"Y-system and functional dilogarithm identities"의 두 판 사이의 차이
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* {{수학노트|url=5항_관계식_(5-term_relation)}} | * {{수학노트|url=5항_관계식_(5-term_relation)}} | ||
+ | * [[5-term relation revisited from the viewpoint of Y-system]] | ||
2013년 8월 22일 (목) 10:17 판
introduction
- 틀:수학노트
- $\mathbb{Y}(X,X')$ the order of $X$ and $X'$ matters!
main results
- Bloch group element
$$ \sum_{(\mathbf{i},u)\in S_{+}} Y_{\mathbf{i}}(u)\wedge (1+Y_{\mathbf{i}}(u))=0\in \Lambda^2 \mathbb{Q}(y)^{\times} $$ where $S_{+}=\{(\mathbf{i},u) |0\leq u \leq 2(h+h')-1,(\mathbf{i},u)\in P_{+}\}$.
- functional dilogarithm identity
$$ \sum_{(\mathbf{i},u)\in S_{+}}L\left(\frac{Y_\mathbf{i}(u)}{1+Y_\mathbf{i}(u)}\right)=h r r' L(1) $$
bicoloring
- what's $P_{+}$?
- We give an alternate bicoloring on the pair of Dynkin diagrams. Let us fix bipartite decompositions of $I$ and $I'$.
- Let $ \mathbf{I}= I\times I'$ and $\mathbf{I}=\mathbf{I}_{+}\sqcup \mathbf{I}_{-}$ where $\mathbf{I}_{+}=(I_{+}\times I'_{+}) \sqcup (I_{-}\times I'_{-})$ and $\mathbf{I}_{-}=(I_{+}\times I'_{-}) \sqcup (I_{-}\times I'_{+})$.
- Let $\epsilon : \mathbf{I}\to \{1,-1\}$ be the function defined by $\epsilon(\mathbf{i})=\pm 1$ for $\mathbf{i}\in \mathbf{I}_{\pm}$ and $P_{\pm} =\{(\mathbf{i},u)\in \mathbf{I}\times\mathbb{Z}| \epsilon(\mathbf{i})(-1)^u=\pm 1\}$.
- Roughly speaking, we want our alternate bicoloring interchanges their colors as $u\in \mathbb{Z}$ changes by 1.
an example
- compute $\mathbb{Y}(A_2,A_1)$ explicitly
- \(y_{m-1}y_{m+1}=y_m+1\)
- Start with two variables \(y_1,y_2\).
- \(y_3y_1=y_2+1\). so \(y_3=\frac{y_2+1}{y_1}\)
- \(y_2y_4=y_3+1 \)implies \(y_4=\frac{y_3+1}{y_2}=\frac{y_1+y_2+1}{y_1y_2}\)
- \(y_3y_5=y_4+1\) implies \(y_5=\frac{y_4+1}{y_3}= \frac{y_1+1}{y_2}\) we are getting Laurent polynomials
- \(y_4y_6=y_5\) implies \(y_6=\frac{y_5+1}{y_4}= \frac{\frac{y_1+1}{y_2}+1}{\frac{y_1+y_2+1}{y_1y_2}}=\frac{y_1(y_1+1)+y_1y_2}{y_1+y_2+1}=y_1\)
- rank 2 cluster algebra
observations
- we saw that $$S=\left\{x,y,\frac{y+1}{x},\frac{x+y+1}{x y},\frac{x+1}{y}\right\}$$ forms a half-period of $\mathbb{Y}(A_2,A_1)$.
- So we have $r=2,h=3$ and $r'=1,h'=2$.
- They are all Laurent polynomials in $x$ and $y$.
dilogarithm identities
- From this, one can get functional dilogarithm identities
\begin{align} &\sum_{a\in S}L\left(\frac{a}{1+a}\right) \notag \\ =& L\left(\frac{x}{1+x}\right)+L\left(\frac{y}{1+y}\right)+L\left(\frac{1+y}{x (1+\frac{1+y}{x})}\right)+L\left(\frac{1+x+y}{x y (1+\frac{1+x+y}{x y})}\right)+L\left(\frac{1+x}{(1+\frac{1+x}{y}) y}\right) \notag \\ =& L\left(\frac{x}{x+1}\right)+L\left(\frac{y}{y+1}\right)+L\left(\frac{y+1}{x+y+1}\right)+L\left(\frac{x+y+1}{x y+x+y+1}\right)+L\left(\frac{x+1}{x+y+1}\right) \notag \\ =&3L(1)=\frac{\pi^2}{2} \notag \end{align} and \begin{align} &\sum_{a\in S}L\left(\frac{1}{1+a}\right) \notag \\ =& L\left(\frac{1}{x+1}\right)+L\left(\frac{1}{y+1}\right)+L\left(\frac{1}{\frac{y+1}{x}+1}\right)+L\left(\frac{1}{\frac{x+y+1}{x y}+1}\right)+L\left(\frac{1}{\frac{x+1}{y}+1}\right) \notag \\ =& L\left(\frac{1}{x+1}\right)+L\left(\frac{1}{y+1}\right)+L\left(\frac{x}{x+y+1}\right)+L\left(\frac{x y}{x y+x+y+1}\right)+L\left(\frac{y}{x+y+1}\right) \notag \\ =&2L(1)=\frac{\pi^2}{3} \notag. \end{align}
history
- 9-term relation and its accessibility
- cluster algebra
- Nahm's equation
- Central charge, L-values and dilogarithm
- dilogarithm and dilogarithm identities
- Bloch group, K-theory and dilogarithm
computational resource
expositions
- Dilogarithm identities in conformal field theory and cluster algebras
- Periodicities in cluster algebras and dilogarithm identities
articles
- Periodic cluster algebras and dilogarithm identities Tomoki Nakanishi, 2010
- Periodicities of T and Y-systems, dilogarithm identities, and cluster algebras I: Type B_r Rei Inoue, Osamu Iyama, Bernhard Keller, Atsuo Kuniba, Tomoki Nakanishi, 2010
- Dilogarithm identities for conformal field theories and cluster algebras: simply laced case Tomoki Nakanishi, 2009
- Chapoton, Frédéric. 2005. Functional Identities for the Rogers Dilogarithm Associated to Cluster Y-Systems. Bulletin of the London Mathematical Society 37, no. 5 (October 1): 755 -760. doi:10.1112/S0024609305004510.
- Thermodynamic Bethe Ansatz and Dilogarithm Identities I Edward Frenkel, Andras Szenes, 1995
- ADE functional dilogarithm identities and integrable models F. Gliozzi, R. Tateo, Phys. Lett. 348B (1995) 84-88.
- Rogers Dilogarithm in Integrable Systems A. Kuniba, T. Nakanishi, 1992
- Spectra in Conformal Field Theories from the Rogers Dilogarithm Atsuo Kuniba, Tomoki Nakanishi, 1992