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Stress engineering of high-quality single crystal diamond by heteroepitaxial lateral overgrowth

MetadataDetails
Publication Date2016-02-01
JournalApplied Physics Letters
AuthorsY.-H. Tang, B. Golding
InstitutionsMichigan State University
Citations42
AnalysisFull AI Review Included

Stress Engineering and Advanced SCD Growth via Heteroepitaxial Lateral Overgrowth (ELO)

Section titled “Stress Engineering and Advanced SCD Growth via Heteroepitaxial Lateral Overgrowth (ELO)”

Analysis of AIP Applied Physics Letters 108, 052101 (2016) by Y.-H. Tang and B. Golding

This paper presents a highly effective method for producing high-quality, low-stress Single Crystal Diamond (SCD) films via Microwave Plasma Chemical Vapor Deposition (MPCVD) using Heteroepitaxial Lateral Overgrowth (ELO). This technique solves critical constraints facing large-area heteroepitaxial diamond used in demanding applications like particle detection.

  • Superior Stress Mitigation: Utilizing a ductile, patterned metal layer (Au) on an Ir-buffered a-plane sapphire substrate, the method virtually eliminates thermal mismatch stress between the diamond film and the non-diamond substrate.
  • Ultra-Low Surface Stress Achieved: A biaxial in-plane stress of 0.00 ± 0.16 GPa was achieved on a 180 ”m thick SCD film, confirmed by averaged Raman shift (reference frequency 1332.4 cm-1). This contrasts sharply with the calculated interfacial stress of -4.55 GPa in non-ELO systems.
  • Effective Dislocation Filtering: The ELO mechanism blocks the propagation of threading dislocations, confining them primarily to the unmasked aperture regions. This results in an extremely low dislocation density in the overgrown areas.
  • High Structural Quality: Dislocation density in the overgrown regions was quantified to be below 108 cm-2, accompanied by a 2x to 3x reduction in Raman linewidth relative to the unmasked area.
  • Simplified Substrate Separation (Lift-Off): The inherent thermal expansion mismatch, accommodated by the Au layer, promotes the delamination of thick diamond films (e.g., 180 ”m) at the diamond-Ir interface, simplifying the creation of freestanding, high-quality SCD plates without extensive processing.
  • 6CCVD Relevance: 6CCVD’s capability to supply thick (up to 500 ”m), custom-sized SCD wafers and provide advanced in-house metalization (Au, Ti, Ir layering) positions us perfectly to replicate or scale this stress-engineering technique for next-generation detectors and optics.
ParameterValueUnitContext
Final Diamond Thickness180”mFor stress measurement (average surface stress)
ELO Growth Time10+hMinimum exposure for lateral overgrowth
Initial Diamond Thickness (Seed Layer)550nmDiamond film 1, grown on Ir buffer
Ir Buffer Layer Thickness300nmGrown on a-plane sapphire
Mask MaterialAu (on 4 nm Ti adhesion layer)nmAu thickness: 85 nm
Mask Stripe Width8”mPeriodic metal-masked region
Aperture Width4”mExposed diamond growth area
Mask Pitch12”mCombined aperture and mask width
Dislocation Density (Overgrown)< 108cm-2Verified by SEM etch pit distribution
Surface Biaxial Stress0.00 ± 0.16GPaFor 180 ”m film, derived from Raman shift
Interfacial Thermal Stress (Non-ELO)-4.55GPaCalculated maximum stress without ELO
Raman Linewidth Reduction2 to 3FactorReduced in overgrown regions vs. apertures
Lateral Growth Rate0.4”m/hUsed during the lateral overgrowth step

The experiment utilized a two-step MPCVD process incorporating photolithography and a metal decoupling layer to achieve high-quality ELO:

  1. Substrate Preparation:

    • A 300 nm epitaxial Ir (001) buffer layer was deposited onto a 1x1 cm2 a-plane sapphire substrate using electron-beam or sputtering deposition at temperatures above 750 °C.
    • The Ir layer was biased at -180 V dc at 700 °C for 1 h in a 2% CH4/H2 plasma (18 Torr) to achieve uniform, high-density diamond nucleation.
  2. Initial Diamond Film Growth (Diamond 1):

    • Subsequent growth occurred at 650 °C for 3 h, forming a continuous, smooth, 550 nm SCD film (Diamond 1). No additional gases were intentionally added.
  3. Patterning and Metal Mask Deposition:

    • A two-step lithography process was used on the 550 nm SCD film.
    • A standard photomask created 8 ”m wide Au stripes along the diamond (110) direction on a 12 ”m pitch, leaving 4 ”m diamond apertures exposed.
    • 4 nm Ti (adhesion layer) and 85 nm Au were thermally evaporated at room temperature and then lifted off.
  4. Heteroepitaxial Lateral Overgrowth (ELO) (Diamond 2):

    • The masked substrate was placed back into the MPCVD reactor.
    • Growth was initiated at 750 °C - 50 °C lower than the final growth temperature to protect the Au mask from plasma damage.
    • The growth gas mixture was 2%-3% CH4/H2 at a pressure of 58-60 Torr.
    • Slow lateral growth (0.4 ”m/h) was maintained until coalescence, reaching a thickness of approximately 10 ”m (Diamond 2, where ELO overgrew the Au mask). Thicker films up to 180 ”m were subsequently grown under similar conditions.

6CCVD is an expert provider of MPCVD diamond solutions, specializing in the materials and processes required to replicate and advance this stress-engineered ELO technique. Our capabilities directly address the complexity and scalability challenges highlighted in this research.

To replicate or extend this research for thicker, detector-grade applications (up to 1-2 mm mentioned in the paper), 6CCVD recommends:

  • Optical Grade SCD (Single Crystal Diamond): For high-quality, ultra-low defect films requiring exceptional purity, essential for high-efficiency energetic particle detection.
  • Custom Substrate Materials: We can source and process the Ir-buffered sapphire necessary for heteroepitaxial nucleation, or work with clients on alternative SCD/PCD seed materials if subsequent homoepitaxial growth is desired.
  • Heavy Boron Doped PCD/SCD (BDD): If the application requires electrically conductive diamond detectors or electrodes, we offer precise BDD materials with controlled doping profiles, suitable for integration into complex devices.

The success of the ELO method is entirely dependent on precise patterning and the metal decoupling layer. 6CCVD provides comprehensive services essential for mastering this technique:

Requirement from Paper6CCVD CapabilityValue Proposition
Thick Film Requirements (1-2 mm)SCD Thickness up to 500 ”m; Substrates up to 10 mmWe exceed the thickness achieved in the paper (180 ”m), enabling true detector-grade SCD plates.
Masking Layer Deposition (Ti/Au)Internal Metalization (Au, Pt, Pd, Ti, W, Cu)We provide high-purity, custom-patterned metal layers crucial for the ELO process and subsequent stress accommodation.
Precise Patterning & Mask GeometryCustom Laser Cutting and MicromachiningWe offer precise patterning of the diamond surface for aperture and mask creation, ensuring the required 12 ”m pitch resolution.
Surface Finish (Post-Growth)Precision Polishing (Ra < 1 nm on SCD)We eliminate surface roughness issues noted in the paper, providing epi-ready surfaces for device integration or subsequent homoepitaxy.
Large Area Scale-UpCustom Dimensions up to 125 mm platesWhile the paper focused on 7.5 mm diameter regions, 6CCVD can scale production to industry-standard wafer sizes, facilitating commercial viability.
Global LogisticsDDU Default Global Shipping (DDP Available)Secure and timely delivery of sensitive CVD diamond materials worldwide.

The use of a metal decoupling layer to manage thermal stress and promote substrate lift-off is an advanced technique. 6CCVD’s in-house PhD team can assist with material selection, process optimization, and substrate transfer strategies for similar energetic particle detector or high-power electronic projects where ultra-low stress SCD is paramount. Our team supports clients in defining ideal MPCVD recipes and layer stacks (Ir/Ti/Au) tailored to specific stress-engineering goals.

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

View Original Abstract

Here, we describe a method for lateral overgrowth of low-stress single crystal diamond by chemical vapor deposition (CVD). The process is initiated by deposition of a thin (550 nm) (001) diamond layer on Ir-buffered a-plane sapphire. The diamond is partially masked by periodic thermally evaporated Au stripes using photolithography. Lateral overgrowth of the Au occurs with extremely effective filtering of threading dislocations. Thermal stress resulting from mismatch of the low thermal expansion diamond and the sapphire substrate is largely accommodated by the ductile Au layer. The stress state of the diamond is investigated by Raman spectroscopy for two thicknesses: at 10 Όm where the film has just overgrown the Au mask and at 180 Όm where the film thickness greatly exceeds the scale of the masking. For the 10-Όm film, the Raman linewidth shows spatial oscillations with the period of the Au stripes with a factor of 2 to 3 reduction relative to the unmasked region. In a 180-Όm thick diamond film, the overall surface stress was extremely low, 0.00 ± 0.16 GPa, obtained from the Raman shift averaged over the 7.5mm diameter of the crystal at its surface. We conclude that the metal mask protects the overgrown diamond layer from substrate-induced thermal stress and cracking. Lastly, it is also responsible for low internal stress by reducing dislocation density by several orders of magnitude.