188 diameters ranging from 860 nm to 4.5 mum and conductivities of 30 S/cm.

189 erials that can reach the practically useful conductivities of 10(-2) S/cm at room temperature (RT).

190 The measurements of the thermal conductivities of bulk TMDs serve as an important benchm

191 Here, we report ultralow lattice thermal conductivities of solution-synthesized, single-crystalli

192 S4 , is developed with an exceptionally high conductivity of 1.46 mS cm(-1) at 25 degrees C and enhan

193 lenedioxy groups on thiophene rings) shows a conductivity of 140 S cm(-1).

194 ctivity increases dramatically and a maximum conductivity of 2.0 +/- 0.1 x 10(7) S m(-1) is achieved.

195 trical conductivity of 38.512 M.S/m, thermal conductivity of 264 W.m(-1).K(-1) and microhardness of 2

196 threaded ZIF-8 membrane exhibits high proton conductivity of 3.40 x 10(-4) S cm(-1) at 25 degrees C a

197 PQTS12 (with sulfur in side chains) shows a conductivity of 350 S cm(-1), the highest reported nonio

198 Electrical conductivity of 38.512 M.S/m, thermal conductivity of 26

199 High electrical conductivity of 94.66 IACS and low TCR of 1,451 10(-6) d

200 the effects of dehydration on the electrical conductivity of antigorite remain poorly understood.

201 Based on these results for the electrical conductivity of antigorite, we conclude that high-conduc

202 nd 29% ( approximately 88 nm) demonstrate DC conductivity of approximately 5736 and approximately 988

203 we report new measurements of the electrical conductivity of both natural and hot-pressed antigorite

204 tment that can seriously damage the electron conductivity of CNTs.

205 600 Omegasq(-1), demonstrating that the high conductivity of graphene is not lost when transferred to

206 ynamics simulations show that the electrical conductivity of liquid SiO2 is semimetallic at the condi

207 We determine the optical conductivity of LMH and find metallic hydrogen's static

208 The ability to engineer the thermal conductivity of materials allows us to control the flow

209 -pressure techniques enhanced the electrical conductivity of Mn2O3 significantly.

210 xcellent agreement with experimental thermal conductivity of nanocrystalline Si [Wang et al.

211 ic bandgap and improvement in the electrical conductivity of nanoribbon-based thin films.

212 s significant air stability, maintaining the conductivity of over 0.1 S cm(-1) in a thick film after

213 has a value close to that expected from the conductivity of physiological saline and the extracellul

214 This route overcame the common issue of low conductivity of poly(ethylene oxide)(PEO)-based solid po

215 cially, for the first time the fully tunable conductivity of ReS2x Se2(1-x) alloys from n-type to bip

216 tant benchmark for understanding the thermal conductivity of single- and few-layer TMDs.

217 Here, the thermal conductivity of single-crystalline ReS2 in a distorted 1

218 The heat conductivity of such metal-insulator-metal (MIM) nanolam

219 room temperature, thus greatly improving the conductivity of the Ag-NW films, outperforming those obt

220 nnectivity is shown to substantially enhance conductivity of the cell interior, as apparent from the

221 shows an improvement in directional thermal conductivity of the composite of up to 400% increase at

222 The low-thermal conductivity of the CuI films is attributed to a combine

223 ne and real urine as indicated by the pH and conductivity of the effluent urine.

224 ring and consequently decreasing the thermal conductivity of the lattice through the design of either

225 tation, the slice selectivity depends on the conductivity of the material, as well as on the frequenc

226 The electrical conductivity of the materials was significantly enhanced

227 ormance is attributed to the high electrical conductivity of the metallic 1T phase of MoS2 nanosheets

228 phase reversibly decreases the axial thermal conductivity of the nanotube by as much as 500%, allowin

229 Proton conductivity of the polymer electrolyte membranes in fue

230 This is due to the lower thermal conductivity of the powder relative to solid material, w

231 ile strength, Young's modulus and electrical conductivity of the PVA/GNR composite at a filling conce

232 due to FI, resulting in increased electrical conductivity of the soil solution, which led to a totall

233 chamber was observed due to the low thermal conductivity of the stainless steel components.

234 experimental data suggests that the thermal conductivity of the surface structures ultimately limits

235 Furthermore, we show that the conductivity of the surfaces as well as the response tow

236 The interlayer magnetoresistivity and Hall conductivity of this material are found to exhibit surpr

237 The ionic conductivity of this series of polyimine COFs has been c

238 hibit semiconducting properties with a redox-conductivity of up to 7.6x10(-4) S m(-1) .

239 adsorption capacity and the lowest hydraulic conductivity of Ze-LS.

240 of subsurface properties, such as hydraulic conductivities or porosities, exerts an important contro

241 for electronic systems with zero electrical conductivity or with zero electron density.

242 s, the unique facet structures, the enhanced conductivities, or even to unclear synergistic effects,

243 temperatures, tunability in the interfacial conductivity over a wide range has been demonstrated usi

244 ut dielectrophoretic cell separation in high conductivity, physiological-like fluids, overcoming the

245 Models and conductivities point to significant mobility increases i

246 As a hallmark of Weyl metals, the nonlinear conductivity provides a venue for nonlinear electronics,

247 size effect, is responsible for the thermal conductivity reduction.

248 e dominant mechanism responsible for thermal conductivity reductions below classical predictions stil

249 el wall permeability coefficients (hydraulic conductivity, reflection coefficient and diffusive solut

250 ctivity of antigorite, we conclude that high-conductivity regions associated with subduction zones ca

251 tructural stability - exceptionally high ion conductivity, rendering them most promising for sodium s

252 EDLCs scale with surface area and electrical conductivity, respectively, porous carbons such as activ

253 nanoparticles due to optimized stability and conductivity, respectively.

254 asts an extraordinary anisotropic electrical conductivity (sigma|| /sigma perpendicular ) in the orde

255 Physicochemical (zeta potential (zeta), conductivity, surface hydrophobicity (H0), protein solub

256 rials can deliver exceptionally higher ionic conductivity than typical solids or how one can design f

257 y to up to 0.62 S cm(-1) , among the highest conductivities that have been reported for solution-proc

258 pproximation is proposed to estimate thermal conductivity that compare favourably to measured data.

259 tion of membrane conductance and cytoplasmic conductivity that depends on the cycling of cytoplasmic

260 n migration led to high anode salinities and conductivity that favored their dominance.

261 Moreover, due to their high conductivity, the carbon shells and the polar Fe3 O4 cor

262 high electrical conductivity and low thermal conductivity, the screen-printed TE layers showed high r

263 for materials with these levels of pure hole conductivity; the power factor compares favorably with p

264 omaterials, allowed to enhance the electrode conductivity thus obtaining a more sensitive antigen det

265 n synchronized spatio-temporal modulation of conductivity to achieve different types of non-reciproca

266 flectivity and low absorption, but also good conductivity to allow effective electrical injection of

267 and sp(3)-hybridized carbon with sufficient conductivity to avoid ohmic potential error.

268 carbonized open wood channels, a low thermal conductivity to avoid thermal loss, and cost effectivene

269 d find metallic hydrogen's static electrical conductivity to be 11,000-15,000 S/cm, substantially hig

270 can increase the sulfur cathode's electrical conductivity to improve the battery's power capability,

271 mal analogy between diffusion and electrical conductivity to link the latter with the diffusional pro

272 ClBDPPV with 25 mol% TBAF boosts electrical conductivity to up to 0.62 S cm(-1) , among the highest

273 rustration can be exploited as a vehicle for conductivity tuning.

274 iro-ionene and polybenzimidazole reach OH(-) conductivities up to 0.12 S cm(-1) at 90 degrees C.

275 This network generates electrical conductivities up to two orders of magnitude higher than

276 LiCl@RT-COF-1 exhibits a conductivity value of 6.45 x 10(-3) S cm(-1) (at 313 K a

277 =250 ppm wt) can account for high electrical conductivity values (10(-2)-10(-1) S/m) observed in the

278 d Mg(2+)-loaded materials exhibit high ionic conductivity values of 4.4 x 10(-5), 1.8 x 10(-5), and 8

279 Accurate models require adjustment of tissue conductivity values reported in the literature, but accu

280 However, low hydraulic conductivity values reported in these sediments seemed t

281 onstrate this compound to exhibit electrical conductivity values up to sigma = 1.4(7) x 10(-2) S/cm (

282 Enhanced electrode conductivity was achieved sequentially by constructing a

283 iation in both ionic conductances and tissue conductivity was necessary to explain the experimentally

284 The thermal conductivities were in the range of 0.2-0.5 W m(-1) K(-1

285 ed LFO and a nanocarbon with high electrical conductivity were successfully synthesized for the use a

286 We observed significantly enhanced conductivities when the antigorite was heated to tempera

287 structure causes a self-enhancing effect in conductivity when employed in a 3D stretchable conductor

288 h UV light and in the neutral state, and low conductivity when treated either with visible light or a

289 The AND gate shows high conductivity when treated with UV light and in the neutr

290 tosylate) have s = 3 and thermally activated conductivity, whereas s = 1 and itinerant conductivity i

291 en in recent focus owing to their high ionic conductivities, which are believed to stem from a softer

292 nventionally coupled to very poor electrical conductivity, which has thus far prevented the use of th

293 ion devices because of their high electrical conductivity, which is promoted by the good interconnect

294 ders of magnitude increase in THz electrical conductivity, which suggests the potential for creating

295 promise for SSLiBs owing to its high Li-ion conductivity, wide potential window, and sufficient ther

296 Therefore, fracture conductivity will change dynamically during hydrocarbon

297 g of TiO2, both boosting the material n-type conductivity, with maximum power conversion efficiency r

298 xcellent mechanical integrity and electrical conductivity within a wide range of tensile and compress

299 Since Mg2 Si shows n-type conductivity without intentional carrier doping, the pre

300 n vivo biocompatibility, and high electrical conductivity without the need for additional conductive