Classification of classical spin liquids: Detailed formalism and suite of examples
Physical Review B, 2024•APS
The hallmark of highly frustrated systems is the presence of many states close in energy to
the ground state. Fluctuations between these states can preclude the emergence of any form
of order and lead to the appearance of spin liquids. Even on the classical level, spin liquids
are not all alike: they may have algebraic or exponential correlation decay, and various
forms of long wavelength description, including vector or tensor gauge theories. Here, we
introduce a classification scheme, allowing us to fit the diversity of classical spin liquids …
the ground state. Fluctuations between these states can preclude the emergence of any form
of order and lead to the appearance of spin liquids. Even on the classical level, spin liquids
are not all alike: they may have algebraic or exponential correlation decay, and various
forms of long wavelength description, including vector or tensor gauge theories. Here, we
introduce a classification scheme, allowing us to fit the diversity of classical spin liquids …
The hallmark of highly frustrated systems is the presence of many states close in energy to the ground state. Fluctuations between these states can preclude the emergence of any form of order and lead to the appearance of spin liquids. Even on the classical level, spin liquids are not all alike: they may have algebraic or exponential correlation decay, and various forms of long wavelength description, including vector or tensor gauge theories. Here, we introduce a classification scheme, allowing us to fit the diversity of classical spin liquids (CSLs) into a general framework as well as predict and construct new kinds. CSLs with either algebraic or exponential correlation-decay can be classified via the properties of the bottom flat band(s) in their soft-spin Hamiltonians. The classification of the former is based on the algebraic structures of gapless points in the spectra, which relate directly to the emergent generalized Gauss's laws that control the low-temperature physics. The second category of CSLs, meanwhile, are classified by the fragile topology of the gapped bottom band(s). Utilizing the classification scheme we construct new models realizing exotic CSLs, including one with anisotropic generalized Gauss's laws and charges with subdimensional mobility, one with a network of pinch-line singularities in its correlation functions and a series of fragile topological CSLs connected by zero-temperature transitions.
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