Thermoelectrics

Bismuth Chalcogenide Thermoelectrics

Bi2Te3-class layered chalcogenides, the only thermoelectrics in mass production. They dominate near-room-temperature Peltier cooling and energy harvesting with zT around 1.

At a glance

Class Statistics

Compounds Tracked
4,877
Multi-Source DFT
0
With Synthesis Routes
57
Avg. Agreement
0.72 / 1.00
Overview

What are Bismuth Chalcogenide Thermoelectrics?

Bismuth chalcogenides represent a class of narrow-bandgap semiconductor materials that serve as the industry standard for thermoelectric applications operating near room temperature. Chemically, these materials are typically based on bismuth telluride (Bi2Te3) and bismuth selenide (Bi2Se3), often alloyed with antimony to fine-tune their electronic properties. Their crystal structure is characterized by a rhombohedral, layered arrangement, which facilitates high electrical conductivity while simultaneously hindering the transport of phonons, thereby resulting in low thermal conductivity. This unique combination of properties is essential for achieving a high dimensionless figure of merit, known as zT, which quantifies the efficiency of thermoelectric energy conversion. Bismuth chalcogenides are currently the only thermoelectric materials that have achieved widespread commercial success, forming the backbone of Peltier cooling modules found in portable refrigerators, laser diode temperature controllers, and electronic cooling systems. Beyond cooling, they are utilized in waste-heat recovery applications where temperature gradients are relatively modest. The importance of this material class lies in its reliability and the maturity of its manufacturing processes, such as zone melting and spark plasma sintering, which allow for the production of high-performance devices. Notable members include bismuth telluride, antimony telluride, and their various solid solutions, which can be doped to create both n-type and p-type materials. Ongoing research focuses on nanostructuring and grain boundary engineering to further suppress thermal transport, aiming to push the efficiency limits of these materials for future sustainable energy technologies.

Members

Top Bismuth Chalcogenide Thermoelectrics

Ranked by data richness — literature synthesis coverage, multi-source DFT corroboration, and patent activity.

FormulaBand GapBest EAH (eV/atom)StabilityDFT SourcesRecipes
Bi2Te30.28–0.63 eV0.0000Stable17
Bi2Se30.30–1.05 eV0.0000Stable13
AgBiSe20.16–0.33 eV0.0000Stable13
BiTe0.21 eV0.0000Stable11
Sb2Te30.03–0.52 eV0.0000Stable12
Sb2Se30.28–0.91 eV0.0000Stable11
BiSb3Te60.12–0.25 eV0.0021Near hull (likely stable)—5
BiSe20.67 eV0.0211Unstable10
AgSbTe2Metallic / not reported0.0000Stable12
CuSbSe20.50–0.63 eV0.0000Stable12
Ge2Sb2Te50.02–0.43 eV0.0048Stable11
SbTe0.08–0.33 eV0.0023Stable10
AgSbSe20.87 eV0.0000Stable11
Sb2Te0.04–0.20 eV0.0027Stable10
BiSbTe30.21 eV0.0045Near hull (likely stable)—2
RbSb3Se50.88–1.34 eV0.0000Stable10
KSbSe20.98–1.62 eV0.0000Stable10
Bi4Te6Metallic / not reported—Not assessed—7
NaSbSe20.48–1.01 eV0.0000Stable10
Bi2Te2Se0.23–0.31 eV0.0000Stable11
LiSbSe20.33–0.59 eV0.0078Stable10
Bi4Te30.03–0.32 eV0.0000Stable10
K3SbSe41.22–1.68 eV0.0000Stable10
Ag1Bi1Se20.43 eV—Not assessed—3
BiSbTe20.14–0.48 eV0.0460Metastable10
BiTeI1.17–1.33 eV0.0000Stable11
GeSb4Te70.23–0.32 eV0.0006Stable10
K3SbSe32.24–2.36 eV0.0000Stable10
Na3SbSe40.99–1.09 eV0.0000Metastable10
LiSbTe20.18 eV0.0722Metastable10
BiSeMetallic / not reported0.0034Stable10
FeSbSe0.46–0.71 eV0.0000Stable10
NaSbTe20.66–0.89 eV0.0000Stable10
SbRuSe0.26–0.86 eV0.0000Stable10
Bi2TeMetallic / not reported0.0838Metastable12
Bi4CsTe60.36–0.63 eV0.0000On hull (stable)—0
Rb3SbSe32.05–2.38 eV0.0000Stable10
Bi2Pb2Se50.41–0.63 eV0.0008Stable10
Cu3SbSe30.49–0.61 eV0.0307Metastable10
K3SbTe31.63–1.94 eV0.0000Stable10
Nb3Sb2Te50.84–1.06 eV0.0000Stable10
TlBiSe20.25–1.16 eV0.0000Stable10
TlSbSe20.23–0.93 eV0.0000Stable10
SbOsSe1.05 eV0.0000Stable10
Bi2TeSe20.29–0.83 eV0.0000Stable10
FeSbTe0.34 eV0.0000Stable10
LaSbTe0.36 eV0.0000Stable10
Sb2TeSe20.30–0.65 eV0.0000Stable10
Bi2Se2S0.65–1.15 eV0.0000Stable10
Bi2Te4Pb0.29–0.62 eV0.0027Stable10
Reference

Frequently Asked Questions

How many bismuth chalcogenide thermoelectrics are in the database?

4,877 bismuth chalcogenide thermoelectrics are tracked, of which 0 have multi-source DFT validation and 57 have documented synthesis routes.

More questions
What is the most data-rich bismuth chalcogenide thermoelectric?
Bi2Te3 is the most thoroughly characterized, with 35 reported structures.
Which bismuth chalcogenide thermoelectric has the widest band gap?
Among the top compounds, Rb3SbSe3 has the widest reported DFT band gap (2.38 eV).
Why are bismuth chalcogenides preferred for room-temperature cooling?
They possess an optimal bandgap and a unique layered crystal structure that allows for high electrical conductivity while maintaining low thermal conductivity, which is the ideal combination for efficient Peltier cooling.
What is the role of alloying in these materials?
Alloying, particularly with antimony or selenium, is used to adjust the carrier concentration and optimize the band structure, which directly enhances the thermoelectric efficiency of the material.
Are bismuth chalcogenides used for high-temperature power generation?
No, they are primarily optimized for near-room-temperature applications. At higher temperatures, their performance degrades significantly due to intrinsic excitation of charge carriers across the narrow bandgap.
How is the performance of these materials improved in modern research?
Researchers utilize techniques like nanostructuring, grain boundary engineering, and the introduction of point defects to scatter phonons more effectively, thereby reducing lattice thermal conductivity without severely impacting electrical transport.
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