Thermoelectrics

Lead Chalcogenide Thermoelectrics

PbTe and its alloys, the chemistry that powered NASA's radioisotope generators. Band convergence and hierarchical nanostructuring have pushed zT beyond 2 at mid temperatures.

At a glance

Class Statistics

Compounds Tracked
2,837
Multi-Source DFT
0
With Synthesis Routes
32
Avg. Agreement
0.75 / 1.00
Overview

What are Lead Chalcogenide Thermoelectrics?

Lead chalcogenides represent a class of narrow-bandgap semiconductor materials, primarily based on lead telluride (PbTe), lead selenide (PbSe), and lead sulfide (PbS), that have long been the gold standard for mid-to-high temperature thermoelectric energy conversion. Chemically, these materials crystallize in a rock-salt structure, characterized by high carrier mobility and a unique electronic band structure that allows for significant optimization of thermoelectric performance. Their historical significance is profound, as lead telluride was the foundational material used in radioisotope thermoelectric generators (RTGs) to power deep-space missions, including the Voyager probes and the Mars Curiosity rover, where reliability in extreme environments is paramount. In recent decades, materials scientists have revolutionized the performance of these chalcogenides through advanced engineering strategies. By employing band convergence—aligning multiple electronic valleys in the conduction or valence bands—researchers have significantly increased the power factor. Simultaneously, hierarchical nanostructuring, which involves the deliberate introduction of defects, precipitates, and grain boundaries at multiple length scales, has drastically reduced lattice thermal conductivity by scattering phonons. Together, these mechanisms have pushed the dimensionless figure of merit, zT, to levels previously thought unattainable, positioning lead chalcogenides as critical components for waste-heat recovery systems in industrial and automotive applications. Despite concerns regarding the toxicity of lead, the exceptional efficiency and long-term stability of these materials ensure they remain at the forefront of thermoelectric research, bridging the gap between fundamental solid-state physics and practical, large-scale energy harvesting solutions.

Members

Top Lead Chalcogenide Thermoelectrics

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

FormulaBand GapBest EAH (eV/atom)StabilityDFT SourcesRecipes
PbS0.13–1.82 eV0.0000Stable14
TePb0.17–1.12 eV0.0000Stable15
PbSe0.34–1.66 eV0.0000Stable12
PbTe0.10–0.81 eV0.0000On hull (stable)—5
Pb1Te10.81 eV—Not assessed—5
Pb1S10.44–0.53 eV—Not assessed—4
Pb4Te40.75 eV—Not assessed—5
PbS20.08–0.83 eV0.0000Metastable10
PbSe20.01–0.50 eV0.0395Metastable10
Bi2PbS41.08–1.18 eV0.0000Stable10
Pb4S40.38–2.05 eV—Not assessed—4
PPbS32.25–2.33 eV0.0000Stable10
Pb2S20.04–1.69 eV—Not assessed—4
Te2Pb0.41 eV0.0614Unstable10
TePb2S0.22–0.76 eV0.0366Metastable11
BaTe2Pb0.36–1.23 eV0.0442Metastable—2
Tl4Te3Pb0.17–0.25 eV0.0000Stable11
Ga2PbSe41.63–2.41 eV0.0000Stable10
Al2PbSe41.11–2.55 eV0.0000Stable10
CdPbS20.93–1.41 eV0.0762Unstable10
Bi2Pb2Se50.41–0.63 eV0.0008Stable10
Bi2Pb3S60.57–0.86 eV0.0000Stable10
Pb1Se10.40 eV—Not assessed—2
Bi2Te4Pb0.29–0.62 eV0.0027Stable10
SnTe2Pb0.36–0.49 eV0.0030Stable10
As5Pb3S100.06–0.49 eV0.0312Metastable—0
B2Pb2S51.66–1.74 eV0.0000On hull (stable)—0
Bi2Te5Pb20.03 eV0.0589Metastable10
Bi4Te7Pb0.42–0.52 eV0.0014Stable10
Bi6Te10Pb0.42–0.48 eV0.0000Stable10
GePb2S41.93–2.03 eV0.0000Stable10
PPbSe31.64–1.75 eV0.0000Stable10
SnPbS30.88–1.04 eV0.0000Stable10
GePbS31.66–1.95 eV0.0000Stable10
Ho2PbS41.97–2.28 eV0.0008Stable10
Pb5S11Sb41.38 eV0.0093Near hull (likely stable)—0
As2Pb2S51.60 eV0.0047Near hull (likely stable)—0
Bi2PbSe40.45 eV0.0000Stable10
CaPbSe20.75–0.87 eV0.0039Stable10
CdPb3Se40.63 eV0.0298Metastable10
Lu2PbS42.18–2.30 eV0.0000Stable10
Nd2PbSe41.66–1.76 eV0.0000Stable10
Pb2STe0.13–0.62 eV0.0225Near hull (likely stable)—1
As9Pb7S200.14 eV0.0288Metastable—0
Pb2S5Sb21.04 eV0.0149Near hull (likely stable)—0
PbTe3Tl40.10 eV0.1018Above hull—1
SnPbS20.14–0.97 eV0.0103Stable10
Pb2Te2Metallic / not reported—Not assessed—5
Mo6PbS8Metallic / not reported0.0157Stable12
ZrPbS30.60–1.27 eV0.0009Stable10
Reference

Frequently Asked Questions

How many lead chalcogenide thermoelectrics are in the database?

2,837 lead chalcogenide thermoelectrics are tracked, of which 0 have multi-source DFT validation and 32 have documented synthesis routes.

More questions
What is the most data-rich lead chalcogenide thermoelectric?
PbS is the most thoroughly characterized, with 165 reported structures.
Which lead chalcogenide thermoelectric has the widest band gap?
Among the top compounds, Al2PbSe4 has the widest reported DFT band gap (2.55 eV).
Why are lead chalcogenides preferred for space exploration?
They offer a unique combination of high thermoelectric efficiency and exceptional long-term structural stability, which is essential for power sources that must operate autonomously for decades in the harsh conditions of deep space.
What is the role of band convergence in these materials?
Band convergence involves engineering the electronic structure so that multiple energy valleys contribute to transport simultaneously, which significantly enhances the electrical conductivity and Seebeck coefficient without sacrificing the power factor.
How does nanostructuring improve thermoelectric performance?
Nanostructuring introduces a variety of scattering centers, such as secondary phases or grain boundaries, that effectively impede the passage of heat-carrying phonons while allowing electrons to pass through, thereby lowering the thermal conductivity.
Are there environmental concerns regarding lead chalcogenides?
Yes, because they contain lead, these materials require careful handling and recycling protocols to prevent environmental contamination, which has led to ongoing research into lead-free alternatives that mimic their favorable electronic properties.
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