We introduce exotic gapless states—“composite Dirac liquids”—that can appear at a strongly interacting surface of a three-dimensional electronic topological insulator. Composite Dirac liquids exhibit a gap to all charge excitations but nevertheless feature a single massless Dirac cone built from emergent electrically neutral fermions. These states thus comprise electrical insulators that, interestingly, retain thermal properties similar to those of the noninteracting topological insulator surface. A variety of novel fully gapped phases naturally descend from composite Dirac liquids. Most remarkably, we show that gapping the neutral fermions via Cooper pairing—which crucially does not violate charge conservation—yields symmetric non-Abelian ...
Recent experiments and theories have suggested that strong spin–orbit coupling effects in certain ba...
In a two-dimensional electron gas under a strong magnetic field, correlations generate emergent exci...
Topological phases of matter are purely quantum mechanical and have no classical analogue. Most phas...
We introduce exotic gapless states—“composite Dirac liquids”—that can appear at a strongly interacti...
We introduce exotic gapless states—“composite Dirac liquids”—that can appear at a strongly interacti...
Topological phases of matter often feature boundary physics that naively seems impossible from the ...
We synthesize and partly review recent developments relating the physics of the half-filled Landau l...
We show that the chiral Dirac and Majorana hinge modes in three-dimensional higher-order topological...
We show that the chiral Dirac and Majorana hinge modes in three-dimensional higher-order...
Three-dimensional topological insulators support gapless Dirac fermion surface states whose rich top...
We introduce a particle-hole-symmetric metallic state of bosons in a magnetic field at odd-integer f...
A topological insulator is a novel state of quantum matter, characterized by symmetry-protected Dira...
We consider electron--hole Cooper pair condensation in a heterostructure formed by a topological ins...
We describe recent progress in our understanding of the interplay between interactions, symmetry, an...
It is well known that the three-dimensional (3D) electronic topological insulator (TI) with charge-c...
Recent experiments and theories have suggested that strong spin–orbit coupling effects in certain ba...
In a two-dimensional electron gas under a strong magnetic field, correlations generate emergent exci...
Topological phases of matter are purely quantum mechanical and have no classical analogue. Most phas...
We introduce exotic gapless states—“composite Dirac liquids”—that can appear at a strongly interacti...
We introduce exotic gapless states—“composite Dirac liquids”—that can appear at a strongly interacti...
Topological phases of matter often feature boundary physics that naively seems impossible from the ...
We synthesize and partly review recent developments relating the physics of the half-filled Landau l...
We show that the chiral Dirac and Majorana hinge modes in three-dimensional higher-order topological...
We show that the chiral Dirac and Majorana hinge modes in three-dimensional higher-order...
Three-dimensional topological insulators support gapless Dirac fermion surface states whose rich top...
We introduce a particle-hole-symmetric metallic state of bosons in a magnetic field at odd-integer f...
A topological insulator is a novel state of quantum matter, characterized by symmetry-protected Dira...
We consider electron--hole Cooper pair condensation in a heterostructure formed by a topological ins...
We describe recent progress in our understanding of the interplay between interactions, symmetry, an...
It is well known that the three-dimensional (3D) electronic topological insulator (TI) with charge-c...
Recent experiments and theories have suggested that strong spin–orbit coupling effects in certain ba...
In a two-dimensional electron gas under a strong magnetic field, correlations generate emergent exci...
Topological phases of matter are purely quantum mechanical and have no classical analogue. Most phas...