ライフサイエンスコーパス: thermoelectric

1 itecture of fabric limits the application in thermoelectrics.

2 f great scientific interest, particularly to thermoelectrics.

3 rls distortion in phase-change materials and thermoelectrics.

4 icant attention in the field of topology and thermoelectrics.

5 ductivity for various applications including thermoelectrics.

6 multaneously when designing high-performance thermoelectrics.

7 terest for energy conversion applications in thermoelectrics.

8 nsic defects in engineering high-performance thermoelectrics.

9 undamental interest and applications such as thermoelectrics.

10 the state-of-the-art n-type Bi(2) (Te,Se)(3) thermoelectric alloys.

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

12 unctional ultra-thin-film devices for future thermoelectric and molecular-scale electronics applicati

13 ribution within conjugated polymer films for thermoelectric and other electronic applications.

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

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

16 semiconducting polymers were synthesized for thermoelectric and transistor applications via a cheap,

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

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

19 g suitable strategies for the improvement of thermoelectrics and potentially other relevant energy co

20 ormances of other types of materials such as thermoelectrics and solid electrolytes.

21 ductivity, which are essential for efficient thermoelectrics and thermal barrier coatings.

22 andidate materials in catalysis, fuel cells, thermoelectrics, and electronics, where electronic trans

23 tabilizing mixed ionic-electronic conduction thermoelectrics, and gives fresh insights into controlli

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

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

26 polymer electrolytes have been proposed for thermoelectric applications because of their giant ionic

27 polycrystalline SnSe offers a wide range of thermoelectric applications for the ease of its synthesi

28 t-emitting devices, sensors, memory devices, thermoelectric applications, and catalysis.

29 ntimony tellurides for near-room-temperature thermoelectric applications.

30 faces may be useful for quantum computing or thermoelectric applications.

31 r a wide temperature range are essential for thermoelectric applications.

32 commercial process, roll-to-roll (R2R), for thermoelectric applications.

33 ion of high-performance n-type materials for thermoelectric applications.

34 904 microW m(-1) K(-2) at 300 K for flexible thermoelectrics, approaching the values achieved in conv

35 Thermoelectrics are promising by directly generating ele

36 ribed here are true textiles, proving active thermoelectrics can be woven into various fabric archite

37 r demonstrated that MoS(2) films show p-type thermoelectric characteristics, while WS(2) is an n-type

38 /4(th)) than in previous work and subsequent thermoelectric characterization.

39 for the strong enhancement in the transverse thermoelectric coefficient, reaching a value of about 5

40 We further find that other thermoelectric coefficients, such as the thermopower and

41 oling over material volume for our optimized thermoelectric cooler is 500% higher than that of the co

42 es and thermoelectric material properties on thermoelectric cooler performance.

43 Thermoelectric coolers are attracting significant attent

44 Efficient thermoelectric coolers demonstrated here can cool the hu

45 nt air is a poor conductor of heat, wearable thermoelectric coolers operate under huge thermally resi

46 Localized cooling by wearable thermoelectric coolers will decrease the usage of tradit

47 bles the utilization of magneto-TE effect in thermoelectric cooling applications.

48 Mg(3)Bi(2)-based materials are promising for thermoelectric cooling applications.

49 However, cost partially limited wider use of thermoelectric cooling devices because of the large amou

50 of ten independently controlled 1.0 x 1.0 cm thermoelectric cooling elements (TECs) to generate dynam

51 ny (Bi-Sb) alloy is a promising material for thermoelectric cooling.

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

53 In a thermoelectric device based on the Nernst geometry, an e

54 A typical spin thermoelectric device consists of a bilayer of a magneti

55 Known technologies-such as solar cells, thermoelectric devices and mechanical generators-have sp

56 s has contributed to the creation of various thermoelectric devices and stimulated the development of

57 gical hard magnetic semimetals for low-power thermoelectric devices based on the Nernst effect and ar

58 Pt is the most commonly used metal in spin thermoelectric devices due to its strong SOC.

59 Thermoelectric devices possess enormous potential to res

60 These applications range from thermoelectric devices to high-capacity fast-charging ba

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

62 -Franz law on the efficiency of conventional thermoelectric devices.

63 d Pt can perform much better than Pt in spin thermoelectric devices.

64 elerating the engineering of next-generation thermoelectric devices.

65 tly, an emerging phenomenon, the spin-driven thermoelectric effect (STE), has garnered much attention

66 such as the piezoelectric, pyroelectric, and thermoelectric effect and electrical energy storage.

67 Here, we report studies of photo-thermoelectric effect of the topological surface states

68 Thermoelectric effect offers an alternative mechanism by

69 sion using these effects (piezo-, pyro-, and thermoelectric effect) can also be enhanced by a change

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

71 Magneto-thermoelectric effects of this Bi-Sb alloy further impro

72 Several key factors which dictate the thermoelectric efficiency and performance of various ele

73 An ideal material for thermoelectric efficiency is the phonon glass-electron c

74 isdom posits that the polymer alone dictates thermoelectric efficiency.

75 ransition that impacts thermal transport and thermoelectric efficiency.

76 (Bi(2)Te(3)) are of significant interest for thermoelectric energy conversion and as topological insu

77 ectrical conduction(1-3), light emission(4), thermoelectric energy conversion(5,6), quantum interfere

78 een widely exploited in applications such as thermoelectric energy conversion.

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

80 Here, we make the valid thermoelectric fabric woven out of thermoelectric fibers

81 the valid thermoelectric fabric woven out of thermoelectric fibers producing an unobtrusive working t

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

83 tralow lattice thermal conductivity and high thermoelectric figure of merit ( zT).

84 major contribution to the improvement in the thermoelectric figure of merit (zT > 2) of high-efficien

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

86 s, to the best of our knowledge, the highest thermoelectric figure of merit reported for solution-pro

87 re and strongly favors achievement of higher thermoelectric figure of merit value of up to 1.98.

88 mising thermoelectric materials, yet further thermoelectric figure of merit ZT improvement is largely

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

90 ntion after a theoretical prediction of high thermoelectric figure of merit, zT > 2.

91 d-temperature range (400-500 K) with maximum thermoelectric figure of merit, zT, reaching ~1.3 in p-t

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

93 ssary for on-chip integration made from high thermoelectric figure-of-merit materials have been unabl

94 or thermoelectric NWs and a summary of their thermoelectric figures of merit (ZT).

95 These SnTe-CdSe nanocomposites possess thermoelectric figures of merit of up to 1.3 at 850 K, w

96 Thermoelectric generation using the anomalous Nernst eff

97 Thermoelectric generator composed of crystalline radical

98 We demonstrated high efficient pn-junction thermoelectric generator device for waste heat recovery

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

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

101 Flexible thermoelectric generators (TEGs) can provide uninterrupt

102 Thermoelectric generators (TEGs) fabricated using additi

103 Microelectronic thermoelectric generators are one potential solution to

104 These Si-based thermoelectric generators have <1 mm(2) areas and can en

105 We present microelectronic thermoelectric generators using Si(0.97)Ge(0.03), made b

106 However, thermoelectric generators with the mm(2) footprint area

107 ocked thermoelectric modules, stretchable 3D thermoelectric generators without substrate can be made

108 designing low-cost, flexible microelectronic thermoelectric generators(11-13).

109 niature generators and coolers, and flexible thermoelectric generators).

110 edioxythiophene) has shown great promise for thermoelectric generators, however, the thick layers of

111 aics, solar thermal power systems, and solar thermoelectric generators, the ability to generate elect

112 Here, we demonstrate that the thermoelectric Hall conductivity alpha(xy) in the three-

113 , non-saturating thermopower and a quantized thermoelectric Hall conductivity approaching a universal

114 the non-saturating thermopower and quantized thermoelectric Hall effect in the topological Weyl semim

115 The thermoelectric Hall effect is the generation of a transv

116 Our work highlights the unique quantized thermoelectric Hall effect realized in a WSM toward low-

117 which is largely attributed to the quantized thermoelectric Hall effect.

118 ic devices harvesting mechanical energy, and thermoelectrics harvesting thermal energy, which now hav

119 onductivity, progress on developing them for thermoelectrics has been limited.

120 However, (sub-)room-temperature thermoelectrics have been a long-standing challenge due

121 n the synthesis of various organic-inorganic thermoelectric hybrid materials, along with the dimensio

122 fast lasers, batteries, supercapacitors, and thermoelectrics is presented by application type, includ

123 Whereas the rigid nature of standard thermoelectrics limits their use, flexible thermoelectri

124 ternal thermal resistances greatly influence thermoelectric material behavior, device design, and dev

125 No single "champion" thermoelectric material exists due to a broad range of m

126 The best known thermoelectric material for near room temperature heat-t

127 The ionic thermoelectric material is a gelatin matrix modulated wi

128 The elastic thermoelectric material is implemented in the first repo

129 of heat source/sink thermal resistances and thermoelectric material properties on thermoelectric coo

130 Successful applications of a thermoelectric material require simultaneous development

131 lvin in a flexible, quasi-solid-state, ionic thermoelectric material using synergistic thermodiffusio

132 ide family has emerged as a state-of-the-art thermoelectric material with low thermal conductivity an

133 mperature gradient between the two ends of a thermoelectric material, in order to ensure continuous e

134 ent, switching a poor nonconventional p-type thermoelectric material, tellurium, into a robust n-type

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

136 gies for the realization of high-performance thermoelectric materials and devices by establishing the

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

138 nd outlooks toward the future development of thermoelectric materials and devices.

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

140 g is crucial for developing high-performance thermoelectric materials and indicates that single-cryst

141 Oxide thermoelectric materials are considered ideal for such a

142 resents the highest value for p-type organic thermoelectric materials based on high-mobility polymers

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

144 utions) have been preferred high-performance thermoelectric materials due to their exceptional electr

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

146 The long-standing popularity of thermoelectric materials has contributed to the creation

147 Discovery of thermoelectric materials has long been realized by the E

148 Thermoelectric materials have a large Peltier effect, ma

149 Recent advances in high performance thermoelectric materials have garnered unprecedented att

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

151 challenge in the rational design of organic thermoelectric materials is to realize simultaneously hi

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

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

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

155 High-efficiency thermoelectric materials require simultaneously high pow

156 onsidered as a new candidate in the field of thermoelectric materials since the last decade owing to

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

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

159 The potential of thermoelectric materials to generate electricity from th

160 at 300 K, which is comparable to commercial thermoelectric materials used at room temperature (n-typ

161 (SnSe), a record holder of high-performance thermoelectric materials, enables high-efficient interco

162 ce in the fields of thermal barrier coating, thermoelectric materials, etc.

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

164 In high-performance thermoelectric materials, there are two main low thermal

165 BiCuSeO oxyselenides are promising thermoelectric materials, yet further thermoelectric fig

166 highest ever reported for Mg(3) Sb(2) -based thermoelectric materials.

167 ative strategy of designing high performance thermoelectric materials.

168 phonon transport properties in half-Heusler thermoelectric materials.

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

170 l properties of semiconductors, particularly thermoelectric materials.

171 the pristine GeTe and other state-of-the-art thermoelectric materials.

172 route to enhance the performance of similar thermoelectric materials.

173 the characteristics of n-type Pb(1-x)Bi(x)Se thermoelectric materials.

174 ry is critical to designing high performance thermoelectric materials.

175 s larger than that of state-of-the-art solid thermoelectric materials; and (2) the liquid electrolyte

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

177 oid volume fraction and partial alignment of thermoelectric micrograins.

178 duce electricity at night using a commercial thermoelectric module.

179 t reported intrinsically stretchable organic thermoelectric module.

180 tric fibers producing an unobtrusive working thermoelectric module.

181 Flexible thermoelectric modules are demonstrated to utilize therm

182 Assembling thermoelectric modules into fabric to harvest energy fro

183 stalline bulks), and advanced device design (thermoelectric modules, miniature generators and coolers

184 zing elasticity originating from interlocked thermoelectric modules, stretchable 3D thermoelectric ge

185 with acrylic fibers are woven into pai-type thermoelectric modules.

186 Highly bendable n-type thermoelectric nanocomposites are successfully developed

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

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

189 r factor achieved for best performing p-type thermoelectric-NFC composite film subjected to pressure

190 phenomena, followed by synthetic methods for thermoelectric NWs and a summary of their thermoelectric

191 e a comprehensive look at various aspects of thermoelectrics of NWs.

192 SnSe have created a paramount importance in thermoelectrics owing to their ultralow lattice thermal

193 ditive manufacturing of TEGs requires active thermoelectric particles to be dispersed in a polymer bi

194 fy the role of featured topological bands in thermoelectrics particularly when there are coexisting c

195 his work, the contribution of Dirac bands to thermoelectric performance and their ability to concurre

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 wing to their great potential to enhance the thermoelectric performance by utilizing the low thermal

199 phenomena and as a promising route for high thermoelectric performance for diverse applications.

200 High thermoelectric performance has been reported in single c

201 cantly reduces the kappa(L) and enhances the thermoelectric performance in rhombohedral (GeSe)(0.9)(A

202 at (GeTe)(100-x)(AgBiSe(2))(x) has promising thermoelectric performance in the mid-temperature range

203 Here, we demonstrate high thermoelectric performance in the rhombohedral crystals

204 Such an extraordinary thermoelectric performance is further verified by the he

205 ures and Fermi surfaces can directly benefit thermoelectric performance it is important to identify t

206 crystals Mg(3) (Sb,Bi)(2) can exhibit higher thermoelectric performance near room temperature by elim

207 ve molecular design strategy to optimize the thermoelectric performance of conjugated polymers, thus

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

209 While the thermoelectric performance of p-type GeTe has been impro

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

211 SnSe wire with rock-salt structure and high thermoelectric performance with diameters from micro- to

212 es effective mass, and strongly enhances the thermoelectric performance.

213 easonable strategies for optimization of the thermoelectric performance.

214 e development of strategies to improve their thermoelectric performance.

215 ombined with other approaches for optimizing thermoelectric performance.

216 tructure prevents further improvement of the thermoelectric performance.

217 ing in excellent electrical conductivity and thermoelectric performance.

218 tric to determine the optimization extent of thermoelectric performance.

219 is the priority to achieve a net increase in thermoelectric performance.

220 roperties and guides strategies towards high thermoelectric performance.

221 group of properties required to achieve high thermoelectric performances.

222 We start with a brief introduction of basic thermoelectric phenomena, followed by synthetic methods

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

224 hts on ways to control phonon propagation in thermoelectrics, photovoltaics, and other materials requ

225 d thermoelectrics limits their use, flexible thermoelectric platforms can find much broader applicati

226 owerful strategy towards rationally designed thermoelectric polymers with state-of-the-art performanc

227 ( 700 S/cm) conductivities, as well as high thermoelectric power (22 muV/K) at room temperature.

228 on charge and heat transport, which dictate thermoelectric power factor and thermal conductivity, re

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

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

231 The thermoelectric power factors of these threads are enhanc

232 tegration of NWs for device applications for thermoelectric power generation and cooling.

233 Thermoelectric power generation can play a key role in a

234 based half-Heuslers are highly promising for thermoelectric power generation.

235 Thermoelectric power plants with once-through cooling sy

236 ensity (both withdrawals and consumption) at thermoelectric power plants.

237 ng this technique, the temperature dependent thermoelectric properties (Seebeck coefficient and elect

238 Lead chalcogenides have exceptional thermoelectric properties and intriguing anharmonic latt

239 The improved thermoelectric properties can be attributed to the fine-

240 The coupling nature of thermoelectric properties determines that optimizing the

241 The thermoelectric properties for this intriguing semimetal-

242 Here, we report the thermoelectric properties of all-inorganic tin based per

243 1) K(-2) constitutes the first report of the thermoelectric properties of an intrinsically conductive

244 we develop a method to directly measure the thermoelectric properties of electrodeposited bismuth te

245 Our analysis demonstrates that the thermoelectric properties of electrodeposited films can

246 However, the measurement of the thermoelectric properties of electrodeposited films is c

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

248 Here, the first thermoelectric properties of n-type Te-doped Mg(3) Sb(2)

249 ectric (PTE) studies have suggested that the thermoelectric properties of polycrystalline metal nanow

250 For the first time, thermoelectric properties of R2R sputtered Bi(2)Te(3) fi

251 Herein, we report the thermoelectric properties of SnTe nanocomposites obtaine

252 s work, we studied the thermal transport and thermoelectric properties of the CsSnBr(3-x)I(x) perovsk

253 Fine tuning the thermoelectric properties of the films is achieved by se

254 We investigate the thermoelectric properties of the relatively unexplored r

255 This cubic n-type phase has promising thermoelectric properties with a band gap of ~0.25 eV an

256 e-crystal rock-salt SnSe fibers possess high thermoelectric properties, significantly enhancing the Z

257 with silver contents demonstrated promising thermoelectric properties, their thermal conductivity an

258 with the dimensional design for tuning their thermoelectric properties.

259 d electronic structures, resulting in n-type thermoelectric properties.

260 profound and predictable influence on their thermoelectric properties.

261 e ternary alloys on the cation vacancies and thermoelectric properties.

262 ng and frustrates the ability to control the thermoelectric properties.

263 Spin thermoelectrics represents a new paradigm of thermoelect

264 The field of thermoelectric research has undergone a renaissance and

265 puzzle of the experimentally observed finite thermoelectric response at the apparent particle-hole sy

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

267 then apply our procedure to measurements of thermoelectric response of a single quantum dot, and dem

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

269 k coefficient range of 202-230 muV K(-1) for thermoelectric semiconductors with lattice thermal condu

270 tion optimization, which is typical for most thermoelectric semiconductors.

271 A nanovolt meter connected to the thermoelectric sensor recorded the voltage change caused

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

273 utperforming other thermoelectrochemical and thermoelectric systems.

274 arly helpful in understanding and optimizing thermoelectric systems.

275 materials have attracted recent interest as thermoelectric (TE) converters due to their low cost and

276 Thermoelectric (TE) energy conversion demands high perfo

277 Phase transition in thermoelectric (TE) material is a double-edged sword-it

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

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

280 Development of high-performance organic thermoelectric (TE) materials is of vital importance for

281 Thermoelectric (TE) materials research plays a vital rol

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

283 erial with low thermal conductivity and high thermoelectric (TE) performance, however, this material

284 Thermoelectric (TE) research is not only a course of mat

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

286 ation of an electronic system, using a rapid thermoelectric technique based on infrared-induced pyroe

287 Thermoelectric technologies are becoming indispensable i

288 oltages and powers competitive with existing thermoelectric technologies, but in what should be a far

289 romising path towards low cost and versatile thermoelectric technology with easily scalable manufactu

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

291 onductive crystalline solids is important to thermoelectrics, thermal barrier coating, and more recen

292 Here we realize continuous, flexible thermoelectric threads via a rapid extrusion of 3D-print

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

294 mportant platform to investigate fundamental thermoelectric transport phenomena and as a promising ro

295 Structural, morphological and thermoelectric transport properties of MoS(2,) and WS(2)

296 Thermoelectric transport studies further demonstrated th

297 cal surface state thus has a large effect on thermoelectric transport, demonstrating great opportunit

298 power of 155 nW, thereby enhancing the photo-thermoelectric voltage by manifold compared to previous

299 spatially uniform illumination to generate a thermoelectric voltage.

300 PSS that cannot support sustained current or thermoelectric voltage.