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Bismuth Antimony Telluride P-Type Sputtering Target, Bi₀.₅Sb₁.₅Te₃

Bismuth Antimony Telluride P-Type Sputtering Target

Introduction

The Bismuth Antimony Telluride P-Type Sputtering Target (Bi₀.₅Sb₁.₅Te₃) is a core material for thermoelectric thin films used in energy harvesting, solid-state cooling, and high-precision thermal management devices. Its P-type characteristics—achieved through controlled Sb doping—enable strong Seebeck performance and excellent compatibility with semiconductor manufacturing processes.

Detailed Description

This sputtering target is produced with a carefully engineered Bi–Sb–Te composition, offering optimized hole concentration and improved thermoelectric power factor.

  • P-type thermoelectric alloy: The substitution of Bi with Sb enhances hole mobility, providing superior P-leg performance in thin-film thermoelectric devices.

  • High-density microstructure: Fabricated through vacuum sintering, hot pressing, or HIP to ensure high densification and minimal porosity, essential for stable sputtering erosion.

  • Consistent sputtering behavior: The balanced stoichiometry minimizes Te loss during deposition, resulting in uniform film thickness and reproducible thermoelectric efficiency.

  • High purity: Available from 3N (99.9%) to 5N (99.999%) purity, supporting research-grade and production-level requirements.

The result is a target optimized for next-generation thermoelectric films where electrical performance, adhesion quality, and film reliability are essential.

Applications

  • Thin-film thermoelectric modules (P-leg materials)

  • Micro-coolers and solid-state cooling devices

  • Energy harvesting and thermal-electric generators

  • Infrared sensors and microelectronic thermal control films

  • MEMS thermoelectric components

  • Research on Bi–Sb–Te alloy systems

Technical Parameters

ParameterTypical Value / RangeImportance
Purity99.9% – 99.999%Clean films and higher thermoelectric performance
CompositionBi₀.₅Sb₁.₅Te₃ (P-type)Provides optimized hole concentration
Diameter25 – 300 mm (custom)Compatible with a wide range of sputtering systems
Thickness3 – 6 mmAffects erosion rate and target lifetime
Density≥ 95% theoreticalEnsures homogenous sputtering
BondingIndium / Elastomer / CopperImproves cooling and prevents cracking

Comparison with Related Materials

MaterialKey AdvantageTypical Application
Bi₀.₅Sb₁.₅Te₃ (P-type)High P-leg performance, stable hole mobilityThermoelectric devices
Bi₂Te₂.₇Se₀.₃ (N-type)Strong Seebeck coefficient, optimized electron concentrationComplementary N-leg films
Bi₂Te₃Economical, widely studiedGeneral thermoelectric R&D

FAQ

QuestionAnswer
Can you customize the size and purity?Yes. Diameter, thickness, purity grade, and bonding are fully customizable.
What is the standard packaging?Vacuum-sealed, foam-protected, and shipped in export-safe cartons or wooden crates.
Which systems can it be used on?Suitable for DC/RF magnetron sputtering systems used in thermoelectric and semiconductor research.
Does the stoichiometry influence film behavior?Yes. Bi/Sb/Te ratio directly affects P-type carrier concentration and Seebeck performance.
Should large targets be bonded?Yes, bonding improves heat transfer and prevents warping/cracking during sputtering.

Packaging

All Bismuth Antimony Telluride P-Type Sputtering Targets are vacuum-sealed and clearly labeled for traceability. Additional cushioning and rigid external packaging prevent chipping, oxidation, or mechanical damage during transport.

Conclusion

The Bi₀.₅Sb₁.₅Te₃ P-Type Sputtering Target provides high thermoelectric efficiency, stable film deposition behavior, and strong compatibility with advanced semiconductor processes. Available in multiple purities and customizable dimensions, it is a reliable solution for both R&D and industrial thin-film production.

For detailed specifications or a quotation, please contact us at sales@keyuematerials.com.

Order Now

BiSbTe TRG Bi₀.₅Sb₁.₅Te₃ P Type, ø76.2x3mm, Bonded to 2mm Cu B/P, 4N

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FAQ

It’s the source material (in solid form) used in sputter deposition to eject atoms or molecules that then form a thin film on a substrate.

Targets can be pure metals (e.g., gold, copper, aluminum), ceramics (e.g., Al₂O₃, SiO₂, TiO₂), alloys, or composites—chosen based on the film’s desired properties.

 

They are produced by processes such as melting/casting for metals or sintering (often with hot isostatic pressing) for ceramics and composite targets to ensure high density and purity.

 

In a vacuum chamber, a plasma (typically argon) bombards the target, ejecting atoms that travel and condense on a substrate, forming a thin film.

 

Key factors include the target’s purity, density, grain structure, and the sputtering yield (i.e. how many atoms are ejected per incident ion), as well as operating conditions like power density and gas pressure.

 

Operators monitor target erosion (often by measuring the depth of the eroded “race track”) or track total energy delivered (kilowatt-hours) until it reaches a threshold that can compromise film quality.

 

Fragile materials (such as many ceramics or certain oxides) and precious metals often require a backing plate to improve cooling, mechanical stability, and to allow thinner targets that reduce material costs.

 

DC sputtering is used for conductive targets, while RF sputtering is necessary for insulating targets (like many oxides) because it prevents charge buildup on the target’s surface.

 

In reactive sputtering, a reactive gas (e.g., oxygen or nitrogen) is introduced to form compound films on the substrate, but it may also “poison” the target surface if not carefully controlled.

 

Many manufacturers prefer to control raw material quality by sourcing their own powders; using external powders can risk impurities and inconsistent target properties.

 

Targets should be stored in clean, dry conditions (often in original packaging or re-wrapped in protective materials) and handled with gloves to avoid contamination, ensuring optimal performance during deposition.

Deposition rate depends on factors such as target material and composition, power density, working gas pressure, substrate distance, and the configuration of the sputtering system (e.g., magnetron design).

 
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