New-type solar cells typically including dye-sensitized solar cells (DSCs), organic solar cells (OSCs) and perovskite solar cells (PSCs) have been attractive reasonably for the low-temperature fabrications (below~150ºC), low thicknesses and unable colors. They potentially overcome Shockley-Queisser limit of 31-41% power efficiency for single bandgap solar cells. Electron transport layer (ETL) and hole transport layer (HTL) are introduced to reduce charge recombination in PSCs and OSCs, and electrolytes are required for harge transport and redox reaction in DSCs. Due to the advantages of abundance, long-term stability, good transparency, high conductivity and mechanical flexibility, carbon nanomaterials including fullerene, carbon nanotubes (CNTs) and graphene have been widely used for ealizing the flexibility and high performance of solar cells. GO and its derivatives exhibit high electron blocking capability and have been used as a qualified hole transport material. As a conductive electrode, carbon nanomaterials (like graphene, CNTs) are a promising substitute for commercial ITO leading to flexible solar cells. Graphene-based materials are also capable of functioning as charge selective and transport components in solar cell buffer layers. Moreover, low air stability and atmospheric degradation of the photovoltaic devices can be improved with graphene encapsulation due to its stable highly packed 2D structure.