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Diamond films obtained on silicone substrates by the CVD method and properties of structures based on them

MetadataDetails
Publication Date2023-06-01
JournalPhysical Sciences and Technology
AuthorsА. С. Саидов, Sh. N. Usmonov, Sh. N. Usmonov, U. Kh. Rakhmonov
InstitutionsAcademy of Sciences Republic of Uzbekistan
AnalysisFull AI Review Included
  • Novel Buffer Layer Identification: Researchers successfully grew polycrystalline diamond films on n-type Si (111) substrates via Chemical Vapor Deposition (CVD) and identified a previously unreported p(15R-SiC)1-x(Cdiamond)x transition buffer layer formed at the interface.
  • High Conductivity: Despite intentional nitrogen doping (via NH3), the resulting diamond films exhibited p-type conductivity with high charge carrier concentrations ((2-4)·1017 cm-3) and high electron mobility (up to 1010 cm2/(V·s)).
  • Electroluminescence Demonstrated: The nSi - p(15R-SiC)1-x(Cdiamond)x heterojunction showed a visible whitish-blue electroluminescence glow during reverse bias breakdown (~14-15 V).
  • Photon Conversion Mechanism: The structure facilitates the absorption of high-energy, short-wavelength photons (blue-violet) and their re-emission as longer-wavelength photons, which can be absorbed efficiently by the underlying silicon.
  • Space Application Potential: This photon conversion and the inherent radiation resistance of diamond make these structures highly promising for enhancing the efficiency and durability of silicon solar cells used in space environments.
ParameterValueUnitContext
Substrate MaterialSingle-crystal Silicon (Si)N/An-type, (111) orientation
Substrate Resistivity~10Ω cmInitial Si substrate
Diamond Film StructurePolycrystallineN/AFine-grained, continuous film
Crystallite Size2-3µmGrain size of individual single crystals
CVD Filament Temperature2100-2150°CDuring diamond deposition
Substrate Temperature850-900°CDuring diamond deposition
Average Growth Rate0.2-0.3µm/hCVD process rate
Total Gas Flow Rate50-60cm3/minCH3OH + H2 + NH3 mixture
Reactor Pressure50-60TorrDuring deposition
H2/Methanol Ratio0.5-1.0%In total gas flow
Transition Layer Polytype15R-SiCN/AForms the p(15R-SiC)1-x(Cdiamond)x solid solution
Raman Shift (Diamond Peak)1351cm-1Corresponds to the polycrystalline diamond structure
Reverse Breakdown Voltage~14-15VnSi - p(15R-SiC)1-x(Cdiamond)x heterojunction
Film Conductivity Typep-typeN/ADespite nitrogen doping
Carrier Concentration(2-4)·1017cm-3Measured via Hall method
Electron Mobility950-1010cm2/(V·s)Measured via Hall method
  1. Substrate Selection: Used n-type single-crystal silicon wafers (10x10x0.3 mm) cut in the (111) direction with a specific resistance of ~10 Ω cm.
  2. Hydrogen Etching Pre-treatment: Silicon surfaces were cleaned immediately prior to epitaxy using hydrogen etching to remove surface SiO2 and create dangling Si bonds.
    • Process conditions: 1800 °C filament temperature, 3 min duration, 1000 cm3/min H2 flow.
  3. Chemical Vapor Deposition (CVD): Diamond films were grown using a well-known CVD technology in a hydrogen-methanol (CH3OH) gas mixture.
    • Ammonia (NH3) was added to the mixture to introduce nitrogen impurities, targeting NV center formation.
  4. Structural Analysis: Film existence and quality were confirmed using microhardness testing, Scanning Electron Microscopy (Jeol JSM-5910LV), and X-ray analysis (JED-2200).
  5. Raman Spectroscopy: Raman spectra (514 nm laser, 300 K) were used to confirm the polycrystalline diamond structure (peak at 1351 cm-1) and identify the 15R-SiC polytype transition layer.
  6. Electrical and Optical Characterization: Dark current-voltage characteristics were measured, revealing reverse breakdown at 14-15 V. Electroluminescence was observed during breakdown. Hall measurements determined carrier concentration and mobility.
  • Space Photovoltaics: Used as a protective, radiation-resistant coating for silicon solar cells, extending operational life under cosmic radiation.
  • Solar Energy Conversion: Functions as an active layer or transparent window that converts high-energy, short-wavelength solar photons into longer-wavelength photons that are more efficiently absorbed by the underlying silicon junction.
  • Quantum Computing and Sensing: Nitrogen doping targets the creation of negatively charged Nitrogen-Vacancy (NV-) defects, which are essential components for solid-state qubits and spin detection.
  • Optoelectronic Devices: The highly conductive p(15R-SiC)1-x(Cdiamond)x layer can serve as a transparent conductive “window” in micro- and optoelectronic devices, including LEDs and lasers based on NV centers.
  • High-Power Electronics: Diamond’s wide bandgap and high thermal conductivity make it suitable for high-voltage and high-temperature diodes, crucial for power electronics operating in extreme conditions.
View Original Abstract

At present, the technology of obtaining diamond films on silicon and other substrates is well studied. However, in all published works to date, there has been no report of a layer of silicon carbide formed between the diamond film and the silicon substrate. The presence of a layer (15R-SiС)1-x(Cdiamond)x in the structure was revealed in the studies of structures with a diamond film obtained by us on silicon substrates by chemical vapor deposition. Diamond films were obtained on single-crystal silicon substrates with (111) orientation and n-type conductivity by the well-known CVD technology in a hydrogen-methanol (CH3OH) mixture with the addition of a certain amount (know-how) of ammonia (NH3). The diamond films consisted of small single crystals 3-5 µm in size, closely interlocked and constituting a continuous film. When studying the current-voltage characteristics of structures created on the basis of the obtained diamond films, a blue-white glow with a blue-violet tint was observed, which is explained by the mixing of blue-violet photons with photons re-emitted in the diamond film.