SiGeSn Quantum Dots in HfO2 for Floating Gate Memory Capacitors
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2022-03-07 |
| Journal | Coatings |
| Authors | CÄtÄlin Palade, A. Slav, Ovidiu Cojocaru, V. S. Teodorescu, T. StoĂŻca |
| Institutions | University of Bucharest, Academy of Romanian Scientists |
| Citations | 12 |
| Analysis | Full AI Review Included |
Executive Summary
Section titled âExecutive SummaryâThis research demonstrates the successful fabrication and characterization of SiGeSn Quantum Dots (QDs) embedded in HfO2 for high-performance, CMOS-compatible floating gate memory capacitors.
- High Performance: The optimized structures achieved high frequency-independent memory windows of 3-4 V and stored electron densities up to 2 x 1013 electrons/cm2.
- Low Thermal Budget: The presence of Sn in the SiGe intermediate layer successfully decreased the SiGe crystallization temperature to 520-530 °C RTA, significantly improving CMOS compatibility compared to pure Si or Ge NC formation.
- Dual QD Formation: Optimal annealing (520-530 °C) resulted in two distinct types of crystalline SiGeSn QDs: low Sn content (2 at.%) QDs positioned inside the floating gate, and high Sn content (up to 12.5 at.%) QDs located at the floating gate/HfO2 interfaces.
- Charge Storage Mechanism: Memory effects are controlled by SiGeSn-related trapping states and low-ordering clusters at lower RTA temperatures (325-450 °C), transitioning to crystalline SiGeSn QDs as the primary storage centers at 520-530 °C.
- Fabrication Method: The 3-layer stack (Gate HfO2/SiGeSn-HfO2/Tunnel HfO2) was fabricated using magnetron sputtering followed by Rapid Thermal Annealing (RTA) for nanocrystallization.
- Failure Mechanism: RTA temperatures of 600 °C or higher led to a pronounced decrease in memory window, attributed to enhanced Sn diffusion and segregation, potentially increasing the conductivity of the HfO2 layers.
Technical Specifications
Section titled âTechnical Specificationsâ| Parameter | Value | Unit | Context |
|---|---|---|---|
| Maximum Memory Window (ÎVFB) | 4.0 | V | M1 structure, 530 °C RTA, 5 min |
| Maximum Stored Electron Density (n) | 2.0 x 1013 | electrons/cm2 | M1 structure, 530 °C RTA, 5 min |
| Optimal RTA Temperature Range | 520-530 | °C | For crystalline QD formation and maximum performance |
| SiGeSn QD Composition (Internal) | ~2.1 | at.% Sn | Low Sn content QDs inside floating gate |
| SiGeSn QD Composition (Interface) | ~12.5 | at.% Sn | High Sn content QDs at HfO2 interfaces |
| SiGeSn QD Diameter (Estimated) | ~5 | nm | Ge-rich QDs (HRTEM) |
| SiGeSn Crystallization Structure | Diamond | N/A | Observed structure, favored by Sn presence |
| Ge-Ge Raman Shift (Peak 1) | ~300 | cm-1 | Low Sn content SiGeSn NCs |
| Ge-Ge Raman Shift (Peak 2) | ~290 | cm-1 | High Sn content SiGeSn NCs |
| Gate HfO2 Thickness (M1 Design) | 16-17 | nm | Control oxide layer |
| Floating Gate Thickness (M1 Design) | 9-10 | nm | Intermediate SiGeSn-HfO2 layer |
| Tunnel HfO2 Thickness (M1 Design) | 7-8 | nm | Tunnel oxide layer |
| HfO2 NC Size (Gate Oxide) | 10-12 | nm | Monoclinic phase (HRTEM/XRD) |
| Si Substrate Resistivity | 7-14 | Ωcm | p-Si (100) |
Key Methodologies
Section titled âKey MethodologiesâThe MOS capacitor structures were fabricated using a combination of magnetron sputtering and rapid thermal annealing (RTA).
- Substrate Preparation:
- (100) p-Si substrates (7-14 Ωcm) were used, followed by standard cleaning procedures.
- Thin Film Deposition (Magnetron Sputtering):
- Tunnel HfO2: Deposited first using an HfO2 target (45-55 W RF power). Thickness range: 4-8 nm.
- Floating Gate (SiGeSn-HfO2): Co-deposited for the intermediate layer (7-12 nm).
- Targets used: SiGe (25-35 W DC), Sn (3.5-10 W DC), and HfO2.
- Designed composition: 10% Sn: 90% SiGe (vol.) and 80% SiGeSn: 20% HfO2 (vol.).
- Gate HfO2 (Control Oxide): Deposited last using an HfO2 target. Thickness range: 16-21 nm.
- Nanostructuring (Rapid Thermal Annealing - RTA):
- Annealing performed in N2 (6N purity) atmosphere.
- Temperature range investigated: 325-600 °C.
- Optimal RTA conditions for QD formation: 520-530 °C for 5-10 min.
- Electrode Deposition:
- Top and bottom Al electrodes were deposited via thermal evaporation.
- Top contacts utilized shadow masks (1 mm x 1 mm area).
- Characterization Techniques:
- Structural/Morphological: Cross-section TEM (XTEM/HRTEM) for layer thickness, lattice fringes (d111), and QD size/location.
- Crystalline Structure: X-ray Diffraction (XRD) for HfO2 monoclinic phase and SiGeSn (111) diamond peak identification.
- Composition/Crystallinity: Raman Spectroscopy (325 nm UV laser excitation) for Ge-Ge mode analysis and Sn content estimation.
- Electrical Performance: Capacitance-Voltage (C-V) hysteresis loops measured at 100, 500 kHz, and 1 MHz to determine memory window (ÎVFB) and stored charge density (n).
Commercial Applications
Section titled âCommercial ApplicationsâThe demonstrated SiGeSn/HfO2 floating gate technology is highly relevant for next-generation micro/nanoelectronics due to its material compatibility and performance metrics.
- High-Density Non-Volatile Memories (NVMs): Directly applicable as high-performance charge storage nodes in Flash memory architectures, offering high stored electron density (up to 2 x 1013 electrons/cm2).
- CMOS Integration: The use of HfO2 (a high-k dielectric already standard in CMOS) and the reduced thermal budget (~530 °C RTA) due to Sn alloying facilitate easier integration into existing silicon manufacturing processes.
- Photonic Flash Memories: The SiGeSn alloy exhibits high Short-Wave Infrared (SWIR) photosensitivity. This enables potential development of memory devices where the threshold voltage shift can be controlled optically, leading to faster access speeds and lower energy consumption.
- Advanced Gate Dielectrics: HfO2 is a key material for post-Si electronic devices. This work validates its use not only as a gate oxide but also as a matrix for embedded Group IV QDs.
- Integrated Ferroelectric Devices: The HfO2 matrix shows potential for nanoscale ferroelectricity, suggesting a pathway for developing integrated ferroelectric memory devices or devices leveraging both charge storage and ferroelectric effects.
View Original Abstract
Group IV quantum dots (QDs) in HfO2 are attractive for non-volatile memories (NVMs) due to complementary metal-oxide semiconductor (CMOS) compatibility. Besides the role of charge storage centers, SiGeSn QDs have the advantage of a low thermal budget for formation, because Sn presence decreases crystallization temperature, while Si ensures higher thermal stability. In this paper, we prepare MOS capacitors based on 3-layer stacks of gate HfO2/floating gate of SiGeSn QDs in HfO2/tunnel HfO2/p-Si obtained by magnetron sputtering deposition followed by rapid thermal annealing (RTA) for nanocrystallization. Crystalline structure, morphology, and composition studies by cross-section transmission electron microscopy and X-ray diffraction correlated with Raman spectroscopy and C-V measurements are carried out for understanding RTA temperature effects on charge storage behavior. 3-layer morphology and Sn content trends with RTA temperature are explained by the strongly temperature-dependent Sn segregation and diffusion processes. We show that the memory properties measured on Al/3-layer stack/p-Si/Al capacitors are controlled by SiGeSn-related trapping states (deep electronic levels) and low-ordering clusters for RTA at 325-450 °C, and by crystalline SiGeSn QDs for 520 and 530 °C RTA. Specific to the structures annealed at 520 and 530 °C is the formation of two kinds of crystalline SiGeSn QDs, i.e., QDs with low Sn content (2 at.%) that are positioned inside the floating gate, and QDs with high Sn content (up to 12.5 at.%) located at the interface of floating gate with adjacent HfO2 layers. The presence of Sn in the SiGe intermediate layer decreases the SiGe crystallization temperature and induces the easier crystallization of the diamond structure in comparison with 3-layer stacks with Ge-HfO2 intermediate layer. High frequency-independent memory windows of 3-4 V and stored electron densities of 1-2 à 1013 electrons/cm2 are achieved.
Tech Support
Section titled âTech SupportâOriginal Source
Section titled âOriginal SourceâReferences
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