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Zero-field Josephson diode effect in dirac semimetal-based asymmetric squids
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Zero-magnetic-field superconducting Josephson diode effect in a Dirac semimetal
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Prospects for Ultra-Low MTE Photocathodes: A Case Study on Dirac Semimetal Cd3As2
Presentation at the Photocathode Physics for Photoinjectors Workshop (Arizona State University, Tempe, AZ, November 13, 2025) on the prospects for Ultra-Low MTE Photocathodes.
High harmonic generation in Weyl-Kondo semimetals
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Extreme response of Weyl-Kondo semimetal to Zeeman coupling
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Strongly correlated topological semimetals
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Anomalous Shaprio steps in a Dirac semimetal Cd3As2-based SQUID.
Abstract not provided.
Weyl-Kondo semimetals: extreme topological tunability and nonlinear optical signatures
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Extreme topological tunability of Weyl-Kondo semimetal to Zeeman coupling
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Weyl-Kondo semimetal: Extreme topological tunability and nonlinear optical exploration
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The Weyl-Kondo semimetal: high-harmonic generation and extreme topological tunability
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Josephson-Leggett modes in a Dirac semimetal Cd3As2-based SQUID.
Abstract not provided.
Shedding Light On Strong Correlations And Topology: Nonlinear Optical Properties Of The Weyl-Kondo Semimetal
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Topological Mott transition in a two band model of spinless fermions with on-site Coulomb repulsion
Highlights: • The effect of the on-site Coulomb repulsion and the spin–orbit Rashba coupling lead to the 2D topological semimetal. • The ground state phase diagram is calculated. • The topological semimetal phase is characterized by the zero energy Majorana states. In the framework of mean field approach, we study topological Mott transition in a two band model of spinless fermions on a square lattice at half filling. We consider the combined effect of the on-site Coulomb repulsion and the spin–orbit Rashba coupling. The ground state phase diagram is calculated as a function of the strength of the spin–orbit Rashba coupling and the Coulomb repulsion. The spin–orbit Rashba coupling leads to a distinct phase of matter, the topological semimetal. We study a new type of phase transition between the non-topological insulator and topological semimetal states. Topological phase state is characterized by the zero energy Majorana states, which there are in defined region of the wave vectors and are localized at the boundaries of the sample. The region of existence of the zero energy Majorana states tends to zero at the point of the Mott phase transition. The zero energy Majorana states are dispersionless (they can be considered as flat bands), the Chern number and Hall conductance are equal to zero (note in two dimensional model).
Giant quantum oscillations in thermal transport in low-density metals via electron absorption of phonons
Oscillations of conductance observed in strong magnetic fields are a striking manifestation of the quantum dynamics of charge carriers in solids. The large charge carrier density in typical metals sets the scale of oscillations in both electrical and thermal conductivity, which characterize the Fermi surface. In semimetals, thermal transport at low-charge carrier density is expected to be phonon dominated, yet several experiments observe giant quantum oscillations in thermal transport. This raises the question of whether there is an overarching mechanism leading to sizable oscillations that survives in phonon-dominated semimetals. In this work, we show that such a mechanism exists. It relies on the peculiar phase-space allowed for phonon scattering by electrons when only a few Landau levels are filled. Our measurements on the Dirac semimetal ZrTe 5 support this counterintuitive mechanism through observation of pronounced thermal quantum oscillations, since they occur in similar magnitude and phase in directions parallel and transverse to the magnetic field. Our phase-space argument applies to all low-density semimetals, topological or not, including graphene and bismuth. Our work illustrates that phonon absorption can be leveraged to reveal degrees of freedom through their imprint on longitudinal thermal transport.
Weyl nodal ring states and Landau quantization with very large magnetoresistance in square-net magnet EuGa 4
Magnetic topological semimetals allow for an effective control of the topological electronic states by tuning the spin configuration. Among them, Weyl nodal line semimetals are thought to have the greatest tunability, yet they are the least studied experimentally due to the scarcity of material candidates. Here, using a combination of angle-resolved photoemission spectroscopy and quantum oscillation measurements, together with density functional theory calculations, we identify the square-net compound EuGa 4 as a magnetic Weyl nodal ring semimetal, in which the line nodes form closed rings near the Fermi level. The Weyl nodal ring states show distinct Landau quantization with clear spin splitting upon application of a magnetic field. At 2 K in a field of 14 T, the transverse magnetoresistance of EuGa 4 exceeds 200,000%, which is more than two orders of magnitude larger than that of other known magnetic topological semimetals. Our theoretical model suggests that the non-saturating magnetoresistance up to 40 T arises as a consequence of the nodal ring state.