ライフサイエンスコーパス: conductivity

1 has negligible influence on lattice thermal conductivity.

2 sel elements in Populus, impacting hydraulic conductivity.

3 emiconducting polymers to improve electrical conductivity.

4 e protein, lignin, chlorophyll, and electric conductivity.

5 mobile ions, resulting in an enhanced ionic conductivity.

6 vessels, and higher leaf and xylem hydraulic conductivity.

7 s leaves and lower percent loss of hydraulic conductivity.

8 ansport, and thus severely degrade the total conductivity.

9 idual anatomical features on the root radial conductivity.

10 t of spin and charge and probed with optical conductivity.

11 ments revealed no recovery of stem hydraulic conductivity.

12 grees C or brief microwaving can improve the conductivity.

13 cellent electrochemical performance and high conductivity.

14 een experiment and theory for the electronic conductivity.

15 digested the film and changed its electrical conductivity.

16 band maximum which is beneficial for p-type conductivity.

17 verage, causing a 46% loss of stem hydraulic conductivity.

18 its high theoretical capacity and electrical conductivity.

19 ilms due to their high strength and metallic conductivity.

20 to be responsible for a low lattice thermal conductivity.

21 esulting in a negligible effect on the ionic conductivity.

22 ionic aggregation is delinked from the ionic conductivity.

23 nal hyperchannels for electrical and thermal conductivity.

24 low electronic conductivity and a high ionic conductivity.

25 bled by their extremely low mass and thermal conductivity.

26 eeds usually exhibits higher lattice thermal conductivity.

27 which result in an enhancement of the ionic conductivity.

28 al solids generally possess very low thermal conductivities.

29 ty of SnTe to give glasslike lattice thermal conductivities.

30 ll largely hampered by their poor electrical conductivities.

31 ions due to their high stabilities and ionic conductivities.

32 arge transport and ultimately the achievable conductivities.

33 ategies that have been harnessed toward high conductivities.

34 ), good UV-blocking ability, and low thermal conductivity (0.24 W m(-1)K(-1)) based on a process of s

35 ters in the ranges of human body conditions (conductivity = 0.0265 S/m - 1.027 S/m, pH = 6.6-7.4, and

36 (TCE) properties, including high electrical conductivity (~11 670 S cm(-1) ) and high work function

37 us (200% increase at 9 wt% BNNT) and thermal conductivity (120% increase at 9 wt% BNNT) without losin

38 y high sp(2) fraction, a moderate electrical conductivity (7.75 x 10(-3) S cm(-1)), and an optical ba

39 er composite electrolytes, each with a Li(+) conductivity above 10(-4) S cm(-1) at 30 degrees C.

40 -principle calculations, we link the optical conductivity above and below 0.2 eV to interband transit

41 The electrical conductivities achieved in the 3D LM composite are among

42 all COF materials, and maintain high proton conductivity across a wide relative humidity (40-100 %)

43 ikingly, the reduction of the anomalous Hall conductivity (AHC) above 90 K linearly follows the disap

44 This modulation of ionic conductivity allows for the development of light-control

45 we demonstrate that the thermoelectric Hall conductivity alpha(xy) in the three-dimensional Dirac se

46 s the potential of 2D c-COFs to display high conductivities and mobilities toward novel (opto)electro

47 ities, effective elastic properties, thermal conductivities and permeabilities of reticulite show a f

48 rategy develops 2 orders of magnitude higher conductivity and 3 orders of magnitude longer-lived shal

49 st Li, and they should have a low electronic conductivity and a high ionic conductivity.

50 c matter content, available water, hydraulic conductivity and available macronutrients, but decreased

51 The results suggested that pH, conductivity and bacterial populations of the soil sampl

52 n biomedicine because of its high electrical conductivity and biocompatibility caused by its hydrophi

53 elative phase between the modulations of the conductivity and capacity.

54 The doping effect increases perovskite dark conductivity and carrier concentration by up to 4737 tim

55 The electrical conductivity and carrier mobility of single crystals exh

56 Despite their high ionic conductivity and desirable mechanical properties, many k

57 chniques including measurements of hydraulic conductivity and dye staining during drought progression

58 (3) using the magnetic field effect (MFE) on conductivity and electroluminescence in their light emit

59 cles (PAMAM/AuNPs) were used to increase the conductivity and enhance the number of antibodies (Abs)

60 structure, and thus enhances the electronic conductivity and facilitates the adsorption/desorption o

61 sulfide electrolytes have the highest ionic conductivity and favorable interface compatibility with

62 This reduces the (photo) conductivity and finally limits the hole-transporting pr

63 ith enhanced mechanical strength and thermal conductivity and furthermore tunable piezoelectric respo

64 able T(c) , coupled with anisotropic thermal conductivity and hard magnetic properties.

65 The design of new molecules with high ionic conductivity and high electrochemical stability is a nov

66 l advantage of the combination of electrical conductivity and magnetic bistability.

67 the temperature-dependent models of thermal conductivity and mass diffusion coefficient.

68 by electrolyte selection because high ionic conductivity and poor electrochemical stability are typi

69 ids increased from 15.3 wt% to 33.8 wt%, the conductivity and relative permittivity of the inner core

70 not detect evolutionary integration between conductivity and resistance to embolism, rejecting a har

71 The high conductivity and rich catalytically active sites of MoB

72 sy carbon electrode to improve the electrode conductivity and specific surface area.

73 y, in terms of change in the soil electrical conductivity and the corresponding change in the amount

74 polymers, resulting in excellent electrical conductivity and thermoelectric performance.

75 h community structure correlated strongly to conductivity and turbidity.

76 ivaled combination of resolution, electrical conductivity, and electronic/wiring density.

77 oviscoelastic responses, energy dissipation, conductivity, and mass diffusivity also need to be consi

78 on characteristics of soil water, electrical conductivity, and nitrate.

79 ving hard inorganic matrix), nanoscale-level conductivity, and outstanding performances in distinctly

80 ed, which posesses high electrical and ionic conductivity, and physically separates Li from the elect

81 d by reduced mechanical dissipation, thermal conductivity, and thermal capacity.

82 t a pressure-induced reduction in electrical conductivity-and the presence of a complex network of pa

83 lecular dynamics simulations show these high conductivities are aided by free rotation of the NH(4) (

84 The Pedersen and Hall conductivities are constrained to at least 10(-5)-10(-4)

85 at display high strength and high electrical conductivity are critical for flexible electronics, such

86 ction and bound-charge oscillation to the ac conductivity are equivalent in a microwave circuit, the

87 roperties because sound velocity and thermal conductivity are linearly proportional according to kine

88 ency over temperature scaling of the optical conductivity as a hallmark of beyond-Landau quantum crit

89 (EA)(2) CuBr(4) (EA=ethylammonium), exhibits conductivity as high as 2x10(-3) S cm(-1) at only 2.6 GP

90 However, efforts to relate complex conductivities associated with IP to intrinsic physical

91 -1) , demonstrate increases of ~80% in their conductivities at strains of 200%, and exhibit no loss i

92 ke TE materials that exhibit lattice thermal conductivity at lower than the amorphous limit due to in

93 ingly, MoS(2) films also display low thermal conductivity at room temperature and strongly favors ach

94 miconducting behavior with a remarkably high conductivity at room temperature.

95 O, such as high strength and high electrical conductivity at the nanoscale.

96 ercolating Cu phase with enhanced electrical conductivity between the active ZnO particles and improv

97 le, ether-based electrolytes have high ionic conductivity but are oxidatively unstable above 4 V, whi

98 s structural integrity and displays enhanced conductivity by 3 orders of magnitude, which is the resu

99 % Si alloyed in Fe substantially reduces its conductivity by about 2 folds at 132 GPa and 3000 K.

100 ty is even more greatly reduced than thermal conductivity by adsorption.

101 ge phonon shifts directly affect the thermal conductivity by altering both the phonon scattering phas

102 ged, i.e., dissociated, ions) with the molar conductivity calculated from ion diffusivities measured

103 t an analog thermal material whose effective conductivity can be in-situ tuned from near-zero to near

104 nits were designed to undergo light-mediated conductivity changes.

105 antized capacitive charging, and anisotropic conductivity characteristics.

106 are promising materials with high electrical conductivity, chemical stability, and high surface area

107 But they suffer from inferior conductivity compared with metal, and limited sites main

108 e studied by scanning a capacitively coupled conductivity contactless detector (C(4)D) along the leng

109 ate and demonstrates that intermediate state conductivity contributes to the unusual versatility of K

110 Its thermal conductivity critically affects Earth's thermal structur

111 Single-crystal conductivity data are consistent with charge transport a

112 nical errors in water-quality (turbidity and conductivity) data collected by automated in situ sensor

113 are determined by crystal phases electrical conductivity, degree of exfoliation, surface functionali

114 table properties (e.g., excellent electronic conductivity, designable topologies, and defined catalyt

115 oresis with capacitively coupled contactless conductivity detection (CE-C(4)D).

116 ere detected by a gas chromatography-thermal conductivity detector and ion chromatography, respective

117 s and IL solutions is by comparing the molar conductivity determined from ionic conductivity measurem

118 Stem VCs, expressed as percent loss of conductivity, differed across genotypes, whereas root VC

119 miconductor with extraordinarily low thermal conductivity due to displacement or "rattling" of K cati

120 ut manifest unusually high, liquidlike ionic conductivities (e.g., 1 mS/cm) at temperatures as low as

121 The Fermi energy-magnetic field-Hall conductivity (E(F)-B(z)-sigma(xy)) and Fermi energy-elec

122 ma(xy)) and Fermi energy-electric field-Hall conductivity (E(F)-E(z)-sigma(xy)) phase diagrams clearl

123 in 60-100 cm soil layer, and the electrical conductivity (EC) and nitrate content gradually decrease

124 ovides superior vapour permeability, thermal conductivity, electrical insulation and anticorrosion pr

125 This light-responsive ionic conductivity enables spatiotemporal and reversible patte

126 s with uniquely designed frequency selective conductivity enabling them to overcome the properties of

127 ctively by existing methods due to their low conductivities, especially the insulating nonpolar organ

128 ith CT, allow for relatively high electrical conductivity even down to very low temperatures.

129 The discovered effect leading to the dc conductivity fall below the MIR limit can be associated

130 This device exhibits a high proton conductivity, fast response time, and extremely large on

131 or (a) and fructose, F/G ratio, proline, pH, conductivity, Fe, Cu, Al, and Mn values were found in th

132 Intrinsically low lattice thermal conductivity ([Formula: see text]) in superionic conduct

133 sities, mean ion masses and consequently the conductivities from orbit 288 to 292.

134 The results indicated that the conductivity (from polypyrrole -PPy) and catalytic activ

135 of tailored structures and properties, high conductivity, good solubility, and excellent stability.

136 -ionic liquid composite, which combines high conductivity (>140 S cm(-1)) with superior stretchabilit

137 talline solids exhibiting glass-like thermal conductivity have attracted substantial attention both f

138 organic solids that exhibit ultralow thermal conductivity, high mechanical stability, and good TE dev

139 igh optical transparency and high electrical conductivity, however, sets a stringent requirement on e

140 Strategies to enhance ionic conductivities in solid electrolytes typically focus on

141 servation of ultralow and glass-like thermal conductivity in a hexagonal perovskite chalcogenide sing

142 n pathways of LM can support high electrical conductivity in a wide range of matrix materials.

143 -anharmonic-induced ultralow lattice thermal conductivity in alpha-MgAgSb.

144 mical synthesis that lead to increased ionic conductivity in an archetypical sodium-ion conductor Na(

145 Li(+) -insulating oxides for improving Li(+) conductivity in composite polymer electrolytes owing to

146 the first time p-type and remarkable n-type conductivity in Ga(2)O(3) which should usher in the deve

147 These results demonstrate that high conductivity in layered MOFs does not necessarily requir

148 han the bulk, are mainly responsible for the conductivity in mesoporous NiO films.

149 of adsorbates increases or decreases thermal conductivity in metal-organic frameworks (MOFs) has been

150 Here the THz anomalous Hall conductivity in Mn(3)Sn thin films is investigated by po

151 and thus high on/off photoswitchable proton conductivity in the hybrid membranes and device.

152 with UV light triggers a circa 70 % drop in conductivity in the solid state that can be recovered up

153 sure, or reduction of interstitial hydraulic conductivity increase tumor growth rate and contribute t

154 e, we introduce particularly high sodium ion conductivity into the zeolitic imidazolate framework ZIF

155 Root hydraulic conductivity is a limiting factor along the water pathwa

156 The AHE conductivity is as large as that of a 3D quantum AHE, wi

157 trical conductivity measurements showed that conductivity is being controlled by ion mobility over th

158 Low thermal conductivity is favorable for preserving the temperature

159 tween the soil and the leaf, and root radial conductivity is itself defined by cell-scale hydraulic p

160 As a result, the system thermal conductivity is lowered to a greater extent than the inc

161 The electrical conductivity is observed surprisingly when the CrN layer

162 eractions with ambient contaminants, the ion conductivity is only marginally affected, decreasing wit

163 In the superfluid, the thermal conductivity is only weakly temperature dependent, requi

164 High electrical conductivity is rare in MOFs, yet it allows for diverse

165 High proton conductivity is reported for unhumidified ammonium boros

166 ller xylem conduits and higher leaf-specific conductivity (K(L) ) than conspecific controls.

167 Stem xylem-specific hydraulic conductivity (K(S) ) represents the potential for plant

168 dataset of hydraulic traits describing xylem conductivity (K(s) ), xylem resistance to embolism (P50)

169 cover intrinsically ultralow lattice thermal conductivity (kappa(L)) in the single crystal of all-ino

170 We show ultralow lattice thermal conductivity (kappa(L)) of 0.74-0.47 W/mK in the 300-723

171 ssesses significantly higher lattice thermal conductivity (kappa(latt)) compared to that of its theor

172 Materials with high thermal conductivity (kappa) are of technological importance and

173 l materials usually possess specific thermal conductivity (kappa), forming a digital set of kappa val

174 ronic devices, their insufficient electrical conductivity, low work function, and complicated electro

175 ngle-resolved photoemission spectroscopy and conductivity measurement, we found the reduction of 2DEG

176 rescence microscopy, and fine root hydraulic conductivity measurements (Lp(r) ), we examined how drou

177 Comparison with electrical conductivity measurements showed that conductivity is be

178 the molar conductivity determined from ionic conductivity measurements such as electrochemical impeda

179 membrane's combined properties of electrical conductivity, mechanical strength, optical transparency,

180 ic materials, there are two main low thermal conductivity mechanisms: the phonon anharmonic in PbTe a

181 ansfer rates, while their remarkable thermal conductivity minimizes hot spots and thermal gradients.

182 d device by demonstrating the stress-induced conductivity modulation of a perovskite oxide thin film,

183 rge-area, high-strength, and high-electrical-conductivity MXene-based films for future electronic app

184 he reduction of 2DEGs and the changes of the conductivity nature of some ferroelectric oxides includi

185 ) ligands linked by Cu nodes with electrical conductivities of 2.73 x 10(-3) to 1.04 x 10(-1) S cm(-1

186 reported clathrates exhibit ultralow thermal conductivities of less than 1 W.m(-1).K(-1) at room temp

187 he poor mechanical properties and electrical conductivities of rGO sheets are limiting factors for th

188 We present the Pedersen and Hall conductivities of the top near-equatorial dayside ionosp

189 We obtain thermal conductivities of up to 1.7 Wm(-1) K(-1) that exceed pri

190 We show that conductivities of up to 2.7 x 10(-)(4) S/cm (at 30 degre

191 that feature outstanding unstrained protonic conductivities of up to ~90 mS cm(-1) , demonstrate incr

192 electric semiconductors with lattice thermal conductivity of 0.4-1.5 W m(-1) K(-1).

193 proximately 1.68 eV, resulting in a moderate conductivity of 0.86 mS cm(-1) and a high Seebeck coeffi

194 (3) PO(4) @COFs) realize an ultrahigh proton conductivity of 1.13x10(-1) S cm(-1) , the highest among

195 al stability window, a high room-temperature conductivity of 1.5 x 10(-4) S cm(-1) , and exceptional

196 COFs show a significant room-temperature ion conductivity of 1.8 x 10(-4) S/cm and 3.5 x 10(-5) S/cm,

197 ovskites require pressures >50 GPa to show a conductivity of 10(-4) S cm(-1) , whereas here a Cu-Br c

198 ase stability, thereby achieving the highest conductivity of 2.3 x 10(-4) S cm(-1) among the three ne

199 m its T(c) of 450 K, together with a thermal conductivity of 20 W m(-1) K(-1) , make Rh(2) CoSb a can

200 an undoped material, a remarkable fast ionic conductivity of 3 mS cm(-1) and a low activation energy

201 ghout the carbon backbone, and an electrical conductivity of 6(2)x10(-4) S cm(-1) upon treatment with

202 An outer core with 15 at% Si would have a conductivity of about 20 W m(-1) K(-1), lower than pure

203 ingle crystals show very low lattice thermal conductivity of about 4 W m(-1) K(-1) at room temperatur

204 er contact surface area and super electronic conductivity of CNT-AuNP clusters, this novel designed 3

205 The conductivity of Cs(7)(H(4)PO(4))(H(2)PO(4))(8) is modera

206 This work brings the compression-induced conductivity of Cu-halide perovskites to more technologi

207 minute electronic specific heat and thermal conductivity of graphene, we develop a superconductor-gr

208 Though the thermal conductivity of LFTFs was 15 times smaller than that of

209 or Ti greatly increases electronic and ionic conductivity of Li(2) S composites and inhibits the poly

210 d ion-selective layer and thus increases the conductivity of macropores.

211 [Ca(2+)](i) transients reflect a 0.4% Ca(2+) conductivity of Na(V) channels.

212 The poor electronic conductivity of NaH is beneficial for the growth of a st

213 band gaps over 0.4 eV and of the electrical conductivity of over 4 orders of magnitude in a series o

214 ns of soil salinity (expressed as electrical conductivity of saturated soil extract) and sodicity (me

215 tunable and reversible way of modifying the conductivity of semiconductors and it is expected to hav

216 namics simulations to predict the electrical conductivity of silicate liquid at the conditions of the

217 The macroscopic electrical conductivity of solid solution MXenes can be controllabl

218 voked to explain the low-temperature thermal conductivity of solids for decades, our study establishe

219 report on the synthesis and enhanced thermal conductivity of stable Ag-decorated 2-D graphene nanocom

220 The ionic conductivity of sulfide electrolytes is comparable with

221 The measured thermal conductivity of the amorphous silicon nanowire appears l

222 The electrical conductivity of the composite containing carbon nanotube

223 Although the conductivity of the composites tends to decrease with th

224 The hydraulic conductivity of the cortex cells of roots grown hydropon

225 Alternatively, conductivity of the DBS eluate can be used for the blood

226 , thereby controlling the spatially averaged conductivity of the film device.

227 y improve the mechanical strength and Li-ion conductivity of the grain boundaries, but also form a st

228 arious interatomic potentials on the thermal conductivity of the heterobilayer.

229 ithin the cavity and accordingly the thermal conductivity of the LFTFs.

230 Single-molecule conductivity of the longest oxa[19]helicene dithiol deri

231 additional plateau-like feature in the Hall conductivity of the lowest Landau level is accompanied b

232 ver several cycles due to the low electronic conductivity of the material, illustrating the nonviabil

233 The treatment-improved electronic conductivity of the peripheral nerves increased mobility

234 e to its components (1.3 eV), and electrical conductivity of the sample was significant increased to

235 by viscosity, surface tension and electrical conductivity of the semiconductor nanosuspensions.

236 At T = 80 degrees C, the conductivity of the studied materials decreases in the o

237 g planar lipid membranes a small but defined conductivity of this channel could be demonstrated.

238 ducing the EES; the total calculated thermal conductivity of this phase is 220 Wm(-1) K(-1) with the

239 nt of view, it was observed that the thermal conductivity of this stable Ag-graphene/EG is significan

240 les facile p doping, resulting in electrical conductivity of up to 10(-2) S/cm and room-temperature p

241 roton intercalation increases the electronic conductivity of WO(3) by increasing both the carrier den

242 0 MPa for a 940 nm thick film and electrical conductivity of ~15 100 S cm(-1) for a 214 nm thick film

243 operties (Seebeck coefficient and electrical conductivity) of electrodeposited thin films have been m

244 es (water potential at 50% loss of hydraulic conductivity) of nonflooded species were significantly m

245 otential determines ion occupancy, and thus, conductivity, of the selectivity filter gate that is cou

246 see text] with large changes in its electric conductivity, optical reflectivity and density.

247 Besides, a sharp experimental optical conductivity peak at low energy, which is absent in the

248 spectrum but is consistent with the optical conductivity peaks obtained by many-body calculations wi

249 us) determined by both the traditional molar conductivity/PFG-NMR method and the rho, eta, lambda met

250 hysical/chemical sensor array for electrical conductivity, pH, and glucose concentration measurement

251 mask-free, green synthesis, good electrical conductivity, porosity, mechanical stability, and large

252 This very low thermal conductivity primarily results from the weak van der Waa

253 ena, we studied the dc transport and optical conductivity properties of nanoscaled multilayered films

254 of melanin optical, paramagnetic redox, and conductivity properties, including photoconductivity, wo

255 (3)CNT (x) MXene, with a moderate electrical conductivity, provides a higher shielding effectiveness

256 cally conductive structures, with electrical conductivities reaching 10(-5) S/cm and surface areas of

257 critical value of ~30 unit cells, a profound conductivity reduction accompanied by unexpected volume

258 impact percolation, leading to similar ionic conductivity regardless of the extent of ion aggregation

259 re, the mechanisms that underlie their ionic conductivity remain poorly understood.

260 fluence of anatomical features on the radial conductivity remains challenging due to complex time-con

261 work together to reduce the lattice thermal conductivity, resulting a record high average ZT(avg) of

262 At the same time, adjustment of the conductivity reveals a shift in the merging regimes and

263 A flexible device with an electrical conductivity sensor, a pH sensor, and a glucose sensor w

264 ion conductivity (sigma(o) ) and electronic conductivity (sigma(e) ) constitute an important family

265 nductors (MIECs) that display high oxide ion conductivity (sigma(o) ) and electronic conductivity (si

266 sistors reveals that the observed electrical conductivity (sigma(RT) <= 1.3 x 10(-2) S/cm) is enabled

267 rties of polymer solutions (type, viscosity, conductivity), solvent type, process parameters (applied

268 single-particle-calculation-derived optical conductivity spectra with the bandwidth-renormalization

269 morphology of PES23Li exhibits higher ionic conductivity than the isotropic layered or hexagonal mor

270 normal state we observe a diffusive thermal conductivity that is approximately temperature independe

271 lent in biology, and demonstrate exceptional conductivity that is enhanced by enzymatic oxidation.

272 esign paradigm for reducing material thermal conductivities, there exists no analogous strategy for h

273 ns and strongly suppress the lattice thermal conductivity to an ultralow value (0.46-0.31 W m(-1) K(-

274 in inorganic materials, imparting electrical conductivity to covalent three-dimensional organic polym

275 roperties, ranging from electrical and ionic conductivity to magnetism and ferroelectricity.

276 f in situ infrared spectroscopy and solution conductivity toward the identification of the solution s

277 o demonstrate the semiconductive-to-metallic conductivity transition, quantized capacitive charging,

278 lyoxafluoronorbornene exhibits an electrical conductivity two orders of magnitude lower than the best

279 e been deployed to realize effective thermal conductivities unattainable in natural materials.

280 als and exhibit reversible 8-fold changes in conductivity upon illumination at modest powers.

281 ly acidic ranges (6.1 +/- 0.5) and mean soil conductivity value for the north east India soils was 78

282 the increasing ceramic content the measured conductivity values are similar to those previously repo

283 rt along the linker stacking direction, with conductivity values only slightly lower than those repor

284 we utilize its characteristically higher net conductivity versus that of spore aggregates and non-via

285 The enhanced conductivity was attributed to scCO(2) preferentially di

286 A higher conductivity was measured with the as-prepared FeTHQ tha

287 fluid, a significant enhancement in thermal conductivity was observed.

288 The conductivity was switched to p-type with acceptor ioniza

289 The T(g)-normalized ionic conductivities were however unaffected by the extent of

290 aps of OMCs were varied by 0.83 eV and their conductivities were modulated by 9 orders of magnitude,

291 ype electrical conduction, both p and n-type conductivity were obtained at different cathodic potenti

292 p-type character and capability of ambipolar conductivity when properly doped, properties that are be

293 eak electric fields, they show extremely low conductivity, whereas under strong fields, they suffer f

294 together lead to anomalous quantum Hall (QH) conductivities which include a well-shape, staircase and

295 2) layers respectively with a large in-plane conductivity, which is understood by a combination of ab

296 ns, resulting in a strong reduction of ionic conductivity, while tensile strain increases the unit-ce

297 en used to estimate the corresponding radial conductivities with the hydraulic model MECHA (model of

298 that exhibit the glassy trend of low thermal conductivity with a monotonic increase with temperature

299 ials alongside the combination of electrical conductivity with porosity or spin transition offers unp

300 to produce a linear increase of the thermal conductivity with temperature that should manifest via a