Weyl Points are Topologically protected points in the Momentum Space of certain crystals, where the Energy of the quasiparticles (akin to the electrons) linearly depends on the momentum around these points, leading to exotic phenomena like Fermi Arcs and Anomalous Hall effects. They serve as Monopoles of Berry curvature in a Three-dimensional Brillouin zone, significantly influencing the Electronic Properties and leading to robust, Gapless states at their location.