ScalingStacks

0PAV

Lemma 7.4.9. Let θ:I→J\theta:I\to J and θ′:I′→I\theta^{\prime}:I^{\prime}\to I be two braids such that θ∘θ′\theta\circ\theta^{\prime} is a braid. The element deg⁡(θ)⋅deg⁡(θ′)⋅deg⁡(θ∘θ′)−1\deg(\theta)\cdot\deg(\theta^{\prime})\cdot\deg(\theta\circ\theta^{\prime})^{-1} of Γ⁡(Z,Ze​x​c+)\Gamma(Z,Z_{exc}^{+}) is in ⨁Ω12​𝐙​eΩ\bigoplus_{\Omega}\frac{1}{2}{\mathbf{Z}}e_{\Omega} and it is equal to

i⁡(θ∘θ′)−i⁡(θ)−i⁡(θ′)+12∑Ω,s′∈I′∩Ze​x​c∩Ωθs′′=id,θs′≠idc′∈C​(s′)+∖θs′​(0+)(mc′−mι⁡(c′))(⟦θ′⟧)eΩ+12∑Ω,s′∈I′∩Ωθs′′≠id,θθs′′​(1)=idc∈C​(θs′′​(1))+∖ι⁡(θs′′​(1−))θs′′​(1)∈Ze​x​c(mc−mι⁡(c))(⟦θ⟧)eΩ.i(\theta\circ\theta^{\prime})-i(\theta)-i(\theta^{\prime})\\ +\frac{1}{2}\sum_{\begin{subarray}{c}\Omega,\ s^{\prime}\in I^{\prime}\cap Z_{exc}\cap\Omega\\ \theta^{\prime}_{s^{\prime}}=\operatorname{id}\nolimits,\ \theta_{s^{\prime}}\neq\operatorname{id}\nolimits\\ c^{\prime}\in C(s^{\prime})^{+}\setminus\theta_{s^{\prime}}(0+)\end{subarray}}(m_{c^{\prime}}-m_{\iota(c^{\prime})})(\llbracket\theta^{\prime}\rrbracket)e_{\Omega}+\frac{1}{2}\sum_{\begin{subarray}{c}\Omega,\ s^{\prime}\in I^{\prime}\cap\Omega\\ \theta^{\prime}_{s^{\prime}}\neq\operatorname{id}\nolimits,\ \theta_{\theta^{\prime}_{s^{\prime}}(1)}=\operatorname{id}\nolimits\\ c\in C(\theta^{\prime}_{s^{\prime}}(1))^{+}\setminus\iota(\theta^{\prime}_{s^{\prime}}(1-))\\ \theta^{\prime}_{s^{\prime}}(1)\in Z_{exc}\end{subarray}}(m_{c}-m_{\iota(c)})(\llbracket\theta\rrbracket)e_{\Omega}.

and is also equal to

12​∑Ω,(s1′,s2′)∈(I′∩Ω)2(s1′,s2′)∉E∪E′(i⁡(θs1∘θs1′′,θs2∘θs2′′)−i⁡(θs1,θs2)−i⁡(θs1′′,θs2′′))​eΩ++∑Ω,(s1′,s2′)∈E∩Ω(i(θs1,θs2∘θ′s2′)−i(θs1,θs2)−mθs1​(0+)+(θ′s2′))eΩ++∑Ω,(s1′,s2′)∈E′∩Ω(i(θ′s1′,θs2∘θ′s2′)−i(θ′s1′,θ′s2′)−mθs1′′​(1−)−(θs2))eΩ\frac{1}{2}\sum_{\begin{subarray}{c}\Omega,(s^{\prime}_{1},s^{\prime}_{2})\in(I^{\prime}\cap\Omega)^{2}\\ (s^{\prime}_{1},s^{\prime}_{2}){\not\in}E\cup E^{\prime}\end{subarray}}\bigl(i(\theta_{s_{1}}\circ\theta^{\prime}_{s^{\prime}_{1}},\theta_{s_{2}}\circ\theta^{\prime}_{s^{\prime}_{2}})-i(\theta_{s_{1}},\theta_{s_{2}})-i(\theta^{\prime}_{s^{\prime}_{1}},\theta^{\prime}_{s^{\prime}_{2}})\bigr)e_{\Omega}+\\ +\sum_{\Omega,\ (s^{\prime}_{1},s^{\prime}_{2})\in E\cap\Omega}\bigl(i(\theta_{s_{1}},\theta_{s_{2}}\circ\theta^{\prime}_{s^{\prime}_{2}})-i(\theta_{s_{1}},\theta_{s_{2}})-m_{\theta_{s_{1}}(0+)}^{+}(\theta^{\prime}_{s^{\prime}_{2}})\bigr)e_{\Omega}+\\ +\sum_{\Omega,\ (s^{\prime}_{1},s^{\prime}_{2})\in E^{\prime}\cap\Omega}\bigl(i(\theta^{\prime}_{s^{\prime}_{1}},\theta_{s_{2}}\circ\theta^{\prime}_{s^{\prime}_{2}})-i(\theta^{\prime}_{s^{\prime}_{1}},\theta^{\prime}_{s^{\prime}_{2}})-m_{\theta^{\prime}_{s^{\prime}_{1}}(1-)}^{-}(\theta_{s_{2}})\bigr)e_{\Omega}

where

  • •

    given (s1′,s2′)∈I′2(s^{\prime}_{1},s^{\prime}_{2})\in I^{\prime 2}, we put si=θsi′′​(1)s_{i}=\theta^{\prime}_{s^{\prime}_{i}}(1)

  • •

    EE is the set of pairs (s1′,s2′)∈I′×I′(s^{\prime}_{1},s^{\prime}_{2})\in I^{\prime}\times I^{\prime} with s1′∈Ze​x​cs^{\prime}_{1}\in\ Z_{exc}, θs1′′=id\theta^{\prime}_{s^{\prime}_{1}}=\operatorname{id}\nolimits, θs1′≠id\theta_{s^{\prime}_{1}}\neq\operatorname{id}\nolimits, θs2′′≠id\theta^{\prime}_{s^{\prime}_{2}}\neq\operatorname{id}\nolimits

  • •

    E′E^{\prime} is the set of pairs (s1′,s2′)∈I′×I′(s^{\prime}_{1},s^{\prime}_{2})\in I^{\prime}\times I^{\prime} with s1∈Ze​x​cs_{1}\in\ Z_{exc}, θs1′′≠id\theta^{\prime}_{s^{\prime}_{1}}\neq\operatorname{id}\nolimits, θs1=id\theta_{s_{1}}=\operatorname{id}\nolimits and θs2≠id\theta_{s_{2}}\neq\operatorname{id}\nolimits.

0PAW

Proof. Given s′∈I′s^{\prime}\in I^{\prime} and s=θs′′​(1)s=\theta^{\prime}_{s^{\prime}}(1), the class θs∘θs′′\theta_{s}\circ\theta^{\prime}_{s^{\prime}} is admissible, hence θs​(0+)∪ι⁡(θs​(0+))=θs′′​(1−)∪ι⁡(θs′′​(1−))\theta_{s}(0+)\cup\iota(\theta_{s}(0+))=\theta^{\prime}_{s^{\prime}}(1-)\cup\iota(\theta^{\prime}_{s^{\prime}}(1-)) unless s∈Ze​x​cs\in Z_{exc} and one of θs\theta_{s} and θs′\theta_{s^{\prime}} is the identity, but not the other.

Given c∈T⁡(Z)c\in T(Z), we put

vc=(mc−mι⁡(c))​(⟦θ⟧)​ec=mc​(⟦θ⟧)​ec+mι⁡(c)​(⟦θ⟧)​eι⁡(c)=vι⁡(c).v_{c}=(m_{c}-m_{\iota(c)})(\llbracket\theta\rrbracket)e_{c}=m_{c}(\llbracket\theta\rrbracket)e_{c}+m_{\iota(c)}(\llbracket\theta\rrbracket)e_{\iota(c)}=v_{\iota(c)}.

Let

a=∑s′∈I′∩Ze​x​cθs′′=id,θs′≠idc′∈C⁡(s′)∖((θs′​(0+)∪ι⁡(θs′​(0+)))CLOSEmc′​(⟦θ′⟧)​ec′=∑s′∈I′∩Ze​x​cθs′′=id,θs′≠idc′∈C​(s′)+∖θs′​(0+)(mc′−mι⁡(c′))​(⟦θ′⟧)​ec′.a=\sum_{\begin{subarray}{c}s^{\prime}\in I^{\prime}\cap Z_{exc}\\ \theta^{\prime}_{s^{\prime}}=\operatorname{id}\nolimits,\ \theta_{s^{\prime}}\neq\operatorname{id}\nolimits\\ c^{\prime}\in C(s^{\prime})\setminus\bigl((\theta_{s^{\prime}}(0+)\cup\iota(\theta_{s^{\prime}}(0+))\bigr)\end{subarray}}m_{c^{\prime}}(\llbracket\theta^{\prime}\rrbracket)e_{c^{\prime}}=\sum_{\begin{subarray}{c}s^{\prime}\in I^{\prime}\cap Z_{exc}\\ \theta^{\prime}_{s^{\prime}}=\operatorname{id}\nolimits,\ \theta_{s^{\prime}}\neq\operatorname{id}\nolimits\\ c^{\prime}\in C(s^{\prime})^{+}\setminus\theta_{s^{\prime}}(0+)\end{subarray}}(m_{c^{\prime}}-m_{\iota(c^{\prime})})(\llbracket\theta^{\prime}\rrbracket)e_{c^{\prime}}.

We have

m⁡(θ∘θ′)−m⁡(θ)−m⁡(θ′)=m(\theta\circ\theta^{\prime})-m(\theta)-m(\theta^{\prime})=
=∑s′∈I′c′∈(θ∘θ′)s′​(0+)∪ι⁡((θ∘θ′)s′​(0+))mc′​(⟦θ⟧)​ec′−∑s∈Ic∈θs​(0+)∪ι⁡(θs​(0+))mc​(⟦θ⟧)​ec−a=\sum_{\begin{subarray}{c}s^{\prime}\in I^{\prime}\\ c^{\prime}\in(\theta\circ\theta^{\prime})_{s^{\prime}}(0+)\cup\iota((\theta\circ\theta^{\prime})_{s^{\prime}}(0+))\end{subarray}}m_{c^{\prime}}(\llbracket\theta\rrbracket)e_{c^{\prime}}-\sum_{\begin{subarray}{c}s\in I\\ c\in\theta_{s}(0+)\cup\iota(\theta_{s}(0+))\end{subarray}}m_{c}(\llbracket\theta\rrbracket)e_{c}-a
=∑s′∈I′θs′′≠idvθs′′​(0+)−∑s′∈I′θs′′≠idθθs′′​(1)≠idvθs′′​(1−)−12​∑s′∈I′θs′′≠idθθs′′​(1)=idc∈C⁡(θs′′​(1))vc−a=\sum_{\begin{subarray}{c}s^{\prime}\in I^{\prime}\\ \theta^{\prime}_{s^{\prime}}\neq\operatorname{id}\nolimits\end{subarray}}v_{\theta^{\prime}_{s^{\prime}}(0+)}-\sum_{\begin{subarray}{c}s^{\prime}\in I^{\prime}\\ \theta^{\prime}_{s^{\prime}}\neq\operatorname{id}\nolimits\\ \theta_{\theta^{\prime}_{s^{\prime}}(1)}\neq\operatorname{id}\nolimits\end{subarray}}v_{\theta^{\prime}_{s^{\prime}}(1-)}-\frac{1}{2}\sum_{\begin{subarray}{c}s^{\prime}\in I^{\prime}\\ \theta^{\prime}_{s^{\prime}}\neq\operatorname{id}\nolimits\\ \theta_{\theta^{\prime}_{s^{\prime}}(1)}=\operatorname{id}\nolimits\\ c\in C(\theta^{\prime}_{s^{\prime}}(1))\end{subarray}}v_{c}-a

Using (7.3.1), we find

⟨⟦θ⟧,⟦θ′⟧⟩\displaystyle\langle\llbracket\theta\rrbracket,\llbracket\theta^{\prime}\rrbracket\rangle =−12∑s′∈I′c′∈θs′′​(0+)∪ι⁡(θs′′​(0+))vc′+12∑s′∈I′c∈θs′′​(1−)∪ι⁡(θs′′​(1−))vc\displaystyle=-\frac{1}{2}\sum_{\begin{subarray}{c}s^{\prime}\in I^{\prime}\\ c^{\prime}\in\theta^{\prime}_{s^{\prime}}(0+)\cup\iota(\theta^{\prime}_{s^{\prime}}(0+))\end{subarray}}v_{c^{\prime}}+\frac{1}{2}\sum_{\begin{subarray}{c}s^{\prime}\in I^{\prime}\\ c\in\theta^{\prime}_{s^{\prime}}(1-)\cup\iota(\theta^{\prime}_{s^{\prime}}(1-))\end{subarray}}v_{c}
=−∑s′∈I′θs′′≠idvθs′′​(0+)+∑s′∈I′θs′′≠idvθs′′​(1−).\displaystyle=-\sum_{\begin{subarray}{c}s^{\prime}\in I^{\prime}\\ \theta^{\prime}_{s^{\prime}}\neq\operatorname{id}\nolimits\end{subarray}}v_{\theta^{\prime}_{s^{\prime}}(0+)}+\sum_{\begin{subarray}{c}s^{\prime}\in I^{\prime}\\ \theta^{\prime}_{s^{\prime}}\neq\operatorname{id}\nolimits\end{subarray}}v_{\theta^{\prime}_{s^{\prime}}(1-)}.

We deduce that

⟨⟦θ⟧,⟦θ′⟧⟩+m(θ∘θ′)−m(θ)−m(θ′)=−∑s′∈I′θs′′≠idθθs′′​(1)=idc∈C​(θs′′​(1))+∖ι⁡(θs′′​(1−))θs′′​(1)∈Ze​x​c(mc−mι⁡(c))(⟦θ⟧)ec−a\langle\llbracket\theta\rrbracket,\llbracket\theta^{\prime}\rrbracket\rangle+m(\theta\circ\theta^{\prime})-m(\theta)-m(\theta^{\prime})=-\sum_{\begin{subarray}{c}s^{\prime}\in I^{\prime}\\ \theta^{\prime}_{s^{\prime}}\neq\operatorname{id}\nolimits\\ \theta_{\theta^{\prime}_{s^{\prime}}(1)}=\operatorname{id}\nolimits\\ c\in C(\theta^{\prime}_{s^{\prime}}(1))^{+}\setminus\iota(\theta^{\prime}_{s^{\prime}}(1-))\\ \theta^{\prime}_{s^{\prime}}(1)\in Z_{exc}\end{subarray}}(m_{c}-m_{\iota(c)})(\llbracket\theta\rrbracket)e_{c}-a

and the first equality of the lemma follows.

Consider s1′≠s2′s^{\prime}_{1}\neq s^{\prime}_{2} in I′I^{\prime}.

If s1′∈Ze​x​cs^{\prime}_{1}\in Z_{exc}, θs1′′=ids1′\theta^{\prime}_{s^{\prime}_{1}}=\operatorname{id}\nolimits_{s^{\prime}_{1}} and θs1≠ids1\theta_{s_{1}}\neq\operatorname{id}\nolimits_{s_{1}}, it follows from Lemma 7.3.21 that

∑s2′∈I′θs2′′≠idi⁡(ids1′,θs2′′)=12​∑s2′∈I′θs2′′≠ids2′c′∈C​(s1′)+(mc′−mι⁡(c′))​(θs2′′)=12​∑c′∈C​(s1′)+(mc′−mι⁡(c′))​(⟦θ′⟧).\sum_{\begin{subarray}{c}s^{\prime}_{2}\in I^{\prime}\\ \theta^{\prime}_{s^{\prime}_{2}}\neq\operatorname{id}\nolimits\end{subarray}}i(\operatorname{id}\nolimits_{s^{\prime}_{1}},\theta^{\prime}_{s^{\prime}_{2}})=\frac{1}{2}\sum_{\begin{subarray}{c}s^{\prime}_{2}\in I^{\prime}\\ \theta^{\prime}_{s^{\prime}_{2}}\neq\operatorname{id}\nolimits_{s^{\prime}_{2}}\\ c^{\prime}\in C(s^{\prime}_{1})^{+}\end{subarray}}(m_{c^{\prime}}-m_{\iota(c^{\prime})})(\theta^{\prime}_{s^{\prime}_{2}})=\frac{1}{2}\sum_{c^{\prime}\in C(s^{\prime}_{1})^{+}}(m_{c^{\prime}}-m_{\iota(c^{\prime})})(\llbracket\theta^{\prime}\rrbracket).

Similarly, if s1∈Ze​x​cs_{1}\in Z_{exc}, θs1′′≠id\theta^{\prime}_{s^{\prime}_{1}}\neq\operatorname{id}\nolimits and θs1=id\theta_{s_{1}}=\operatorname{id}\nolimits, we have

∑s2′∈I′θs2≠idi⁡(ids1,θs2)=12​∑c∈C​(s1)+(mc−mι⁡(c))​(⟦θ⟧).\sum_{\begin{subarray}{c}s^{\prime}_{2}\in I^{\prime}\\ \theta_{s_{2}}\neq\operatorname{id}\nolimits\end{subarray}}i(\operatorname{id}\nolimits_{s_{1}},\theta_{s_{2}})=\frac{1}{2}\sum_{c\in C(s_{1})^{+}}(m_{c}-m_{\iota(c)})(\llbracket\theta\rrbracket).

The second equality of the lemma follows. ∎

Original mathematics by the credited authors. Source collection and HTML conversion remain in progress.

Andrew Manion, Raphael Rouquier

Original source: arXiv:2009.09627v2