Integrable spin-1/2 Richardson-Gaudin XYZ models in an arbitrary magnetic field

Abstract

We establish the most general class of spin-1/2 integrable Richardson-Gaudin models including an arbitrary magnetic field, returning a fully anisotropic (XYZ) model. The restriction to spin-1/2 relaxes the usual integrability constraints, allowing for a general solution where the couplings between spins lack the usual antisymmetric properties of Richardson-Gaudin models. The full set of conserved charges are constructed explicitly and shown to satisfy a set of quadratic equations, allowing for the numerical treatment of a fully anisotropic central spin in an external magnetic field. While this approach does not provide expressions for the exact eigenstates, it allows their eigenvalues to be obtained, and expectation values of local observables can then be calculated from the Hellmann-Feynman theorem.

arXiv comment11 pages, 1 figure

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• Strong-coupling emergence of dark states in XX central spin models
• Dissipative dynamics in open XXZ Richardson-Gaudin models
• Integrability and quench dynamics in the spin-1 central spin XX model
• Read-Green points and level crossings in XXZ central spin models and $p_x+i{p}_y$ topological superconductors
• Ground-state energy of a Richardson-Gaudin integrable BCS model
• Topological Burning Glass Effect
• Separability and parity transitions in $XYZ$ spin systems under nonuniform fields