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High thermal conductivity in wafer-scale cubic silicon carbide crystals

MetadataDetails
Publication Date2022-11-23
JournalNature Communications
AuthorsZhe Cheng, Jianbo Liang, Keisuke Kawamura, Hao Zhou, Hidetoshi Asamura
InstitutionsAir Water (Japan), Georgia Institute of Technology
Citations125
AnalysisFull AI Review Included

Technical Analysis: High Thermal Conductivity in Wafer-Scale Cubic Silicon Carbide Crystals

Section titled “Technical Analysis: High Thermal Conductivity in Wafer-Scale Cubic Silicon Carbide Crystals”

This research demonstrates the exceptional thermal performance of high-purity, wafer-scale cubic silicon carbide (3C-SiC), positioning it as a leading material for next-generation power electronics and thermal management.

  • Record Thermal Conductivity: Isotropic thermal conductivity ($\kappa$) exceeding $500 \text{ W m}^{-1}\text{K}^{-1}$ was achieved at room temperature in bulk 3C-SiC crystals, resolving a long-standing puzzle regarding its theoretical potential.
  • Second Highest Among Large Crystals: This $\kappa$ value is the second highest among all large crystals, surpassed only by single crystal diamond (SCD).
  • High Purity & Quality: The high $\kappa$ is attributed to exceptional crystal quality (FWHM 158 arcsec) and ultra-low boron impurity concentration (< $3 \times 10^{13} \text{ atoms cm}^{-3}$), which minimizes defect-phonon scattering.
  • Wafer Scale Potential: The demonstrated 2-inch free-standing wafers are scalable up to 6-inch, addressing a key limitation of other high-$\kappa$ materials like boron arsenide (BAs) and boron phosphide (BP).
  • Superior Thin Films: Corresponding 3C-SiC thin films exhibited record-high in-plane and cross-plane $\kappa$, exceeding diamond thin films of equivalent thickness.
  • Exceptional Integration: Thermal Boundary Conductance (TBC) at the 3C-SiC/Si interface ($\sim 620 \text{ MW m}^{-2}\text{K}^{-1}$) is among the highest reported for semiconductor interfaces, facilitating heterogeneous integration.
  • 6CCVD Value Proposition: While 3C-SiC is a strong competitor, 6CCVD’s Single Crystal Diamond (SCD) offers intrinsic thermal conductivity exceeding $2000 \text{ W m}^{-1}\text{K}^{-1}$, providing the ultimate solution for extreme heat flux management where 3C-SiC performance is insufficient.

The following hard data points were extracted from the analysis of the high-quality 3C-SiC crystals:

ParameterValueUnitContext
Bulk Thermal Conductivity ($\kappa$)> 500W m-1K-1Room Temperature (RT), Isotropic
Wafer Scalability (Potential)Up to 6inchFree-standing 3C-SiC
Demonstrated Wafer Size2inchFree-standing 3C-SiC
Bulk Thickness (Free-standing)$\sim 100$”mUsed for TDTR measurements
Thin Film Thickness Range0.93 to 2.52”mEpitaxial 3C-SiC on Si
Growth Temperature (LT-CVD)1300KLow-Temperature Chemical Vapor Deposition
XRD FWHM ((111) Peak)158arcsecHigh Crystal Quality
Stacking Fault Density$\sim 1000$cm-1Observed on the growth face
Boron (B) Impurity Concentration< $3 \times 10^{13}$atoms cm-3Below SIMS detection limit (Key to high $\kappa$)
Nitrogen (N) Impurity Concentration$5.8 \times 10^{15}$atoms cm-3Measured on the growth face
Thermal Boundary Conductance (TBC)$\sim 620$MW m-2K-13C-SiC/Si interface
TBC Comparison (Diamond/Si)$\sim 62$MW m-2K-13C-SiC TBC is 10x higher than diamond/Si interfaces37

The high thermal conductivity 3C-SiC crystals were fabricated and characterized using advanced CVD and ultrafast thermal metrology techniques:

  1. Growth Method: Low-Temperature Chemical Vapor Deposition (LT-CVD) was used in a customized CVD reactor.
  2. Substrate and Orientation: Growth occurred on (111) Si substrates. The specific orientation and low growth temperature (1300 K) were critical for achieving high crystal quality 3C-SiC layers with low stacking fault density.
  3. Bulk Crystal Fabrication: Free-standing bulk 3C-SiC crystals ($\sim 100 \text{ ”m}$ thick) were obtained by etching away the Si substrate using HNA (HF: HNO3: H2O).
  4. Thermal Characterization (Bulk/Cross-Plane): Time-Domain Thermoreflectance (TDTR) was used to measure $\kappa$ and TBC. Measurements utilized a $90 \text{ nm}$-thick Al transducer layer.
    • TDTR Parameters: $5\times$ objective (spot size $10.7 \text{ ”m}$) and $9.3 \text{ MHz}$ modulation frequency were primarily used for bulk $\kappa$.
  5. Thermal Characterization (In-Plane): Beam-Offset Time-Domain Thermoreflectance (BO-TDTR) was employed to measure the in-plane $\kappa$ of 3C-SiC thin films, utilizing an offset pump beam relative to the probe beam.
  6. Structural Analysis: Crystal quality was confirmed using X-ray Diffraction (XRD) rocking curves (FWHM 158 arcsec) and High-Resolution Scanning Transmission Electron Microscopy (HR-STEM) with Selected Area Electron Diffraction (SAED).
  7. Purity Analysis: Secondary Ion Mass Spectrometry (SIMS) was used to confirm ultra-low concentrations of critical impurities (Boron, Nitrogen, Oxygen), validating the high-purity requirement for high $\kappa$.

The research highlights 3C-SiC as a powerful thermal management material, second only to diamond. For engineers and scientists requiring the absolute highest thermal performance, 6CCVD provides MPCVD diamond solutions that surpass 3C-SiC’s capabilities, particularly in high-power density applications where heat flux is critical.

While 3C-SiC achieves $500 \text{ W m}^{-1}\text{K}^{-1}$, 6CCVD’s CVD diamond offers significantly higher intrinsic thermal conductivity, making it the definitive choice for extreme thermal management:

6CCVD MaterialApplication FocusThermal Conductivity ($\kappa$)3C-SiC Comparison
Optical Grade Single Crystal Diamond (SCD)Ultimate Heat Spreaders, Active Devices, Quantum> $2000 \text{ W m}^{-1}\text{K}^{-1}$4x higher than 3C-SiC
Thermal Grade Polycrystalline Diamond (PCD)Large-Area Substrates, Cost-Effective Heat Sinks$\sim 1000 - 1800 \text{ W m}^{-1}\text{K}^{-1}$2x to 3.6x higher than 3C-SiC
Boron-Doped Diamond (BDD)Electrochemical, Sensing, Active Device ElectrodesTunable (Semiconducting)Used where electrical conductivity is required

The paper emphasizes the challenge of integrating high-$\kappa$ materials with high TBC. 6CCVD directly addresses this integration challenge through comprehensive customization services:

  • Custom Dimensions and Thickness:
    • 6CCVD offers SCD plates/wafers in thicknesses ranging from $0.1 \text{ ”m}$ up to $500 \text{ ”m}$, matching or exceeding the bulk and thin-film dimensions used in this 3C-SiC study ($\sim 100 \text{ ”m}$).
    • For large-area thermal management, 6CCVD provides PCD wafers up to $125 \text{ mm}$ in diameter, addressing the scalability requirement noted in the research.
  • Advanced Metalization Services:
    • TBC measurements rely heavily on the metal transducer layer (Al in this study) and subsequent device metalization (e.g., Ti/Pt/Au mentioned in related TBC literature).
    • 6CCVD provides in-house metalization capabilities, including Au, Pt, Pd, Ti, W, and Cu, allowing researchers to optimize TBC for diamond/SiC or diamond/Si interfaces, crucial for replicating or extending the high TBC findings observed with 3C-SiC.
  • Surface Preparation:
    • The high quality of the 3C-SiC was achieved partly through careful polishing. 6CCVD guarantees ultra-smooth surfaces: Ra < $1 \text{ nm}$ for SCD and Ra < $5 \text{ nm}$ for inch-size PCD, ensuring optimal interface quality for TBC maximization.

6CCVD’s in-house PhD team specializes in optimizing CVD diamond properties for extreme applications. We can assist researchers and engineers with material selection for similar Wide-Bandgap Semiconductor Thermal Management projects, ensuring the correct balance between thermal performance, electrical properties, and integration compatibility.

6CCVD supports global research efforts with reliable worldwide shipping (DDU default, DDP available), ensuring prompt delivery of custom diamond materials to meet demanding research timelines.

For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.