ライフサイエンスコーパス: thermoelectric

1 multaneously when designing high-performance thermoelectrics.

2 nd practical importance in materials such as thermoelectrics.

3 gress has led to surging interest in organic thermoelectrics.

4 viour, such as required for high-performance thermoelectrics.

5 iconductors widely used in photovoltaics and thermoelectrics.

6 improving the efficiency of Si/Ge-based SNW thermoelectrics.

7 l conductivity, which is very attractive for thermoelectrics.

8 ductivity for various applications including thermoelectrics.

9 ations in optoelectronics, photovoltaics and thermoelectrics.

10 tors and electrodes to "smart" membranes and thermoelectrics.

11 entially low cost compared with conventional thermoelectrics.

12 oelectric, upconversion, semiconducting, and thermoelectric 1D nanocrystals, among others, as well as

13 lack-phosphorus (BP), we devise plasma-wave, thermoelectric and bolometric nano-detectors with a sele

14 the unified characterization of electrical, thermoelectric and energy dissipation characteristics of

15 hows that it originates from the coupling of thermoelectric and flexoelectric effects caused by a str

16 piezoelectric, triboelectric, flexoelectric, thermoelectric and photovoltaic effects.

17 option for use in power electronics such as thermoelectric and piezoelectric generators, as well as

18 We employ two local gates to fully tune the thermoelectric and plasmonic behaviour of the graphene.

19 c phonons, with benefits for nanoelectronic, thermoelectric and spintronic devices.

20 e/h-BN heterostructures enable us to explore thermoelectric and thermal transport on nanometer length

21 ltivalley band structure, which is ideal for thermoelectrics and also promotes the formation of Ge va

22 id-state electrolytes in batteries, improved thermoelectrics and fast-ion conductors in super-capacit

23 ving energy conversion technologies, such as thermoelectrics and photovoltaics.

24 features examples of topological insulators, thermoelectrics and piezoelectrics, but only 83 out of 4

25 uld be equally applicable for solid solution thermoelectrics and provides a strategy for improving zT

26 ntial applications in low-power electronics, thermoelectrics and spintronics.

27 step towards their deployment as electronic, thermoelectric, and phononic materials.

28 ies potentially useful for opto-electronics, thermoelectrics, and quantum computing.

29 ds promising candidates for high temperature thermoelectric applications and thus merits further expe

30 K demonstrate a new field of low-temperature thermoelectric applications unlocked by organic metals.

31 ric cooling and also high figure of merit ZT thermoelectric applications.

32 material for electronic, optoelectronic and thermoelectric applications.

33 904 microW m(-1) K(-2) at 300 K for flexible thermoelectrics, approaching the values achieved in conv

34 me resolutions down to the picosecond range, thermoelectric-based photodetectors are much more afford

35 The simpler 4-layered structure with the thermoelectric Bi2Te3 used as the absorption layer may p

36 monstrate its applicability to lightly doped thermoelectric bulk insulator PbSe.

37 This work opens up a new venue toward better thermoelectrics by harnessing nonequilibrium phonons.

38 SnSe is a robust thermoelectric candidate for energy conversion applicati

39 fabricate other porous phase-transition and thermoelectric chalcogenide materials and will pave the

40 Using laminates, we describe a thermoelectric cloak capable of hiding objects from ther

41 we observe experimentally a positive magneto-thermoelectric conductance in the Weyl semimetal niobium

42 thermal conductivities for high-performance thermoelectric conversion and thermal barrier coatings.

43 gnets, but the films' high resistance limits thermoelectric conversion efficiency.

44 Further, a thermoelectric cooler confirmed the performance with a m

45 ernally with simple, small-footprint Peltier thermoelectric coolers (TECs), and the times required fo

46 -based alloys have been intensively used for thermoelectric coolers and generators due to their high

47 Such materials have great potential for thermoelectric cooling and also high figure of merit ZT

48 Herein, a flexible thermoelectric copper selenide (Cu2 Se) thin film, consi

49 However, in thermoelectric detectors, achieving broadband or wavelen

50 nds, almost four times shorter than the same thermoelectric device covered with a conventional absorb

51 A flexible thermoelectric device fabricated using the printed films

52 ax) of heat conversion into electricity by a thermoelectric device in terms of the dimensionless figu

53 A solid-state thermoelectric device is attractive for diverse technolo

54 One prototype is the three-terminal hopping thermoelectric device where electron hopping between qua

55 Organic thermoelectric devices (OTEDs) are recognized one of the

56 thway to high-performance flexible thin film thermoelectric devices from relatively earth-abundant el

57 of durable, silent and scalable solid-state thermoelectric devices has been a long standing goal.

58 Such three-terminal hopping thermoelectric devices have potential in achieving high

59 icity and vice versa by means of solid state thermoelectric devices is extremely appealing.

60 Transverse thermoelectric devices produce electric fields perpendic

61 Thermoelectric devices that are flexible and optically t

62 such materials and the attempts to fabricate thermoelectric devices using nanoparticle-based nanopowd

63 Current thermoelectric devices, however, require energy intensiv

64 the interface points toward applications in thermoelectric devices, or the inclusion of an acoustic

65 elerating the engineering of next-generation thermoelectric devices.

66 application of molecular junctions in viable thermoelectric devices.

67 elopments of high-performance nanostructured thermoelectric devices.

68 ocessable photovoltaics, photodetectors, and thermoelectric devices.

69 photovoltaic devices and photodetectors, and thermoelectric devices.

70 rest for high-performance optoelectronic and thermoelectric devices.

71 or diverse applications such as phononic and thermoelectric devices.

72 e findings indicate that one may control the thermoelectric effect in DNA by varying its sequence and

73 Studying the thermoelectric effect in DNA is important for unravellin

74 Here we report a study of the thermoelectric effect in single DNA molecules.

75 In contrast, the thermoelectric effect is large and sensitive to the leng

76 The thermoelectric effect is small and insensitive to the mo

77 nic heat-directly into a voltage through the thermoelectric effect.

78 The defect structures were investigated by thermoelectric-effect spectroscopy (TEES), and first-pri

79 Thermoelectric effects allow the generation of electrica

80 als have already led to substantially higher thermoelectric efficiencies, further improvements are ex

81 The thermoelectric efficiency is determined by the device di

82 A transparent and flexible CuI-based thermoelectric element is demonstrated.

83 However, development of invisible thermoelectric elements is hindered by the lack of p-typ

84 tential of these materials, such as enhanced thermoelectric energy conversion and improved thermal in

85 ess the thermal conductivity and enhance the thermoelectric energy conversion efficiency.

86 and miniature sensors, the low-cost flexible thermoelectric energy harvester is highly desired as a p

87 The performance of thermoelectric energy harvesters can be improved by nano

88 ere opens up many opportunities to transform thermoelectric energy harvesting and cooling application

89 y conversion (photovoltaics, photocatalysis, thermoelectrics), energy storage (lithium-ion batteries,

90 of-the-art of this technology applied to the thermoelectric field, including the synthesis of nanopar

91 ximately 0.7 W/m.K) and a significantly high thermoelectric figure of merit (ZT = 2.1 at 630 K) in th

92 The thermoelectric figure of merit (zT), both parallel and p

93 fully densified materials and enhancement in thermoelectric figure of merit are achieved in porous bu

94 A large enhancement of the thermoelectric figure of merit is reported in single-cry

95 Accordingly, we achieve a large thermoelectric figure of merit of ZT=0.21 at 300 K for t

96 The resultant maximum thermoelectric figure of merit value reached 0.132 under

97 Although the thermoelectric figure of merit zT above 300 K has seen s

98 Here we demonstrate a thermoelectric figure of merit ZT of 2.5 at 923 K by the

99 voltage relations, the thermopower S and the thermoelectric figure of merit ZT of single-molecule dev

100 We predict that values of electronic thermoelectric figure of merit ZTe up to 160 are achieva

101 tivity as low as 0.4 Wm(-1) K(-1) and a high thermoelectric figure of merit, which can be explained b

102 a consequence, we have achieved an improved thermoelectric figure of merit, zT approximately 1, in S

103 ectronic performance is enhanced, and a high thermoelectric figure of merit, zT, of approximately 2.2

104 ductivity has impeded efforts to improve the thermoelectric figure of merit.

105 ts, providing a new way for accessing a high thermoelectric figure-of-merit in topological-insulator-

106 gh which the valleytronics can influence the thermoelectric figure-of-merit ZT is derived and discuss

107 beta-Zn8Sb7 exhibits a promising thermoelectric figure-of-merit, zT, of 0.33 at 400 K, wh

108 of the material transport properties provide thermoelectric figures of merit up to 1.7 at 850 K.

109 Thermoelectric films of several tens of microns thicknes

110 the highest values reported in all flexible thermoelectric films to date ( approximately 0.5 mW/(m K

111 lectric cloak capable of hiding objects from thermoelectric flow.

112 interference, decay, thermal diffusion, and thermoelectric generation.

113 Thermoelectric generator composed of crystalline radical

114 any other heat engine, the performance of a thermoelectric generator increases as the temperature di

115 A zigzag thermoelectric generator is built using Cu/Ag-decorated

116 ent studies have demonstrated that segmented thermoelectric generators (TEGs) can operate over large

117 In this study, segmented thermoelectric generators (TEGs) have been simulated wit

118 ffect and thus have potential application as thermoelectric generators and Peltier coolers.

119 r complementary circuitry or, as shown here, thermoelectric generators made from a single solution.

120 difficulties to synthesize high-performance thermoelectric inks and the poor density and electrical

121 ctivity is the lowest among state-of-the-art thermoelectrics; it is attributed to a previously unreco

122 btained by combining resonant absorption and thermoelectric junctions within a single suspended membr

123 umed that as more heat is forced through the thermoelectric legs, their performance increases.

124 nd to confine the heat transport through the thermoelectric legs.

125 The thermoelectric magnetic forces (TEMF) causing torque and

126 We approach thermoelectric material design using the chemical intuit

127 t properties required to create an efficient thermoelectric material necessitates a thorough understa

128 Improvements in thermoelectric material performance over the past two de

129 r identifies nanoporous silicene as an ideal thermoelectric material with the potential for unprecede

130 e of a topological insulator and a potential thermoelectric material, Bi2Se3.

131 e, which is typically anticipated for a good thermoelectric material, cannot be a general design rule

132 ere, we describe the fabrication of a p-type thermoelectric material, copper selenide (Cu2Se), utiliz

133 A new p-type thermoelectric material, CsAg5 Te3 , is presented that e

134 These results reveal that Sc3N@C80 is a bi-thermoelectric material, exhibiting both positive and ne

135 a promising n-type and extremely poor p-type thermoelectric material, the cubic analogue is calculate

136 as emerged as a promising flexible thin film thermoelectric material.

137 e and low cost process to fabricate flexible thermoelectric materials and devices demonstrated here o

138 roduction cost and low efficiency of current thermoelectric materials and devices.

139 To enhance the performance of thermoelectric materials and enable access to their wide

140 pounds are potential transparent conductors, thermoelectric materials and topological semimetals.

141 nsport in thermal nanodevices, inventing new thermoelectric materials and understanding nanoscale ene

142 Oxide thermoelectric materials are considered ideal for such a

143 which is comparable to the state-of-the-art thermoelectric materials based on binary zinc antimonide

144 Nanocrystalline thermoelectric materials based on Si have long been of i

145 High-throughput explorations of novel thermoelectric materials based on the Materials Genome I

146 designed and prepared magnetic nanocomposite thermoelectric materials consisting of BaFe12O19 nanopar

147 en widely used to assess the desirability of thermoelectric materials for devices.

148 ially broader class of resonant nanophotonic thermoelectric materials for optoelectronic applications

149 e elements have been well known as potential thermoelectric materials for the last five decades, whic

150 The broad-based implementation of thermoelectric materials in converting heat to electrici

151 trates that the performance deterioration of thermoelectric materials in the intrinsic excitation reg

152 to suppress the performance deterioration of thermoelectric materials in the intrinsic excitation reg

153 High-performance thermoelectric materials lie at the heart of thermoelect

154 ilitates complementary p- and n-type organic thermoelectric materials of high electrical conductivity

155 e attracting increasing interest as flexible thermoelectric materials owing to material abundance, ea

156 is a IV-VI semiconductor, like the excellent thermoelectric materials PbTe and SnSe.

157 cal and thermal transport properties of bulk thermoelectric materials remains a key challenge due to

158 High-performance thermoelectric materials require ultralow lattice therma

159 In its recent 60-year history, the field of thermoelectric materials research has stalled several ti

160 ape will be reshaped if the current trend in thermoelectric materials research is sustained into the

161 attice thermal conductivity of carrier-doped thermoelectric materials such as Ti-doped NbFeSb compoun

162 d in this direction, it is essential to have thermoelectric materials that are environmentally friend

163 eat, extensive efforts seek high-performance thermoelectric materials that possess large differences

164 nt an approach to synthesize n-type flexible thermoelectric materials through a facile electrochemica

165 s open a new avenue towards developing novel thermoelectric materials through crystal phase engineeri

166 e for the synthesis of high-performance bulk thermoelectric materials through dopants optimization.

167 a new avenue to adjust the S of Bi2Te3-based thermoelectric materials through flexoelectric polarizat

168 The potential of thermoelectric materials to generate electricity from th

169 ance indicator that shows how multicomponent thermoelectric materials with high entropy can be design

170 However, obtaining flexible thermoelectric materials with high figure of merit ZT th

171 ion is proposed to fabricate nanoporous bulk thermoelectric materials with well-controlled pore sizes

172 tion of material properties is promising for thermoelectric materials, it remains largely unexplored.

173 For some non-degenerate bands in thermoelectric materials, this may have profound consequ

174 to develop high-performance polycrystalline thermoelectric materials.

175 s hindered by the lack of p-type transparent thermoelectric materials.

176 on efficiency, large area, and high scalable thermoelectric materials.

177 s to produce consolidated yet nanostructured thermoelectric materials.

178 e whole set of thermoelectric properties for thermoelectric materials.

179 or are essential for production of efficient thermoelectric materials.

180 t-effective environmentally friendly organic thermoelectric materials.

181 g the highest reported ZT values in flexible thermoelectric materials.

182 tion for rational design of high performance thermoelectric materials.

183 tivity for the development of high efficient thermoelectric materials.

184 he lattice thermal conductivity (kappaL ) in thermoelectric materials.

185 is important for developing high-performance thermoelectric materials.

186 noparticles of a soft magnetic material in a thermoelectric matrix we achieve dual control of phonon-

187 Thermoelectric modules can, in principle, enhance heat r

188 However, state-of-the-art bulk thermoelectric modules have a maximum cooling flux qmax

189 ieved in thin-film Bi2Te3-based superlattice thermoelectric modules.

190 Highly bendable n-type thermoelectric nanocomposites are successfully developed

191 cursor material for Pb-doped Bi0.7 Sb1.3 Te3 thermoelectric nanocomposites.

192 een printing allows for direct conversion of thermoelectric nanocrystals into flexible energy harvest

193 Here, we show subwavelength thermoelectric nanostructures designed for resonant spec

194 Electric sector water use, in particular for thermoelectric operations, is a critical component of th

195 a full-scale computation of the whole set of thermoelectric parameters particularly attractive, while

196 vides a new avenue for an improvement of the thermoelectric performance beyond the current methods an

197 as been predicted theoretically to have good thermoelectric performance but is difficult to dope expe

198 te compounds, it is believable that the best thermoelectric performance can be achieved at a certain

199 High thermoelectric performance has been reported in single c

200 The main constraint in the way of optimizing thermoelectric performance of GeTe is the high lattice t

201 The thermoelectric performance of materials relies substanti

202 atures) is responsible for the extraordinary thermoelectric performance of n-type CoSb3 skutterudites

203 We report a significant enhancement of the thermoelectric performance of p-type SnTe over a broad t

204 ere we present the superior room-temperature thermoelectric performance of p-type transparent copper

205 Here we demonstrate that the thermoelectric performance of silicene nanoribbons can b

206 scopic length scales and thereby improve the thermoelectric performance of the resulting nanocomposit

207 bility might be used to boost electrical and thermoelectric performance over the current single-junct

208 as an effective guide to greatly improve the thermoelectric performance through either a significantl

209 te molecular levels could play a key role in thermoelectric performance, but no direct experimental e

210 dgap, and the capability to support enhanced thermoelectric performance, topological superconductivit

211 lattice thermal conductivity and improve the thermoelectric performance.

212 potentially lead to further enhancements in thermoelectric performance.

213 hich up to now have shown the most promising thermoelectric performance.

214 perties may be used in strategies to improve thermoelectric performance.

215 ombined with other approaches for optimizing thermoelectric performance.

216 tructure prevents further improvement of the thermoelectric performance.

217 group of properties required to achieve high thermoelectric performances.

218 we present transformation optics applied to thermoelectric phenomena, where thermal and electric flo

219 generating TE systems are described-a solar thermoelectric-photovoltaic hybrid system and a vehicle

220 warming will reduce the efficiency (eta) of thermoelectric plants by 0.12-0.45% for each 1 degrees C

221 Our findings suggest that thermoelectric plants, particularly closed-loop plants,

222 e rheological and mechanical properties of a thermoelectric plastic.

223 Thermoelectric plastics are a class of polymer-based mat

224 ations highlights the unique advantages that thermoelectric plastics promise to offer.

225 h regard to the four main building blocks of thermoelectric plastics: (1) organic semiconductors and

226 ( 700 S/cm) conductivities, as well as high thermoelectric power (22 muV/K) at room temperature.

227 3 meV forms, and a nearly 40% enhancement of thermoelectric power at T = 120 K is clearly observed.

228 ic transport and developing ideas to improve thermoelectric power factor are essential for production

229 processed n-type conjugated polymers, with a thermoelectric power factor of 0.63 microW m(-1) K(-2) i

230 k coefficient of 130 muV K(-1) , producing a thermoelectric power factor of 1825 muW m(-1) K(-2) .

231 This gives a thermoelectric power factor of 371 microW m(-1) K(-2) ,

232 Here, we report a significantly large thermoelectric power factor of approximately 31.4 muW/cm

233 ght and heavy bands, which results in a high thermoelectric power factor.

234 xhibit excellent electrical conductivity and thermoelectric power factors (S(2) sigma) at 550 K.

235 Thermoelectric power generation can play a key role in a

236 can be deployed to enhance the resilience of thermoelectric power generation systems.

237 ractive p-type material for high-temperature thermoelectric power generation.

238 e amounts of water, most notably for cooling thermoelectric power generators and moving hydroelectric

239 Thermoelectric power generators are used to convert heat

240 The quest for materials showing large thermoelectric power has long been one of the important

241 We show that the thermoelectric power is an extremely sensitive probe of

242 Here we report our study of the thermoelectric power of single-crystalline ZrSiS that is

243 Thermoelectric power plants demand large quantities of c

244 It also requires a lot of water for cooling thermoelectric power plants.

245 Thermoelectric power production in the United States pri

246 The resultant deposits show sensitivity to thermoelectric properties and under certain optimal cond

247 onjugated polymers that promise to show good thermoelectric properties are explored, followed by an o

248 Temperature-dependent changes of the thermoelectric properties are well-understood and correl

249 erful approach to calculate the whole set of thermoelectric properties for thermoelectric materials.

250 Herein, we investigate the thermoelectric properties of GeSe alloyed with AgSbSe2 ,

251 In this work, we measure the thermal and thermoelectric properties of large-area Si0.8Ge0.2 nano-

252 cuss the recent advances in the study of the thermoelectric properties of molecular junctions.

253 Thermoelectric properties of semiconductors are intimate

254 The thermoelectric properties of sub-stoichiometric TiO2-x d

255 We investigate the thermoelectric properties of the relatively unexplored r

256 elluride/selenide alloys exhibit exceptional thermoelectric properties that could be harnessed for po

257 riorate or ameliorate any or all of the main thermoelectric properties.

258 e spatial carrier density profiles and local thermoelectric properties.

259 tinctive electronic, spintronic, optical and thermoelectric properties.

260 theoretically predicted to exhibit superior thermoelectric properties; however a crystalline phase w

261 a small quantum oscillation frequency in the thermoelectric response and in the c-axis resistance.

262 We report a detailed study of the thermoelectric response function alphaxx of Weyl fermion

263 Here, we report the observation of enhanced thermoelectric response in polycrystalline Ca3Co4O9 on d

264 This distinct behavior in the thermoelectric response is explained by a strong deviati

265 conditions leading to a maximization of the thermoelectric response of aqueous solutions.

266 rm, Ca3Co4O9 is known to exhibit much weaker thermoelectric response than in single crystal form.

267 ect (SSE), that is, measuring the transverse thermoelectric response to a temperature gradient across

268 sed to interpret thermodiffusion (Soret) and thermoelectric (Seebeck) effects.

269 luid evaporation as well as highly sensitive thermoelectric sensing, the approach enables accurate an

270 with the robustness and linear response of a thermoelectric sensor, we present a hybrid detector for

271 minimize the lattice thermal conductivity in thermoelectrics, strategies typically focus on the scatt

272 We report the Seebeck coefficient for our thermoelectric structure to be -215 muV/K.

273 lenges and enable a successful deployment of thermoelectric systems in their wide application range,

274 mance air-stable solution-processable n-type thermoelectric (TE) conjugated polymers.

275 could offer a scalable approach to fabricate thermoelectric (TE) devices on flexible substrates for p

276 ntly reported polymer composites that show a thermoelectric (TE) effect and thus have potential appli

277 ed to traditional TEGs, comprising of single thermoelectric (TE) material.

278 ctronic- and thermal-transport properties of thermoelectric (TE) materials and are thus a central ing

279 Thermoelectric (TE) materials convert heat energy direct

280 Seeking for thermoelectric (TE) materials with high figure of merit

281 d the remaining is dissipated as waste heat, thermoelectric (TE) materials, which offer a direct and

282 The thermal stability of joints in thermoelectric (TE) modules, which are degraded during i

283 d to be the key challenge for improvement of thermoelectric (TE) performance in BiTeI.

284 Previously we showed that the thermoelectric (TE) performance of bulk n-type Bi2Te2.7S

285 s the critical Te content, presents the best thermoelectric (TE) performance with dimensionless figur

286 o decades have witnessed the rapid growth of thermoelectric (TE) research.

287 The widespread use of thermoelectric technology is constrained by a relatively

288 Thermoelectric technology, harvesting electric power dir

289 thermoelectric materials lie at the heart of thermoelectrics, the simplest technology applicable to d

290 technique and device structure to probe the thermoelectric transport across Au/h-BN/graphene heteros

291 ovide an excellent platform for studying the thermoelectric transport at these interfaces.

292 ces to stimulate studies of both thermal and thermoelectric transport in molecular junctions where th

293 omplementary tool for the study of nanoscale thermoelectric transport in two-dimensional materials.

294 We present a theory of thermoelectric transport in weakly disordered Weyl semim

295 (omega) is applied to the ITO heater and the thermoelectric voltage across the Au/h-BN/graphene heter

296 The thermoelectric voltage generated at an atomically abrupt

297 The thermoelectric voltage generated at the graphene/h-BN in

298 spatially uniform illumination to generate a thermoelectric voltage.

299 PSS that cannot support sustained current or thermoelectric voltage.

300 ge-scale fabrication of low-cost oxide based thermoelectric with potential applicability at moderate