2023
DOI: 10.1002/adfm.202214854
|View full text |Cite
|
Sign up to set email alerts
|

In Situ Design of High‐Performance Dual‐Phase GeSe Thermoelectrics by Tailoring Chemical Bonds

Abstract: Composite engineering favors high thermoelectric performance by tuning the carrier and phonon transport. Herein, orthorhombic and rhombohedral dualphase GeSe are designed in situ by tailoring chemical bonds. Atom probe tomography verifies the coexistence of a covalently bonded orthorhombic phase and a metavalently bonded rhombohedral phase in GeSe-InTe alloys. The production of the rhombohedral phase simultaneously increases the carrier concentration, the carrier mobility, the band degeneracy, and the density-… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

2
6
2

Year Published

2023
2023
2024
2024

Publication Types

Select...
6

Relationship

3
3

Authors

Journals

citations
Cited by 18 publications
(16 citation statements)
references
References 74 publications
2
6
2
Order By: Relevance
“…Therefore, the low 𝜈 and strong anharmonicity contribute to the low 𝜅 lat for AgBiTe 2 -alloyed samples. Compared with the 𝜅 lat in previous reports, [26][27][28]31,[53][54][55] the 𝜅 lat of 0.25 W m −1 K −1 is the lowest value for GeSe-based materials (Figure 6c). [31] Ge 0.97 Pb 0.03 Se(InTe 3/2 ) 0.15 (GeSe-InTe 3/2 ), [28] Ge 0.94 Cd 0.03 Ag 0.03 Se(InTe) 0.15 (GeSe-InTe), [55] GeSe 0.55 Te 0.45 , [30] Ge 0.96 Bi 0.04 Se(MnCdTe 2 ) 0.10 (GeSe-MnCdTe 2 ), [26] and GeSe-0.2(AgSbTe 2 ); [27] (b) the comparison of PF avg values from 323 to 773 K with previous reports, including Ge 0.94 Cd 0.03 Ag 0.03 Se(InTe) 0.15 (GeSe-InTe), [55] Ge 0.97 Pb 0.03 Se(InTe 3/2 ) 0.15 (GeSe-InTe 3/2 ), [28] GeSe 0.55 Te 0.45 , [30] and Ge 0.9 Sb 0.08 Cd 0.02 Se 0.75 Te 0.25 (Ge(SbCd)SeTe).…”
Section: Thermal Conductivitycontrasting
confidence: 60%
See 1 more Smart Citation
“…Therefore, the low 𝜈 and strong anharmonicity contribute to the low 𝜅 lat for AgBiTe 2 -alloyed samples. Compared with the 𝜅 lat in previous reports, [26][27][28]31,[53][54][55] the 𝜅 lat of 0.25 W m −1 K −1 is the lowest value for GeSe-based materials (Figure 6c). [31] Ge 0.97 Pb 0.03 Se(InTe 3/2 ) 0.15 (GeSe-InTe 3/2 ), [28] Ge 0.94 Cd 0.03 Ag 0.03 Se(InTe) 0.15 (GeSe-InTe), [55] GeSe 0.55 Te 0.45 , [30] Ge 0.96 Bi 0.04 Se(MnCdTe 2 ) 0.10 (GeSe-MnCdTe 2 ), [26] and GeSe-0.2(AgSbTe 2 ); [27] (b) the comparison of PF avg values from 323 to 773 K with previous reports, including Ge 0.94 Cd 0.03 Ag 0.03 Se(InTe) 0.15 (GeSe-InTe), [55] Ge 0.97 Pb 0.03 Se(InTe 3/2 ) 0.15 (GeSe-InTe 3/2 ), [28] GeSe 0.55 Te 0.45 , [30] and Ge 0.9 Sb 0.08 Cd 0.02 Se 0.75 Te 0.25 (Ge(SbCd)SeTe).…”
Section: Thermal Conductivitycontrasting
confidence: 60%
“…Temperature-dependent a) total thermal conductivity, 𝜅 tot ; b) lattice thermal conductivity, 𝜅 lat ; and c) comparison of the temperature-dependent 𝜅 lat for x = 0.12 sample with previous reports, including (GeSe) 0.9 (AgBiTe 2 ) 0.1 , [53] GeAg 0.2 Sb 0.2 Se 1.4 , [54] GeSe-0.2(AgSbTe 2 ), [27] Ge 0.94 Cd 0.03 Ag 0.03 Se(InTe) 0.15 (GeSe-InTe), [55] Ge 0.9 Sb 0.08 Cd 0.02 Se 0.75 Te 0.25 (Ge(SbCd)SeTe), [31] Ge 0.96 Bi 0.04 Se(MnCdTe 2 ) 0.10 (GeSe-MnCdTe 2 ), [26] and Ge 0.97 Pb 0.03 Se(InTe 3/2 ) 0.15 (GeSe-InTe 3/2 ). [28] (GeSe-InTe), [55] Ge 0.97 Pb 0.03 Se(InTe 3/2 ) 0.15 (GeSe-InTe 3/2 ), [28] GeSe 0.55 Te 0.45 , [30] and Ge 0.9 Sb 0.08 Cd 0.02 Se 0.75 Te 0.25 (Ge(SbCd)SeTe). [31] hexagonal Ge 4 Se 3 Te, the rhombohedral Ge 4 Se 3 Te, and AgBiTe 2alloyed Ge 4 Se 3 Te rhombohedral phase were calculated (Figure 8).…”
Section: Electronic Structure Dft Calculationsmentioning
confidence: 70%
“…[ 1–4 ] The performance of a TE material is usually gauged by a dimensionless figure of merit (ZT), defined as ZT=S2σT/κ${\rm{ZT}} = {S}^2\sigma T/\kappa $, where S is the Seebeck coefficient, σ is the electrical conductivity, T is the absolute temperature, and κ is the total thermal conductivity contributed by the lattice vibration κ lat and the carrier transport κ e . [ 5 ] Boosting ZT is still the leading goal for TE research, which can be realized by various strategies such as band engineering, [ 6–8 ] microstructural engineering, [ 5,9–13 ] chemical bonding engineering, [ 14–15 ] and grain boundary (GB) engineering. [ 16–18 ] Owing to the solid‐state working principle, TE technologies can be utilized for cooling DNA synthesizers, semiconductor lasers, microprocessors, and low‐wattage power generators.…”
Section: Introductionmentioning
confidence: 99%
“…In the present work, the total thermal conductivity κ tot of the CZFCTS-1 thin films was determined by TFA. The electronic thermal conductivity κ ele was calculated from the electrical transport measurements using the Wiedemann–Franz Law as (eq ) κ ele = L σ T where the Lorenz number L was estimated using eq L = ( 1.5 + exp true[ prefix− false| S false| 116 true] ) × 10 8 0.25em V 2 0.25em K 2 …”
Section: Resultsmentioning
confidence: 99%
“…In the present work, the total thermal conductivity κ tot of the CZFCTS-1 thin films was determined by TFA. The electronic thermal conductivity κ ele was calculated from the electrical transport measurements using the Wiedemann−Franz Law as (eq 2) 65 L T ele =…”
Section: Enhancement Of Thermoelectric Properties By Postdeposition A...mentioning
confidence: 99%