Free fermions behind the disguise
Samuel J. Elman, Adrian Chapman, Steven T. Flammia

TL;DR
This paper introduces a graph-based method to map certain quantum spin systems to free fermions, enabling explicit solutions even without traditional transformations, broadening the class of solvable models.
Contribution
The authors develop a graph-theoretic approach to find free-fermion solutions for spin Hamiltonians using the frustration graph structure, extending beyond known methods.
Findings
Explicit free-fermion solutions for (even-hole, claw)-free graphs
Polynomial-time recognition of solvable models based on graph properties
Application to models without Jordan-Wigner solutions
Abstract
An invaluable method for probing the physics of a quantum many-body spin system is a mapping to noninteracting effective fermions. We find such mappings using only the frustration graph of a Hamiltonian , i.e., the network of anticommutation relations between the Pauli terms in in a given basis. Specifically, when is (even-hole, claw)-free, we construct an explicit free-fermion solution for using only this structure of , even when no Jordan-Wigner transformation exists. The solution method is generic in that it applies for any values of the couplings. This mapping generalizes both the classic Lieb-Schultz-Mattis solution of the XY model and an exact solution of a spin chain recently given by Fendley, dubbed "free fermions in disguise." Like Fendley's original example, the free-fermion operators that solve the model are generally highly nonlinear and nonlocal, but…
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