Abstract
Cation–π interactions between molecules and graphene are known to have a profound effect on the properties of the molecule/graphene nanohybrids and motivate this study to quantify the attachment of the rhodamine 6G (R6G) dye molecules on graphene and the photocarrier transfer channel formed across the R6G/graphene interface. By increasing the R6G areal density of the R6G on graphene field‐effect transistor (GFET) from 0 up to ≈3.6 × 1013 cm−2, a linear shift of the Dirac point of the graphene from originally 1.2 V (p‐doped) to −1 V (n‐doped) is revealed with increasing number of R6G molecules. This indicates that the attachment of the R6G molecules on graphene is determined by the cation–π interaction between the NH+ in R6G and π electrons in graphene. Furthermore, a linear dependence of the photoresponse on the R6G molecule concentration to 550 nm illumination is observed on the R6G/graphene nanohybrid, suggesting that the cation–π interaction controls the R6G attachment configuration to graphene to allow formation of identical photocarrier transfer channels. On R6G/graphene nanohybrid with 7.2 × 107 R6G molecules, high responsivity up to 5.15 × 102 A W−1 is obtained, suggesting molecule/graphene nanohybrids are promising for high‐performance optoelectronics.
This work reveals that the cation–π interaction controls the attachment configuration of the rhodamine 6G (R6G) molecule on graphene with its NH+ cation directing towards graphene, generating the molecular gating effect on graphene as well as providing effective charge transfer channels that are proportional linearly to the number of R6G molecules attached.