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Schottky Barrier Height Analysis of Diamond SPIND Using High Temperature Operation up to 873 K

MetadataDetails
Publication Date2020-01-01
JournalIEEE Journal of the Electron Devices Society
AuthorsMohamadali Malakoutian, Manpuneet Benipal, Franz A. Koeck, R. J. Nemanich, Srabanti Chowdhury
InstitutionsStanford University, Arizona State University
Citations25
AnalysisFull AI Review Included

Technical Documentation & Analysis: High-Temperature Diamond SPIND

Section titled ā€œTechnical Documentation & Analysis: High-Temperature Diamond SPINDā€

This research successfully demonstrates the exceptional thermal stability and high-power performance of a diamond Schottky PIN Diode (SPIND), validating diamond’s role in extreme environment power electronics.

  • Extreme Temperature Operation: Stable, explicit diode rectification was demonstrated up to 723 K, with functional operation and stability confirmed up to 873 K (600 °C).
  • High Current Density: The SPIND achieved an excellent forward current density exceeding 3000 A/cm² at 8 V, confirming high-power capability.
  • Exceptional Stability: The device exhibited no degradation in I-V characteristics after 10 high-temperature cycles, totaling 120 hours of exposure up to 873 K.
  • High Rectification: Rectification factors were measured at >10⁹ at 298 K and 1100 at 673 K, indicating excellent diode quality.
  • Barrier Inhomogeneity Confirmed: The study utilized Tung’s modified thermionic emission model and Conductive Atomic Force Microscopy (C-AFM) to confirm and analyze inhomogeneous Schottky barrier heights (SBHs).
  • Model Validation: The modified model successfully resolved the discrepancy in the Richardson’s constant, yielding an extracted value (A** = 81.16 ± 8.9 A/cm²·K²) that closely matches the theoretical value (90 A/cm²·K²).

The following hard data points were extracted from the analysis of the diamond Schottky PIN Diode (SPIND) performance and fabrication.

ParameterValueUnitContext
Maximum Operating Temperature873KStable operation demonstrated
Forward Current Density (JF)>3000A/cm²Measured at 8 V (Device #1)
Rectification Factor (R)>10⁹N/AMeasured at 298 K (Room Temperature)
Rectification Factor (R)1100N/AMeasured at 673 K
Minimum Specific On-Resistance (Ron.sp)5.7mΩ·cm²Achieved at 873 K (1.5 V bias)
Substrate Doping (p-type)~1 x 10²⁰cm⁻³Highly Boron-Doped (Type IIb)
N-Layer Doping (n-type)<10¹⁹cm⁻³Phosphorus-Doped
Intrinsic (i) Layer Thickness500nmCVD Grown
N-Layer Thickness100nmCVD Grown
Extracted Richardson’s Constant (A**)81.16 ± 8.9A/cm²·K²Using Tung’s Inhomogeneity Model
Metal Stack CompositionTi/Pt/AuN/A50nm/50nm/150nm

The diamond SPIND structure was fabricated using high-quality CVD growth on HPHT substrates, followed by standard semiconductor processing techniques.

  1. Substrate Selection: Used (100)-oriented Type IIb Boron-Doped diamond substrate (p-type, ~1 x 10²⁰ cm⁻³).
  2. CVD Growth of I-Layer: Intrinsic diamond layer (500 nm) grown in three stages using Hā‚‚ (392-400 sccm), CHā‚„ (0.75 sccm), and Oā‚‚ (0.75 sccm) at 60 Torr pressure and temperatures ranging from 704 °C to 807 °C.
  3. CVD Growth of N-Layer: N-type phosphorus-doped layer (100 nm, <10¹⁹ cm⁻³) grown in two stages using Hā‚‚ (357-400 sccm), CHā‚„ (7.0 sccm), and TMP/Hā‚‚ (40 sccm) at 65-75 Torr pressure and temperatures up to 1025 °C.
  4. Mesa Isolation: Al hard mask patterning followed by Inductively Coupled Plasma / Reactive Ion Etching (ICP/RIE) using Oā‚‚/SF₆ plasma, etching down to the middle of the i-layer.
  5. Surface Treatment: Samples were immersed in a Hā‚‚SOā‚„:HNOā‚ƒ (3:1) acid mixture at 220 °C to achieve oxygen termination and remove surface conduction.
  6. Metal Contact Deposition: Ti/Pt/Au (50nm/50nm/150nm) metal contacts were deposited via e-beam evaporation and patterned using a lift-off process.
  7. Contact Annealing: Metal contacts were annealed at 850 °C to ensure stability and adhesion.
  8. Characterization: I-V measurements were conducted from 298 K to 873 K using a high-temperature stage. Conductive AFM (C-AFM) was used to map local current flow and confirm barrier inhomogeneity.

6CCVD is uniquely positioned to supply the advanced MPCVD diamond materials and fabrication services required to replicate, optimize, and scale this high-temperature SPIND technology. Our capabilities directly address the material and processing needs highlighted in this research.

Requirement from Paper6CCVD Solution & CapabilityTechnical Advantage for Replication/Scaling
Heavily Doped Substrate (p-type, ~10²⁰ cm⁻³)Heavy Boron-Doped Diamond (BDD) Substrates. We offer BDD layers and substrates up to 10mm thick, ensuring high conductivity for the p+ layer.Guarantees low series resistance and efficient backside ohmic contact, critical for achieving high forward current density (>3000 A/cm²).
High-Quality Intrinsic (i) Layer (500 nm)High Purity Single Crystal Diamond (SCD). We supply SCD layers with thicknesses from 0.1 µm up to 500 µm, polished to Ra < 1 nm.Provides the necessary wide bandgap material quality to minimize defects, ensuring high rectification factors (>10⁹) and high breakdown voltage stability at extreme temperatures.
Custom N-Type Doping (Phosphorus)Custom MPCVD Doping Services. 6CCVD can precisely control the incorporation of dopants (e.g., Phosphorus) to achieve the required N-type concentration (<10¹⁹ cm⁻³).Allows researchers to fine-tune the doping profile and layer thickness (100 nm) necessary for optimizing the Schottky barrier height (SBH) and ideality factor (n).
Custom Metalization Stack (Ti/Pt/Au)In-House Metalization Capability. We routinely deposit complex metal stacks including Ti, Pt, and Au, as well as Pd, W, and Cu.We can replicate the exact Ti/Pt/Au stack (50nm/50nm/150nm) used for the stable high-temperature Schottky contact, ensuring thermal reliability up to 873 K.
Large Area Device ScalingLarge Format PCD/SCD Wafers. We offer plates and wafers up to 125mm (PCD) and large-area SCD, polished to Ra < 5 nm (PCD).Enables the transition from research-scale devices to commercial-scale power modules, maintaining uniformity and quality across large areas.
Engineering Support for SBH ControlIn-House PhD Engineering Team. Our experts specialize in diamond surface termination and interface engineering, crucial for controlling SBH inhomogeneity.Provides direct consultation to assist engineers in material selection and surface preparation protocols to achieve desired device characteristics and thermal stability for high-temperature applications (e.g., Venus environment).

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

View Original Abstract

In this work, the high temperature performance of a diamond Schottky PIN diode is reported in the range of 298-873 K. The diamond diode exhibited an explicit rectification up to 723 K with an excellent forward current density of &gt;3000 A/cm<sup>2</sup>. The stability of the diode was investigated by exposing the sample to high temperature cycles (up to 873 K) for more than 10 times (totaling up to 120 hours), which exhibited no change between the I-V characteristics measured in each cycle. The dependence of ideality factor and Schottky barrier height on temperature along with an extracted Richardson’s constant much smaller than the theoretical value (0.0461 A/cm<sup>2</sup>.K<sup>2</sup>), motivated us to study the possible reason for this anomaly. A modified thermionic emission model following Tung’s analysis was used to explain the experimental observations. The model assumed the presence of inhomogeneous Schottky barrier heights leading to a reduced effective area and yielded a Richardson’s constant closer to the theoretical value. Conductive atomic force microscopy studies were conducted, which concurred with the electrical data and confirmed the presence of inhomogeneous Schottky barrier heights.

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