2008/06/30 by O. Cepas, O. Cépas, Manson Cheuk‐Man Fong +3 · 2 citations
Physics and Astronomy · #Advanced Condensed Matter Physics #Antiferromagnetism #Condensed matter physics #Coupling (piping) #Critical point (mathematics) #Materials science #Phase (matter) #Phase transition #Physics #Physics of Superconductivity and Magnetism #Quantum #Quantum critical point #Quantum fluctuation #Quantum mechanics #Quantum phase transition #Scaling #Topological Materials and Phenomena #cond-mat.str-el
paper · pdf · doi:10.1103/physrevb.78.140405
published as Phys. Rev. B 78, 140405(R) (2008) · 5 pages, 4 figures; v2: add. data included, show that D=0.1J is at a quantum critical point
arxiv created 2008/07/09 · openalex publication_date 2008/10/23 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/06
We argue that the S=1/2 kagome antiferromagnet undergoes a quantum phase transition when the Dzyaloshinskii-Moriya coupling is increased. For D<Dc the system is in a moment-free phase, and for D>Dc the system develops antiferromagnetic long-range order. The quantum critical point is found to be Dc\ensuremath≃0.1J using exact diagonalizations and finite-size scaling. This suggests that the kagome compound ZnCu3(OH)6Cl3 may be in a quantum critical region controlled by this fixed point.