ライフサイエンスコーパス: thermal conductivity

1 sound speeds usually exhibits higher lattice thermal conductivity.

2 oundaries contribute nearly one-third of the thermal conductivity.

3 at point defects typically lower the lattice thermal conductivity.

4 , plays the dominant role in determining the thermal conductivity.

5 so provide a path to dynamically control the thermal conductivity.

6 within the SnTe matrix, thereby reducing the thermal conductivity.

7 how a phase transition affects the measured thermal conductivity.

8 the challenges in characterizing anisotropic thermal conductivity.

9 ing, but has negligible influence on lattice thermal conductivity.

10 t causes the additional reduction of lattice thermal conductivity.

11 have been developed to establish the reduced thermal conductivity.

12 nd long-wavelength phonons thus reducing the thermal conductivity.

13 ables nanostructuring, which greatly reduces thermal conductivity.

14 led pore sizes and distributions to suppress thermal conductivity.

15 sults in the added benefit of increasing the thermal conductivity.

16 any, connection between relaxation times and thermal conductivity.

17 largely been based on decreasing the phonon thermal conductivity.

18 re found to be responsible for a low lattice thermal conductivity.

19 dimensional hyperchannels for electrical and thermal conductivity.

20 acoustic phonons to achieve the low lattice thermal conductivity.

21 of low density, ease of processing, and high thermal conductivity.

22 tes, enabled by their extremely low mass and thermal conductivity.

23 s into the microscopic origins of their high thermal conductivity.

24 re simultaneously high power factors and low thermal conductivities.

25 rmonic lattice dynamics underlying their low thermal conductivities.

26 anocrystal solids generally possess very low thermal conductivities.

27 d velocity of SnTe to give glasslike lattice thermal conductivities.

28 ion is responsible for intrinsic low lattice thermal conductivities.

29 es between high (0.35 W m(-1) K(-1)) and low thermal conductivity (0.10 W m(-1) K(-1)) states.

30 of ~ 93%), good UV-blocking ability, and low thermal conductivity (0.24 W m(-1)K(-1)) based on a proc

31 's modulus (200% increase at 9 wt% BNNT) and thermal conductivity (120% increase at 9 wt% BNNT) witho

32 , we achieve a approximately 25x increase in thermal conductivity (4.7 +/- 0.2 Wm(-1)K(-1)) over the

33 -W) that exhibits two- to threefold enhanced thermal conductivity (62 +/- 2.28 W m(-1) K(-1) for gall

34 oms in the large cages results in a very low thermal conductivity, a unique feature of the clathrate

35 In this work, we show that the local thermal conductivity along a single Si nanowire can be t

36 s an unprecedented combination of metal-like thermal conductivity, an elastic compliance similar to s

37 enhancement in the optical transparency and thermal conductivity, an exceptionally lower-level of el

38 ed porosities, effective elastic properties, thermal conductivities and permeabilities of reticulite

39 Calculated thermal conductivity and diffusivity of the different fl

40 ematic data set allows for constraining both thermal conductivity and equation-of-state models.

41 osites with enhanced mechanical strength and thermal conductivity and furthermore tunable piezoelectr

42 The combination of low thermal conductivity and good transport properties resul

43 e a suitable T(c) , coupled with anisotropic thermal conductivity and hard magnetic properties.

44 -of-the-art thermoelectric material with low thermal conductivity and high thermoelectric (TE) perfor

45 rmoelectrics owing to their ultralow lattice thermal conductivity and high thermoelectric figure of m

46 daries, has been shown to reduce the lattice thermal conductivity and improve the thermoelectric perf

47 The thermal conductivity and interface thermal conductance o

48 are responsible for the remarkable drops in thermal conductivity and large thermal resistances in ca

49 The electrolyte-gating-induced changes in thermal conductivity and lattice dimensions are reversib

50 ing Purgatorio model or Sesame S27314 for Al thermal conductivity and LEOS for Au/Al release equation

51 ations that require materials with both high thermal conductivity and low mechanical stiffness.

52 by using the temperature-dependent models of thermal conductivity and mass diffusion coefficient.

53 ermine the optimal conditions, i.e., maximum thermal conductivity and minimum nanofluid viscosity, ba

54 gly, it is found that both the through-plane thermal conductivity and the Al/TMD interface conductanc

55 d promising thermoelectric properties, their thermal conductivity and the silver content dependence r

56 eling and multiobjective optimization of the thermal conductivity and viscosity of water-based spinel

57 y a wide optical transparency window, a high thermal conductivity, and an extraordinary robustness du

58 electrical conductivity, kappa is the total thermal conductivity, and T is the absolute temperature.

59 affected by reduced mechanical dissipation, thermal conductivity, and thermal capacity.

60 ess excellent photothermal property with low thermal conductivity, and thus is an ideal candidate for

61 The thermal conductivities approach the theoretical minimum

62 hermal properties because sound velocity and thermal conductivity are linearly proportional according

63 PE)/graphene nanocomposite films with a high thermal conductivity are successfully fabricated by solu

64 This leads to a lattice thermal conductivity as low as 0.4 Wm(-1) K(-1) and a hi

65 weakly bound substructures, exhibits lattice thermal conductivity as low as ca. 0.5 W/mK near room te

66 At the same time, the small electrical and thermal conductivities at high temperatures imply that n

67 ptionally high power factors and low lattice thermal conductivities at room temperature.

68 iquid-like TE materials that exhibit lattice thermal conductivity at lower than the amorphous limit d

69 rials at bulk length-scales, engineering the thermal conductivity at micro- and nano-scale dimensions

70 Interestingly, MoS(2) films also display low thermal conductivity at room temperature and strongly fa

71 phonon transport and to derive the intrinsic thermal conductivity at the thermal equilibrium limit.

72 It was found that the calculated thermal conductivity at two temperatures, 40 and 730 deg

73 Hf2CO2 is determined to exhibit a thermal conductivity better than MoS2 and phosphorene.

74 This presents new avenues to control lattice thermal conductivity, beyond phonon scattering.

75 on, which not only significantly reduced the thermal conductivity but also mitigated a segregation ef

76 Notably, Ti2CO2 presents relatively lower thermal conductivity but much higher carrier mobility th

77 studies have shown polymers can achieve high thermal conductivity, but the transport mechanisms have

78 iffusivity is even more greatly reduced than thermal conductivity by adsorption.

79 the large phonon shifts directly affect the thermal conductivity by altering both the phonon scatter

80 20 K to 320 K, and demonstrate their tunable thermal conductivity by varying the length of alkyl chai

81 anol exhibited a significant increase in the thermal conductivity (by approximately 50%) relative to

82 Here we move beyond thermal conductivity calculations and provide a rigorous

83 The thermal conductivity can be dynamically varied by a fact

84 We find that their thermal conductivity can be tuned by atomic mass modific

85 Dependencies of thermal conductivity coefficient of coatings, MIM interf

86 Its thermal conductivity critically affects Earth's thermal

87 cs, molecular dynamics (MD) and experimental thermal conductivity data, we back-calculated the phonon

88 nlet and a valve that transfers the H2S to a thermal conductivity detector (TCD), enables a precise h

89 lution were detected by a gas chromatography-thermal conductivity detector and ion chromatography, re

90 plications yet are limited by their moderate thermal conductivity, difficulty in surface-spreading, a

91 A drastic decrease in lattice thermal conductivity down below the minimum value of the

92 ugh either a significantly depressed lattice thermal conductivity down to its theoretical minimum val

93 -type semiconductor with extraordinarily low thermal conductivity due to displacement or "rattling" o

94 standing and measuring temperature-dependent thermal conductivity during phase transitions are import

95 ransport pathways in the HSMs to lower their thermal conductivities efficiently.

96 onic devices are also discussed, such as the thermal conductivity, electric transportation, electroni

97 -SSWC provides superior vapour permeability, thermal conductivity, electrical insulation and anticorr

98 printed porous evaporator with intrinsic low thermal conductivity enables heat localization and effec

99 The recent observation of unusually high thermal conductivity exceeding 1000 W m(-1) K(-1) in sin

100 lene fibers and oriented films with uniaxial thermal conductivity exceeding 50 [Formula: see text] ha

101 phase-change materials relies on adding high thermal-conductivity fillers to improve the thermal-diff

102 eshes of the same average pitch, and reduced thermal conductivities for nanomeshes with smaller pitch

103 We measure identical (within 6% uncertainty) thermal conductivities for periodic and aperiodic nanome

104 ion between lattice dynamics and an ultralow thermal conductivity for series CsSnBr(3-x)I(x) reaching

105 We first compute the thermal conductivity for the case with aligned circular

106 and design crystalline solids with ultralow thermal conductivity for various applications including

107 d thus provides a novel strategy to engineer thermal conductivity for various applications.

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

109 e have used torque magnetization to 45 T and thermal conductivity [Formula: see text] to construct th

110 locons contribute more than 10% to the total thermal conductivity from 400 K to 800 K and they are la

111 d problem, where one can now calculate their thermal conductivity from first principles using express

112 d composite NPs into the matrix improves the thermal conductivity, from 0.205 Wm(-1)K(-1) for neat ny

113 persion of salinity and temperature, and the thermal conductivity greatly affected pore water signals

114 that the inclusion of particles with a lower thermal conductivity has a significant influence on the

115 grain boundary scattering and its effect on thermal conductivity has impeded efforts to improve the

116 Crystalline solids exhibiting glass-like thermal conductivity have attracted substantial attentio

117 Polymer composites with high thermal conductivity have recently attracted much attent

118 nt light absorbability, wood matrix with low thermal conductivity, hierarchical micro- and nanochanne

119 nI3 possesses a rare combination of ultralow thermal conductivity, high electrical conductivity (282

120 lline inorganic solids that exhibit ultralow thermal conductivity, high mechanical stability, and goo

121 t the observation of ultralow and glass-like thermal conductivity in a hexagonal perovskite chalcogen

122 The ultralow thermal conductivity in alpha-MgAgSb is attributed to it

123 h phonon-anharmonic-induced ultralow lattice thermal conductivity in alpha-MgAgSb.

124 This work shines new light on studies of thermal conductivity in fields of energy materials, micr

125 resence of adsorbates increases or decreases thermal conductivity in metal-organic frameworks (MOFs)

126 resonance confinement to the abnormal lower thermal conductivity in the MIM metamaterial with Ag lay

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

128 vity of 5.48 x 10(3) S m(-1), relatively low thermal conductivity in the range of 1.5 to 2 W m(-1) K(

129 To minimize the lattice thermal conductivity in thermoelectrics, strategies typi

130 lue of ca. 0.66(6) ps, resulting in ultralow thermal conductivity in TlInTe(2) .

131 c phonons that likely causes the low lattice thermal conductivity in TlInTe2.

132 domain thermoreflectance (FDTR), we measure thermal conductivity in two series of SACs: the unary co

133 tress at 1400 degrees C, as well as ultralow thermal conductivity in vacuum [~2.4 milliwatts per mete

134 In particular, the thermal conductivity increases significantly with proton

135 y diffraction measurements, we attribute the thermal conductivity increases to the crystal growth and

136 hed mechanisms, the unusually low electronic thermal conductivity is a signature of the absence of qu

137 The influence of micro/nanostructure on thermal conductivity is a topic of great scientific inte

138 Thermal conductivity is a very basic property that deter

139 This threefold change in the thermal conductivity is achieved by modulation of chain

140 The high thermal conductivity is attributed to the pai-pai intera

141 The measured in-plane thermal conductivity is exceptionally high, 2292 +/- 159

142 Low thermal conductivity is favorable for preserving the tem

143 The in-plane thermal conductivity is higher along the Re-chains, (70

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

145 Thermal conductivity is one of the most crucial physical

146 In the superfluid, the thermal conductivity is only weakly temperature dependen

147 The lattice thermal conductivity is the lowest among state-of-the-ar

148 e weak interlayer bonding, the through-plane thermal conductivity is the lowest observed to date for

149 The cross-plane thermal conductivity (k) of beta-W films is determined a

150 ynamics of phonon transport, which constrain thermal conductivity (k) to decrease monotonically with

151 A power law for the sample's thermal conductivity kappa = (8.7 +/- 0.3) x 10(-5) T (1

152 rent phonons and thereby reduces the lattice thermal conductivity kappa l .

153 We investigate lattice thermal conductivity kappa of MgSiO3 perovskite (pv) by

154 , we discover intrinsically ultralow lattice thermal conductivity (kappa(L)) in the single crystal of

155 and exhibits intrinsically ultralow lattice thermal conductivity (kappa(L)) of 0.62-0.4 W/mK in the

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

157 GeTe possesses significantly higher lattice thermal conductivity (kappa(latt)) compared to that of i

158 in large quantities, with high porosity, low thermal conductivity (kappa) and excellent figure of mer

159 rement of the impact of encapsulation on the thermal conductivity (kappa) and thermopower (S) of sing

160 Materials with high thermal conductivity (kappa) are of technological import

161 pon Bi4O4Cu1.7Se2.7Cl0.3: a room-temperature thermal conductivity (kappa) of 0.4(1) W/mK was measured

162 g thermal materials usually possess specific thermal conductivity (kappa), forming a digital set of k

163 r ) in the order of 10(11) , and anisotropic thermal conductivity (kappa|| /kappa perpendicular ) of

164 Many low-thermal-conductivity (kappa(L)) crystals show intriguing

165 cause a non-monotonic pressure dependence of thermal conductivity, kappa, which first increases simil

166 primary strategy for minimizing the lattice thermal conductivity (kappaL ) in thermoelectric materia

167 tric performance of GeTe is the high lattice thermal conductivity (kappalat).

168 ical conductivity, thermopower, and moderate thermal conductivities led to the optimized TE performan

169 es of 1000 K these compounds exhibit lattice thermal conductivity less than 1 W/mK.

170 work suggest an opportunity to discover low thermal conductivity materials among unexplored inorgani

171 In the pursuit of low thermal conductivity materials for thermal management, o

172 contrast to the conventional wisdom that low thermal conductivity materials should be explored in the

173 g dielectric permittivity, heat capacity and thermal conductivity measured down to 66 mK, to reveal t

174 By performing transient thermal conductivity measurements at 94 degrees C, we fi

175 arsenide single crystals have been grown and thermal conductivity measurements have verified the rela

176 Here we present the first thermal conductivity measurements of aluminum at 0.5-2.7

177 beck coefficient, electrical resistivity and thermal conductivity measurements were performed.

178 We complement our thermal-conductivity measurements with mechanical nanoin

179 moelectric materials, there are two main low thermal conductivity mechanisms: the phonon anharmonic i

180 p with an Arduino logger, a pressure sensor, thermal conductivity methane sensor, and a solenoid valv

181 unction, enabling new avenues for systematic thermal conductivity minimization and potentially accele

182 mass transfer rates, while their remarkable thermal conductivity minimizes hot spots and thermal gra

183 Here, we report the thermal conductivities of Ag(3.9)Sb(33.6)Te(62.5) and Ag

184 The measurements of the thermal conductivities of bulk TMDs serve as an importan

185 ts, the reported clathrates exhibit ultralow thermal conductivities of less than 1 W.m(-1).K(-1) at r

186 Here we directly measured thermal conductivities of solid Fe and Fe-Si alloys up t

187 Here, we report ultralow lattice thermal conductivities of solution-synthesized, single-c

188 However, the effective thermal conductivities of such mixing-based thermal meta

189 We report on the out-of-plane thermal conductivities of tetragonal L10 FePt (001) easy

190 cumented results reveals the relationship of thermal conductivities of the HSMs and the size and dens

191 unlike the varying temperature trends in the thermal conductivities of the two phases, the electronic

192 The anisotropic basal-plane thermal conductivities of thin black phosphorus obtained

193 We obtain thermal conductivities of up to 1.7 Wm(-1) K(-1) that ex

194 r thermoelectric semiconductors with lattice thermal conductivity of 0.4-1.5 W m(-1) K(-1).

195 lows from its T(c) of 450 K, together with a thermal conductivity of 20 W m(-1) K(-1) , make Rh(2) Co

196 Electrical conductivity of 38.512 M.S/m, thermal conductivity of 264 W.m(-1).K(-1) and microhardn

197 ere we report polyethylene films with a high thermal conductivity of 62 Wm(-1) K(-1), over two orders

198 are largely responsible for the increase in thermal conductivity of a-SiO2 above room temperature.

199 s, but single crystals show very low lattice thermal conductivity of about 4 W m(-1) K(-1) at room te

200 aling at 160 degrees C, the room-temperature thermal conductivity of Ag(3.9)Sb(33.6)Te(62.5) and AgSb

201 of silver contents has little impact on the thermal conductivity of Ag(3.9)Sb(33.6)Te(62.5) and lead

202 62.5) and leads to a strong reduction in the thermal conductivity of AgSbTe(2) thin films.

203 Here, we studied the ultralow-temperature thermal conductivity of an effective spin-1/2 triangular

204 hermal insulation relies on the reduction of thermal conductivity of appropriate materials that are e

205 rst-principles calculations predict that the thermal conductivity of boron arsenide is second only to

206 scattering that induces the ultralow lattice thermal conductivity of CsSnBr(3-x)I(x).

207 sure both the in-plane and the through-plane thermal conductivity of four kinds of layered TMDs (MoS2

208 The high thermal conductivity of graphene and few-layer graphene

209 present study, we take advantage of the high thermal conductivity of graphene nanomaterials to develo

210 interplay of the absorption, electrical and thermal conductivity of graphene via the device geometry

211 lize the minute electronic specific heat and thermal conductivity of graphene, we develop a supercond

212 We find that the thermal conductivity of HKUST-1 decreases by 40 - 80% de

213 Though the thermal conductivity of LFTFs was 15 times smaller than

214 t of the large polaron volume due to the low thermal conductivity of LHPs.

215 hus sought to investigate to what extent the thermal conductivity of local regions in a titanium Ti-6

216 he flammability and enhance the strength and thermal conductivity of material composites.

217 The ability to engineer the thermal conductivity of materials allows us to control t

218 obtain excellent agreement with experimental thermal conductivity of nanocrystalline Si [Wang et al.

219 The increase in the thermal conductivity of nanoMIL-101(Cr) MOHCs due to GO

220 transport, we broadly categorize the work on thermal conductivity of NWs into five different effects:

221 Thanks to the low thermal conductivity of nylon and its anisotropic therma

222 rmoelectric performance by utilizing the low thermal conductivity of organic materials and the high S

223 Due to low thermal conductivity of rock, the heat generated at the

224 an important benchmark for understanding the thermal conductivity of single- and few-layer TMDs.

225 Here, the thermal conductivity of single-crystalline ReS2 in a dis

226 Here, we numerically study the thermal conductivity of single-stranded carbon-chain pol

227 been invoked to explain the low-temperature thermal conductivity of solids for decades, our study es

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

229 The measured thermal conductivity of the amorphous silicon nanowire a

230 The out-of-plane thermal conductivity of the chemically ordered L10 phase

231 reatment shows an improvement in directional thermal conductivity of the composite of up to 400% incr

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

233 ng Fe and Pt layers is ~23% greater than the thermal conductivity of the disordered A1 phase at room

234 act of various interatomic potentials on the thermal conductivity of the heterobilayer.

235 ow ~350 nm is more favorable to decrease the thermal conductivity of the HSMs because of the possible

236 n scattering and consequently decreasing the thermal conductivity of the lattice through the design o

237 nsport within the cavity and accordingly the thermal conductivity of the LFTFs.

238 resence of bacteria in a liquid enhances the thermal conductivity of the liquid itself.

239 aqueous phase reversibly decreases the axial thermal conductivity of the nanotube by as much as 500%,

240 he finding sheds new light on enhancement of thermal conductivity of the polymeric composites which c

241 This is due to the lower thermal conductivity of the powder relative to solid mat

242 The measured thermal conductivity of the samples decreases monotonica

243 the SN2 chamber was observed due to the low thermal conductivity of the stainless steel components.

244 d on the experimental data suggests that the thermal conductivity of the surface structures ultimatel

245 n, the technique reveals local variations in thermal conductivity of this elegant natural material.

246 ence, reducing the EES; the total calculated thermal conductivity of this phase is 220 Wm(-1) K(-1) w

247 sfer point of view, it was observed that the thermal conductivity of this stable Ag-graphene/EG is si

248 Thermal conductivity of two-dimensional (2D) materials i

249 d corrected energy functional on the lattice thermal conductivity of wurtzite ZnO calculated using de

250 room temperature, we determined an in-plane thermal conductivity of ~ 1452 W/m-K for an infinite len

251 gistically give rise to the ultralow lattice thermal conductivity of ~0.18 W/mK at 873 K.

252 A record low thermal conductivity of ~1.5 W m(-1) K(-1) near 100 K wa

253 In addition, a high specific thermal conductivity of ~75 W m(-1) K(-1) rho(-1) of the

254 rriers results in a substantial reduction in thermal conductivity on a nanosecond timescale.

255 Here, an anomalous dependence of the lattice thermal conductivity on point defects is demonstrated in

256 d the amorphous region has a remarkably high thermal conductivity, over ~16 Wm(-1) K(-1).

257 This very low thermal conductivity primarily results from the weak van

258 hotovoltaic materials, but, despite ultralow thermal conductivity, progress on developing them for th

259 Mechanical and thermal conductivity properties were determined and appl

260 as confirmed by the highest elastic constant/thermal conductivity ratio, as well as the diffused wave

261 lassical size effect, is responsible for the thermal conductivity reduction.

262 ring, the dominant mechanism responsible for thermal conductivity reductions below classical predicti

263 namics leading to superionicity and ultralow thermal conductivity remain poorly understood.

264 The extraction of the true thermal conductivity requires removing the contributions

265 hich dictate thermoelectric power factor and thermal conductivity, respectively.

266 es: the stiffer the hydrogel, the higher the thermal conductivity resulting in lower photothermal hea

267 e matrix work together to reduce the lattice thermal conductivity, resulting a record high average ZT

268 at the assessment of the average single cell thermal conductivity, sample concentration, and informat

269 than previously assumed, while the inferred thermal conductivity should provide a crucial experiment

270 ls that can be switched between low and high thermal conductivity states would advance the control an

271 The anisotropic thermal-conductivity tensor of bulk black phosphorus (BP

272 medium approximation is proposed to estimate thermal conductivity that compare favourably to measured

273 mental and practical interest for their high thermal conductivity that exceeds that of many metals.

274 In the normal state we observe a diffusive thermal conductivity that is approximately temperature i

275 a band gap of ~0.25 eV and ultralow lattice thermal conductivity that ranges between 0.3 and 0.6 W/m

276 ith the high electrical conductivity and low thermal conductivity, the screen-printed TE layers showe

277 eneral design paradigm for reducing material thermal conductivities, there exists no analogous strate

278 standing is that structural defects decrease thermal conductivity through phonon scattering where the

279 xcitations and strongly suppress the lattice thermal conductivity to an ultralow value (0.46-0.31 W m

280 surface carbonized open wood channels, a low thermal conductivity to avoid thermal loss, and cost eff

281 law requires the electronic contribution to thermal conductivity to be proportional to electrical co

282 We attribute this ultralow thermal conductivity to the cluster rattling mechanism,

283 ar thermal components of absorption, such as thermal conductivity, to overcome the lack of experiment

284 multiscale microstructures, and low lattice thermal conductivity toward higher-performance TE materi

285 oelectric materials require ultralow lattice thermal conductivity typically through either shortening

286 ials have been deployed to realize effective thermal conductivities unattainable in natural materials

287 suppressed sound velocities and low lattice thermal conductivity, underscoring the need to understan

288 reases to the crystal growth and explain the thermal conductivity variations with the degree of cryst

289 the base fluid, a significant enhancement in thermal conductivity was observed.

290 The thermal conductivities were in the range of 0.2-0.5 W m(

291 envisage and develop materials with ultralow thermal conductivity, which are essential for efficient

292 Lattice defects typically reduce lattice thermal conductivity, which has been widely exploited in

293 by Sb(2) Te(3) significantly suppresses the thermal conductivity while retaining eligible carrier co

294 discontinuity of the dc conductivity and the thermal conductivity, while both the reflectivity and ab

295 rystals that exhibit the glassy trend of low thermal conductivity with a monotonic increase with temp

296 tering rate analysis, where the behaviour of thermal conductivity with dose is attributed to the accu

297 expected to produce a linear increase of the thermal conductivity with temperature that should manife

298 erfections leads to a non-monotonic trend of thermal conductivity with temperature.

299 impedance changes and evidence of increased thermal conductivity within the tissue.

300 letely accounts for the reduction in lattice thermal conductivity, without the introduction of additi