Early study on the Dirac Fermion utilized two-dimensional (2D) systems like graphene, while more recent work on the subject has focused on three-dimensional Dirac semimetals (3D DSM). 3D DSM has a key structural advantage over graphene monolayer in that it shows linear band dispersion with a macroscopic thickness. Similar to graphene, the Dirac band structure of 3D DSM confers very high optical nonlinearities. Since Dirac physics describes charge carriers in both 2D and 3D DSM, 3D DSM should have similar optical properties to graphene, such as tunable optical conductivity, high nonlinear optical coefficients, and stronger light confinement. Also, 3D DSM is better for plasmonic waveguides than 2D graphene because it has a 3D structure, which gives it an extra degree of freedom. Based on these great qualities, 3D DSMs are a good replacement for 2D DSMs. Cadmium arsenide (Cd3As2) is a popular 3D DSM because of its chemical stability in air and exceptional optical properties.