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This three-dimensionality is required for the transformation of Dirac into Weyl fermions to take place. It consists of layers of sodium and bismuth atoms that arrange to form a three-dimensional equivalent of graphene. This material is a so-called three-dimensional Dirac semimetal.
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In the present work, the team around Angel Rubio used high-level computational simulations of material properties to show how this optical transformation from Dirac fermions to Weyl fermions can be achieved in a real material – Na 3Bi. Inducing chirality into a Dirac fermion material by combining those fermions with photons from the laser beam to form new quasiparticles can thus transform it into a Weyl fermion material. “It was realized about ten years ago that the so-called Floquet theory − a theory for laser-driven systems that oscillate periodically in time − allows us to engineer parameters and symmetries in materials that can change their topology,” explains Michael Sentef, Emmy Noether group leader at the MPSD in Hamburg. One approach to create chirality in a material is to drive it with a laser beam. Dirac fermions, by contrast, do not have this property. The two partners are almost identical, yet they cannot be superimposed. Just like our left and right hands, Weyl fermions occur in pairs, where one particle is a mirrored version of the other. The 2016 Nobel Prize in Physics was just awarded to Michael Kosterlitz, Duncan Haldane, and David Thouless for the discovery of such topological phases of matter.ĭirac and Weyl fermions differ by their chirality. This chirality, or handedness, is topological in the sense that right-handed and left-handed chiralities are discrete states that cannot be continuously deformed into each other. Topology is a property of the particles that leads to peculiar properties, for example metallic chiral edge states that form a collisionless one-way quantum highway along the edge of a topological insulator. In particular, the coupling to photons can affect the topology of quasiparticles. It has now been found, however, that by irradiating a material with a laser, it is also possible to combine a quasiparticle with the photons of the laser field to form a new quasiparticle that, again, can behave fundamentally differently. The hunt for other materials hosting quasiparticles behaving like fundamental particles has thus focused on the crystal structure of materials so far. These particles cooperatively forming new particles with different properties are called quasiparticles.
#Fundamental particles free#
Although each individual electron interacts with its surrounding ions and electrons via electrostatic forces, the particular pattern of carbon ions in graphene’s honeycomb layer structure causes the electrons to behave collectively like massless, free fermions – Dirac fermions. The observation of Dirac fermions in the properties of graphene originates from a complex interaction of the large number of electrons and ions that make up the material. First observation of Dirac fermions in graphene While any known material only hosts one kind of these fermions in its equilibrium state, in the present work it is demonstrated how one can transform the fermion nature within specific materials by using tailored light pulses. This sparked the search for materials where these fundamental particles could be observed and only last year the first materials hosting Weyl fermions were discovered. With the discovery of graphene in 2004, however, it was realized that the behaviour of relativistic free particles could be observed in the electronic properties of materials.
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However, despite being predicted almost a hundred years ago, of these three kinds of particles only Dirac fermions have been observed as elementary particles in nature so far. Quantum theory predicts that elementary fermions could exist as three different kinds: Dirac, Weyl, and Majorana fermions, named after Paul Dirac, Hermann Weyl, and Ettore Majorana. In the standard model of particle physics, the fundamental particles that make up all matter around us – electrons and quarks – are so-called fermions, named after the famous Italian physicist Enrico Fermi.