4.6 Article

Hybrid rank-1 and rank-2 U(1) lattice gauge theory, the F3 model, and its effective field theory

Journal

PHYSICAL REVIEW B
Volume 106, Issue 15, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.106.155154

Keywords

-

Funding

  1. Quantum Computing Development Program [2019M3E4A1080227]
  2. EPIQS Moore theory centers at Harvard
  3. Massachusetts Institute of Technology
  4. education and training program of the Quantum Information Research Support Center through the National Research Foundation of Korea (NRF) by the Ministry of Science and ICT (MSIT) of the Korean government [2021M3H3A103657313]
  5. National Research Foundation of Korea [NRF-2021M3E4A1038308, NRF-2021M3H3A1038085, NRF-2021R1A2C4001847, NRF-2020R1A4A3079707, NRF-2022R1I1A1A01065149]

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The study reveals that the parent LGT of the F3 model is a hybrid of rank-1 and rank-2 U(1) LGT, and develops the corresponding field theory. The resulting Lagrangian of the F3 model connects the dynamics of fractons to that of fluxons.
A number of exactly solvable spin models, including the Kitaev toric code in two and three dimensions and the X-cube model in three dimensions, can be related to their respective parent lattice gauge theories (LGTs) through the mathematical process of Higgsing. Field theories of the low-energy excitations of these spin models can be developed subsequently, building upon the symmetry of the parent LGTs. Recently, two of the present authors proposed a variant of the three-dimensional toric code which we now call the F3 model, whose elementary excitations consist of freeon and fluxon excitations of the three-dimensional toric code and fracton excitations of the X-cube model. In this work, we identify the parent LGT of the F3 model as the hybrid rank-1 and rank-2 U(1) LGT and develop the corresponding field theory. The resulting Lagrangian of the F3 model is that of a three-dimensional toric code with an extra term, which ties the dynamics of fractons to that of fluxons. The matter part of the effective action for the F3 model can be derived as well by carefully keeping track of the gauge invariance of the F3 model. Hydrodynamic equations of motion of the quasiparticles are derived which properly reflect their constrained dynamics. Finally, we present a tight-binding model for the quasiparticle motion in the F3 model.

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