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PreprintCC BY 4.0arXiv

Non-backtracking Laplacian for hypergraphs

Abstract

We extend the non-backtracking Laplacian for graphs, introduced by Jost, Mulas and Torres, to hypergraphs. The operator is defined on the permutations of the edges and is normalized by the number of edges through which a non-backtracking walk can continue. We show that it satisfies a symmetry that generalizes the graph case, and that it can be obtained from the random walk Laplacian of a directed graph by rescaling if and only if all edges have the same cardinality. Moreover, we show that, up to copies of the eigenvalue $1$, its spectrum can be computed from a much smaller matrix indexed by the incidences of the hypergraph, and we use this reduction to bound the remaining eigenvalues away from $1$.

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BibTeX
@misc{andreotti2026nonbacktracking,
  title = {{Non-backtracking Laplacian for hypergraphs}},
  author = {Eleonora Andreotti and Raffaella Mulas},
  howpublished = {arXiv},
  year = {2026},
  month = nov,
  doi = {10.48550/arxiv.2611.01121},
  eprint = {2611.01121},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2611.01121},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Non-backtracking Laplacian for hypergraphs
AU  - Eleonora Andreotti
AU  - Raffaella Mulas
PY  - 2026
DA  - 2026/11/01
PB  - arXiv
DO  - 10.48550/arxiv.2611.01121
UR  - https://arxiv.org/abs/2611.01121
AB  - We extend the non-backtracking Laplacian for graphs, introduced by Jost, Mulas and Torres, to hypergraphs. The operator is defined on the permutations of the edges and is normalized by the number of edges through which a non-backtracking walk can continue. We show that it satisfies a symmetry that generalizes the graph case, and that it can be obtained from the random walk Laplacian of a directed graph by rescaling if and only if all edges have the same cardinality. Moreover, we show that, up to copies of the eigenvalue $1$, its spectrum can be computed from a much smaller matrix indexed by the incidences of the hypergraph, and we use this reduction to bound the remaining eigenvalues away from $1$.
ER  -