Nowadays, the problem of environmental pollution and energy shortage caused by the burning of a large number of fossil fuels (coal, oil and gas) is becoming more and more serious. Finding an efficient, green, low-cost and sustainable energy material is the focus of energy science research now. Thermoelectric technology is able to generate a temperature gradient by collecting waste heat from factories, cars and so on and converts it into electricity through the Seebeck effect, and through the Peltier effect, it can be used for refrigeration. Thermoelectric material is the key to the thermoelectric technology. Therefore, the performance research of thermoelectric materials will play an important role in solving energy problems in the future. As a green environmental material, Bi2O3 possesses a low cost and high Seebeck coefficient of thermoelectric materials. Due to poor electrical conductivity; however, the power factor (PF) of Bi2O3 has so far been less than
河南省教育厅科学技术研究重点项目(14B430010)
河南省SnSe空心微纳球的气敏性质研究创新型科技团队(111)
河南省教育厅重点项目(14b430010)
河南省自然科学基金研究项目(162300410040)
河南省基础与前沿技术研究计划(162300410040)
国家自然科学基金(21371049)
[1] Zhou X S, Deng Y, Wei G D, et al. Study on the synthesis and properties of Sn(Pb)Te-Bi2Te3 series thermoelectric materials by solvent thermal method (in Chinese). Sci China Ser E-Tech Sci, 2003, 33: 217–221 [周西松, 邓元, 韦国丹, 等. 溶剂热法合成Sn(Pb)Te-Bi2Te3系热电材料及其性能研究. 中国科学: 技术科学, 2003, 33: 217–221]. Google Scholar
[2]
Wu
Q S,
Liu
J W,
Wang
G S, et al.
A surfactant-free route to synthesize Ba
[3]
Liu Y W, Wang X X,
[4] Li Z, Xiao C, Fan S, et al. Dual vacancies: An effective strategy realizing synergistic optimization of thermoelectric property in BiCuSeO. J Am Chem Soc, 2015, 137: 6587-6593 CrossRef PubMed Google Scholar
[5] Xie W, He J, Kang H J, et al. Identifying the specific nanostructures responsible for the high thermoelectric performance of (Bi,Sb)2Te3 Nanocomposites. Nano Lett, 2010, 10: 3283-3289 CrossRef PubMed ADS Google Scholar
[6] Boukai A I, Bunimovich Y, Tahir-Kheli J, et al. Silicon nanowires as efficient thermoelectric materials. Nature, 2008, 451: 168-171 CrossRef PubMed ADS Google Scholar
[7]
Liu
W S,
Zhang
Q,
Lan
Y, et al.
Thermoelectric property studies on Cu-doped n-type Cu
[8] Heremans J P, Thrush C M, Morelli D T, et al. Thermoelectric power of bismuth nanocomposites. Phys Rev Lett, 2002, 88: 216801 CrossRef PubMed ADS Google Scholar
[9]
Li
S,
Funahashi
R,
Matsubara
I, et al.
Synthesis and thermoelectric properties of the new oxide materials Ca3?
[10]
Soni
A,
Yanyuan
Z,
Ligen
Y, et al.
Enhanced thermoelectric properties of solution grown Bi2Te 3–
[11] Harman T C, Walsh M P, Laforge B E, et al. Nanostructured thermoelectric materials. J Elec Mater, 2005, 34: L19-L22 CrossRef ADS Google Scholar
[12] Eom J H, Jung H J, Han J H, et al. Formation of bismuth nanocrystals in Bi2O3 thin films grown at 300 K by pulsed laser deposition for thermoelectric applications. ECS J Solid State Sci Tech, 2014, 3: P315-P319 CrossRef Google Scholar
[13] Han J, Song Y, Liu X, et al. Sintering behavior and thermoelectric properties of LaCoO3 ceramics with Bi2O3-B2O3-SiO2 as a sintering aid. RSC Adv, 2014, 4: 51995-52000 CrossRef Google Scholar
[14] Wu F, Shi W, Hu X. Preparation and thermoelectric properties of flower-like nanoparticles of Ce-doped Bi2Te3. Electron Mater Lett, 2015, 11: 127-132 CrossRef ADS Google Scholar
[15]
Wu
F,
Song
H,
Jia
J, et al.
Thermoelectric properties of Ce-doped n-type Ce
[16] Tan Q, Wu C F, Sun W, et al. Solvothermally synthesized SnS nanorods with high carrier mobility leading to thermoelectric enhancement. RSC Adv, 2016, 6: 43985-43988 CrossRef Google Scholar
[17] Tarachand , Sharma V, Bhatt R, et al. A catalyst-free new polyol method synthesized hot-pressed Cu-doped Bi2S3 nanorods and their thermoelectric properties. Nano Res, 2016, 9: 3291-3304 CrossRef Google Scholar
[18] Zhang Y, Lin L X, Yan Z F, et al. Copper nanorods were prepared by low temperature MOCVD method (in Chinese). Chin Sci Bull, 2006, 51: 2309–2314 [张颖, 林梁旭, 阎子峰, 等. 低温MOCVD法制备铜纳米棒. 科学通报, 2006, 51: 2309–2314]. Google Scholar
[19] Liufu S C, Chen L D, Yao Q, et al. Assembly of one-dimensional nanorods into Bi2S3 films with enhanced thermoelectric transport properties. Appl Phys Lett, 2007, 90: 112106 CrossRef ADS Google Scholar
[20] Wan B, Hu C, Feng B, et al. Synthesis and thermoelectric properties of PbTe nanorods and microcubes. Mater Sci Eng-B, 2009, 163: 57-61 CrossRef Google Scholar
[21] Carlton C E, Kuryak C A, Liu W, et al. Disordered stoichiometric nanorods and ordered off-stoichiometric nanoparticles in n-type thermoelectric Bi2Te2.7Se0.3. J Appl Phys, 2012, 112: 093518 CrossRef ADS Google Scholar
[22] Zhou C, Li L. Electronic structures and thermoelectric properties of La or Ce-doped Bi2Te3 alloys from first principles calculations. J Phys Chem Solids, 2015, 85: 239-244 CrossRef ADS Google Scholar
[23]
Wu
F,
Song
H,
Jia
J, et al.
Effects of Ce, Y,
Figure 1
(Color online) Temperature dependence of thermal diffusion of samples on different doping concentration.
Figure 2
(Color online) Temperature dependence of density of samples on different doping concentration.
Figure 3
(Color online)
Figure 4
(Color online) XRD spectra (a) and HRXRD spectra (b) of doped Bi2O3 and undoped Bi2O3 nanorods.
Figure 5
XPS spectra of Ce-doped Bi2O3 nanorods. (a) Bi?4f; (b) Ce?3d; (c) O?1s; (d) C?1s.
Figure 6
SEM image (a)
Figure 7
HRTEM image ((a), (b)) and SAED patterns (c) of Ce-doped Bi2O3 nanorods.
Figure 8
(Color online) Temperature dependence of Seebeck coefficient of samples on different doping concentration.
Figure 9
(Color online) Resistivity spectra of samples with different doping concentration and temperature.
Figure 10
(Color online) Thermal conductivity spectra of samples with different doping concentration and temperature.
Figure 11
(Color online) Spectra of power factor of different doping concentration with temperature.
Figure 12
(Color online) ZT spectra of samples with different doping concentration and temperature.
Copyright 2019 Science China Press Co., Ltd. 科学大众杂志社有限责任公司 版权所有
京ICP备18024590号-1