Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Communications in Theoretical Physics

A Free-Fermion Type Solution of Quantum Dynamical Yang–Baxter Equation

Ju Guo-Xing, Luo XuDong, Wang ShiKun, Ke Wu

Published Dec 15, 1999• 2 citations
Publisher

Abstract

The symmetries of the quantum dynamical Yang-Baxter (QDYB) equation without spectral parameters for gl(2) are discussed. The classification of the six-vertex type solutions to the QDYB equation without spectral parameters is given and a free-fermion type solution is obtained.
DOI
10.1088/0253-6102/32/4/557

Related papers

Lax Pairs for Integrable Six-Vertex Model with Color Parameters

Ju Guo-Xing

Using the colored Yang–Baxter equation, the Lax pairs for the system with color parameters and periodic boundary conditions are derived. The explicit expressions of the Lax pairs for the six-vertex standard matrices of both the Baxter and free-Fermion types are given.

Communications in Theoretical Physics•Mar 15, 2003•0 citations

Lax Pairs for Integrable Six—Vertex Model with Color Paramters

JUGuo-Xing

Using the colored Yang-Baxter equation,the Lax pairs for the system with color parameters and periodic boundary conditions are derived.The explicit expressions of the Lax pairs for the six-vertex standard R matrices of both the Baxter and free-Fermion types are given.

理论物理通讯:英文版•Jan 1, 2003•0 citations

SOLUTIONS OF YANG-BAXTER EQUATIONWITH SPECTRAL PARAMETER FORSIX-VERTEX MODEL

S Wang

In this paper, we obtain all solutions of Yang-Baxter equation with spectral parameter for six-vertex model in theory of exactly solved statistical models by four sets of non-degenarate basic solutions and seven sets of degenerate basic solutions up to five solution transformations. The unitary condition of the solutions is also discussed.

Acta Physica Sinica•Jan 1, 1995•0 citations

The Six-Vertex Yang-Baxter Groupoid

Daniel Bump, Slava Naprienko

A parametrized Yang-Baxter equation is usually defined to be a map from a group to a set of R-matrices, satisfying the Yang-Baxter commutation relation. These are a mainstay of solvable lattice models. We will show how the parameter space can sometimes be enlarged to a groupoid, and give two examples of such groupoid parametrized Yang-Baxter equations, within the six vertex model. A groupoid parametrized Yang-Baxter equation consists of a groupoid $\mathfrak{G}$ together with a map $π:\mathfrak{G}\to\operatorname{End}(V\otimes V)$ for some vector space $V$ such that the Yang-Baxter commutator $[[ π(u),π(w),π(v)]]=0$ if $u,v\in\mathfrak{G}$ are such that the groupoid composition $w=u\star v$ is defined. An important role is played by an object map $Δ:\mathfrak{G}\to M$ for some set $M$ such that $Δ(u)=Δ(v')$, $Δ(w)=Δ(v)$ and $Δ(w')=Δ(u')$, where $v\mapsto v'$ is the groupoid inverse map. There are two main regimes of the six-vertex model: the free-fermionic point, and everything else. For the free-fermionic point, there exists a parametrized Yang-Baxter equation with a large parameter group $\operatorname{GL}(2)\times\operatorname{GL}(1)$. For non-free-fermionic six-vertex matrices, there are also well-known (group) parametrized Yang-Baxter equations, but these do not account for all possible interactions. Instead we will construct a groupoid parametrized Yang-Baxter equation that accounts for essentially all possible Yang-Baxter equations in the six-vertex model. We will also exhibit a separate groupoid for the five-vertex model. We will show how to construct solvable lattice models based on groupoid parametrized Yang-Baxter equations.

arXiv:2503.05960•Mar 7, 2025•0 citations

New type of solutions of Yang-Baxter equations, quantum entanglement and related physical models

Li-Wei Yu, Mo-Lin Ge

Starting from the Kauffman-Lomonaco braiding matrix transforming the natural basis to Bell states, the spectral parameter describing the entanglement is introduced through Yang-Baxterization. It gives rise to a new type of solutions for Yang-Baxter equation, called the type-II that differs from the familiar solution called type-I of YBE associated with the usual chain models. The Majorana fermionic version of type-II yields the Kitaev Hamiltonian. The introduced ℓ 1 -norm leads to the maximum of the entanglement by taking the extreme value and shows that it is related to the Wigner's D-function. Based on the Yang-Baxter equation the 3-body S-Matrix for type-II is explicitly given. Different from the type-I solution, the type-II solution of YBE should be considered in describing quantum information. The idea is further extended to 3 parafermion model based on SU (3) principal representation. The type-II is in difference from the familiar type-I in many respects. For example, the quantities corresponding to velocity in the chain models obey the Lorentzian additivity rather than Galilean rule ( u + v ). Most possibly, for the type-II solutions of YBE there may not exist RTT relation. Further more, for 3 parafermion model we only need the rational Yang-Baxterization, which seems like trigonometric. Similar discussions are also made in terms of generalized Yang-Baxter equation with three spin spaces .

arXiv:1810.09813•Journal of Physics Conference Series•Apr 1, 2019•2 citations

Free Fermion Conditions and the Symmetries of Integrability

C.-M. Viallet

We show that free-fermion conditions on vertex models amount to degeneration conditions for the inversion relations and the symmetries of the Yang-Baxter equations. We also show how solutions of the tetrahedron equations enjoy a similar property, and analyze the phenomenon.

International Journal of Modern Physics B•Jan 20, 1997•3 citations
A parametrized Yang-Baxter equation is usually defined to be a map from a group to a set of R-matrices, satisfying the Yang-Baxter commutation relation. These are a mainstay of solvable lattice models. We will show how the parameter space can sometimes be enlarged to a groupoid, and give two examples of such groupoid parametrized Yang-Baxter equations, within the six vertex model. A groupoid parametrized Yang-Baxter equation consists of a groupoid G\mathfrak{G}G together with a map π:G→End⁡(V⊗V)π:\mathfrak{G}\to\operatorname{End}(V\otimes V)π:G→End(V⊗V) for some vector space VVV such that the Yang-Baxter commutator [[π(u),π(w),π(v)]]=0[[ π(u),π(w),π(v)]]=0[[π(u),π(w),π(v)]]=0 if u,v∈Gu,v\in\mathfrak{G}u,v∈G are such that the groupoid composition w=u⋆vw=u\star vw=u⋆v is defined. An important role is played by an object map Δ:G→MΔ:\mathfrak{G}\to MΔ:G→M for some set MMM such that Δ(u)=Δ(v′)Δ(u)=Δ(v')Δ(u)=Δ(v′), Δ(w)=Δ(v)Δ(w)=Δ(v)Δ(w)=Δ(v) and Δ(w′)=Δ(u′)Δ(w')=Δ(u')Δ(w′)=Δ(u′), where v↦v′v\mapsto v'v↦v′ is the groupoid inverse map. There are two main regimes of the six-vertex model: the free-fermionic point, and everything else. For the free-fermionic point, there exists a parametrized Yang-Baxter equation with a large parameter group GL⁡(2)×GL⁡(1)\operatorname{GL}(2)\times\operatorname{GL}(1)GL(2)×GL(1). For non-free-fermionic six-vertex matrices, there are also well-known (group) parametrized Yang-Baxter equations, but these do not account for all possible interactions. Instead we will construct a groupoid parametrized Yang-Baxter equation that accounts for essentially all possible Yang-Baxter equations in the six-vertex model. We will also exhibit a separate groupoid for the five-vertex model. We will show how to construct solvable lattice models based on groupoid parametrized Yang-Baxter equations.
Starting from the Kauffman-Lomonaco braiding matrix transforming the natural basis to Bell states, the spectral parameter describing the entanglement is introduced through Yang-Baxterization. It gives rise to a new type of solutions for Yang-Baxter equation, called the type-II that differs from the familiar solution called type-I of YBE associated with the usual chain models. The Majorana fermionic version of type-II yields the Kitaev Hamiltonian. The introduced ℓ 1 -norm leads to the maximum of the entanglement by taking the extreme value and shows that it is related to the Wigner's D-function. Based on the Yang-Baxter equation the 3-body S-Matrix for type-II is explicitly given. Different from the type-I solution, the type-II solution of YBE should be considered in describing quantum information. The idea is further extended to 3 parafermion model based on SU (3) principal representation. The type-II is in difference from the familiar type-I in many respects. For example, the quantities corresponding to velocity in the chain models obey the Lorentzian additivity rather than Galilean rule ( u + v ). Most possibly, for the type-II solutions of YBE there may not exist RTT relation. Further more, for 3 parafermion model we only need the rational Yang-Baxterization, which seems like trigonometric. Similar discussions are also made in terms of generalized Yang-Baxter equation with three spin spaces .