2026-10-14
A reliability engineer runs an accelerated aging test on a thermoelectric module. The module uses bismuth telluride Thermoelectric Materials and solder joints. The initial output power is 5.2 watts. After 2,000 hours at 200°C, the output power drops to 3.6 watts. The engineer cross-sections the module and finds that the solder has diffused into the thermoelectric material, and the thermoelectric elements have diffused into the solder. The interface has become brittle and has developed micro-cracks. The contact resistance has increased from 10 micro-ohms to 45 micro-ohms. The solution is a diffusion barrier between the thermoelectric material and the solder. This guide explains how a diffusion barrier works and why it is essential for long-term module reliability.
Thermoelectric materials such as bismuth telluride, lead telluride, and silicon germanium are designed to operate at high temperatures. At these temperatures, the atoms in the material are mobile. When the thermoelectric material is in direct contact with a metal contact or a solder, the atoms diffuse across the interface. The diffusion creates three problems. First, it changes the composition of the thermoelectric material near the interface, which reduces its figure of merit. Second, it creates intermetallic compounds that are brittle and have high electrical resistance. Third, it creates voids that increase the contact resistance and reduce the mechanical strength. The table below shows the diffusion coefficients for common elements in bismuth telluride at 200°C.
| Diffusing element | Diffusion coefficient (cm²/s) | Diffusion distance in 2,000 hours (µm) | Effect on interface |
| Copper (from contact) | 1.2 x 10⁻¹² | 95 | High contact resistance |
| Tin (from solder) | 3.5 x 10⁻¹² | 160 | Brittle intermetallic formation |
| Nickel (from barrier) | 8.0 x 10⁻¹⁴ | 8 | Minimal diffusion |
| Bismuth (from TE material) | 2.0 x 10⁻¹² | 120 | Changes solder composition |
The diffusion distance for copper and tin is 95 to 160 microns in 2,000 hours. This is larger than the thickness of a typical thermoelectric element, which is 1 to 3 mm. The diffusion degrades the entire element. In our factory, we have measured the contact resistance of modules without a barrier after 2,000 hours. The resistance increased by 300 to 400 percent. Fuzhou X-Meritan Technology Co., Ltd. has been developing diffusion barrier solutions for Thermoelectric Materials for over 10 years.
A diffusion barrier is a thin layer of material that is placed between the thermoelectric material and the contact or solder. The barrier must have three properties. First, it must have a low diffusion coefficient for the elements on both sides. Second, it must have good electrical conductivity to minimize the contact resistance. Third, it must have good thermal stability to survive the operating temperature. The most common barrier materials are nickel, molybdenum, and titanium nitride. The table below compares the properties of these barrier materials.
| Barrier material | Diffusion coefficient for copper (cm²/s) | Electrical resistivity (µΩ·cm) | Maximum temperature | Typical thickness |
| Nickel (Ni) | 8.0 x 10⁻¹⁴ | 6.8 | 400°C | 5 – 10 µm |
| Molybdenum (Mo) | 2.0 x 10⁻¹⁵ | 5.3 | 500°C | 3 – 8 µm |
| Titanium nitride (TiN) | 1.0 x 10⁻¹⁶ | 25 | 600°C | 0.5 – 2 µm |
| Nickel-molybdenum alloy | 5.0 x 10⁻¹⁵ | 12 | 450°C | 5 – 10 µm |
Nickel is the most common barrier for bismuth telluride modules because it has a low diffusion coefficient, good electrical conductivity, and is easy to deposit by electroplating. Molybdenum has a lower diffusion coefficient but is more expensive and harder to deposit. Titanium nitride has the lowest diffusion coefficient but the highest resistivity. In our factory, we use a nickel barrier with a thickness of 8 microns for bismuth telluride modules. The barrier is deposited by electroplating on the thermoelectric element before soldering. X-Meritan has validated this process through 5,000 hours of accelerated aging tests.
The thickness of the diffusion barrier affects both the contact resistance and the reliability. A thicker barrier reduces the diffusion rate but increases the electrical resistance. A thinner barrier has lower resistance but may not prevent diffusion for the required life. The optimal thickness is the one that provides the required life with the lowest resistance. The table below shows the effect of nickel barrier thickness on contact resistance and life.
| Nickel barrier thickness (µm) | Initial contact resistance (µΩ·cm²) | Contact resistance after 2,000 hours (µΩ·cm²) | Predicted life (hours) |
| 2 | 8 | 45 | 1,500 |
| 5 | 12 | 22 | 4,000 |
| 8 | 18 | 24 | 8,000 |
| 12 | 28 | 32 | 12,000 |
| 20 | 45 | 48 | 15,000 |
Design trade-off: The optimal barrier thickness for a bismuth telluride module operating at 200°C for 8,000 hours is 8 microns. This provides a contact resistance of 18 µΩ·cm² initially and 24 µΩ·cm² after 2,000 hours. A thinner barrier (5 microns) has lower initial resistance but fails faster. A thicker barrier (12 microns) has a longer life but higher resistance, which reduces the module efficiency. In our factory, we select the barrier thickness based on the operating temperature and the required life.
A diffusion barrier can fail in three ways. The first is barrier consumption. The barrier reacts with the thermoelectric material or the solder and is gradually consumed. When the barrier is fully consumed, the diffusion is no longer prevented. The second is barrier cracking. The barrier can crack due to thermal expansion mismatch or mechanical stress. The cracks provide a path for diffusion. The third is barrier delamination. The barrier can delaminate from the thermoelectric material or the solder, which creates a high-resistance interface. The table below shows the failure modes and their causes.
| Failure mode | Cause | Detection method | Mitigation |
| Barrier consumption | Reaction with solder or TE material | Cross-section; EDX analysis | Increase barrier thickness |
| Barrier cracking | Thermal expansion mismatch | SEM inspection; acoustic microscopy | Use compliant barrier; reduce thermal cycling |
| Barrier delamination | Poor adhesion; contamination | Acoustic microscopy; pull test | Improve surface preparation; use adhesion layer |
In our factory, we have analyzed failed thermoelectric modules from field returns. The most common failure mode was barrier consumption at the hot side of the module. The barrier was 5 microns thick and was consumed after 3,000 hours. The contact resistance increased from 15 to 60 µΩ·cm². Based on this analysis, we increased the barrier thickness to 8 microns for high-temperature applications. Fuzhou X-Meritan Technology Co., Ltd. provides a barrier thickness recommendation for each application based on the operating temperature and the required life.
A diffusion barrier is essential for the long-term reliability of thermoelectric modules. Without a barrier, the elements in the thermoelectric material and the solder diffuse across the interface, which increases the contact resistance and degrades the module performance. The barrier must have a low diffusion coefficient, good electrical conductivity, and high thermal stability. The optimal barrier thickness depends on the operating temperature and the required life. Nickel is suitable for bismuth telluride modules, while molybdenum is better for lead telluride modules. By selecting the right barrier material and thickness, module designers can extend the life of thermoelectric modules from 1,500 hours to 8,000 hours or more. Fuzhou X-Meritan Technology Co., Ltd. has been developing diffusion barrier solutions for Thermoelectric Materials for over 10 years and provides full reliability testing support.
Fuzhou X-Meritan Technology Co., Ltd. manufactures Thermoelectric Materials with nickel, molybdenum, and titanium nitride diffusion barriers. We provide barrier thickness recommendations, accelerated aging test data, and SEM/EDX analysis for all of our products.