Mn-intercalated MoSe2 under pressure - Electronic structure and vibrational characterization of a dilute magnetic semiconductor
At a Glance
Section titled āAt a Glanceā| Metadata | Details |
|---|---|
| Publication Date | 2020-09-22 |
| Journal | The Journal of Chemical Physics |
| Authors | Shunda Chen, Virginia L. Johnson, Davide Donadio, Kristie J. Koski, Shunda Chen |
| Institutions | University of California, Davis, George Washington University |
| Citations | 9 |
| Analysis | Full AI Review Included |
Technical Documentation & Analysis: High-Pressure 2D Material Characterization
Section titled āTechnical Documentation & Analysis: High-Pressure 2D Material CharacterizationāExecutive Summary
Section titled āExecutive SummaryāThis research investigates the electronic and vibrational properties of Mn-intercalated Molybdenum Diselenide (MoSeā) under high pressure, a study critically dependent on high-quality diamond components.
- Core Application: Development of dilute magnetic semiconductors (DMS) and new materials for spintronic applications by chemically and thermodynamically tuning 2D layered materials.
- Methodology: Pressure-dependent Raman scattering was performed using a Diamond Anvil Cell (DAC) up to 7 GPa, requiring robust, high-purity diamond anvils for optical access and mechanical integrity.
- Key Material Modification: Intercalation of manganese (Mn) into the van der Waals gap of MoSeā shifts the Fermi level into the conduction band, resulting in an n-type semiconductor with significant spin polarization.
- Pressure Effects: High pressure activates previously Raman-inactive phonon modes (Aāu) and induces a new Mn-Se collective vibrational mode (~250 cmā»Ā¹) upon decompression, suggesting pressure-induced bonding and structural transitions.
- Mechanical Enhancement: Mn intercalation increases the materialās stiffness, raising the isothermal bulk modulus (BT) from 45.7 GPa (pristine MoSeā) to 51.3 GPa (Mn0.125MoSeā).
- Strategic Advantage: The technique of intercalation combined with high pressure offers a route to bypass concentration limitations typically found in dilute magnetic doping, enabling high concentrations of spin-polarized carriers (up to ~2 x 1020 cmā»Ā³).
Technical Specifications
Section titled āTechnical SpecificationsāHard data extracted from the research paper detailing experimental and calculated parameters.
| Parameter | Value | Unit | Context |
|---|---|---|---|
| Maximum Applied Pressure | 7 | GPa | Hydrostatic conditions maintained in the DAC |
| DAC Anvil Culet Diameter | 0.6 | mm | Size of the Boehler anvils used for compression |
| Gasket Hole Diameter | 250 | µm | Sample containment area within the DAC |
| MoSeā Platelet Size | 1 - 100 | µm | Single-crystal platelets used for intercalation |
| MoSeā Thickness Range | Tens of nm to microns | µm | Thickness of the layered material |
| Intercalant Concentration (Experimental) | ~1 - 2 | atomic % | Mn0.02MoSeā |
| Experimental Lattice Parameter āaā (Mn0.02MoSeā) | 3.336 (±0.005) | Ć | 1.5% in-plane expansion upon intercalation |
| Experimental Lattice Parameter ācā (Mn0.02MoSeā) | 12.940 (±0.005) | Ć | Cross-plane expansion upon intercalation |
| Ambient Magnetic Moment (Mn0.03MoSeā) | 5.00 | µB | Total magnetic moment at 0 GPa |
| Calculated Bulk Modulus (Pristine MoSeā) | 47.9 | GPa | DFT calculation (Experimental: 45.7 GPa) |
| Calculated Bulk Modulus (Mn0.125MoSeā) | 51.3 | GPa | DFT calculation, indicating increased stiffness |
| New Mn-Se Raman Mode Frequency | ~250 | cmā»Ā¹ | Observed post decompression |
| Spin-Polarized Carrier Concentration (2H Phase) | Up to ~2 x 1020 | cmā»Ā³ | Predicted maximum for spintronic applications |
Key Methodologies
Section titled āKey MethodologiesāA concise, ordered list detailing the experimental and computational recipe parameters.
- Host Material Preparation: Molybdenum diselenide (MoSeā) single-crystal platelets were deposited onto fused silica substrates.
- Manganese Intercalation: Zero-valent manganese was intercalated via the decomposition of dimanganese decacarbonyl (C10O10Mn2) in dilute acetone.
- Reaction Conditions: The reaction was conducted under an inert Nā atmosphere at a controlled temperature of 48 °C for approximately 1.5 to 2.5 hours.
- High-Pressure Setup: Pressures up to 7 GPa were generated using an Alamax EasyLab mini-Bragg Diamond Anvil Cell (DAC) equipped with 0.6 mm culets.
- Pressure Medium: A 4:1 v/v methanol:ethanol solution was used to ensure relatively hydrostatic pressure conditions.
- Raman Excitation: Raman spectra were acquired using a 532 nm Coherent Sapphire laser operating at <1 mW power on the sample, utilizing an 1800 groove/mm grating for high resolution.
- Structural Confirmation: Intercalation and structural integrity were confirmed using Scanning Electron Microscopy (SEM), Energy Dispersive X-ray Spectroscopy (EDX), Transmission Electron Microscopy (TEM), and X-ray Diffraction (XRD).
- Computational Modeling: Density Functional Theory (DFT) calculations were performed using the LSDA+U method (Hubbard Ueff = 4 eV for Mo and Mn) and Density-Functional Perturbation Theory (DFPT) to model phonon frequencies under pressure.
6CCVD Solutions & Capabilities
Section titled ā6CCVD Solutions & CapabilitiesāThis research highlights the critical need for high-performance optical components capable of withstanding extreme mechanical stress while maintaining optical clarity. 6CCVD specializes in the MPCVD diamond materials necessary to replicate and advance high-pressure studies in spintronics and 2D materials.
Applicable Materials for High-Pressure Research
Section titled āApplicable Materials for High-Pressure Researchā| Application Requirement | 6CCVD Material Recommendation | Technical Justification |
|---|---|---|
| Diamond Anvil Cell (DAC) Anvils | Optical Grade Single Crystal Diamond (SCD) | SCD offers the highest mechanical strength and lowest defect density, essential for achieving and maintaining hydrostatic pressures up to 7 GPa and far beyond. Our SCD is Type IIa, ensuring excellent transparency for the 532 nm Raman laser used in this study. |
| High-Resolution Optical Measurements | Ultra-Low Birefringence SCD | Critical for polarized Raman scattering and minimizing signal distortion under high strain. 6CCVDās SCD is grown and processed to achieve Ra < 1 nm polishing, ensuring minimal light scattering and superior optical performance. |
| High-Pressure Substrates | SCD Substrates (up to 10 mm thick) | For future experiments requiring integrated electrical contacts or thermal management, our thick SCD substrates provide unmatched thermal conductivity and mechanical stability. |
| Integrated Spintronic Devices | Boron-Doped Diamond (BDD) | For electrical resistivity studies mentioned in the conclusions, BDD offers a stable, conductive platform for creating electrodes or active layers in high-pressure environments. |
Customization Potential for Advanced Spintronics
Section titled āCustomization Potential for Advanced SpintronicsāThe complexity of 2D material research often demands non-standard geometries and integrated functionalities. 6CCVD is uniquely positioned to support the next generation of high-pressure spintronic experiments:
- Custom Dimensions and Shaping: While the paper used 0.6 mm culets, 6CCVD can supply SCD plates and wafers up to 125 mm in size, which can be custom-cut and shaped using our in-house laser processing capabilities to meet precise DAC anvil geometries, including specific culet sizes and bevels.
- Advanced Metalization: The development of spintronic devices requires precise electrode deposition. 6CCVD offers internal metalization services, including deposition of Au, Pt, Pd, Ti, W, and Cu, allowing researchers to integrate electrical contacts directly onto diamond substrates or protective layers for in situ resistivity measurements under pressure.
- Surface Finish: Our SCD polishing capability achieves surface roughness (Ra) < 1 nm, ensuring optimal optical coupling and minimal scattering losses, crucial for sensitive Raman and optical measurements.
Engineering Support
Section titled āEngineering Supportā6CCVDās in-house PhD team can assist with material selection for similar High-Pressure 2D Material Intercalation projects. We provide consultation on optimizing diamond grade, orientation, and geometry to maximize experimental pressure limits and optical throughput for DAC applications.
For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.
View Original Abstract
Intercalation offers a promising way to alter the physical properties of two-dimensional (2D) layered materials. Here, we investigate the electronic and vibrational properties of 2D layered MoSe2 intercalated with atomic manganese at ambient and high pressure up to 7 GPa by Raman scattering and electronic structure calculations. The behavior of optical phonons is studied experimentally with a diamond anvil cell and computationally through density functional theory calculations. Experiment and theory show excellent agreement in optical phonon behavior. The previously Raman inactive A2u mode is activated and enhanced with intercalation and pressure, and a new Raman mode appears upon decompression, indicating a possible onset of a localized structural transition, involving the bonding or trapping of the intercalant in 2D layered materials. Density functional theory calculations reveal a shift of the Fermi level into the conduction band and spin polarization in MnxMoSe2 that increases at low Mn concentrations and low pressure. Our results suggest that intercalation and pressurization of van der Waals materials may allow one to obtain dilute magnetic semiconductors with controllable properties, providing a viable route for the development of new materials for spintronic applications.
Tech Support
Section titled āTech SupportāOriginal Source
Section titled āOriginal SourceāReferences
Section titled āReferencesā- 2010 - First-principles theory of dilute magnetic semiconductors [Crossref]
- 2010 - A ten-year perspective on dilute magnetic semiconductors and oxides [Crossref]
- 2010 - A window on the future of spintronics [Crossref]
- 2014 - Dilute ferromagnetic semiconductors: Physics and spintronic structures [Crossref]
- 2013 - Mn-doped monolayer MoS2: An atomically thin dilute magnetic semiconductor [Crossref]
- 2013 - Long-range ferromagnetic ordering in manganese-doped two-dimensional dichalcogenides [Crossref]
- 2016 - Robust ferromagnetism in Mn-doped MoS2 nanostructures [Crossref]
- 2015 - Manganese doping of monolayer MoS2: The substrate is critical [Crossref]
- 2018 - Tunable magnetic coupling in Mn-doped monolayer MoS2 under lattice strain [Crossref]
- 2017 - Intrinsic ferromagnetism in Mn-Substituted MoS2 nanosheets achieved by supercritical hydrothermal reaction [Crossref]