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In quantum field theory, Weyl fermions are relativistic particles that travel at the speed of light and strictly obey the celebrated Lorentz symmetry. Their low-energy condensed matter analogs are Weyl semimetals, which are conductors whose electronic excitations mimic the Weyl fermion equation of motion. Although the traditional (type I) emergent Weyl fermions observed in TaAs still approximately respect Lorentz symmetry, recently, the so-called type II Weyl semimetal has been proposed, where the emergent Weyl quasiparticles break the Lorentz symmetry so strongly that they cannot be smoothly connected to Lorentz symmetric Weyl particles. Despite some evidence of nontrivial surface states, the direct observation of the type II bulk Weyl fermions remains elusive. We present the direct observation of the type II Weyl fermions in crystalline solid lanthanum aluminum germanide (LaAlGe) based on our photoemission data alone, without reliance on band structure calculations. Moreover, our systematic data agree with the theoretical calculations, providing further support on our experimental results.
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http://dx.doi.org/10.1126/sciadv.1603266 | DOI Listing |
Commun Math Phys
September 2025
Institute of Mathematics, University of Zurich, Winterthurerstrasse 190, 8057 Zurich, Switzerland.
We give a rigorous derivation of the Hartree equation for the many-body dynamics of pseudo-relativistic Fermi systems at high density , on arbitrarily large domains, at zero temperature. With respect to previous works, we show that the many-body evolution can be approximated by the Hartree dynamics locally, proving convergence of the expectation of observables that are supported in regions with fixed volume, independent of . The result applies to initial data describing fermionic systems at equilibrium confined in arbitrarily large domains, under the assumption that a suitable local Weyl-type estimate holds true.
View Article and Find Full Text PDFRep Prog Phys
September 2025
TU Dresden, Institut für Theoretische Physik, Dresden, 01062, GERMANY.
A central concept in the theory of phase transitions beyond the Landau-Ginzburg-Wilson paradigm is fractionalization: the formation of new quasiparticles that interact via emergent gauge fields. This concept has been extensively explored in the context of continuous quantum phase transitions between distinct orders that break different symmetries. We propose a mechanism for continuous order-to-order quantum phase transitions that operates independently of fractionalization.
View Article and Find Full Text PDFJ Phys Condens Matter
September 2025
Department of Physics, University of Calcutta, 92 A P C Road, Kolkata 700009, India.
The discovery of magnetic Weyl semimetals (WSMs) has drawn significant interest due to their exceptional topological properties and anomalous transport behaviors, presenting exciting possibilities for advanced technological applications. Co-based Heusler compounds, with their unique band structures, have emerged as key materials for exploring the interplay between magnetism and topology. In this work, we perform a detailed first-principles study on Co2-xCrMnGe Heusler alloys (0⩽⩽1), proposing new candidates with significantly enhanced nontrivial transport properties.
View Article and Find Full Text PDFPhys Rev Lett
July 2025
The University of Tokyo, Department of Electrical Engineering and Information Systems, Bunkyo, Tokyo 113-8656, Japan.
In transition-metal compounds, the transition-metal d electrons play an important role in their physical properties; however, the effects of the electron correlation between the ligand p electrons have not been clear yet. In this Letter, the Ru 4d and O 2p partial density of states (PDOS) in transition-metal oxide SrRuO_{3} involving Weyl fermions are investigated by resonant photoemission spectroscopy. The observations demonstrate that the O 2p PDOS is distorted from that predicted by first-principles calculations than the Ru 4d PDOS.
View Article and Find Full Text PDFNat Commun
July 2025
Leibniz Institute for Solid State and Materials Research (IFW Dresden), Helmholtzstraße 20, Dresden, Germany.
Topological materials, such as topological insulators or semimetals, usually not only reveal the non-trivial properties of their electronic wavefunctions through the appearance of stable boundary modes, but also through very specific electromagnetic responses. The anisotropic longitudinal magnetoresistance of Weyl semimetals, for instance, carries the signature of the chiral anomaly of Weyl fermions. However for topological nodal line semimetals-materials where the valence and conduction bands cross each other on one-dimensional curves in the three-dimensional Brillouin zone-such a characteristic has been lacking.
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