2019/12/18 by Darshan G. Joshi, Chenyuan Li, Grigory Tarnopolsky +2 · 1 citation
Physics and Astronomy · #Advanced Condensed Matter Physics #Condensed matter physics #Critical exponent #Critical phenomena #Critical point (mathematics) #Doping #Fermi liquid theory #Heisenberg model #Magnet #Phase diagram #Physics #Physics of Superconductivity and Magnetism #Quantum #Quantum critical point #Quantum many-body systems #Quantum mechanics #Quantum phase transition #Renormalization group #Spin (aerodynamics) #Theoretical and Computational Physics #cond-mat.str-el #hep-th
paper · pdf · doi:10.1103/physrevx.10.021033
published as Phys. Rev. X 10, 021033 (2020) · 22+32 pages, 13 figures
openalex publication_date 2019/12/18 · openalex created_date 2019/12/26 · arxiv created 2020/02/18 · arxiv updated 2020/05/20 · openalex updated_date 2026/08/06
We describe the phase diagram of electrons on a fully connected lattice with random hopping, subject to a random Heisenberg spin exchange interactions between any pair of sites and a constraint of no double occupancy. A perturbative renormalization group analysis yields a critical point with fractionalized excitations at a non-zero critical value pc of the hole doping p away from the half-filled insulator. We compute the renormalization group to two loops, but some exponents are obtained to all loop order. We argue that the critical point pc is flanked by confining phases: a disordered Fermi liquid with carrier density 1+p for p>pc, and a metallic spin glass with carrier density p for p<pc. Additional evidence for the critical behavior is obtained from a large M analysis of a model which extends the SU(2) spin symmetry to SU(M). We discuss the relationship of the vicinity of this deconfined quantum critical point to key aspects of cuprate phenomenology.