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High-Quality SiO2/O-Terminated Diamond Interface - Band-Gap, Band-Offset and Interfacial Chemistry

MetadataDetails
Publication Date2022-11-22
JournalNanomaterials
AuthorsJ. Cañas, D.F. Reyes, Alter Zakhtser, Christian Dussarrat, Takashi Teramoto
InstitutionsCentre National de la Recherche Scientifique, Institut polytechnique de Grenoble
Citations8
AnalysisFull AI Review Included

This research successfully characterizes the high-quality interface formed by Atomic Layer Deposition (ALD) of amorphous silicon oxide (SiO2) on oxygen-terminated (100) p-type diamond, validating its potential as a gate dielectric for diamond electronics.

  • Gate Oxide Quality: Amorphous SiO2 was synthesized successfully via ALD, exhibiting a homogeneous ultra-wide band-gap (Eg) of 9.4 ± 0.2 eV across the layer, confirming its suitability for high-voltage applications.
  • Band Alignment: A highly favorable straddling band setting was established between SiO2 and diamond, crucial for minimizing leakage currents in both accumulation and inversion regimes.
  • High Energy Barriers: Substantial band offsets were measured: a Valence Band Offset (VBO) of 2.0 eV and a Conduction Band Offset (CBO) of 1.9 eV. These barriers are significantly higher than those reported for other oxides on diamond.
  • Interfacial Chemistry: The interface bonding is dominated by single- and double-carbon-oxygen (C-O, C=O) bonds, with a scarce presence of silicon-carbon (C-Si) bonds, correlating with the previously reported low density of interface states.
  • Device Potential: The combination of wide band-gap, high band offsets, and low interface state density opens the route for fabricating stable, high-power diamond MOSFETs, including inversion-based devices requiring a large electron barrier.
ParameterValueUnitContext
Diamond Typep-type (100) CVD-O-terminated surface
Nominal Boron Conc.~1016cm-3Doping level of the active layer
CVD Growth Temperature900°CEpitaxy conditions
CVD Pressure33TorrEpitaxy conditions
SiO2 Thicknesses2 and 40nmALD layer thicknesses studied
SiO2 PhaseAmorphous-Confirmed by XPS VB peaks
SiO2 Band-Gap (VEELS)9.4 ± 0.2eVBulk measurement (more reliable)
SiO2 Band-Gap (PEELS)9.0 ± 0.2eVSurface-sensitive measurement
Diamond Band-Gap (Eg)5.5eVReference value (Figure 5)
Valence Band Offset (VBO)2.0eVBarrier for holes
Conduction Band Offset (CBO)1.9eVBarrier for electrons
Diamond Breakdown FieldUp to 10MV/cmSuperior material property [1]
Interface Bonding Ratio (C=O)50%Relative area of C(1s) components
Interface Bonding Ratio (C-O)35%Relative area of C(1s) components
Interface Bonding Ratio (C-Si)15%Relative area of C(1s) components

The study combined advanced microscopy and spectroscopy techniques to characterize the heterojunction, focusing on precise band-gap and band-offset determination.

  1. Diamond Epitaxy:

    • p-type diamond layers (~1 ”m thick) were grown via Microwave Plasma Chemical Vapor Deposition (MPCVD) on High Pressure High Temperature (HPHT) Ib substrates.
    • Gas mixture included CH4/H2 = 1% and O2/H2 = 0.25%, with B/C = 60 ppm.
  2. Surface Termination:

    • The diamond surface was oxidized using an ozone plasma treatment.
    • Conditions: 120 minutes at 500 mbar, utilizing a Xenon EXCIMER UV lamp (172 nm) to achieve O-termination.
  3. Gate Oxide Deposition:

    • Silicon oxide (SiO2) layers (2 nm and 40 nm) were grown using Atomic Layer Deposition (ALD).
  4. Scanning Transmission Electron Microscopy (STEM-EELS):

    • Used to determine the bulk band-gap and interfacial chemistry at nanometer resolution.
    • VEELS (Valence EELS): Measured the SiO2 band-gap (9.4 eV). A low accelerating voltage (60 kV) was used to mitigate the Cherenkov effect, ensuring accurate band-gap estimation.
    • Interface Analysis: EELS spectra (O K-edge and Si L-edge) confirmed C-O bonding dominance at the interface, with no detectable silicon signal on the diamond side.
  5. X-ray Photoelectron Spectroscopy (XPS):

    • Used for precise band alignment and interfacial bond quantification.
    • Conditions: High-resolution monochromatic Al-Kα radiation (hΜ = 1486.7 eV), mild Ar+ cleaning (0.5 kV).
    • PEELS (Photoelectron EELS): Measured the SiO2 band-gap (9.0 eV) from the O(1s) core level energy loss spectrum.
    • C(1s) Deconvolution: Identified and quantified interfacial bonds: C=O (50%), C-O (35%), and C-Si (15%).
    • Band Offset Calculation: VBO and CBO were calculated using the core level and Valence Band Maximum (VBM) data from the 40 nm (bulk) and 2 nm (interface) samples.

The successful integration of high-quality SiO2 as a gate dielectric on O-terminated diamond enables the development of next-generation power and high-frequency electronics.

  • High-Power Switching Devices:

    • Product: Diamond Metal-Oxide-Semiconductor Field-Effect Transistors (MOSFETs).
    • Benefit: Utilizes diamond’s 10 MV/cm breakdown field and the high CBO (1.9 eV) and VBO (2.0 eV) barriers provided by the SiO2 gate, minimizing leakage and enabling high-voltage operation.
  • High-Temperature Electronics:

    • Industry: Aerospace, Automotive (EV power management), Geothermal Sensing.
    • Benefit: O-terminated diamond and SiO2 are thermally stable (O-termination up to 700 K), allowing device operation in environments exceeding the limits of silicon carbide (SiC) devices.
  • Normally-Off Transistors:

    • Product: Depletion and Inversion-based MOSFETs.
    • Benefit: The O-termination naturally depletes holes, facilitating normally-off operation. The large CBO (1.9 eV) is critical for achieving stable inversion regimes, a key requirement for energy-efficient power electronics.
  • Harsh Environment Systems:

    • Industry: Nuclear, Defense, Space.
    • Benefit: Diamond’s inherent radiation hardness, combined with a stable, low-defect gate oxide interface, ensures reliability in high-radiation or high-vibration environments.
View Original Abstract

Silicon oxide atomic layer deposition synthesis development over the last few years has open the route to its use as a dielectric within diamond electronics. Its great band-gap makes it a promising material for the fabrication of diamond-metal-oxide field effects transistor gates. Having a sufficiently high barrier both for holes and electrons is mandatory to work in accumulation and inversion regimes without leakage currents, and no other oxide can fulfil this requisite due to the wide diamond band-gap. In this work, the heterojunction of atomic-layer-deposited silicon oxide and (100)-oriented p-type oxygen-terminated diamond is studied using scanning transmission electron microscopy in its energy loss spectroscopy mode and X-ray photoelectron spectroscopy. The amorphous phase of silicon oxide was successfully synthesized with a homogeneous band-gap of 9.4 eV. The interface between the oxide and diamond consisted mainly of single- and double-carbon-oxygen bonds with a low density of interface states and a straddling band setting with a 2.0 eV valence band-offset and 1.9 eV conduction band-offset.

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