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
6,469
Multi-Source DFT
325
With Synthesis Routes
0
Avg. Agreement
0.63 / 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
Bi2Te30.34–0.46 eV0.0000On hull (stable)40
BiSe20.67 eV0.0211Near hull (likely stable)30
Sb2Se30.49–0.76 eV0.0000On hull (stable)30
Bi2Se30.38–0.96 eV0.0000On hull (stable)30
Sb2Te30.13 eV0.0000On hull (stable)40
KSbSe21.12–1.45 eV0.0000On hull (stable)50
Ge2Sb2Te50.02–0.25 eV0.0118Near hull (likely stable)40
AgSbTe2Metallic / not reported0.0214Near hull (likely stable)40
AgBiSe20.02–0.26 eV0.0040Near hull (likely stable)30
NaSbSe20.64 eV0.0000On hull (stable)30
LiSbSe20.23–0.33 eV0.0078Near hull (likely stable)30
BiSbTe20.12–0.48 eV0.0021Near hull (likely stable)30
Bi2Se40.67 eV0.0211Near hull (likely stable)20
Bi8Se120.38–0.96 eV0.0000On hull (stable)20
Bi4Se80.67 eV0.0211Near hull (likely stable)20
GeSbTe0.10 eV0.0198Near hull (likely stable)10
Rb4Sb12Se200.68–1.26 eV0.0000On hull (stable)20
TlBiSe20.23 eV0.0000On hull (stable)20
Bi4I4Se41.58 eV0.0128Near hull (likely stable)20
RbSb3Se50.68–1.26 eV0.0000On hull (stable)10
TlSbSe20.07–0.83 eV0.0000On hull (stable)20
Bi7Cs3Se120.61 eV0.0036Near hull (likely stable)10
SbTe2Metallic / not reported0.0000On hull (stable)30
Bi2Te4Pb0.17–0.49 eV0.0011Near hull (likely stable)20
Bi2TeSe20.44–0.93 eV0.0014Near hull (likely stable)20
BiSeMetallic / not reported0.0038Near hull (likely stable)20
BiTeMetallic / not reported0.0003On hull (stable)20
Sb2Te2Se0.13–0.48 eV0.0000On hull (stable)20
Sb2TeSe20.49–0.55 eV0.0000On hull (stable)20
Sb4Se8Tl40.07–0.83 eV0.0000On hull (stable)20
BaSbSe21.10 eV0.0000On hull (stable)20
Bi1Mn1Te20.49 eV0.0107Near hull (likely stable)10
Bi2Te2S0.08–0.75 eV0.0000On hull (stable)20
BiSe2Tl0.23 eV0.0000On hull (stable)20
K4Sb4Se81.12–1.45 eV0.0000On hull (stable)20
NaSbTe20.66 eV0.0000On hull (stable)20
SbOsSe1.12 eV0.0000On hull (stable)20
SbSe2Tl0.07–0.83 eV0.0000On hull (stable)20
Bi1Ge1Te20.50 eV0.0132Near hull (likely stable)10
Ge2Bi2Te50.06–0.56 eV0.0157Near hull (likely stable)20
Bi2Se2S1.17 eV0.0233Near hull (likely stable)20
Bi2Te2Se0.54 eV0.0000On hull (stable)20
Bi4Te7Pb0.42 eV0.0013Near hull (likely stable)20
Bi6Te10Pb0.32 eV0.0068Near hull (likely stable)20
BiGaSe0.16 eV0.5423Above hull20
BiKSe20.81 eV0.0543Metastable20
BiNaSe20.71–1.09 eV0.0000On hull (stable)20
BiSeBr1.69 eV0.0095Near hull (likely stable)20
BiTeCl1.51 eV0.0000On hull (stable)20
CsSbSe21.14 eV0.0000On hull (stable)20
Reference

Frequently Asked Questions

How many bismuth chalcogenide thermoelectrics are in the database?

6,469 bismuth chalcogenide thermoelectrics are tracked, of which 325 have multi-source DFT validation and 0 have documented synthesis routes.

More questions
What is the most data-rich bismuth chalcogenide thermoelectric?
Bi2Te3 is the most thoroughly characterized, with 32 reported structures.
Which bismuth chalcogenide thermoelectric has the widest band gap?
Among the top compounds, BiSeBr has the widest reported DFT band gap (1.69 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.
Explore

Related Material Classes

Screen bismuth chalcogenide thermoelectrics computationally

Evaluate stability, supply-chain risk, and patent whitespace before committing lab resources.

Explore the Platform →