TY - JOUR

T1 - Resonating quantum three-coloring wave functions for the kagome quantum antiferromagnet

AU - Changlani, Hitesh J.

AU - Pujari, Sumiran

AU - Chung, Chia Min

AU - Clark, Bryan K.

N1 - Funding Information:
H.J.C. and B.K.C. thank E. Fradkin, D. Kochkov, and K. Kumar for an earlier collaboration. We thank O. Vafek, S. Sachdev, O. Tchernyshyov, P. Nikolic, V. Dobrosavljevic, F. Verstraete, A. Ralko, Y-C. He, and M. Lawler for their encouragement and for useful discussions. This work was supported through the Institute for Quantum Matter at Johns Hopkins University, by the U.S. Department of Energy, Division of Basic Energy Sciences, Grant No. DE-FG02-08ER46544. H.J.C. acknowledges start up funds at Florida State University. S.P. acknowledges the support (17IRCCSG011) of IRCC, IIT Bombay. We gratefully acknowledge the Johns Hopkins Homewood High Performance Cluster (HHPC) and the Maryland Advanced Research Computing Center (MARCC), funded by the State of Maryland, for computing resources. This research is also part of the BlueWaters sustained petascale computing project, which is supported by the National Science Foundation (Awards No. OCI-0725070 and No. ACI-1238993) and the State of Illinois. The DMRG calculations were performed using the ITensor C++ library (version 2.1.1), https://itensor.org/.
Publisher Copyright:
© 2019 American Physical Society.

PY - 2019/3/27

Y1 - 2019/3/27

N2 - Motivated by the recent discovery of a macroscopically degenerate exactly solvable point of the spin-1/2XXZ model for Jz/J=-1/2 on the kagome lattice [H. J. Changlani Phys. Rev. Lett. 120, 117202 (2018)PRLTAO0031-900710.1103/PhysRevLett.120.117202] - a result that holds for arbitrary magnetization - we develop an exact mapping between its exact "quantum three-coloring" wave functions and the characteristic localized and topological magnons. This map, involving "resonating two-color loops," is developed to represent exact many-body ground state wave functions for special high magnetizations. Using this map we show that these exact ground state solutions are valid for any Jz/J≥-1/2. This demonstrates the equivalence of the ground-state wave function of the Ising, Heisenberg, and XY regimes all the way to the Jz/J=-1/2 point for these high magnetization sectors. In the hardcore bosonic language, this means that a certain class of exact many-body solutions, previously argued to hold for purely repulsive interactions (Jz≥0), actually hold for attractive interactions as well, up to a critical interaction strength. For the case of zero magnetization, where the ground state is not exactly known, we perform density matrix renormalization group calculations. Based on the calculation of the ground state energy and measurement of order parameters, we provide evidence for a lack of any qualitative change in the ground state on finite clusters in the Ising (Jz J), Heisenberg (Jz=J), and XY (Jz=0) regimes, continuing adiabatically to the vicinity of the macroscopically degenerate Jz/J=-1/2 point. These findings offer a framework for recent results in the literature and also suggest that the Jz/J=-1/2 point is an unconventional quantum critical point whose vicinity may contain the key to resolving the spin-1/2 kagome problem.

AB - Motivated by the recent discovery of a macroscopically degenerate exactly solvable point of the spin-1/2XXZ model for Jz/J=-1/2 on the kagome lattice [H. J. Changlani Phys. Rev. Lett. 120, 117202 (2018)PRLTAO0031-900710.1103/PhysRevLett.120.117202] - a result that holds for arbitrary magnetization - we develop an exact mapping between its exact "quantum three-coloring" wave functions and the characteristic localized and topological magnons. This map, involving "resonating two-color loops," is developed to represent exact many-body ground state wave functions for special high magnetizations. Using this map we show that these exact ground state solutions are valid for any Jz/J≥-1/2. This demonstrates the equivalence of the ground-state wave function of the Ising, Heisenberg, and XY regimes all the way to the Jz/J=-1/2 point for these high magnetization sectors. In the hardcore bosonic language, this means that a certain class of exact many-body solutions, previously argued to hold for purely repulsive interactions (Jz≥0), actually hold for attractive interactions as well, up to a critical interaction strength. For the case of zero magnetization, where the ground state is not exactly known, we perform density matrix renormalization group calculations. Based on the calculation of the ground state energy and measurement of order parameters, we provide evidence for a lack of any qualitative change in the ground state on finite clusters in the Ising (Jz J), Heisenberg (Jz=J), and XY (Jz=0) regimes, continuing adiabatically to the vicinity of the macroscopically degenerate Jz/J=-1/2 point. These findings offer a framework for recent results in the literature and also suggest that the Jz/J=-1/2 point is an unconventional quantum critical point whose vicinity may contain the key to resolving the spin-1/2 kagome problem.

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U2 - 10.1103/PhysRevB.99.104433

DO - 10.1103/PhysRevB.99.104433

M3 - Article

AN - SCOPUS:85064136599

SN - 2469-9950

VL - 99

JO - Physical Review B

JF - Physical Review B

IS - 10

M1 - 104433

ER -