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Diamond Metal-Oxide-Semiconductor Field-Effect Transistors on a Large-Area Wafer

MetadataDetails
Publication Date2023-07-21
AuthorsJiangwei Liu, Hirotaka Ohsato, Bo Da, Yasuo Koide
InstitutionsNational Institute for Materials Science
AnalysisFull AI Review Included

Diamond Metal-Oxide-Semiconductor Field-effect Transistors on a Large-area Wafer: Engineering Analysis

Section titled “Diamond Metal-Oxide-Semiconductor Field-effect Transistors on a Large-area Wafer: Engineering Analysis”

This study successfully demonstrates the fabrication and electrical characterization of hydrogen-terminated (H-diamond) Metal-Oxide-Semiconductor Field-Effect Transistors (MOSFETs) on large-area diamond wafers (8 x 8 mm2), a critical step toward commercial viability.

  • Large-Area Fabrication: MOSFETs were fabricated on 8 x 8 mm2 Ib-type diamond substrates, significantly larger than the typical 3 x 3 mm2 research size, enabling the integration of 720 devices per wafer.
  • T-type Performance Superiority: The T-type MOSFET geometry demonstrated superior performance compared to the planar-type, achieving a maximum drain current (ID,max) of -3.0 mA/mm and an on-resistance (RON) of 3.0 x 103 Ω mm (at LG = 3.0 ”m).
  • RON Reduction: The T-type structure achieved an RON approximately four times lower than the planar-type (1.2 x 104 Ω mm) by eliminating the highly resistive H-diamond surface interspaces between the source/drain and gate electrodes.
  • Gate Stack Engineering: A high-k Al2O3/HfSiO2 bilayer was employed as the gate insulator. Atomic Layer Deposition (ALD) Al2O3 (4.0 nm) served as a buffer layer to protect the sensitive H-diamond surface during subsequent Sputtering Deposition (SD) of HfSiO2.
  • P-type Characteristics: Both device types exhibited clear p-type characteristics and distinct pinch-off behavior, confirming effective modulation of the two-dimensional hole gas (2DHG) channel.
ParameterValueUnitContext
Wafer Size8 x 8mm2Ib-type diamond (100) substrate
Substrate Thickness0.3mmIb-type diamond (100) substrate
Epitaxial Layer Thickness~150nmH-diamond homoepitaxial layer
H2 Flow Rate (CVD)500sccmMicrowave plasma-enhanced CVD
CH4 Flow Rate (CVD)0.5sccmMicrowave plasma-enhanced CVD
Deposition Temperature900-940°CH-diamond epitaxial growth
Deposition Pressure80TorrH-diamond epitaxial growth
Gate Width (WG)100”mStandardized width for all 720 devices
Gate Length (LG) Range3.0 to 31.0”mTested range for planar MOSFETs
Planar S/D-Gate Interspace3.5”mDistance between contacts (Planar type)
T-type S/D-Gate Interspace0”mDistance between contacts (T-type)
ALD-Al2O3 Thickness4.0nmBuffer layer contacting H-diamond
T-type ID,max (LG=3.0 ”m)-3.0mA/mmMeasured at VGS = -20.0 V
Planar ID,max (LG=3.0 ”m)-0.8mA/mmMeasured at VGS = -20.0 V
T-type RON (LG=3.0 ”m)3.0 x 103Ω mmOn-resistance at VGS = -20.0 V
Planar RON (LG=3.0 ”m)1.2 x 104Ω mmOn-resistance at VGS = -20.0 V

The H-diamond MOSFETs were fabricated using a multi-step process involving CVD growth, plasma etching, and electron-gun evaporation for contacts.

  1. Substrate Cleaning: Ib-type diamond (100) substrate (8 x 8 mm2) was cleaned in H2SO4+HNO3 acid solution at 300 °C for 3 hours.
  2. Epitaxial Growth: H-diamond homoepitaxial layer (~150 nm thick) was grown using microwave plasma-enhanced CVD at 900-940 °C and 80 Torr, utilizing H2 (500 sccm) and CH4 (0.5 sccm) for 1.5 hours.
  3. Mesa Structure Formation: The H-diamond was etched in an O2 ambient using a capacitively-coupled plasma Reactive Ion Etching (RIE) system (100 sccm O2, 10 Pa, 50 W) for 90 seconds.
  4. Ohmic Contact Formation: Source/drain electrodes (Pd/Ti/Au, 10/20/200 nm) were formed via electron-gun evaporation.
  5. Gate Oxide Deposition:
    • A 4.0 nm Al2O3 buffer layer was deposited directly onto the H-diamond surface using Atomic Layer Deposition (ALD).
    • A high dielectric constant HfSiO2 layer was subsequently deposited via Sputtering Deposition (SD).
  6. Gate Contact Formation: Gate electrodes (Ti/Au, 10/200 nm) were formed using electron-gun evaporation.
  7. Characterization: Electrical properties were measured using a four-probe system at room temperature.

The development of large-area diamond MOSFETs leverages diamond’s intrinsic properties (wide band gap, high breakdown field, high carrier mobility, and large thermal conductivity) for extreme environment and high-efficiency electronics.

  • High-Power Electronics:
    • Power switching devices (MOSFETs, IGBTs) for electric vehicles (EVs) and hybrid electric vehicles (HEVs).
    • High-voltage converters and inverters for smart grids and renewable energy systems (solar/wind power).
  • High-Frequency/RF Applications:
    • High-frequency amplifiers and switches for 5G/6G base stations, radar systems, and satellite communications, benefiting from diamond’s high carrier mobility.
  • Extreme Environment Operation:
    • Electronics designed for high-temperature environments (e.g., aerospace, geothermal drilling) due to diamond’s wide band gap and thermal stability.
  • Thermal Management:
    • Integration into high-density electronic modules where diamond’s superior thermal conductivity (highest known material) is essential for heat dissipation.
View Original Abstract

Diamond is promising for high-power, highfrequency, and high-temperature applications.By now, most of diamond metal-oxide-semiconductor field-effect transistors (MOSFETs) are fabricated on small-area diamond wafers (3 × 3 mm 2 ).In order to push forward the diamond electronic devices for future practical application, it is necessary to investigate the electrical properties of them on the large-area wafers.In this study, we fabricate planar-type and T-type hydrogen-terminated diamond MOSFETs on a large-area wafer (8 × 8 mm 2 ).Electrical properties of them are investigated and discussed.

  1. 2008 - Diamond as an electronic material [Crossref]