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Section

Physical Sciences

Abstract

This work reports on silicon nitride (SiNx) thin film deposited by the Plasma-Enhanced Chemical Vapour Deposition (PECVD) technique. The film was characterized by Variable Angle Spectroscopic Ellipsometry (VASE) to obtain optical constants 𝑛, π‘˜ and thickness using the Cauchy layer built on the Lorentz oscillator model and the B-spline model. The determined optical band gap πΈπ‘œπ‘π‘‘π‘–π‘π‘Žπ‘™ for direct transition was 3.2 𝑒𝑉 and that for indirect transition was 2.13 𝑒𝑉. Film characterization was performed by Fourier Transform Infra-Red spectroscopy (FTIR) at two different angles of incidence of 15 degrees to probe deep layers and 65 degrees (Brewster’s angle) to excite both Longitudinal and Transversal Optical (LO and TO) modes, respectively. In the FTIR experiment photons in the IR region revealed dominant bond vibrations of excited covalent bonds e.g. 𝑆𝑖 βˆ’ 𝑁 stretching mode at 850 π‘π‘šβˆ’1 (TO) and the 𝑆𝑖 βˆ’ 𝑁 rocking mode at 1180 π‘π‘šβˆ’1 (LO). We could also see the 𝑁 βˆ’ 𝐻2 scissors and 𝑆𝑖 βˆ’ 𝐻 stretching mode at 2180 π‘π‘šβˆ’1 and 3350 π‘π‘šβˆ’1 , respectively. X-ray Photoemission Spectroscopy (XPS) characterization assisted us in performing elemental composition analysis of the sample. In the XPS spectrum 𝑆𝑖 2𝑝 peak of 𝑆𝑖𝑁π‘₯ was located at 101.4 eV, and that of 𝑆𝑖𝑂2 due to oxygen contamination was located at 102.764 eV. High-Resolution Scanning Electron Microscope (HR-SEM) and Atomic Force Microscope (AFM) characterization indicated good surface roughness suitable for optical device fabrication based on 𝑆𝑖𝑁π‘₯ as an antireflection coating and passivation layer for Si-based solar cells, as well as an insulating layer in microelectronics. A Hall-effect Measurement System (HMS) was used to obtain the film carrier concentration of 1.595 Γ— 1017 π‘π‘šβˆ’3 , mobility of ~1.155 1 π‘π‘š2 π‘‰π‘œπ‘™π‘‘βˆ’π‘ π‘’π‘ , resistivity of ~3.387 Γ— 101 Ξ©cm and the conductivity of 2.952 Γ— 10βˆ’2 . Film compressive and tensile Ξ©cm stress was determined using a Veeco Dektak Stylus profilometer. The measured stress induced in the film in the directions π‘₯ βˆ’ and 𝑦 βˆ’ are 𝜎π‘₯ = 93.46 π‘€π‘π‘Ž and πœŽπ‘¦ = 137.13 π‘€π‘π‘Ž, respectively. Such films are also common in microelectronics as diffusion barriers and low-temperature superconducting devices where amorphous 𝑆𝑖𝑁π‘₯ films exhibit less dielectric loss than silicon dioxide (𝑆𝑖𝑂2 ) films.

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