2021
DOI: 10.1016/j.scriptamat.2020.113670
|View full text |Cite
|
Sign up to set email alerts
|

High thermoelectric performance in ZnSb-SnTe pseudo-binary materials

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
5

Citation Types

0
5
0

Year Published

2022
2022
2024
2024

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 11 publications
(5 citation statements)
references
References 34 publications
0
5
0
Order By: Relevance
“…31 By adding 27.3% SnTe to (ZnSb) 72.7 , the transition temperature is lowered to 487 K, permitting an insulation-metal transition (IMT). Sn diffusion creates nanocrystallites, improving s and retaining the S, resulting in a high S 2 s of 3383 mW m −1 K −2 at 573 K. 32 At 13.3% Bi doping, Sb migration is inhibited, preventing hole formation and promoting Zn-Sb/Bi-Sb phases. This concentration signicantly improves S to −362.8 mV K −1 and an S 2 s of ∼3.5 mW m −1 K −2 at ∼793 K. 33 Due to measurement difficulty (out-of-plane direction), fabrication complexity (e.g., chemical vapor deposition, molecular beam epitaxy, and sputtering), interface degradation susceptibility, mechanical stress, uniformity and reliability over large areas, thin lm based thermoelectrics remains a challenging task in the thermoelectric community.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…31 By adding 27.3% SnTe to (ZnSb) 72.7 , the transition temperature is lowered to 487 K, permitting an insulation-metal transition (IMT). Sn diffusion creates nanocrystallites, improving s and retaining the S, resulting in a high S 2 s of 3383 mW m −1 K −2 at 573 K. 32 At 13.3% Bi doping, Sb migration is inhibited, preventing hole formation and promoting Zn-Sb/Bi-Sb phases. This concentration signicantly improves S to −362.8 mV K −1 and an S 2 s of ∼3.5 mW m −1 K −2 at ∼793 K. 33 Due to measurement difficulty (out-of-plane direction), fabrication complexity (e.g., chemical vapor deposition, molecular beam epitaxy, and sputtering), interface degradation susceptibility, mechanical stress, uniformity and reliability over large areas, thin lm based thermoelectrics remains a challenging task in the thermoelectric community.…”
Section: Introductionmentioning
confidence: 99%
“…31 By adding 27.3% SnTe to (ZnSb) 72.7 , the transition temperature is lowered to 487 K, permitting an insulation–metal transition (IMT). Sn diffusion creates nano-crystallites, improving σ and retaining the S , resulting in a high S 2 σ of 3383 μW m −1 K −2 at 573 K. 32 At 13.3% Bi doping, Sb migration is inhibited, preventing hole formation and promoting Zn–Sb/Bi–Sb phases. This concentration significantly improves S to −362.8 μV K −1 and an S 2 σ of ∼3.5 mW m −1 K −2 at ∼793 K. 33 Due to measurement difficulty (out-of-plane direction), fabrication complexity ( e.g.…”
Section: Introductionmentioning
confidence: 99%
“…In specific, when an out-of-plane ferromagnetic order is introduced into a TCI film, the quantum anomalous Hall effect (QAHE) with a tunable large Chern number can be produced, distinguished from the case in topological insulator (TI) films with a Chern number of ±1/±2. , Multiferroicity can be expected otherwise in the ferroelectric SnTe film with the introduced magnetic order, which can greatly extend its potential applications. Moreover, the Sn-based alloys are also found to have improved thermoelectric (TE) properties upon transition metal (TM) addition. Thus, much effort has been paid to introduce magnetism in SnTe films, either through magnetic doping of elements with unpaired electrons , or the magnetic proximity effect. , …”
Section: Introductionmentioning
confidence: 99%
“…12 It had been proven that the introduction of structural defects can induce the phonon scattering by defects, nano-interfaces, nanostructure, and dislocations, 12−25,32−35 which can effectively reduce the κ of ZnO. 36,37 However, despite these approaches, it is still a huge challenge to simultaneously optimize the S, σ, and κ for a high power factor (PF) (PF = σS 2 ) and a high ZT with good stability at high temperature through tunable doping.…”
Section: ■ Introductionmentioning
confidence: 99%
“…Nevertheless, ZnO thin films exhibited a much lower κ when compared to the bulk ZnO, whereby its κ value as low as 1.4 W m –1 K –1 could be achieved for sol–gel-grown ZnO thin film with a thickness of 80 nm and 1.8 W m –1 K –1 for dual Ga- and In-doped ZnO nanostructured thin films . It had been proven that the introduction of structural defects can induce the phonon scattering by defects, nano-interfaces, nanostructure, and dislocations, , which can effectively reduce the κ of ZnO. , However, despite these approaches, it is still a huge challenge to simultaneously optimize the S , σ, and κ for a high power factor (PF) (PF = σ S 2 ) and a high ZT with good stability at high temperature through tunable doping.…”
Section: Introductionmentioning
confidence: 99%