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Gauss Law, Monodromy Defect, Magnetic Lattice Translation, and Lattice Duality

Abstract

In a Hamiltonian lattice gauge theory, the physical Hilbert space is fixed by the Gauss law, by choosing an eigenspace of the Gauss law operator which generates the gauge transformation. Choosing a non-trivial eigenspace is referred to as the modified Gauss law. In 2+1d dynamical U(1) pure gauge theory, we show that these physical Hilbert spaces are defect Hilbert spaces associated with non-topological monodromy defects for monopole operators and topological defects for U(1) 1-form symmetry, inserted along the time direction. We also construct the corresponding lattice translation operators. Under a nontrivially modified Gauss law, these translations obey a magnetic translation algebra. Finally, we discuss how the modified Gauss laws are manifested in 2+1d compact bosons, via exact duality on the lattice.

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BibTeX
@misc{wei2026gauss,
  title = {{Gauss Law, Monodromy Defect, Magnetic Lattice Translation, and Lattice Duality}},
  author = {Pengcheng Wei and Yunqin Zheng},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.11417},
  eprint = {2609.11417},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.11417},
}
RIS
TY  - UNPB
TI  - Gauss Law, Monodromy Defect, Magnetic Lattice Translation, and Lattice Duality
AU  - Pengcheng Wei
AU  - Yunqin Zheng
PY  - 2026
DA  - 2026/09/10
PB  - arXiv
DO  - 10.48550/arxiv.2609.11417
UR  - https://arxiv.org/abs/2609.11417
AB  - In a Hamiltonian lattice gauge theory, the physical Hilbert space is fixed by the Gauss law, by choosing an eigenspace of the Gauss law operator which generates the gauge transformation. Choosing a non-trivial eigenspace is referred to as the modified Gauss law. In 2+1d dynamical U(1) pure gauge theory, we show that these physical Hilbert spaces are defect Hilbert spaces associated with non-topological monodromy defects for monopole operators and topological defects for U(1) 1-form symmetry, inserted along the time direction. We also construct the corresponding lattice translation operators. Under a nontrivially modified Gauss law, these translations obey a magnetic translation algebra. Finally, we discuss how the modified Gauss laws are manifested in 2+1d compact bosons, via exact duality on the lattice.
ER  -