Skip to content

Thermal Conductivity of Diamond/SiC Nano-Polycrystalline Composites and Phonon Scattering at Interfaces

MetadataDetails
Publication Date2017-05-26
JournalACS Omega
AuthorsHuicong Dong, Bin Wen, Yuwen Zhang, Roderick Melnik
InstitutionsYanshan University, Wilfrid Laurier University
Citations22
AnalysisFull AI Review Included

Diamond/SiC Nano-Polycrystalline Composites: Tailoring Thermal Resistance via Heterogeneous Interfaces

Section titled “Diamond/SiC Nano-Polycrystalline Composites: Tailoring Thermal Resistance via Heterogeneous Interfaces”

An Analysis of Advanced Thermal Management Strategies using 6CCVD Materials


This technical analysis of the research paper concerning Diamond/SiC nano-polycrystalline composites validates the critical role of interface engineering in advanced thermal management applications (e.g., MEMS/NEMS).

  • Core Finding: Phonon scattering and resulting thermal boundary resistance (TBR) are significantly stronger at heterogeneous (Diamond/SiC) interfaces compared to homogeneous (Diamond/Diamond or SiC/SiC) interfaces.
  • Mechanism Verified: Molecular Dynamics (NEMD) and Phonon Wave Packet (PWP) simulations attribute the enhanced TBR to combined effects: reduced energy transmission coefficients and prolonged phonon transmission time (phonon trapping).
  • Quantitative Results: Mean heterogeneous TBR (RSiC→Dia) reaches 7.63 x 10-10 m2 K/W, nearly 4 times the homogeneous RDia→Dia (1.92 x 10-10 m2 K/W).
  • Thermal Rectification: Thermal rectification (RSiC→Dia > RDia→SiC) is observed at the heterogeneous interface, offering pathways for directional heat flow control.
  • Design Guidance: Findings provide crucial guidance for engineers designing polycrystalline materials to deliberately adjust thermal resistance through the strategic introduction of heterogeneous phase boundaries.
  • 6CCVD Value: Replicating and extending this research requires high-purity, custom Polycrystalline Diamond (PCD) substrates with precise thickness control and ultra-low surface roughness, all available through 6CCVD’s MPCVD capabilities.

The following table summarizes the quantitative results and simulation parameters extracted from the research paper, focusing on thermal resistance values critical for composite design.

ParameterValueUnitContext
Simulation Temperature300KAll NEMD simulations
Polycrystalline Grain Size2nmNano-composite structure modeling
Homogeneous Interface Thermal Resistance (RDia→Dia)1.92 x 10-10m2 K/WMean value (Diamond/Diamond)
Homogeneous Interface Thermal Resistance (RSiC→SiC)4.69 x 10-10m2 K/WMean value (SiC/SiC)
Heterogeneous Interface Thermal Resistance (RDia→SiC)3.85 x 10-10m2 K/WMean value (Heat flow Dia → SiC)
Heterogeneous Interface Thermal Resistance (RSiC→Dia)7.63 x 10-10m2 K/WMean value (Heat flow SiC → Dia)
Thermal Rectification FactorRSiC→Dia / RDia→SiC ratio is ~1.98N/AObserved asymmetry in heat flux direction
PWP Simulation Time (Diamond/SiC)6.15 to 7.3psTransmission time for 1.15 to 18.3 THz phonons
Transmission Coefficient (αDia→SiC) (Low Frequency)Approx. 0.96N/AFor incident frequency $\omega$ < 6 THz
Transmission Coefficient Ratio (RDia→SiC / RDia→Dia)1.2 to 2.6N/AFrequency-dependent ratio verified by PWP
Transmission Coefficient Ratio (RSiC→Dia / RSiC→SiC)0.17 to 1.52N/AFrequency-dependent ratio verified by PWP

The study relied on high-fidelity computational methods to model phonon behavior and thermal transport at the nano-scale.

  1. Material Construction: Atomic structures of diamond/SiC polycrystalline composites were generated using the three-dimensional Voronoi tessellation method, modeling a precise 2 nm grain size.
  2. Interatomic Potentials: The C-C and Si-C bonding interactions were described using the verified Tersoff potential, accurate for thermal conductivity calculations.
  3. Thermal Conductivity (Bulk): Non-Equilibrium Molecular Dynamics (NEMD) simulations were performed at 300 K under the NVE ensemble to calculate bulk thermal conductivity based on Fourier’s law.
  4. Interface Resistance (TBR): NEMD simulations were used on 40 nm cell lengths with varying twist angles (e.g., 0° and 53.13°) to calculate interface thermal resistance (R = $\Delta$T/J).
  5. Phonon Transport Analysis: The Phonon Wave Packet (PWP) method was applied to quantify frequency-dependent properties, including the energy transmission coefficient ($\alpha$) and the energy transmission time ($\Gamma$).
  6. Interface Modeling: The study specifically modeled three interface types: homogeneous (Diamond/Diamond, SiC/SiC) and heterogeneous (Diamond/SiC) to isolate scattering mechanisms.

This research demonstrates the immense potential of integrating distinct material phases (like Diamond and SiC) at the nano-scale to engineer specific thermal properties for demanding applications (thermal barrier coatings, bioMEMs, micro-/nano-devices). 6CCVD is uniquely positioned to supply the advanced MPCVD diamond materials necessary to transition this theoretical work into practical device fabrication.

To replicate or extend this research by fabricating real-world Diamond/SiC composites, engineers require high-purity diamond substrates with tailored properties:

  • Thermal Grade Polycrystalline Diamond (PCD): The primary material studied. 6CCVD offers high-purity PCD wafers for the fabrication of diamond components in the composite structure. Our grain sizes can be precisely controlled, crucial for matching the nano-scale dimensions studied in the MD simulations.
  • Optical Grade Single Crystal Diamond (SCD): While the paper focused on PCD, SCD substrates (available from 0.1”m to 500”m thick) offer ultimate structural and purity control for foundational studies or hybrid composite designs requiring diamond layers.

The creation of layered or composite structures like Diamond/SiC relies heavily on precise material handling, surface preparation, and integration steps.

Custom Capability6CCVD OfferingResearch Link & Application
Custom DimensionsPlates/wafers up to 125mm (PCD)Required for large-scale composite fabrication, especially for MEMS/NEMS devices.
Thickness ControlSCD/PCD from 0.1”m to 500”mEnables precise control over the bulk material fraction (e.g., SiC volume fraction PSiC) as defined in the modified Maxwell model (Eq. 3).
Ultra-Low RoughnessPolishing Ra < 5nm (Inch-size PCD)Critical for minimizing interfacial defects in heterogeneous bonding, ensuring results align with the idealized interfaces modeled in PWP simulations.
Custom MetalizationIn-house capability (Au, Pt, Pd, Ti, W, Cu)Essential for subsequent processing or direct bonding to SiC components (SiC is commonly integrated using metal diffusion bonding or direct wafer bonding). 6CCVD can pre-deposit Ti/Pt/Au contact layers for composite stack readiness.

The complexity of thermal transport in heterogeneous systems—especially the observed dependence on phonon frequency and directional heat flow—necessitates expert material consultation.

  • 6CCVD’s in-house PhD team specializes in CVD material physics and can assist researchers in selecting the optimal polycrystalline morphology (e.g., grain orientation, size, and surface finish) required for similar Thermal Barrier Coating or Micro/Nano-Electromechanical Device (MEMS/NEMS) projects.
  • We offer technical guidance to ensure the supplied MPCVD diamond material properties (density, crystal orientation, purity) meet the stringent requirements for reproducible experimental validation of these interface-engineered thermal composites.

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

View Original Abstract

To compare the thermal properties of heterogeneous and homogeneous interfaces, polycrystalline composites are proposed. Thermal properties of heterogeneous and homogeneous interfaces in the composites are investigated using molecular dynamics simulations. The results indicate that when the inflow of heat arises from the same material, phonon scattering at heterogeneous interfaces is stronger than that at homogeneous interfaces. The phonon wave packet simulations indicate that the stronger phonon scattering at heterogeneous interfaces is caused by the combined actions of transmission coefficients and transmission time.