Skip to content

Direct-bandgap emission from hexagonal Ge and SiGe alloys

MetadataDetails
Publication Date2020-04-08
JournalNature
AuthorsElham Fadaly, Alain Dijkstra, Jens RenĂš Suckert, Dorian Ziss, Marvin A. J. van Tilburg
InstitutionsFriedrich Schiller University Jena, Technical University of Munich
Citations351
AnalysisFull AI Review Included
  • Direct Bandgap Breakthrough: The research demonstrates efficient, direct bandgap light emission from hexagonal (WZ structure) Germanium (Ge) and Silicon-Germanium (SiGe) alloys, overcoming the indirect bandgap limitation of conventional cubic Si and Ge.
  • Si-Compatibility: Hexagonal Si1-xGex is presented as an ideal material system for monolithic integration, fully uniting electronic and optoelectronic functionalities on a single silicon chip.
  • High Emission Efficiency: The radiative recombination lifetime is measured to be sub-nanosecond (~1 ns), comparable to conventional direct bandgap III-V semiconductors (like GaAs or InP).
  • Tunability: The direct bandgap emission wavelength can be continuously tuned across the 0.3 eV to 0.7 eV range by controlling the Ge content (x > 0.65) in the Hex-Si1-xGex alloy.
  • Radiative Performance: The calculated radiative coefficient (B-coefficient) for Hex-Si0.20Ge0.80 is 0.7 x 10-10 cm3/s to 11 x 10-10 cm3/s, which is up to 5 orders of magnitude larger than cubic Si.
  • Thermal Stability: The radiative efficiency is nearly temperature independent up to 220 K for high-quality samples, confirming strong evidence for pure radiative recombination in the degenerate doping limit.
ParameterValueUnitContext
Direct Bandgap Conditionx > 0.65Ge Content (x)Hex-Si1-xGex alloy
Tunable Emission Range0.3 - 0.7eVHex-Si1-xGex alloy
Hex-Ge Bandgap (4 K)0.353eVLowest temperature measurement
Hex-Ge Bandgap (300 K)0.28eVRoom temperature measurement
Radiative Lifetime (Hex-Si0.20Ge0.80)~1nsLow temperature (4 K)
Radiative Lifetime (Hex-Si0.20Ge0.80)0.46 - 0.98nsRange across 60 wires at 300 K
Radiative Coefficient (Brad)0.7 x 10-10 to 11 x 10-10cm3/sHex-Si0.20Ge0.80 (Comparable to GaAs)
Unintentional n-Doping (As)9 x 1018cm-3Estimated donor concentration
Stacking Fault Density2 - 4SFs/”mAlong the crystalline [0001] direction
Hex-Ge Debye Temperature66KFitted from bandgap shrinkage (Vina equation)
PL Quenching Ratio (4K/300K)15 - 100FactorHex-SiGe, favorable compared to III-V
Hex-Si0.20Ge0.80 Lattice Parameter (a)3.9505 ± 0.0008AngstromIn-plane lattice parameter (XRD)
Hex-Si0.20Ge0.80 Lattice Parameter (c)6.5257 ± 0.0001AngstromOut-of-plane lattice parameter (XRD)
  1. Template Preparation: Gold (Au) catalyst seeds were deposited onto a GaAs (111)B substrate using electron beam lithography.
  2. Core Nanowire (NW) Growth (MOVPE VLS): Wurtzite (WZ) Gallium Arsenide (GaAs) core NWs (~35 nm diameter) were grown via Metal Organic Vapor Phase Epitaxy (MOVPE) using the Vapor-Liquid-Solid (VLS) mechanism.
    • Temperature: 650 °C.
    • Precursors: Trimethylgallium (TMGa) and Arsine (AsH3).
    • V/III Ratio: 2.4.
  3. Catalyst Removal: The Au catalytic particles were removed using wet chemical etching (cyanide-based solution) to prevent gold contamination in the subsequent shell growth.
  4. Shell Growth (MOVPE Epitaxy): Thick (200-400 nm) Hexagonal (WZ) Si1-xGex shells were grown epitaxially around the WZ-GaAs cores.
    • Temperature: 650-700 °C.
    • Precursors: Germane (GeH4) and Disilane (Si2H6).
  5. Structural Characterization: High-resolution X-ray Diffraction (XRD) using synchrotron radiation (DESY P08 beamline) and Transmission Electron Microscopy (TEM/HAADF-STEM) confirmed the hexagonal crystal structure (ABAB stacking) and high crystal quality.
  6. Compositional Analysis: Electron Dispersive X-ray (EDX) spectroscopy and Atom Probe Tomography (APT) were used to confirm core/shell geometry and determine Ge content and unintentional Arsenic (As) doping levels.
  7. Optical Characterization: Power and temperature-dependent Photoluminescence (PL) spectroscopy and Time-Correlated Single Photon Counting (TCSPC) were performed on single nanowires to measure emission spectra, lifetimes, and efficiency. Data were fitted using the Lasher-Stern-WĂŒrfel (LSW) model to confirm Band-to-Band (BtB) recombination.
  • Silicon Photonics and Optoelectronics: Enabling the monolithic integration of efficient light sources (lasers, LEDs, modulators) directly onto silicon chips, reducing stray capacitances and energy consumption.
  • Optical Interconnects: High-speed, low-energy data transfer within computing systems and data centers, particularly relevant for 2 ”m communications.
  • Quantum Photonic Circuits: Potential use in silicon-based quantum technologies due to the direct bandgap and strong optical matrix element.
  • Optical Sensing: Applications in integrated optical sensors and detectors, leveraging the tunable emission spectrum (0.3 eV to 0.7 eV).
  • Green Information Technology: Reducing the energy footprint of information and communication technologies by improving the efficiency of on-chip light generation.