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Semi-Dirac fermion

From Wikipedia, the free encyclopedia

Semi-Dirac fermions are a class of quasiparticles that are fermions with the unusual property that their mass changes dependent on their direction of motion.[1] Their theoretical properties have been studied for some time.[2][3]

Their first observation in a solid was in ZrSiS, a topological semi-metal, and was published in 2024.[4]

See also

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References

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  1. ^ "Particle that only has mass when moving in one direction observed for first time | Penn State University". www.psu.edu. Retrieved 2024-12-12.
  2. ^ Uryszek, Mikolaj D.; Christou, Elliot; Jaefari, Akbar; Krüger, Frank; Uchoa, Bruno (2019-10-01). "Quantum criticality of semi-Dirac fermions in 2 + 1 dimensions". Physical Review B. 100 (15). doi:10.1103/PhysRevB.100.155101. ISSN 2469-9950.
  3. ^ Mohanta, Narayan; Ok, Jong Mok; Zhang, Jie; Miao, Hu; Dagotto, Elbio; Lee, Ho Nyung; Okamoto, Satoshi (2021-12-10). "Semi-Dirac and Weyl fermions in transition metal oxides". Physical Review B. 104 (23). doi:10.1103/PhysRevB.104.235121. ISSN 2469-9950.
  4. ^ Shao, Yinming (2024). "Semi-Dirac Fermions in a Topological Metal". Physical Review X. 14 (4). doi:10.1103/PhysRevX.14.041057.