Thermal stress modelling of diamond on GaN/III-Nitride membranes
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2020-11-27 |
| Journal | Carbon |
| Authors | Jerome A. Cuenca, Matthew D. Smith, D. Field, Fabien Massabuau, Soumen Mandal |
| Institutions | University of Strathclyde, University of Glasgow |
| Citations | 43 |
| Analysis | Full AI Review Included |
Executive Summary
Section titled âExecutive SummaryâThis study investigates the thermal stress and deformation (bow) induced when integrating polycrystalline CVD diamond directly onto GaN/III-N membranes, proposing a bonding-free heat spreading solution for high-power electronics.
- Core Challenge Identified: High-temperature CVD growth combined with the Coefficient of Thermal Expansion (CTE) mismatch between GaN/III-N, Si, and diamond induces significant thermal stresses and large membrane bow upon cooling.
- Modeling Accuracy: Simplified analytical (Stoney) models proved inadequate, underestimating the bow by a factor of 3-4, demonstrating the critical need for Finite Element Modeling (FEM) that accounts for the stresses originating from the surrounding Si frame border.
- Stress Validation: Experimental Raman spectroscopy confirmed that the residual tensile stress in the GaN layers of small membranes (0.5 mm and 2 mm) was approximately 1.0 ±0.2 GPa, which is safely below the GaN tensile strength limit (4 to 7.5 GPa).
- Deformation Limit: Membrane bow was measured up to 58 ”m for the 5 mm sample, a deformation level that severely challenges standard device fabrication techniques like contact lithography.
- Lock-in Mechanism: FEM demonstrated that a CVD diamond layer as thin as 1 ”m is sufficient to lock the membrane into the highly bowed state achieved during the initial heating phase, due to diamondâs extreme stiffness.
- Interface Discovery: Cross-sectional analysis (STEM/EDX) revealed an unexpected thin layer of SiO2 at the diamond/AlN interface, potentially formed by Si redeposition during plasma pre-treatment, which may facilitate carbide bonding to the N-polar face.
- Proposed Solution: To realize a viable platform, the GaN/III-N membrane must be sufficiently pre-stressed in the opposite direction prior to diamond growth, ensuring the final structure is flat at room temperature.
Technical Specifications
Section titled âTechnical Specificationsâ| Parameter | Value | Unit | Context |
|---|---|---|---|
| GaN Tensile Strength (Reported) | 4 to 7.5 | GPa | Mechanical limit of GaN at room temperature. |
| Measured GaN Tensile Stress | 1.0 ±0.2 | GPa | Residual stress in 0.5 mm and 2 mm membranes post-CVD. |
| Maximum Measured Membrane Bow | 58 | ”m | Net bow for the 5 mm diameter membrane. |
| CVD Growth Temperature (Tg) | 720 to 750 | °C | Measured by pyrometer during MPCVD process. |
| CVD Forward Power | 5.5 | kW | Microwave plasma assisted CVD (MPCVD). |
| CVD Pressure | 110 to 120 | Torr | Growth pressure range. |
| Methane Concentration (CH4) | 3 | % | In H2 gas mixture. |
| Final Diamond Thickness | 38 to 57 | ”m | Achieved after 19 hours of growth. |
| Diamond Youngâs Modulus (EDia) | 1000 | GPa | Value used in numerical modeling. |
| GaN E2(high) Peak Shift (0.5 mm) | -2.8 ± 0.7 | cm-1 | Corresponds to measured tensile stress. |
| Si Handle Thickness (tSi) | 75 | ”m | Base model thickness. |
| GaN Layer Thickness (tGaN) | 2 | ”m | Base model thickness. |
| III-N Layer Thickness (tIII-N) | 3 | ”m | Base model thickness (lumped AlN/AlGaN). |
| Diamond Thermal Conductivity | 2270 | W/mK | Single crystal diamond reference value. |
| GaN Thermal Conductivity | 253 | W/mK | Reference value. |
Key Methodologies
Section titled âKey MethodologiesâThe investigation combined analytical modeling, numerical simulation, and experimental fabrication/characterization to understand thermal stress in the GaN-on-diamond membrane system.
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Membrane Fabrication:
- Starting Material: GaN/III-N heterostructure grown on a Si wafer, diced into 15 mm x 15 mm squares.
- Si Etch: High-power Inductively Coupled Plasma (ICP) etch (900 W) from the Si side to thin the wafer.
- Membrane Patterning: Photolithography followed by a lower power ICP etch (600 W) to fully remove Si in circular regions (0.5 mm, 2 mm, 5 mm diameter), exposing the N-polar AlN layer.
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Diamond Seeding and Pre-treatment:
- Plasma Pre-treatment: N2/H2 microwave plasma (1.5 kW, 20 Torr) was applied to the exposed GaN/III-N membranes to control seeding density and modify the AlN surface.
- Seeding: A nano-diamond colloid solution was pipetted onto the exposed membrane and Si border (non-ultrasonic method used to prevent membrane damage).
-
CVD Diamond Growth:
- Method: Microwave Plasma Assisted Chemical Vapour Deposition (MPCVD) using a Carat systems CTS6U reactor.
- Recipe: 5.5 kW forward power, 110-120 Torr pressure, 3% CH4 in H2 gas mixture.
- Temperature Control: Growth temperature was maintained at 720-750 °C, monitored by a dual-wavelength pyrometer.
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Numerical Modeling (FEM):
- Software: COMSOL Multiphysics (Thermal Stress module).
- Process Steps: A four-step simulation was used: 1) Initial heating to Tg (determining initial bow), 2) Diamond layer deformation to fit the bowed structure, 3) Isolated cooling of the diamond layer (stress-free deposition assumption), and 4) Integration of cooled diamond with the initial membrane structure to find final stress and bow.
- Refinement: Model accuracy was significantly improved by introducing a linear spatial temperature gradient (T(x,y)) across the sample, counteracting the central bow predicted by uniform temperature models.
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Characterization:
- Stress Measurement: Raman spectroscopy (514 nm laser) was used to measure the shift of the GaN E2(high) peak, correlating the shift to residual biaxial tensile stress (using a 2.9 cm-1 GPa-1 relation).
- Deformation Measurement: Surface profilometry was used to quantify the membrane bow (z displacement) before and after diamond growth.
- Interface Analysis: High Angle Annular Dark Field Scanning Transmission Electron Microscopy (HAADF-STEM) and Energy Dispersive X-ray Spectroscopy (EDX) were used to analyze the diamond/III-N interface, confirming the presence of a thin SiO2 layer.
Commercial Applications
Section titled âCommercial ApplicationsâThis research directly addresses a critical manufacturing bottleneckâthermal managementâfor high-performance GaN devices by developing a robust, bonding-free integration method for diamond heat spreaders.
- High Power RF and Microwave Devices: GaN High Electron Mobility Transistors (HEMTs) are primary targets. Diamond heat spreaders are essential to mitigate self-heating, enabling higher power density and improved reliability in 5G/6G infrastructure and radar systems.
- Advanced Thermal Management: The technology provides a pathway for integrating ultra-high thermal conductivity materials (diamond, >2000 W/mK) directly onto semiconductor stacks without relying on complex and thermally resistive wafer bonding processes.
- Micro-Electro-Mechanical Systems (MEMS): The fabrication of robust, large-area GaN/III-N membranes is relevant for various MEMS applications, including pressure sensors and photonic devices, where controlled mechanical deformation is crucial.
- Heterogeneous Integration: The methodology for managing extreme thermal stress during high-temperature deposition is applicable to other material systems requiring the integration of stiff, high-CTE-mismatch films onto thin, fragile semiconductor membranes.
Tech Support
Section titled âTech SupportâOriginal Source
Section titled âOriginal SourceâReferences
Section titled âReferencesâ- 2014 - âGaN-on-diamond: a brief history,â in 2014 lester eastman Conference on high performance devices (LEC)
- 2019 - Thermal conductivity of GaN, 71GaN, and SiC from 150 K to 850 K [Crossref]
- 2014 - Low thermal resistance GaN-on-diamond transistors characterized by three-dimensional Raman thermography mapping [Crossref]
- 1993 - Thermal conductivity of isotopically modified single crystal diamond [Crossref]
- 2011 - AlGaN/GaN high-electron mobility transistors with low thermal resistance grown on single-crystal diamond (111) substrates by metalorganic vapor-phase epitaxy [Crossref]
- 2012 - Reduced self-heating in AlGaN/GaN HEMTs using nanocrystalline diamond heat-spreading films [Crossref]
- 2017 - Thermal characterization of polycrystalline diamond thin film heat spreaders grown on GaN HEMTs [Crossref]
- 2015 - Thermal management of hotspots using diamond heat spreader on Si microcooler for GaN devices [Crossref]
- 2018 - Transfer of AlGaN/GaN RF-devices onto diamond substrates via van der Waals bonding [Crossref]