Boron-carbon (BxC) thin films enriched in 10B are potential neutron converting layers for 10Bbased solid-state neutron detectors given the good neutron absorption cross-section of 10B atoms in the thin film. Chemical Vapour Deposition (CVD) of such films faces the challenge that the maximum temperature tolerated by the aluminium substrate is 660 °C and low temperature CVD routes for BxC films are thus needed. This thesis presents the use of two different organoboron precursors, triethylboron –B(C₂H₅)₃ (TEB) and trimethylboron – B(CH₃)₃ (TMB) as single-source precursors for CVD of BxC thin films.

The CVD behaviour of TEB in thermal CVD has been studied by both BxC thin film deposition and quantum chemical calculations of the gas phase chemistry at the corresponding CVD conditions. The calculations predict that the gas phase reactions are dominated by β-hydride eliminations of C₂H₄ to yield BH3. In addition, a complementary bimolecular reaction path based on H2-assisted C₂H₆ elimination to BH₃ is also present at lower temperatures in the presence of hydrogen molecules. A temperature window of 600 – 1000 °C for deposition of X-ray amorphous B_xC films with 2.5 ≤ x ≤ 4.5 is identified showing good film density (2.40 – 2.65 g/cm³) which is close to the bulk density of crystalline B4C, 2.52 g/cm³ and high hardness (29 – 39 GPa). The impurity level of H is lowered to < 1 at. % within the temperature window.

Plasma chemical vapour deposition has been studied using TMB as single-source precursor in Ar plasma for investigating B_xC thin film deposition at lower temperature than allowed by thermal CVD and further understanding of thin film deposition process. The effect of plasma power, total pressure, TMB and Ar gas flow on film composition and morphology are investigated. The highest B/C ratio of 1.9 is obtained at highest plasma power of 2400 W and TMB flow of 7 sccm. The H content in the films seems constant at 15±5 at. %. The B-C bond is dominant in the films with small amount of C-C and B-O bonds, which are likely due to the formation of amorphous carbon and surface oxidation, respectively. The film density is determined as 2.16±0.01 g/cm³ and the internal compressive stresses are measured to be <400 MPa.