nLab Yang-Baxter equation

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Contents

Contents

Idea

A Yang-Baxter equation (YBE) is, in some form or other, an algebraic reflection of this isotopy of braids:


(1)

which is also known as the 2nd Artin braid relation or the 3rd Reidemeister move for framed links.

Quantum YBE

Plain form

Interpreting the isotopy (1) as an equality of string diagrams in a braided monoidal category (𝒞,)(\mathcal{C}, \otimes), with each strand/string labeled by the same given object V𝒞V \in \mathcal{C}, it says that the braiding R:VVVVR \colon\, V \otimes V \to V \otimes V satisfies

(2)(Rid)(idR)(Rid)=(idR)(Rid)(idR) (R \otimes id) \circ (id \otimes R) \circ (R \otimes id) \;\; = \;\; (id \otimes R) \circ (R \otimes id) \circ (id \otimes R)

as an equation in End ( V V V ) End(V \otimes V \otimes V) (where we are notationally suppressing associators, in full this is diagram B7 in Joyal & Street 1985 p 7).

This equation (2) — on any map RR of the form R:VVVVR \,\colon\, V \otimes V \to V \otimes V (not necessarily the ambient braiding structure map) — is called the plain quantum Yang-Baxter equation.

If VVV \otimes V is the tensor product of a finite-dimensional vector space VV with itself, then any choice of linear basis Vk dV \simeq k^d identifies the linear map RR with a matrix (R n 1,n 2 m 1,m 2) n i,m i=1 d(R_{n_1, n_2}^{m_1, m_2})_{n_i, m_i = 1}^{d}, thus traditionally called an R-matrix.

In a symmetric monoidal category like Vect Vect , with symmetric braiding σ:VVVV\sigma \,\colon\, V \otimes V \to V \otimes V, it is traditional to define

RˇσRandRˇ ijϕ i,j(σR), \check R \,\coloneqq\, \sigma \circ R \;\;\;\; \text{and} \;\;\;\; \check R_{i j} \,\coloneqq\, \phi_{i,j}(\sigma \circ R) \mathrlap{\,,}

where

ϕ i,j:End(VV)End(VVV)for1i<j3 \phi_{i,j} \,\colon\, End(V \otimes V) \hookrightarrow End(V \otimes V \otimes V) \;\;\;\;\; \text{for} \; 1 \leq i \lt j \leq 3

identifies VVV \otimes V with the tensor product of the iith and the jjth copy of VV in VVVV \otimes V \otimes V (inserting an identity on the remaining copy).

In terms of this “check-R matrix” Rˇ\check R, the plain quantum Yang-Baxter equation (2) is equivalent to

(3)Rˇ 23Rˇ 13Rˇ 12=Rˇ 12Rˇ 13Rˇ 23. \check R_{23} \circ \check R_{13} \circ \check R_{12} \;=\; \check R_{12} \circ \check R_{13} \circ \check R_{23} \,.


Braid representations. In either form, any solution to the plain Yang-Baxter equation in Vect Vect defines linear representations of the braid groups Br nBr_n (braid representations), by representing the iith Artin braid generator b ib_i by

b iid i1Rid ni1. b_i \;\; \mapsto \;\; id^{\otimes_{i-1}} \otimes R \otimes id^{\otimes_{n-i-1}} \,.

This is manifest from the Artin presentation of the braid group, see there.

If, in addition, the RR-matrix is involutive in that RR=idR \circ R = id, then these braid representations actually are (factor through) representations of the symmetric group Sym nSym_n.


Parameterized form

The plain form (3) of the Yang-Baxter equation generalizes to the case where Rˇ ij\check R_{i j} is taken to dependent on a pair of parameters u,uUu, u' \in U (typically taken from U=U = \mathbb{C} the complex numbers), in which case one says that the condition

(4)Rˇ 23(u 2,u 3)Rˇ 13(u 1,u 3)Rˇ 12(u 1,u 2)=Rˇ 12(u 1,u 2)Rˇ 13(u 1,u 3)Rˇ 23(u 2,u 3) \check R_{23}(u_2, u_3) \circ \check R_{13}(u_1, u_3) \circ \check R_{12}(u_1, u_2) \;=\; \check R_{12}(u_1, u_2) \circ \check R_{13}(u_1, u_3) \circ \check R_{23}(u_2, u_3)

is the parameterized quantum Yang-Baxter equation.

In the special case of this generalization where U ×U \equiv \mathbb{C}^\times is the multiplicative group of complex numbers and restricting the dependence to be on the quotient of the parameters

Rˇ(u,u)=Rˇ(u/u), \check R(u, u') \,=\, \check R( u/u') \,,

the parameterized quantum Yang-Baxter equation (4) becomes (identifying uu 1/u 2u \coloneqq u_1/u_2 and vu 2/u 3v \coloneqq u_2/u_3)

(5)Rˇ 23(v)Rˇ 13(uv)Rˇ 12(u)=Rˇ 12(u)Rˇ 13(uv)Rˇ 23(v), \check R_{23}(v) \circ \check R_{13}(u v) \circ \check R_{12}(u) \;=\; \check R_{12}(u) \circ \check R_{13}(u v) \circ \check R_{23}(v) \,,

and one speaks of the parameterized quantum Yang-Baxter equation with “multiplicative spectral parameter”.

Yet again redefining by passage to logarithms of the parameters, ulnuu \mapsto ln u (or rather, understanding the previous parameters a exponentials), the equation (6) assumes the form with “additive spectral parameter”:

(6)Rˇ 23(v)Rˇ 13(u+v)Rˇ 12(u)=Rˇ 12(u)Rˇ 13(u+v)Rˇ 23(v). \check R_{23}(v) \circ \check R_{13}(u + v) \circ \check R_{12}(u) \;=\; \check R_{12}(u) \circ \check R_{13}(u + v) \circ \check R_{23}(v) \,.

This spectral form (6) is close to the historical origin of Yang-Baxter equation, whence some authors refer to this form by default as the “the Yang-Baxter equation” (cf. Jimbo 1989 (2.1)).

Classical YBE

(…)

Variants

Beware that the term Yang-Baxter equation can mean (or be interpreted in the context of) any of several related but different concepts:

Yang-Baxter equations

References

for more see at quantum YBE, classical YBE, etc.

The (quantum) Yang-Baxter equation was named (cf. Perk & Au-Yang 2006) by Ludwig Fadeev in the late 1970s, in honor of:

and

Reviews:

  • Michio Jimbo: Introduction to the Yang-Baxter Equation, International Journal of Modern Physics A 4 15 (1989) 3717-3757 [doi:10.1142/S0217751X89001497]

    reprinted in: Braid Group, Knot Theory and Statistical Mechanics, Advanced Series in Mathematical Physics 9, World Scientific (1991) [doi:10.1142/0796]

  • Jacques H. H. Perk, Helen Au-Yang: Yang-Baxter Equations, Encyclopedia of Mathematical Physics 5 (2006) 465-473 [arXiv:math-ph/0606053]

Literature collection with focus on application to integrable systems:

  • Michio Jimbo (ed.): Yang-Baxter Equation in Integrable Systems, Advanced Series in Mathematical Physics 10, World Scientific (1990) [doi:10.1142/1021]

See also:

Last revised on February 15, 2025 at 15:46:57. See the history of this page for a list of all contributions to it.