A crystalline material where electrons behave as massless particles, mimicking curved spacetime.A Weyl semimetal is a crystalline material in which electrons behave as massless particles, mimicking the behavior of particles in curved spacetime. In these materials, the energy of electrons depends linearly on their momentum, just like photons, but with a much lower speed. This unusual property arises from the material's electronic band structure, where two non-degenerate bands touch at points called Weyl nodes. Near these nodes, the electrons are described by the Weyl equation, the same equation used in high-energy physics for massless fermions.
The concept of Weyl fermions in condensed matter was proposed by Hermann Weyl in 1929 for particle physics, but the first experimental observation of Weyl semimetals in crystals was reported in 2015, with tantalum arsenide (TaAs) being a prominent example.
In a Weyl semimetal, the conduction and valence bands cross at discrete points in momentum space, called Weyl nodes. These nodes come in pairs of opposite chirality (left-handed and right-handed). Electrons near a Weyl node behave as massless particles, with their spin locked to their momentum. The linear dispersion means that the effective mass of the electrons is zero, and they move at a constant speed. The chirality of the nodes leads to a phenomenon called the chiral anomaly, where charge can be pumped between nodes of opposite chirality in the presence of parallel electric and magnetic fields.
Weyl semimetals are studied for potential applications in spintronics and quantum computing, as their unique electronic properties could enable dissipationless current flow and novel topological devices.
In a Weyl semimetal, electrons can behave as if they are in a gravitational field, allowing the simulation of curved spacetime phenomena in a laboratory crystal.






