Abstract
Fractionalization is a ubiquitous phenomenon in topological states of matter. In this work, we study the collective behavior of fractionalized topological charges and their instabilities, through the J_{1}-J_{2}-J_{3} Ising model on a kagome lattice. This model can be mapped onto a Hamiltonian of interacting topological charges under the constraint of Gauss' law. We find that the recombination of topological charges gives rise to a yet unexplored classical spin liquid. This spin liquid is characterized by an extensive residual entropy, as well as the formation of hexamers of same-sign topological charges. The emergence of hexamers is reflected by a half-moon signal in the magnetic structure factor, which provides a signature of this new spin liquid in elastic neutron-scattering experiments. To study this phase, a worm algorithm has been developed which does not require the usual divergence-free condition.
Highlights
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We study the collective behavior of fractionalized topological charges and their instabilities, through the J1-J2-J3 Ising model on a kagome lattice, which can be mapped to a model of interacting topological charges under the constraint of Gauss’ law
We study the cooperative phenomena of fractionalized topological charges in the kagome classical spin liquid (CSL) [18,19,20,21] of the J1-J2-J3 Ising model
Summary
We base our arguments on the Gauss’ law as introduced in Eq (3) in the main text. This equation results from the definition of charge defined on a triangle, p: Qp = ηp σiz,. If we consider a set of triangles, D, and sum Eq (1) over D, we obtain the. As noted in the main text, ∂D means the sites on its boundary, and pD(i) is a triangle in D that includes the site i. The summation of ηpD(i)σiz vanishes for internal sites of D, leaving only the boundary contribution. (2), (3) and (4), we can obtain various information regarding the ground states On the basis of Eqs. (2), (3) and (4), we can obtain various information regarding the ground states
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