1996/11/30 by K. Farakos, Nick E. Mavromatos, N. E. Mavromatos
Mathematics · Physics and Astronomy · #Abelian group #Advanced Condensed Matter Physics #Charge (physics) #Combinatorics #Gauge theory #Geometry #Homogeneous space #Mathematical physics #Mathematics #Physics #Physics of Superconductivity and Magnetism #Quantum and electron transport phenomena #Quantum mechanics #cond-mat #hep-lat #hep-th
paper · pdf · doi:10.1103/physrevb.57.3017
published as Phys.Rev.B57:3017-3030,1998 · 32 pages LATEX, one figure. (More details given in the passage from the Hubbard model to the long wavelength lattice gauge theory; one figure added; no changes in the conclusions.)
arxiv created 1997/07/09 · openalex publication_date 1998/02/01 · arxiv updated 2009/11/30 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We investigate the possibility of hidden non-Abelian local phase symmetries in large-U doped planar Hubbard antiferromagnets, believed to simulate the physics of two-dimensional (magnetic) superconductors. We present a spin-charge separation ansatz, appropriate to incorporate holon spin flip, which allows for such a hidden local gauge symmetry to emerge in the effective action. The group is of the form SU(2)\ensuremath\bigotimesUS(1)\ensuremath\bigotimesUem(1), where SU(2) is a local non-Abelian group associated with the spin degrees of freedom, Uem(1) is that of ordinary electromagnetism, associated with the electric charge of the holes, and US(1) is a ``statistical'' Abelian gauge group pertaining to the fractional statistics of holes on the spatial plane. In certain regime of the parameters of the model, namely, strong US(1) and weak SU(2), there is the possibility of dynamical formation of a holon condensate. This leads to a dynamical breaking of SU(2)\ensuremath→U(1). The resulting Abelian effective theory is closely related to an earlier model proposed as the continuum limit of large-spin planar doped antiferromagnets, which lead to an unconventional scenario for two-dimensional parity-invariant superconductivity.