Investigation and Comparison of the DIBL Parameter and Thermal Effects of SOD Transistors and SOI Transistors and Improving Them with the Change of Their BOX Thicknesses
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2018-01-01 |
| Journal | Journal of Electronics Cooling and Thermal Control |
| Authors | Nooshien Laderian, Arash Daghighi |
| Institutions | Shahrekord University |
| Analysis | Full AI Review Included |
6CCVD Technical Documentation: High-Power Density CMOS Enabling
Section titled â6CCVD Technical Documentation: High-Power Density CMOS EnablingâAnalysis of Silicon-on-Diamond (SOD) Transistor Thermal and Electrical Optimization
Section titled âAnalysis of Silicon-on-Diamond (SOD) Transistor Thermal and Electrical OptimizationâPaper Analyzed: Laderian, N. and Daghighi, A. (2018) Investigation and Comparison of the DIBL Parameter and Thermal Effects of SOD Transistors and SOI Transistors and Improving Them with the Change of Their BOX Thicknesses.
Executive Summary
Section titled âExecutive SummaryâThis paper validates the use of ultra-high thermal conductivity MPCVD diamond films as the Buried Oxide (BOX) layer in MOSFETs, demonstrating significant performance enhancements necessary for next-generation, high-power integrated circuits.
- Self-Heating Elimination: Replacing standard SiO2 (k = 1.4 W/K·m) with diamond (k ~ 2000 W/K·m) in the BOX layer reduces the active transistor lattice temperature by over 140 K (from 480 K to 330 K), effectively eliminating the critical self-heating effect (SHE) found in Silicon-on-Insulator (SOI) devices.
- High Power Density Enabled: Silicon-on-Diamond (SOD) transistors are shown to sustain power densities over 10 times higher than comparable SOI transistors at the same junction temperature.
- Thermal Crosstalk Challenge: Initial implementations using thick buried diamond layers (100 nm) cause uniform heat distribution, leading to increased thermal crosstalk and high off-currents in neighboring transistors.
- Optimal Geometry Solution: The proposed optimizationâreducing the buried diamond thicknessâdramatically improves performance. Reducing the layer from 100 nm down to 10 nm reduces the thermal tail transferred to neighboring devices (improving thermal crosstalk immunity) and substantially improves the Drain Induced Barrier Lowering (DIBL) factor.
- Critical Need for CVD Diamond: Replicating or extending this research requires high-purity, uniform, ultra-thin diamond films with precise thickness control in the nanometer range, directly aligning with 6CCVDâs core MPCVD capabilities.
Technical Specifications
Section titled âTechnical Specificationsâ| Parameter | Value | Unit | Context |
|---|---|---|---|
| Channel Length | 22 | nm | Standard Transistor Geometry |
| Diamond Thermal Conductivity (k) | 2000 | W/K·m | Material substitute for BOX layer (vs. SiO2) |
| SiO2 Thermal Conductivity (k) | 1.4 | W/K·m | Standard SOI BOX layer |
| SOI Active T (Max Lattice) | 480 | K | Worst-case self-heating effect (SHE) |
| SOD Active T (Max Lattice) | 330 | K | After diamond BOX substitution (75 K reduction) |
| Power Density Sustained (SOD) | 10x | - | Higher than SOI at identical junction T |
| Standard Diamond BOX Thickness | 100 | nm | Initial SOD test thickness |
| Optimized Diamond BOX Thickness | 10 | nm | Achieves identical, optimized DIBL as SOI at 10 nm |
| DIBL (SOI, 100 nm BOX) | 76 | mV/V | Drain Induced Barrier Lowering |
| DIBL (SOD, 100 nm BOX) | 82 | mV/V | Degraded DIBL due to thick diamond layer |
| DIBL Improvement | 8% | - | DIBL of SOD improved by reducing thickness to 10 nm |
| Neighboring T Reduction (100 nm to 10 nm) | 63 | K | Thermal tail reduction (447 K down to 384 K) |
Key Methodologies
Section titled âKey MethodologiesâThe research utilizes advanced simulation techniques to compare and optimize the thermal and electrical performance of SOI and SOD devices.
- Simulation Model: Hydrodynamic Model was used, solving energy conservation equations simultaneously for holes, electrons, and lattice temperature to obtain accurate temperature profiles (Lattice Temperature TL).
- Device Structure: Two structures were compared: Standard SOI MOSFET and SOD MOSFET. Both structures utilized a 22 nm channel length.
- Core Material Change: The Buried Insulating Layer (BOX) material was changed from Silicon Dioxide to MPCVD Diamond.
- Modeling Inclusions: Simulations included complex physical models such as carrier mobility dependence on doping and lattice temperature, Shockley-Reed-Hall recombination, Auger recombination, and temperature-dependent saturation velocities.
- Critical Parameter Sweep: The thickness of the buried diamond layer was systematically varied to determine the optimal structure for mitigating thermal crosstalk and improving DIBL. Tested thicknesses included:
- 100 nm
- 60 nm
- 40 nm
- 10 nm
6CCVD Solutions & Capabilities
Section titled â6CCVD Solutions & CapabilitiesâThe successful implementation of high-performance Silicon-on-Diamond technology hinges on the ability to deposit and process high-quality, ultra-thin diamond films with nanometric precision, a core capability of 6CCVDâs MPCVD manufacturing line.
Applicable Materials
Section titled âApplicable MaterialsâTo replicate and extend the performance demonstrated in this research, engineers require MPCVD materials with exceptional purity and high thermal conductivity:
- Electronic/Optical Grade Single Crystal Diamond (SCD): Required for applications demanding the highest quality, most uniform thermal properties, and minimal defects, ensuring maximum thermal dissipation efficiency (k ~ 2000 W/K·m).
- High-Purity Polycrystalline Diamond (PCD): Applicable for large-area SOD wafers (up to 125mm) where maximizing heat spread across the integrated circuit is paramount for thermal stability.
Customization Potential for SOD Device Fabrication
Section titled âCustomization Potential for SOD Device FabricationâThe key finding of this research is the critical requirement for controlling the diamond BOX layer thickness between 10 nm and 100 nm. 6CCVD is uniquely positioned to supply substrates tailored for this application:
| Requirement from Paper | 6CCVD Capability | Application Benefit |
|---|---|---|
| Ultra-Thin BOX Layers (10 nm to 100 nm) | Precise deposition control from 0.1 ”m (100 nm) and advanced post-processing services (etching/polishing). | Enables optimization of DIBL parameter and thermal crosstalk immunity. |
| Large Scale Integration | Plates/wafers available up to 125mm (PCD). | Supports scaling from R&D (small pieces) to high-volume IC manufacturing. |
| Surface Quality | Polishing capabilities to achieve Ra < 1nm (SCD) or Ra < 5nm (Inch-size PCD). | Ensures low-defect interfaces necessary for high-mobility channel regions in MOSFET fabrication. |
| Contact Integration | In-house custom metalization services (Au, Pt, Ti, W, Cu). | Facilitates reliable ohmic contacts and integration with CMOS fabrication processes. |
| Global Logistics | Global shipping services (DDU default, DDP available). | Ensures rapid delivery of specialized diamond substrates worldwide for time-sensitive R&D projects. |
Engineering Support
Section titled âEngineering SupportâSOD technology represents a major leap in thermal management for high-power density electronics. 6CCVDâs in-house PhD material scientists and technical engineers specialize in characterizing and tuning MPCVD diamond properties. We provide critical support for:
- Determining the optimal material grade (SCD vs. PCD) based on required thermal budget and channel mobility.
- Consultation on achieving precise thickness tolerances and surface preparation (polishing) required for advanced High Power Density CMOS projects.
For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.
View Original Abstract
In this paper, thermal effects and Drain Induced barrier lowering (DIBL) of silicon-on-insulator (SOI) and silicon-on-diamond (SOD) transistors with 22 nm channel lengths using hydrodynamic simulations have been investigated. Thermal conductivity of diamond in contrast to thermal conductivity of silicon dioxide is significantly higher. Hence, the heat transfers faster in silicon-on-diamond transistors. Lattice temperature of SODs is lower than that of similar SOIs. By using SODs in Integrated circuits with the first transistor turning on and active, neighboring transistors will have the same level of heat as the active transistor. As a result, the DIBL factor will be increased; this is an undesired phenomenon in CMOS applications. To resolve this issue, we propose a new method which is the thickness reduction of buried diamond layers inside of transistors. Due to this change, DIBL of active transistor will be improved, the exceeding lattice heat of side transistors will be evacuated through the devices and their temperatures will be deduced in large scale.