Direct growth of graphene on dielectric or insulating materials via chemical vapor deposition (CVD) offers a novel, transfer-free approach for various applications. However, challenges remain in growing graphene on non-catalytic substrates. In particular, the low growth rate of graphene remains a significant barrier to its large-scale production. In this study, propane (C₃H₈) was used as the carbon source to prepare graphene on commercial alumina fiber fabric (AFF) via CVD, resulting in the synthesis of a novel material: graphene-skinned alumina fiber fabric (GAFF). Through comparative analysis of the graphene growth behaviors using C₃H₈ and traditional carbon sources (CH₄ and C₂H₄) on AFF, the growth mechanism of C₃H₈ was elucidated. The pyrolysis of C₃H₈ generates the unique carbon species C₃H, which exhibits distinct advantages in terms of migration, nucleation, and growth on AFF. Graphene nucleation density using C₃H₈ was found to be 160 times higher than that of CH₄ and 50 times higher than C₂H₄. The resulting GAFF exhibits a wide tunable electrical conductivity range (1 to 7000 Ω·sq⁻¹), high tensile strength (> 170 MPa), lightweight properties, flexibility, and a hierarchical macrostructure. These characteristics make GAFF a promising candidate for various applications, including electromagnetic interference (EMI) shielding.

Direct chemical vapor deposition (CVD) growth of graphene on dielectric/insulating materials promises transfer-free applications of graphene. However, growing graphene on non-catalytic substrates faces significant challenges, particularly due to its limited growth rate, restricting large-scale production and potential applications. Here, we develop graphene-skinned glass fiber fabric (GGFF) by growing graphene CVD on commercial glass fiber fabric (GFF). This study utilizes propane as a carbon source to prepare GGFF rapidly. The active carbon source (C₂H) derived from propane plays a significant role in facilitating the rapid growth of graphene films. It accelerated growth rates (~ 50 times faster), and reduced growth temperature (~ 100 °C lower) compared to the conventional carbon source methane. Additionally, propane consistently maintains a higher graphene growth rate than methane at equivalent growth temperatures. The lightweight flexibility, excellent thermal radiation properties, and energy efficiency of GGFF make it an outstanding material for infrared radiation drying.

Transition metal catalyzed chemical vapor deposition (CVD) is considered as the most promising approach to synthesize high-quality graphene films, and low-temperature growth of defect-free graphene films is long-term challenged because of the high energy barrier for precursor dissociation and graphitization. Reducing the growth temperature can also bring advantages on wrinkle-free graphene films owing to the minimized thermal expansion coefficient mismatch. This work focuses on density functional theory (DFT) calculations of the carbon source precursor with hydroxyl group, especially CH₃OH, on low-temperature CVD growth of graphene on Cu and CuNi substrate. We calculated all the possible cleavage paths for CH₃OH on transition metal substrates. The results show that, firstly, the cleavage barriers of CH₃OH on transition metal substrates are slightly lower than those of CH₄, and once CO appears, it is difficult to break the C–O bond. Secondly, the CO promotes a better formation and retention of perfect rings in the early stage of graphene nucleation and reduces the edge growth barriers. Thirdly, these deoxidation barriers of CO are reduced after CO participates in graphene edge growth. This paper provides a strategy for the low-temperature growth of wrinkles-free graphene on transition metal substrates using CH₃OH.