The Hofstadter butterfly of lattice electrons in a strong magnetic field is a cornerstone of condensed matter physics, exploring the competition between periodicities imposed by the lattice and the field. Here, we introduce and characterize the Weyl butterfly, which emerges when a large magnetic field is applied to a three-dimensional Weyl semimetal. Using an experimentally motivated lattice model for cold-atomic systems, we solve this problem numerically. We find that Weyl nodes reemerge at commensurate fluxes and propose using wave-packet dynamics to reveal their chirality and location. Moreover, we show that the chiral anomaly-a hallmark of the topological Weyl semimetal-does not remain proportional to the magnetic field at large fields,...
A Weyl semimetal has Weyl nodes that always come in pairs with opposite chiralities. Notably, differ...
A Weyl semimetal has Weyl nodes that always come in pairs with opposite chiralities. Notably, differ...
Weyl semimetals are three-dimensional crystalline systems where pairs of bands touch at points in mo...
The Hofstadter butterfly of lattice electrons in a strong magnetic field is a cornerstone of condens...
Weyl semimetals are three-dimensional crystalline systems where pairs of bands touch at points in mo...
International audienceCondensed matter systems realizing Weyl fermions exhibit striking phenomenolog...
International audienceCondensed matter systems realizing Weyl fermions exhibit striking phenomenolog...
In the Weyl semimetals, a recently discovered class of bulk materials, inverted band gap closes in t...
In disordered Weyl semimetals, mechanisms of topological origin lead to the protection against Ander...
In Weyl semimetals, the application of parallel electric and magnetic fields leads to valley polariz...
In Weyl semimetals the application of parallel electric and magnetic fields leads to valley polariza...
In Weyl semimetals, the application of parallel electric and magnetic fields leads to valley polariz...
Weyl semimetal is a topologically non-trivial phase of matter with pairs of Weyl nodes in the k-spac...
Weyl fermions can be created in materials with both time reversal and inversion symmetry by applying...
A Weyl semimetal has Weyl nodes that always come in pairs with opposite chiralities. Notably, differ...
A Weyl semimetal has Weyl nodes that always come in pairs with opposite chiralities. Notably, differ...
A Weyl semimetal has Weyl nodes that always come in pairs with opposite chiralities. Notably, differ...
Weyl semimetals are three-dimensional crystalline systems where pairs of bands touch at points in mo...
The Hofstadter butterfly of lattice electrons in a strong magnetic field is a cornerstone of condens...
Weyl semimetals are three-dimensional crystalline systems where pairs of bands touch at points in mo...
International audienceCondensed matter systems realizing Weyl fermions exhibit striking phenomenolog...
International audienceCondensed matter systems realizing Weyl fermions exhibit striking phenomenolog...
In the Weyl semimetals, a recently discovered class of bulk materials, inverted band gap closes in t...
In disordered Weyl semimetals, mechanisms of topological origin lead to the protection against Ander...
In Weyl semimetals, the application of parallel electric and magnetic fields leads to valley polariz...
In Weyl semimetals the application of parallel electric and magnetic fields leads to valley polariza...
In Weyl semimetals, the application of parallel electric and magnetic fields leads to valley polariz...
Weyl semimetal is a topologically non-trivial phase of matter with pairs of Weyl nodes in the k-spac...
Weyl fermions can be created in materials with both time reversal and inversion symmetry by applying...
A Weyl semimetal has Weyl nodes that always come in pairs with opposite chiralities. Notably, differ...
A Weyl semimetal has Weyl nodes that always come in pairs with opposite chiralities. Notably, differ...
A Weyl semimetal has Weyl nodes that always come in pairs with opposite chiralities. Notably, differ...
Weyl semimetals are three-dimensional crystalline systems where pairs of bands touch at points in mo...