Skip to content

Enabling room temperature ferromagnetism in monolayer MoS2 via in situ iron-doping

MetadataDetails
Publication Date2020-04-27
JournalNature Communications
AuthorsShichen Fu, Kyungnam Kang, Kamran Shayan, Anthony Yoshimura, Siamak Dadras
InstitutionsRensselaer Polytechnic Institute, University of Rochester
Citations176
AnalysisFull AI Review Included

This research successfully demonstrates a scalable method for creating room-temperature (RT) ferromagnetic two-dimensional (2D) dilute magnetic semiconductors (DMS), overcoming major limitations of previous extrinsic doping techniques.

  • Core Achievement: Enabling robust ferromagnetism in monolayer Molybdenum Disulfide (MoS2) at 300 K via in situ substitutional Iron (Fe) doping during Low-Pressure Chemical Vapor Deposition (LPCVD).
  • Scalable Synthesis: The Fe atoms substitute Molybdenum (Mo) sites, achieving a doping concentration of 0.3 to 0.5% using a contact-growth LPCVD method, which is highly scalable compared to mechanical exfoliation or ion implantation.
  • RT Ferromagnetism Confirmation: Ferromagnetism is confirmed at ambient conditions (300 K) using both spatially integrating Superconducting Quantum Interference Devices (SQUIDs) and spatially resolving Nitrogen-Vacancy (NV-) center magnetometry.
  • Local Magnetic Field: NV- center magnetometry measured a significant local magnetic field up to 0.5 ± 0.1 mT at room temperature, providing clear evidence of preserved magnetization.
  • Spectroscopic Signature: An unambiguous Fe-related photoluminescence (PL) emission peak was discovered at 2.28 eV, which is stable up to RT and displays pronounced ferromagnetic hysteresis in Magnetic Circular Dichroism (MCD) measurements.
  • Defect Control: Fe doping was found to suppress native sulfur vacancies, resulting in a lower native point defect density compared to undoped CVD-grown MoS2.
ParameterValueUnitContext
Curie Temperature (Tc)>300KFerromagnetism confirmed at ambient conditions (RT).
Fe Doping Concentration0.3 to 0.5%Atomic concentration determined by X-ray Photoelectron Spectroscopy (XPS).
Local Magnetic Field (RT)0.5 ± 0.1mTMeasured via NV- center magnetometry.
Fe-Related PL Emission Peak2.28eVStable up to RT; exhibits strong MCD hysteresis.
Magnetic Circular Dichroism (CD)~40%Observed for the Fe-related emission at 4 K and RT.
Monolayer Thickness0.8nmMeasured via Atomic Force Microscopy (AFM).
MoS2 Raman Mode (E12g)385.4cm-1In-plane vibration mode.
MoS2 Raman Mode (A1g)405.8cm-1Out-of-plane vibration mode.
STEM Intensity Ratio (Fe/Mo)0.38(unitless)Consistent with the atomic number ratio (ZFe=26, ZMo=42).
SQUID Coercive Field (5 K)~3TPronounced M-H hysteresis loop at cryogenic temperature.

The Fe:MoS2 monolayers were synthesized using a Low-Pressure Chemical Vapor Deposition (LPCVD) contact-growth method.

  • Mo Source: A thin MoO3 layer was prepared via Physical Vapor Deposition (PVD) onto a Si substrate with 300 nm thermal oxide.
  • Fe Source: Fe3O4 particles were evenly cast onto a separate SiO2/Si substrate.
  • Contact Growth: The MoO3-deposited substrate and the Fe3O4-coated SiO2/Si substrate were contacted face-to-face.
  • Pre-Annealing: The Fe3O4-coated substrate was annealed at 110 °C for 5 min on a hot plate prior to growth.
  • Ramping: Furnace heated with a ramping rate of 18 °C min-1.
  • Hold Conditions: Held at 850 °C for 15 min.
  • Gas Flow (Initial): Argon (Ar) gas (30 s.c.c.m.) supplied starting at 300 °C.
  • Gas Flow (Reduction): Hydrogen (H2) gas (15 s.c.c.m.) delivered starting at 760 °C.
  • Sulfurization: Sulfur (S) was supplied when the furnace temperature reached 790 °C.
  • Structural/Compositional:
    • High-Angle Annular Dark-Field Scanning Transmission Electron Microscopy (HAADF-STEM) confirmed substitutional Fe incorporation at Mo sites.
    • X-ray Photoelectron Spectroscopy (XPS) determined the Fe atomic concentration (0.3-0.5%).
  • Optical/Electronic:
    • Raman and Photoluminescence (PL) spectroscopy confirmed lattice incorporation and identified the 2.28 eV Fe-related emission.
    • Density Functional Theory (DFT) calculations corroborated the microscopic origin of the 2.28 eV transition.
  • Magnetic:
    • SQUID Magnetometry: Measured bulk magnetization (M-H loops) at 5 K and 300 K, confirming RT ferromagnetism.
    • NV- Center Magnetometry: Nanodiamonds containing NV- centers were spin-coated onto the Fe:MoS2 surface to perform optically detected magnetic resonance (ODMR) measurements, quantifying the local magnetic field (up to 0.5 mT) at RT.

This development of a scalable, RT ferromagnetic 2D semiconductor opens doors for integration into advanced electronic and quantum systems.

  • Spintronics and Data Storage:
    • Development of ultra-low power, high-density non-volatile magnetic memory (MRAM) utilizing spin-polarized charge carriers.
    • Minimizing bit storage size in next-generation computing architectures.
  • Quantum Information Science:
    • Enabling on-chip magnetic manipulation and control of quantum states in 2D heterostructures.
    • Integration into quantum devices requiring localized, stable magnetic fields at ambient conditions.
  • Flexible Electronics:
    • The atomically thin nature of the material allows for potential use in flexible spintronic devices and wearable technology.
  • Advanced Sensors:
    • Creation of highly sensitive magnetic field sensors based on the integration of the ferromagnetic Fe:MoS2 with other 2D materials.