Cote n° 142 · pages 2–120
· 358 displayed formulas · Action de Galois sur Teichmüller : notes manuscrites (s.d.).
Inventory dating : [à partir de 1978]
Édition de démonstration
\[(1)\qquad \mathrm{Hom}_{\mathrm{isot}}(X,Y)=\text{ensemble des composantes connexes}\]
LaTeX source
\[
(1)\qquad \mathrm{Hom}_{\mathrm{isot}}(X,Y)=\text{ensemble des composantes connexes}
\]\[(2)\qquad F\colon X\times I\longrightarrow Y\times I,\qquad I=[0,1]\]
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\[ (2)\qquad F\colon X\times I\longrightarrow Y\times I,\qquad I=[0,1] \]
\[(3)\qquad F(x,0)=(f(x),0),\qquad F(x,1)=(g(x),1)\qquad\forall x\in X .\]
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\[ (3)\qquad F(x,0)=(f(x),0),\qquad F(x,1)=(g(x),1)\qquad\forall x\in X . \]
\[Y'\longmapsto Y'\times I\]
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\[ Y'\longmapsto Y'\times I \]
\[(4)\qquad \alpha\colon X\times I\xrightarrow{\ \sim\ }Y'\times I\]
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\[
(4)\qquad \alpha\colon X\times I\xrightarrow{\ \sim\ }Y'\times I
\]\[(6)\qquad f=pf_{0},\qquad g=pg_{0}\qquad (p\colon Y'\to Y\ \text{la projection}),\]
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\[
(6)\qquad f=pf_{0},\qquad g=pg_{0}\qquad (p\colon Y'\to Y\ \text{la projection}),
\]\[(7)\qquad f_{0}\colon X\xrightarrow{\ \sim\ }Y',\qquad g_{0}\colon X\xrightarrow{\ \sim\ }Y'\]
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\[
(7)\qquad f_{0}\colon X\xrightarrow{\ \sim\ }Y',\qquad g_{0}\colon X\xrightarrow{\ \sim\ }Y'
\]\[(8)\qquad g_{0}=f_{0}\circ u,\]
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\[
(8)\qquad g_{0}=f_{0}\circ u,
\]\[(9)\qquad u\colon X\xrightarrow{\ \sim\ }X\]
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\[
(9)\qquad u\colon X\xrightarrow{\ \sim\ }X
\]\[g=pg_{0}=p(f_{0}\circ u)=(pf_{0})u=f\circ u .\]
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\[
g=pg_{0}=p(f_{0}\circ u)=(pf_{0})u=f\circ u .
\]\[(10)\qquad X\xrightarrow[\ \sim\ ]{\ f_{0}\ }Y'\xrightarrow{\ p\ }Y\]
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\[
(10)\qquad X\xrightarrow[\ \sim\ ]{\ f_{0}\ }Y'\xrightarrow{\ p\ }Y
\]\[(11)\qquad (\gamma f_{0}\sim f_{0})\Longrightarrow\gamma=\mathrm{id}_{Y'}\ ?\]
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\[
(11)\qquad (\gamma f_{0}\sim f_{0})\Longrightarrow\gamma=\mathrm{id}_{Y'}\ ?
\]\[(12)\qquad \widehat{\mathrm{Hom}}_{\mathrm{ét}}(X,Y)=\mathrm{Hom}_{\mathrm{ét}}(X,Y)\wedge^{T_{X}}\widehat{T}_{X}\]
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\[
(12)\qquad \widehat{\mathrm{Hom}}_{\mathrm{ét}}(X,Y)=\mathrm{Hom}_{\mathrm{ét}}(X,Y)\wedge^{T_{X}}\widehat{T}_{X}
\]\[(13)\qquad
\begin{cases}
\widehat{\mathrm{Hom}}_{\mathrm{ét}}(X,Y)\times\widehat{\mathrm{Hom}}_{\mathrm{ét}}(Y,Z)\longrightarrow\widehat{\mathrm{Hom}}_{\mathrm{ét}}(X,Z)\\
\qquad (u,v)\longmapsto v\circ u
\end{cases}\]
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\[
(13)\qquad
\begin{cases}
\widehat{\mathrm{Hom}}_{\mathrm{ét}}(X,Y)\times\widehat{\mathrm{Hom}}_{\mathrm{ét}}(Y,Z)\longrightarrow\widehat{\mathrm{Hom}}_{\mathrm{ét}}(X,Z)\\
\qquad (u,v)\longmapsto v\circ u
\end{cases}
\]\[(14)\qquad
\begin{cases}
\mathrm{Hom}(X,Y)\times\mathrm{Hom}(Y,Z)\longrightarrow\mathrm{Hom}(X,Z)\\
\qquad (u,v)\longmapsto vu
\end{cases}\]
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\[
(14)\qquad
\begin{cases}
\mathrm{Hom}(X,Y)\times\mathrm{Hom}(Y,Z)\longrightarrow\mathrm{Hom}(X,Z)\\
\qquad (u,v)\longmapsto vu
\end{cases}
\]\[(g,f,g',f')\longmapsto (g'vf'^{-1})\circ(guf^{-1}),\]
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\[
(g,f,g',f')\longmapsto (g'vf'^{-1})\circ(guf^{-1}),
\]\[\mathrm{Aut}(Y)\times\mathrm{Aut}(X)\times\mathrm{Aut}(Z)\times\mathrm{Aut}(Y)\longrightarrow\mathrm{Hom}(X,Z)\]
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\[
\mathrm{Aut}(Y)\times\mathrm{Aut}(X)\times\mathrm{Aut}(Z)\times\mathrm{Aut}(Y)\longrightarrow\mathrm{Hom}(X,Z)
\]\[(15)\qquad \mathrm{Aut}(Y)\longrightarrow\mathrm{Hom}(X,Z),\qquad \varphi\longmapsto v\varphi u\]
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\[
(15)\qquad \mathrm{Aut}(Y)\longrightarrow\mathrm{Hom}(X,Z),\qquad \varphi\longmapsto v\varphi u
\]\[G_{u}\subset\mathrm{Aut}(X)\times\mathrm{Aut}(Y),\qquad
G_{u}=\{\psi,\varphi \mid \varphi u\psi^{-1}=u \text{ i.e. } \varphi u=u\psi\},\]
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\[
G_{u}\subset\mathrm{Aut}(X)\times\mathrm{Aut}(Y),\qquad
G_{u}=\{\psi,\varphi \mid \varphi u\psi^{-1}=u \text{ i.e. } \varphi u=u\psi\},
\]\[G_{u}\xrightarrow{\ \mathrm{pr}_{2}\ }\mathrm{Aut}(Y)\longrightarrow\mathrm{Hom}(X,Z)\]
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\[
G_{u}\xrightarrow{\ \mathrm{pr}_{2}\ }\mathrm{Aut}(Y)\longrightarrow\mathrm{Hom}(X,Z)
\]\[v(\alpha_{i}\varphi)u=v\alpha_{i}u\psi .\]
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\[
v(\alpha_{i}\varphi)u=v\alpha_{i}u\psi .
\]\[(17)\qquad \mathrm{Hom}_{\widehat{C}_{0}}(X,Y)=\mathrm{Hom}_{C_{0}}(X,Y)\wedge^{\mathrm{Aut}(X)\times\mathrm{Aut}(Y)^{\circ}}\bigl(\widehat{\mathrm{Aut}}(X)\times\widehat{\mathrm{Aut}}(Y)\bigr)\]
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\[
(17)\qquad \mathrm{Hom}_{\widehat{C}_{0}}(X,Y)=\mathrm{Hom}_{C_{0}}(X,Y)\wedge^{\mathrm{Aut}(X)\times\mathrm{Aut}(Y)^{\circ}}\bigl(\widehat{\mathrm{Aut}}(X)\times\widehat{\mathrm{Aut}}(Y)\bigr)
\]\[\simeq\ \mathrm{Hom}_{C_{0}}(X,Y)\wedge^{\mathrm{Aut}(X)}\widehat{\mathrm{Aut}}(X)\]
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\[
\simeq\ \mathrm{Hom}_{C_{0}}(X,Y)\wedge^{\mathrm{Aut}(X)}\widehat{\mathrm{Aut}}(X)
\]\[(18)\qquad \hat{f}\colon X\longrightarrow Y\]
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\[
(18)\qquad \hat{f}\colon X\longrightarrow Y
\]\[(19)\qquad X\xrightarrow[\ \sim\ ]{\ \hat{f}_{0}\ }Y'\xrightarrow{\ u\ }Y\]
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\[
(19)\qquad X\xrightarrow[\ \sim\ ]{\ \hat{f}_{0}\ }Y'\xrightarrow{\ u\ }Y
\]\[\mathrm{Aut}_{Y}(Y')\longrightarrow\mathrm{Aut}(Y')\longrightarrow\mathrm{Aut}(Y')^{\wedge}\]
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\[
\mathrm{Aut}_{Y}(Y')\longrightarrow\mathrm{Aut}(Y')\longrightarrow\mathrm{Aut}(Y')^{\wedge}
\]\[(20)\qquad Y\xrightarrow[\ \sim\ ]{\ \hat{g}_{0}\ }Z'\xrightarrow{\ v\ }Z,\]
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\[
(20)\qquad Y\xrightarrow[\ \sim\ ]{\ \hat{g}_{0}\ }Z'\xrightarrow{\ v\ }Z,
\]\[\hat{g}_{0}=w\hat{\varphi},\qquad \hat{\varphi}\in\hat{H}_{u}\subset\widehat{\mathrm{Aut}}_{C_{0}}(Y)\]
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\[
\hat{g}_{0}=w\hat{\varphi},\qquad \hat{\varphi}\in\hat{H}_{u}\subset\widehat{\mathrm{Aut}}_{C_{0}}(Y)
\]\[(22)\qquad \hat{g}\hat{f}=(v\hat{g}_{0})(u\hat{f}_{0})=(vw\hat{\varphi})(u\hat{f}_{0})=\underbrace{(vwu)}_{\in\,\mathrm{Fl}\,C_{0}}\underbrace{(\hat{\varphi}'\hat{f}_{0})}_{\in\,\mathrm{Fl\,iso.}(\widehat{C}_{0})}\]
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\[
(22)\qquad \hat{g}\hat{f}=(v\hat{g}_{0})(u\hat{f}_{0})=(vw\hat{\varphi})(u\hat{f}_{0})=\underbrace{(vwu)}_{\in\,\mathrm{Fl}\,C_{0}}\underbrace{(\hat{\varphi}'\hat{f}_{0})}_{\in\,\mathrm{Fl\,iso.}(\widehat{C}_{0})}
\]\[(23)\qquad X=Y\setminus T\hookrightarrow Y\]
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\[ (23)\qquad X=Y\setminus T\hookrightarrow Y \]
\[(24)\qquad
\begin{array}{ccc}
X & \hookrightarrow & \hat{X}\\
\downarrow & & \downarrow\\
Y & \hookrightarrow & \hat{Y}
\end{array}\]
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\[
(24)\qquad
\begin{array}{ccc}
X & \hookrightarrow & \hat{X}\\
\downarrow & & \downarrow\\
Y & \hookrightarrow & \hat{Y}
\end{array}
\]\[(25)\qquad S\supset\hat{X}\,|\,T\]
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\[
(25)\qquad S\supset\hat{X}\,|\,T
\]\[(1)\quad
\begin{cases}
a_i^{\omega} : R_i^{\omega} \to R_i^{\omega'} \\
b_i^{\omega} : R^{\omega}_{\omega i} \to R^{\omega'}_{\omega' i}
\end{cases}\]
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\[
(1)\quad
\begin{cases}
a_i^{\omega} : R_i^{\omega} \to R_i^{\omega'} \\
b_i^{\omega} : R^{\omega}_{\omega i} \to R^{\omega'}_{\omega' i}
\end{cases}
\]\[(2)\quad
\begin{cases}
\text{a)}\ \ b_i^{\omega} b_i^{\omega'} = 1 \\
\text{b)}\ \ a_i^{\omega} b^{\omega}_{\omega' i} a_i^{\omega'} b^{\omega}_{\omega i} a^{\omega'}_{\omega i} b_i^{\omega} = 1
\end{cases}\]
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\[
(2)\quad
\begin{cases}
\text{a)}\ \ b_i^{\omega} b_i^{\omega'} = 1 \\
\text{b)}\ \ a_i^{\omega} b^{\omega}_{\omega' i} a_i^{\omega'} b^{\omega}_{\omega i} a^{\omega'}_{\omega i} b_i^{\omega} = 1
\end{cases}
\]\[(3)\quad a_i^{\omega'} a_i^{\omega} = \lambda_i^{\omega} = \varphi_i^{\omega}(l_0)\]
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\[
(3)\quad a_i^{\omega'} a_i^{\omega} = \lambda_i^{\omega} = \varphi_i^{\omega}(l_0)
\]\[(4)\quad \varphi_i^{\omega} : \Pi_{0,3} = \pi_1(M_{0,3}\,;R_0^{+}) \hookrightarrow \pi_1(\Sigma^{*}, R_i^{\omega})\]
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\[
(4)\quad \varphi_i^{\omega} : \Pi_{0,3} = \pi_1(M_{0,3}\,;R_0^{+}) \hookrightarrow \pi_1(\Sigma^{*}, R_i^{\omega})
\]\[\Pi_{0,3} = \{\, l_0, l_1, l_\infty \mid l_\infty l_1 l_0 = 1 \,\}
\subset \widetilde{\Pi}_{0,3} = \pi_1(M_{0,3}, \mathfrak{S}_3\,; R_0^{+}),\]
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\[
\Pi_{0,3} = \{\, l_0, l_1, l_\infty \mid l_\infty l_1 l_0 = 1 \,\}
\subset \widetilde{\Pi}_{0,3} = \pi_1(M_{0,3}, \mathfrak{S}_3\,; R_0^{+}),
\]\[l_0 \mapsto a_i^{\omega'} a_i^{\omega}, \qquad
l_1 \mapsto (b^{\omega}_{\omega' i})^{-1} a^{\omega}_{\omega i} a^{\omega'}_{\omega i} b_i^{\omega}\]
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\[
l_0 \mapsto a_i^{\omega'} a_i^{\omega}, \qquad
l_1 \mapsto (b^{\omega}_{\omega' i})^{-1} a^{\omega}_{\omega i} a^{\omega'}_{\omega i} b_i^{\omega}
\]\[(5)\quad \tau\varphi_i^{\omega}(g) = \varphi_i^{\omega}(\tau_\infty(g)) \quad \text{où } \tau_\infty \in \widetilde{\Pi}_{0,3},\]
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\[
(5)\quad \tau\varphi_i^{\omega}(g) = \varphi_i^{\omega}(\tau_\infty(g)) \quad \text{où } \tau_\infty \in \widetilde{\Pi}_{0,3},
\]\[\tau_\infty(l_0) = l_0^{-1}, \quad \tau_\infty(l_1) = l_1^{-1}, \quad
\tau_\infty(l_\infty) = l_0 l_1 = \mathrm{int}(l_0)\, l_\infty^{-1}\]
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\[
\tau_\infty(l_0) = l_0^{-1}, \quad \tau_\infty(l_1) = l_1^{-1}, \quad
\tau_\infty(l_\infty) = l_0 l_1 = \mathrm{int}(l_0)\, l_\infty^{-1}
\]\[(6)\quad
\begin{cases}
a_i^{\omega}(\varphi_i^{\omega}(g)) = \varphi_i^{\omega'}(\varepsilon_0(g)) \\
b_i^{\omega}(\varphi^{\omega}_{\omega i}(g)) = \varphi^{\omega'}_{\omega' i}(\sigma_\infty(g))
\end{cases}
\qquad \varepsilon_0^2 = l_0\]
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\[
(6)\quad
\begin{cases}
a_i^{\omega}(\varphi_i^{\omega}(g)) = \varphi_i^{\omega'}(\varepsilon_0(g)) \\
b_i^{\omega}(\varphi^{\omega}_{\omega i}(g)) = \varphi^{\omega'}_{\omega' i}(\sigma_\infty(g))
\end{cases}
\qquad \varepsilon_0^2 = l_0
\]\[\sigma_\infty(l_0) = l_1, \quad \sigma_\infty(l_1) = l_0, \quad
\sigma_\infty(l_\infty) = (l_0 l_1)^{-1} = l_1^{-1} l_0^{-1} = \mathrm{int}(l_0)\, l_\infty\]
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\[
\sigma_\infty(l_0) = l_1, \quad \sigma_\infty(l_1) = l_0, \quad
\sigma_\infty(l_\infty) = (l_0 l_1)^{-1} = l_1^{-1} l_0^{-1} = \mathrm{int}(l_0)\, l_\infty
\]\[(7)\quad \tilde b_i^{\omega} = a^{\omega'}_{\omega' i} b_i^{\omega} : R^{\omega}_{\omega i} \to R^{\omega}_{\omega' i} ;\]
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\[
(7)\quad \tilde b_i^{\omega} = a^{\omega'}_{\omega' i} b_i^{\omega} : R^{\omega}_{\omega i} \to R^{\omega}_{\omega' i} ;
\]\[(8)\quad \tilde b^{\omega}_{\omega^2 i}\, \tilde b^{\omega}_{\omega i}\, \tilde b_i^{\omega} = 1\]
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\[
(8)\quad \tilde b^{\omega}_{\omega^2 i}\, \tilde b^{\omega}_{\omega i}\, \tilde b_i^{\omega} = 1
\]\[(9)\quad \tilde b_i^{\omega}(\varphi^{\omega}_{\omega i}(g)) = \varphi^{\omega}_{\omega' i}(\rho^{-1}(g))
\qquad \rho^{-1} = \varepsilon_0 \sigma_\infty,
\quad
\begin{cases}
\rho(l_0) = l_1 \\
\rho(l_1) = l_\infty \\
\rho(l_\infty) = l_0
\end{cases}\]
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\[
(9)\quad \tilde b_i^{\omega}(\varphi^{\omega}_{\omega i}(g)) = \varphi^{\omega}_{\omega' i}(\rho^{-1}(g))
\qquad \rho^{-1} = \varepsilon_0 \sigma_\infty,
\quad
\begin{cases}
\rho(l_0) = l_1 \\
\rho(l_1) = l_\infty \\
\rho(l_\infty) = l_0
\end{cases}
\]\[(\text{\struck{\ill{}}})\quad \tilde b_{\omega^2 i}\, \tilde b_{\omega i}\, \tilde b_i = 1\]
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\[
(\text{\struck{\ill{}}})\quad \tilde b_{\omega^2 i}\, \tilde b_{\omega i}\, \tilde b_i = 1
\]\[u(a_i^{\omega}) = a_i^{\omega} \varphi_i^{\omega}(l_0^{\gamma}) = \varphi_i^{\omega'}(l_0^{\gamma})\, a_i^{\omega}
\qquad \text{($\varphi_i^{\omega}(l_0^{\gamma}) = (\lambda_i^{\omega})^{\gamma}$)}\]
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\[
u(a_i^{\omega}) = a_i^{\omega} \varphi_i^{\omega}(l_0^{\gamma}) = \varphi_i^{\omega'}(l_0^{\gamma})\, a_i^{\omega}
\qquad \text{($\varphi_i^{\omega}(l_0^{\gamma}) = (\lambda_i^{\omega})^{\gamma}$)}
\]\[u(a_i^{\omega'} a_i^{\omega}) = \varphi_i^{\omega}(l_0^{2\gamma+1}), \qquad
u(\underbrace{\varphi_i^{\omega}(l_0)}_{\lambda_i^{\omega}}) = \varphi_i^{\omega}(l_0^{p}) = (\lambda_i^{\omega})^{p},
\qquad \gamma = \frac{p-1}{2}\]
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\[
u(a_i^{\omega'} a_i^{\omega}) = \varphi_i^{\omega}(l_0^{2\gamma+1}), \qquad
u(\underbrace{\varphi_i^{\omega}(l_0)}_{\lambda_i^{\omega}}) = \varphi_i^{\omega}(l_0^{p}) = (\lambda_i^{\omega})^{p},
\qquad \gamma = \frac{p-1}{2}
\]\[\begin{cases}
u(a_i^{\omega}) = a_i^{\omega} \varphi_i^{\omega}(l_0^{\gamma}) \\
u(b_i^{\omega}) = b_i^{\omega} \varphi^{\omega}_{\omega i}(\beta)
\quad (= \varphi^{\omega'}_{\omega' i}(\sigma_\infty \beta)\, b_i^{\omega})
\end{cases}
\qquad \gamma = \frac{p-1}{2}, \quad p \in \hat{\mathbb{Z}}^{*} \text{ multiplicateur}, \quad \beta \in \widehat{\Pi}_{0,3}\]
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\[
\begin{cases}
u(a_i^{\omega}) = a_i^{\omega} \varphi_i^{\omega}(l_0^{\gamma}) \\
u(b_i^{\omega}) = b_i^{\omega} \varphi^{\omega}_{\omega i}(\beta)
\quad (= \varphi^{\omega'}_{\omega' i}(\sigma_\infty \beta)\, b_i^{\omega})
\end{cases}
\qquad \gamma = \frac{p-1}{2}, \quad p \in \hat{\mathbb{Z}}^{*} \text{ multiplicateur}, \quad \beta \in \widehat{\Pi}_{0,3}
\]\[u(\tilde b_i^{\omega}) = \tilde b_i^{\omega} \varphi^{\omega}_{\omega i}(\underbrace{l_1^{\gamma} \beta}_{\sigma_\infty(\lambda) \beta})
= \varphi^{\omega'}_{\omega' i}(l_0^{\gamma} \rho^{-1}(\beta))\, \tilde b_i^{\omega}\]
LaTeX source
\[
u(\tilde b_i^{\omega}) = \tilde b_i^{\omega} \varphi^{\omega}_{\omega i}(\underbrace{l_1^{\gamma} \beta}_{\sigma_\infty(\lambda) \beta})
= \varphi^{\omega'}_{\omega' i}(l_0^{\gamma} \rho^{-1}(\beta))\, \tilde b_i^{\omega}
\]\[(12)\quad
\begin{cases}
\beta\, \sigma_\infty(\beta) = 1 \\
\alpha\, \rho^{-1}(\alpha)\, \rho^{-2}(\alpha) = 1
\quad \text{où } \text{\struck{$\alpha = l_1^{-\gamma} \beta$}} \\
\alpha = \underbrace{l_1^{\gamma}}_{\sigma_\infty(\lambda)} \beta
\end{cases}\]
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\[
(12)\quad
\begin{cases}
\beta\, \sigma_\infty(\beta) = 1 \\
\alpha\, \rho^{-1}(\alpha)\, \rho^{-2}(\alpha) = 1
\quad \text{où } \text{\struck{$\alpha = l_1^{-\gamma} \beta$}} \\
\alpha = \underbrace{l_1^{\gamma}}_{\sigma_\infty(\lambda)} \beta
\end{cases}
\]\[Q_i \xrightarrow{\;c_i^{\omega}\;} R^{\omega'}_{\omega' i}\]
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\[
Q_i \xrightarrow{\;c_i^{\omega}\;} R^{\omega'}_{\omega' i}
\]\[(13)\quad b_i^{\omega} = c_i^{\omega} (c_i^{\omega'})^{-1}\]
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\[
(13)\quad b_i^{\omega} = c_i^{\omega} (c_i^{\omega'})^{-1}
\]\[(14)\quad \tilde a_i^{\omega} = (c^{\omega}_{\omega i})^{-1} a_i^{\omega} c^{\omega'}_{\omega' i} : Q_{\omega i} \to Q_{\omega' i}\]
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\[
(14)\quad \tilde a_i^{\omega} = (c^{\omega}_{\omega i})^{-1} a_i^{\omega} c^{\omega'}_{\omega' i} : Q_{\omega i} \to Q_{\omega' i}
\]\[(15)\quad \tau(\tilde a_i^{\omega}) = (\tilde a_i^{\omega'})^{-1}\]
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\[
(15)\quad \tau(\tilde a_i^{\omega}) = (\tilde a_i^{\omega'})^{-1}
\]\[(16)\quad \tilde a^{\omega}_{\omega^2 i}\, \tilde a^{\omega}_{\omega i}\, \tilde a_i^{\omega} = 1\]
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\[
(16)\quad \tilde a^{\omega}_{\omega^2 i}\, \tilde a^{\omega}_{\omega i}\, \tilde a_i^{\omega} = 1
\]\[(17)\quad \psi_i^{\omega} : \Pi_{0,3} \xrightarrow{\ \sim\ } \pi(Q_i)\]
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\[
(17)\quad \psi_i^{\omega} : \Pi_{0,3} \xrightarrow{\ \sim\ } \pi(Q_i)
\]\[(18)\quad \psi_i^{\omega}(g) = \psi_i^{\omega'}(\sigma_\infty(g))\]
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\[
(18)\quad \psi_i^{\omega}(g) = \psi_i^{\omega'}(\sigma_\infty(g))
\]\[(19)\quad
\begin{aligned}
\tilde a_i^{\omega}(\psi^{\omega'}_{\omega i}(g)) &= \psi^{\omega}_{\omega' i}(\varepsilon_0(g)) = \psi^{\omega'}_{\omega' i}(\sigma_\infty \varepsilon_0(g)) \\
\tilde a_i^{\omega}(\psi^{\omega}_{\omega i}(g)) &= \psi^{\omega}_{\omega' i}(\underbrace{(\varepsilon_0 \sigma_\infty)}_{\rho^{-1}}(g)) = \psi^{\omega'}_{\omega' i}(\sigma_\infty \varepsilon_0 \sigma_\infty(g))
\end{aligned}\]
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\[
(19)\quad
\begin{aligned}
\tilde a_i^{\omega}(\psi^{\omega'}_{\omega i}(g)) &= \psi^{\omega}_{\omega' i}(\varepsilon_0(g)) = \psi^{\omega'}_{\omega' i}(\sigma_\infty \varepsilon_0(g)) \\
\tilde a_i^{\omega}(\psi^{\omega}_{\omega i}(g)) &= \psi^{\omega}_{\omega' i}(\underbrace{(\varepsilon_0 \sigma_\infty)}_{\rho^{-1}}(g)) = \psi^{\omega'}_{\omega' i}(\sigma_\infty \varepsilon_0 \sigma_\infty(g))
\end{aligned}
\]\[(20)\quad u(a_i^{\omega}) = a_i^{\omega} \varphi_i^{\omega}(l_0^{\gamma})
\qquad \gamma = \frac{p-1}{2} \in \hat{\mathbb{Z}}, \quad p \in \hat{\mathbb{Z}}^{*}\]
LaTeX source
\[
(20)\quad u(a_i^{\omega}) = a_i^{\omega} \varphi_i^{\omega}(l_0^{\gamma})
\qquad \gamma = \frac{p-1}{2} \in \hat{\mathbb{Z}}, \quad p \in \hat{\mathbb{Z}}^{*}
\]\[(21)\quad u(c_i^{\omega}) = \varphi^{\omega'}_{\omega' i}(\eta)\, c_i^{\omega} = c_i^{\omega} \psi_i^{\omega}(\eta)
\qquad \eta \in \widehat{\Pi}_{0,3} \text{ indépendant de } i, \omega\]
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\[
(21)\quad u(c_i^{\omega}) = \varphi^{\omega'}_{\omega' i}(\eta)\, c_i^{\omega} = c_i^{\omega} \psi_i^{\omega}(\eta)
\qquad \eta \in \widehat{\Pi}_{0,3} \text{ indépendant de } i, \omega
\]\[(22)\quad u(b_i^{\omega}) = b_i^{\omega} \varphi^{\omega}_{\omega i}(\beta)\]
LaTeX source
\[
(22)\quad u(b_i^{\omega}) = b_i^{\omega} \varphi^{\omega}_{\omega i}(\beta)
\]\[(23)\quad \beta = \sigma_\infty(\eta)\, \eta^{-1}\]
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\[
(23)\quad \beta = \sigma_\infty(\eta)\, \eta^{-1}
\]\[(24)\quad \text{\struck{$l_1^{-\gamma}\sigma_\infty(\eta)\eta^{-1}$}}\ \ \alpha \rho^{-1}(\alpha) \rho^{-2}(\alpha) = 1
\quad \text{avec } \alpha = \underbrace{l_1^{\gamma}}_{\sigma_\infty(\lambda)} \underbrace{\sigma_\infty(\eta)\eta^{-1}}_{\beta}.\]
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\[
(24)\quad \text{\struck{$l_1^{-\gamma}\sigma_\infty(\eta)\eta^{-1}$}}\ \ \alpha \rho^{-1}(\alpha) \rho^{-2}(\alpha) = 1
\quad \text{avec } \alpha = \underbrace{l_1^{\gamma}}_{\sigma_\infty(\lambda)} \underbrace{\sigma_\infty(\eta)\eta^{-1}}_{\beta}.
\]\[(25)\quad u(\tilde a_i^{\omega}) = \psi^{\omega^*}_{\omega i}(\underbrace{\eta^{-1} l_0^{\gamma} \varepsilon_0(\eta)}_{\tilde\alpha = \eta^{-1}\varepsilon_0(\lambda\eta)})\, \tilde a_i^{\omega}
= \tilde a_i^{\omega}\, \psi^{\omega'}_{\omega' i}(\underbrace{\varepsilon_0^{-1}(\eta^{-1}) l_0^{\gamma} \eta}_{\varepsilon_0^{-1}(\tilde\alpha)})\]
LaTeX source
\[
(25)\quad u(\tilde a_i^{\omega}) = \psi^{\omega^*}_{\omega i}(\underbrace{\eta^{-1} l_0^{\gamma} \varepsilon_0(\eta)}_{\tilde\alpha = \eta^{-1}\varepsilon_0(\lambda\eta)})\, \tilde a_i^{\omega}
= \tilde a_i^{\omega}\, \psi^{\omega'}_{\omega' i}(\underbrace{\varepsilon_0^{-1}(\eta^{-1}) l_0^{\gamma} \eta}_{\varepsilon_0^{-1}(\tilde\alpha)})
\]\[(\text{25\,bis})\quad \alpha = \rho(\eta \tilde\alpha \rho^{-1}(\eta)^{-1})\]
LaTeX source
\[
(\text{25\,bis})\quad \alpha = \rho(\eta \tilde\alpha \rho^{-1}(\eta)^{-1})
\]\[(26)\quad \tilde\alpha\, \rho^{-1}(\tilde\alpha)\, \rho^{-2}(\tilde\alpha) = 1, \qquad
\boxed{(27)\quad \tilde\alpha = \eta^{-1} l_0^{\gamma} \varepsilon_0(\eta)}\]
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\[
(26)\quad \tilde\alpha\, \rho^{-1}(\tilde\alpha)\, \rho^{-2}(\tilde\alpha) = 1, \qquad
\boxed{(27)\quad \tilde\alpha = \eta^{-1} l_0^{\gamma} \varepsilon_0(\eta)}
\]\[(27)\quad \tau Q_i = Q_i, \qquad \tau \tilde a_i^{\omega} = (\tilde a_i^{\omega'})^{-1}\]
LaTeX source
\[
(27)\quad \tau Q_i = Q_i, \qquad \tau \tilde a_i^{\omega} = (\tilde a_i^{\omega'})^{-1}
\]\[(28)\quad \tilde\lambda_i^{\omega} = \tilde a_i^{\omega'} \tilde a_i^{\omega} \in \pi(Q_{\omega' i})
\qquad (\lambda_i^{\omega} = a_i^{\omega'} a_i^{\omega})\]
LaTeX source
\[
(28)\quad \tilde\lambda_i^{\omega} = \tilde a_i^{\omega'} \tilde a_i^{\omega} \in \pi(Q_{\omega' i})
\qquad (\lambda_i^{\omega} = a_i^{\omega'} a_i^{\omega})
\]\[(29)\quad u(\tilde\lambda_i^{\omega}) = \psi^{\omega'}_{\omega' i}(\tilde\alpha\, \varepsilon_0(\tilde\alpha))\, \tilde\lambda_i^{\omega}
= \psi^{\omega'}_{\omega' i}(\tilde\alpha\, \varepsilon_0(\tilde\alpha)\, l_0)\]
LaTeX source
\[
(29)\quad u(\tilde\lambda_i^{\omega}) = \psi^{\omega'}_{\omega' i}(\tilde\alpha\, \varepsilon_0(\tilde\alpha))\, \tilde\lambda_i^{\omega}
= \psi^{\omega'}_{\omega' i}(\tilde\alpha\, \varepsilon_0(\tilde\alpha)\, l_0)
\]\[(30)\quad \tilde\alpha\, \varepsilon_0(\tilde\alpha)\, l_0 = \eta^{-1} l_0^{p} \eta \qquad (p = 2\gamma+1) ;\]
LaTeX source
\[
(30)\quad \tilde\alpha\, \varepsilon_0(\tilde\alpha)\, l_0 = \eta^{-1} l_0^{p} \eta \qquad (p = 2\gamma+1) ;
\]\[(31)\quad \tilde\alpha' = \varepsilon_0 \tau_\infty(\tilde\alpha^{-1}) = \underbrace{\rho^{-1} \tilde\sigma_\infty}_{\tilde\sigma_0}(\tilde\alpha^{-1})\]
LaTeX source
\[
(31)\quad \tilde\alpha' = \varepsilon_0 \tau_\infty(\tilde\alpha^{-1}) = \underbrace{\rho^{-1} \tilde\sigma_\infty}_{\tilde\sigma_0}(\tilde\alpha^{-1})
\]\[\tilde\sigma_i(l_i) = l_i^{-1}, \qquad
\tilde\sigma_i(l_j) = l_k^{-1} \quad \text{si } \{0, 1, \infty\} = \{i, j, k\}\]
LaTeX source
\[
\tilde\sigma_i(l_i) = l_i^{-1}, \qquad
\tilde\sigma_i(l_j) = l_k^{-1} \quad \text{si } \{0, 1, \infty\} = \{i, j, k\}
\]\[x\, \rho^{-1}(x)\, \rho^{-2}(x) = 1\]
LaTeX source
\[
x\, \rho^{-1}(x)\, \rho^{-2}(x) = 1
\]\[(32)\quad \Theta_g x = g \cdot x^{\chi(g)}\]
LaTeX source
\[
(32)\quad \Theta_g x = g \cdot x^{\chi(g)}
\]\[(33)\quad \tilde\alpha' = \Theta_{\tilde\sigma_0}(\tilde\alpha).\]
LaTeX source
\[
(33)\quad \tilde\alpha' = \Theta_{\tilde\sigma_0}(\tilde\alpha).
\]\[d_i^{\omega} : P^{\omega} \to Q_i\]
LaTeX source
\[
d_i^{\omega} : P^{\omega} \to Q_i
\]\[(34)\quad \tau(P^{\omega}) = P^{\omega'}, \qquad \tau(d_i^{\omega}) = d_i^{\omega'}\]
LaTeX source
\[
(34)\quad \tau(P^{\omega}) = P^{\omega'}, \qquad \tau(d_i^{\omega}) = d_i^{\omega'}
\]\[(35)\quad (d^{\omega}_{\omega' i})^{-1} \tilde a_i^{\omega} d_i^{\omega} = 1\]
LaTeX source
\[
(35)\quad (d^{\omega}_{\omega' i})^{-1} \tilde a_i^{\omega} d_i^{\omega} = 1
\]\[(36)\quad
\begin{cases}
u(\tilde a_i^{\omega}) = \psi^{\omega}_{\omega i}(\tilde\alpha)\, \tilde a_i^{\omega} & \tilde\alpha \in \widehat{\Pi}_{0,3} \ \text{(indép. de } i, \omega) \\
u(d_i^{\omega}) = \psi_i^{\omega}(\zeta)\, d_i^{\omega} \quad (= d_i^{\omega} \tilde\varphi_i^{\omega}(\zeta)) & \zeta \in \widehat{\Pi}_{0,3}\ \ldots
\end{cases}\]
LaTeX source
\[
(36)\quad
\begin{cases}
u(\tilde a_i^{\omega}) = \psi^{\omega}_{\omega i}(\tilde\alpha)\, \tilde a_i^{\omega} & \tilde\alpha \in \widehat{\Pi}_{0,3} \ \text{(indép. de } i, \omega) \\
u(d_i^{\omega}) = \psi_i^{\omega}(\zeta)\, d_i^{\omega} \quad (= d_i^{\omega} \tilde\varphi_i^{\omega}(\zeta)) & \zeta \in \widehat{\Pi}_{0,3}\ \ldots
\end{cases}
\]\[(37)\quad \tilde\alpha = \zeta \cdot \rho^{-1}(\zeta^{-1})\]
LaTeX source
\[
(37)\quad \tilde\alpha = \zeta \cdot \rho^{-1}(\zeta^{-1})
\]\[(39)\quad \tilde\psi^{\omega}_{\omega i}(g) = \tilde\psi_i^{\omega}(\rho g) \quad \text{i.e.} \quad \tilde\psi_{\omega i} = \tilde\psi_i \circ \rho,\]
LaTeX source
\[
(39)\quad \tilde\psi^{\omega}_{\omega i}(g) = \tilde\psi_i^{\omega}(\rho g) \quad \text{i.e.} \quad \tilde\psi_{\omega i} = \tilde\psi_i \circ \rho,
\]\[(40)\quad \tilde d_i^{\omega} : P^{\omega} \to P^{\omega'}, \qquad \tilde d_i^{\omega} = (d_i^{\omega'})^{-1} d_i^{\omega},\]
LaTeX source
\[
(40)\quad \tilde d_i^{\omega} : P^{\omega} \to P^{\omega'}, \qquad \tilde d_i^{\omega} = (d_i^{\omega'})^{-1} d_i^{\omega},
\]\[(41)\quad \tau(\tilde d_i^{\omega}) = \tilde d_i^{\omega'}, \qquad \tilde d_i^{\omega} \tilde d_i^{\omega'} = 1\]
LaTeX source
\[
(41)\quad \tau(\tilde d_i^{\omega}) = \tilde d_i^{\omega'}, \qquad \tilde d_i^{\omega} \tilde d_i^{\omega'} = 1
\]\[(42)\quad \tilde d_i^{\omega}(\tilde\psi_i^{\omega}(g)) = \tilde\psi_i^{\omega'}(\sigma_\infty g).\]
LaTeX source
\[
(42)\quad \tilde d_i^{\omega}(\tilde\psi_i^{\omega}(g)) = \tilde\psi_i^{\omega'}(\sigma_\infty g).
\]\[(43)\quad u(\tilde d_i^{\omega}) = \tilde\psi_i^{\omega'}(\sigma_\infty \tilde\beta)\, \tilde d_i^{\omega} = \tilde d_i^{\omega}\, \tilde\psi_i^{\omega}(\tilde\beta)\]
LaTeX source
\[
(43)\quad u(\tilde d_i^{\omega}) = \tilde\psi_i^{\omega'}(\sigma_\infty \tilde\beta)\, \tilde d_i^{\omega} = \tilde d_i^{\omega}\, \tilde\psi_i^{\omega}(\tilde\beta)
\]\[(44)\quad \tilde\beta = \zeta\, \sigma_\infty(\zeta)^{-1}.\]
LaTeX source
\[
(44)\quad \tilde\beta = \zeta\, \sigma_\infty(\zeta)^{-1}.
\]\[(45)\quad \tilde\beta\, \sigma_\infty(\tilde\beta) = 1\]
LaTeX source
\[ (45)\quad \tilde\beta\, \sigma_\infty(\tilde\beta) = 1 \]
\[(46)\quad u(\tilde d_i^{\omega}) = \tilde d_i^{\omega} \tilde\psi_i^{\omega}(\tilde\beta)
\qquad \text{avec } \tilde\beta \in \widehat{\Pi}_{0,3} \text{ indépendant de } i, \omega\]
LaTeX source
\[
(46)\quad u(\tilde d_i^{\omega}) = \tilde d_i^{\omega} \tilde\psi_i^{\omega}(\tilde\beta)
\qquad \text{avec } \tilde\beta \in \widehat{\Pi}_{0,3} \text{ indépendant de } i, \omega
\]\[(47)\quad \tilde\beta\, \sigma_\infty(\tilde\beta) = 1\]
LaTeX source
\[ (47)\quad \tilde\beta\, \sigma_\infty(\tilde\beta) = 1 \]
\[(48)\quad (d^{\omega}_{\omega i})^{-1} (c^{\omega'}_{\omega i})^{-1} (a^{\omega}_{\omega i})^{-1} c_i^{\omega} d_i^{\omega} = 1\]
LaTeX source
\[
(48)\quad (d^{\omega}_{\omega i})^{-1} (c^{\omega'}_{\omega i})^{-1} (a^{\omega}_{\omega i})^{-1} c_i^{\omega} d_i^{\omega} = 1
\]\[(49)\quad
\begin{cases}
\tau(R_i^{\omega}) = R_i^{\omega'}, \quad \tau Q_i = Q_i, \quad \tau(P^{\omega}) = P^{\omega'} \\
\tau(a_i^{\omega}) = (a_i^{\omega'})^{-1}, \quad \tau(c_i^{\omega}) = c_i^{\omega'}, \quad \tau(d_i^{\omega}) = d_i^{\omega'}
\end{cases}\]
LaTeX source
\[
(49)\quad
\begin{cases}
\tau(R_i^{\omega}) = R_i^{\omega'}, \quad \tau Q_i = Q_i, \quad \tau(P^{\omega}) = P^{\omega'} \\
\tau(a_i^{\omega}) = (a_i^{\omega'})^{-1}, \quad \tau(c_i^{\omega}) = c_i^{\omega'}, \quad \tau(d_i^{\omega}) = d_i^{\omega'}
\end{cases}
\]\[(50)\quad
\begin{cases}
\Pi_{0,3} \xrightarrow{\ \varphi_i^{\omega}\ } \pi(R_i^{\omega}) \quad \text{\struck{$\to \pi($}} \\
\Pi_{0,3} \xrightarrow{\ \psi_i^{\omega}\ } \pi(Q_i) \\
\Pi_{0,3} \xrightarrow{\ \tilde\psi_i^{\omega}\ } \pi(P^{\omega})
\end{cases}\]
LaTeX source
\[
(50)\quad
\begin{cases}
\Pi_{0,3} \xrightarrow{\ \varphi_i^{\omega}\ } \pi(R_i^{\omega}) \quad \text{\struck{$\to \pi($}} \\
\Pi_{0,3} \xrightarrow{\ \psi_i^{\omega}\ } \pi(Q_i) \\
\Pi_{0,3} \xrightarrow{\ \tilde\psi_i^{\omega}\ } \pi(P^{\omega})
\end{cases}
\]\[(51)\quad
\begin{cases}
d_i^{\omega}(\tilde\psi_i^{\omega}(g)) = \psi_i^{\omega}(g) \\
c_i^{\omega} \psi_i^{\omega}(g) = \varphi_i^{\omega}(g)
\end{cases}\]
LaTeX source
\[
(51)\quad
\begin{cases}
d_i^{\omega}(\tilde\psi_i^{\omega}(g)) = \psi_i^{\omega}(g) \\
c_i^{\omega} \psi_i^{\omega}(g) = \varphi_i^{\omega}(g)
\end{cases}
\]\[(52)\quad \psi_i^{\omega}(g) = \psi_i^{\omega'}(\sigma_\infty(g))\]
LaTeX source
\[
(52)\quad \psi_i^{\omega}(g) = \psi_i^{\omega'}(\sigma_\infty(g))
\]\[(53)\quad a_i^{\omega} \varphi_i^{\omega}(g) = \varphi_i^{\omega'}(\varepsilon_0(g))\]
LaTeX source
\[
(53)\quad a_i^{\omega} \varphi_i^{\omega}(g) = \varphi_i^{\omega'}(\varepsilon_0(g))
\]\[(54)\quad
\begin{cases}
u(a_i^{\omega}) = a_i^{\omega} \varphi_i^{\omega}(\lambda) \\
u(c_i^{\omega}) = \varphi^{\omega'}_{\omega' i}(\eta)\, c_i^{\omega} = c_i^{\omega} \psi_i^{\omega}(\eta) \\
u(d_i^{\omega}) = \psi_i^{\omega}(\zeta)\, d_i^{\omega} = d_i^{\omega} \tilde\psi_i^{\omega}(\zeta)
\end{cases}\]
LaTeX source
\[
(54)\quad
\begin{cases}
u(a_i^{\omega}) = a_i^{\omega} \varphi_i^{\omega}(\lambda) \\
u(c_i^{\omega}) = \varphi^{\omega'}_{\omega' i}(\eta)\, c_i^{\omega} = c_i^{\omega} \psi_i^{\omega}(\eta) \\
u(d_i^{\omega}) = \psi_i^{\omega}(\zeta)\, d_i^{\omega} = d_i^{\omega} \tilde\psi_i^{\omega}(\zeta)
\end{cases}
\]\[(55)\quad \tilde\alpha = \eta^{-1} \varepsilon_0(\lambda\eta) \quad \text{et} \quad \tilde\alpha = \zeta \rho^{-1}(\zeta^{-1})\]
LaTeX source
\[
(55)\quad \tilde\alpha = \eta^{-1} \varepsilon_0(\lambda\eta) \quad \text{et} \quad \tilde\alpha = \zeta \rho^{-1}(\zeta^{-1})
\]\[(56)\quad \eta^{-1} \varepsilon_0(\lambda\eta) = \zeta \rho^{-1}(\zeta)^{-1}\]
LaTeX source
\[
(56)\quad \eta^{-1} \varepsilon_0(\lambda\eta) = \zeta \rho^{-1}(\zeta)^{-1}
\]\[(57)\quad
\begin{cases}
\beta = \sigma_\infty(\eta)\eta^{-1} & (u(b_i^{\omega}) = b_i^{\omega} \varphi^{\omega}_{\omega i}(\beta)) \\
\alpha = \sigma_\infty(\lambda)\beta & (u(\tilde b_i^{\omega}) = \tilde b_i^{\omega} \varphi^{\omega}_{\omega i}(\alpha)) \\
\tilde\alpha = \eta^{-1}\varepsilon_0(\lambda\eta) = \zeta\rho^{-1}(\zeta)^{-1} & (u(\tilde a_i^{\omega}) = \psi^{\omega}_{\omega i}(\tilde\alpha)\, \tilde a_i^{\omega})
\end{cases}\]
LaTeX source
\[
(57)\quad
\begin{cases}
\beta = \sigma_\infty(\eta)\eta^{-1} & (u(b_i^{\omega}) = b_i^{\omega} \varphi^{\omega}_{\omega i}(\beta)) \\
\alpha = \sigma_\infty(\lambda)\beta & (u(\tilde b_i^{\omega}) = \tilde b_i^{\omega} \varphi^{\omega}_{\omega i}(\alpha)) \\
\tilde\alpha = \eta^{-1}\varepsilon_0(\lambda\eta) = \zeta\rho^{-1}(\zeta)^{-1} & (u(\tilde a_i^{\omega}) = \psi^{\omega}_{\omega i}(\tilde\alpha)\, \tilde a_i^{\omega})
\end{cases}
\]\[(58)\quad
\begin{cases}
\beta' = \beta^{-1} \ (= \sigma_\infty(\beta)) = \eta\, \sigma_\infty(\eta)^{-1} \\
\alpha' = \alpha^{-1} = \beta^{-1} \sigma_\infty(\lambda)^{-1} = \beta' \sigma_\infty(\lambda^{-1})
\end{cases}
\qquad \text{donc } \beta' = \alpha' \sigma_\infty(\lambda)\]
LaTeX source
\[
(58)\quad
\begin{cases}
\beta' = \beta^{-1} \ (= \sigma_\infty(\beta)) = \eta\, \sigma_\infty(\eta)^{-1} \\
\alpha' = \alpha^{-1} = \beta^{-1} \sigma_\infty(\lambda)^{-1} = \beta' \sigma_\infty(\lambda^{-1})
\end{cases}
\qquad \text{donc } \beta' = \alpha' \sigma_\infty(\lambda)
\]\[(59)\quad
\begin{aligned}
\beta' &= \eta\, \sigma_\infty(\eta)^{-1} \quad \text{\struck{\ill{}}} \\
\alpha' &= \text{\struck{\ill{}}}\ \beta' \sigma_\infty(\lambda^{-1}) \quad \text{i.e.} \quad \beta' = \alpha' \sigma_\infty(\lambda)
\end{aligned}\]
LaTeX source
\[
(59)\quad
\begin{aligned}
\beta' &= \eta\, \sigma_\infty(\eta)^{-1} \quad \text{\struck{\ill{}}} \\
\alpha' &= \text{\struck{\ill{}}}\ \beta' \sigma_\infty(\lambda^{-1}) \quad \text{i.e.} \quad \beta' = \alpha' \sigma_\infty(\lambda)
\end{aligned}
\]\[(60)\quad
\begin{cases}
\alpha' = \zeta' \rho^{-1}(\zeta')^{-1} \\
\text{i.e.}\quad \eta\, \sigma_\infty(\eta)^{-1} = (\zeta' \rho^{-1}(\zeta')^{-1})\, \sigma_\infty(\lambda)
\end{cases}\]
LaTeX source
\[
(60)\quad
\begin{cases}
\alpha' = \zeta' \rho^{-1}(\zeta')^{-1} \\
\text{i.e.}\quad \eta\, \sigma_\infty(\eta)^{-1} = (\zeta' \rho^{-1}(\zeta')^{-1})\, \sigma_\infty(\lambda)
\end{cases}
\]\[\alpha = \rho(\eta \tilde\alpha \rho^{-1}(\eta)^{-1})\]
LaTeX source
\[
\alpha = \rho(\eta \tilde\alpha \rho^{-1}(\eta)^{-1})
\]\[\tilde\alpha' = \tilde\alpha^{-1}\]
LaTeX source
\[
\tilde\alpha' = \tilde\alpha^{-1}
\]\[(61)\quad \alpha' = \rho(\rho^{-1}(\eta)\, \tilde\alpha'\, \eta^{-1}) = \eta\, \rho(\tilde\alpha')\, \rho(\eta)^{-1}\]
LaTeX source
\[
(61)\quad \alpha' = \rho(\rho^{-1}(\eta)\, \tilde\alpha'\, \eta^{-1}) = \eta\, \rho(\tilde\alpha')\, \rho(\eta)^{-1}
\]\[\tilde\alpha' = \rho^{-1}(\zeta)\, \zeta^{-1}\]
LaTeX source
\[
\tilde\alpha' = \rho^{-1}(\zeta)\, \zeta^{-1}
\]\[\rho(\tilde\alpha') = \zeta\, \rho(\zeta)^{-1}\]
LaTeX source
\[
\rho(\tilde\alpha') = \zeta\, \rho(\zeta)^{-1}
\]\[\alpha' = \eta\zeta\, \rho(\zeta^{-1}\eta^{-1}) \qquad \text{\struck{i.e.\ $\alpha'$ \ill{} (60)}}\]
LaTeX source
\[
\alpha' = \eta\zeta\, \rho(\zeta^{-1}\eta^{-1}) \qquad \text{\struck{i.e.\ $\alpha'$ \ill{} (60)}}
\]\[\zeta' = \eta\zeta.\]
LaTeX source
\[ \zeta' = \eta\zeta. \]
\[(62)\quad \{(\lambda, \eta, \zeta') \in \widehat{\Pi}_{0,3} \times \widehat{\Pi}_{0,3} \times \widehat{\Pi}_{0,3}\}\]
LaTeX source
\[
(62)\quad \{(\lambda, \eta, \zeta') \in \widehat{\Pi}_{0,3} \times \widehat{\Pi}_{0,3} \times \widehat{\Pi}_{0,3}\}
\]\[(63)\quad
\boxed{
\begin{aligned}
&\beta' = \alpha' \sigma_\infty(\lambda) \qquad (= \alpha' l_1^{\gamma} \ \text{si}\ \lambda = l_0^{\gamma}) \\
&\text{avec}\quad \alpha' = \zeta' \rho^{-1}(\zeta')^{-1} \\
&\phantom{\text{avec}\quad} \beta' = \eta\, \sigma_\infty(\eta)^{-1}
\end{aligned}
}\]
LaTeX source
\[
(63)\quad
\boxed{
\begin{aligned}
&\beta' = \alpha' \sigma_\infty(\lambda) \qquad (= \alpha' l_1^{\gamma} \ \text{si}\ \lambda = l_0^{\gamma}) \\
&\text{avec}\quad \alpha' = \zeta' \rho^{-1}(\zeta')^{-1} \\
&\phantom{\text{avec}\quad} \beta' = \eta\, \sigma_\infty(\eta)^{-1}
\end{aligned}
}
\]\[(64)\quad b_i'^{\omega} = (b_i^{\omega})^{-1} \ (= b_i^{\omega'}), \qquad \tilde b_i'^{\omega} = (\tilde b_i^{\omega})^{-1}, \qquad \tilde a_i'^{\omega} = (\tilde a_i^{\omega})^{-1}\]
LaTeX source
\[
(64)\quad b_i'^{\omega} = (b_i^{\omega})^{-1} \ (= b_i^{\omega'}), \qquad \tilde b_i'^{\omega} = (\tilde b_i^{\omega})^{-1}, \qquad \tilde a_i'^{\omega} = (\tilde a_i^{\omega})^{-1}
\]\[(65)\quad
\begin{cases}
u(b_i'^{\omega}) = \varphi^{\omega}_{\omega i}(\beta')\, b_i'^{\omega} \\
u(\tilde b_i'^{\omega}) = \varphi^{\omega}_{\omega i}(\alpha')\, \tilde b_i'^{\omega} \\
u(\tilde a_i'^{\omega}) = \tilde a_i'^{\omega}\, \psi^{\omega}_{\omega i}(\tilde\alpha')
\end{cases}\]
LaTeX source
\[
(65)\quad
\begin{cases}
u(b_i'^{\omega}) = \varphi^{\omega}_{\omega i}(\beta')\, b_i'^{\omega} \\
u(\tilde b_i'^{\omega}) = \varphi^{\omega}_{\omega i}(\alpha')\, \tilde b_i'^{\omega} \\
u(\tilde a_i'^{\omega}) = \tilde a_i'^{\omega}\, \psi^{\omega}_{\omega i}(\tilde\alpha')
\end{cases}
\]\[(66)\quad \tilde d_i'^{\omega} : P^{\omega} \to R_i^{\omega'}, \qquad \tilde d_i'^{\omega} = c^{\omega}_{\omega i} \cdot d^{\omega}_{\omega i}\]
LaTeX source
\[
(66)\quad \tilde d_i'^{\omega} : P^{\omega} \to R_i^{\omega'}, \qquad \tilde d_i'^{\omega} = c^{\omega}_{\omega i} \cdot d^{\omega}_{\omega i}
\]\[(67)\quad u(\tilde d_i'^{\omega}) = \varphi_i^{\omega'}(\underbrace{\zeta'}_{\eta\zeta})\, \tilde d_i'^{\omega}\]
LaTeX source
\[
(67)\quad u(\tilde d_i'^{\omega}) = \varphi_i^{\omega'}(\underbrace{\zeta'}_{\eta\zeta})\, \tilde d_i'^{\omega}
\]\[(66')\quad d_i^{\omega} : P^{\omega} \to R_i^{\omega}, \qquad d_i^{\omega} = c^{\omega'}_{\omega' i} \cdot d^{\omega}_{\omega' i}\]
LaTeX source
\[
(66')\quad d_i^{\omega} : P^{\omega} \to R_i^{\omega}, \qquad d_i^{\omega} = c^{\omega'}_{\omega' i} \cdot d^{\omega}_{\omega' i}
\]\[(67')\quad u(\tilde d_i^{\omega}) = \varphi_i^{\omega}(\eta\, \sigma_\infty(\zeta))\, \tilde d_i^{\omega}\]
LaTeX source
\[
(67')\quad u(\tilde d_i^{\omega}) = \varphi_i^{\omega}(\eta\, \sigma_\infty(\zeta))\, \tilde d_i^{\omega}
\]\[(69)\quad (\lambda, \beta', \zeta') \in \widehat{\Pi}_{0,3} \times \widehat{\Pi}_{0,3} \times \widehat{\Pi}_{0,3}\]
LaTeX source
\[
(69)\quad (\lambda, \beta', \zeta') \in \widehat{\Pi}_{0,3} \times \widehat{\Pi}_{0,3} \times \widehat{\Pi}_{0,3}
\]\[(70)\quad
\begin{cases}
\beta' = \alpha' \sigma_\infty(\lambda) \quad \text{où} \quad \alpha' = \zeta' \rho^{-1}(\zeta')^{-1} \\
\beta' \sigma_\infty(\beta') = 1 \quad \text{i.e.} \quad \alpha' \sigma_\infty(\lambda)\, \sigma_\infty(\alpha')\, \lambda = 1
\end{cases}\]
LaTeX source
\[
(70)\quad
\begin{cases}
\beta' = \alpha' \sigma_\infty(\lambda) \quad \text{où} \quad \alpha' = \zeta' \rho^{-1}(\zeta')^{-1} \\
\beta' \sigma_\infty(\beta') = 1 \quad \text{i.e.} \quad \alpha' \sigma_\infty(\lambda)\, \sigma_\infty(\alpha')\, \lambda = 1
\end{cases}
\]\[(69')\quad (\lambda, \eta, \alpha') \in \widehat{\Pi}_{0,3} \times \widehat{\Pi}_{0,3} \times \widehat{\Pi}_{0,3}\]
LaTeX source
\[
(69')\quad (\lambda, \eta, \alpha') \in \widehat{\Pi}_{0,3} \times \widehat{\Pi}_{0,3} \times \widehat{\Pi}_{0,3}
\]\[(70')\quad
\begin{cases}
\beta' = \alpha' \sigma_\infty(\lambda) \quad \text{où} \quad \beta' = \eta\, \sigma_\infty(\eta)^{-1} \\
\alpha' \rho(\alpha') \rho^{2}(\alpha') = 1
\end{cases}\]
LaTeX source
\[
(70')\quad
\begin{cases}
\beta' = \alpha' \sigma_\infty(\lambda) \quad \text{où} \quad \beta' = \eta\, \sigma_\infty(\eta)^{-1} \\
\alpha' \rho(\alpha') \rho^{2}(\alpha') = 1
\end{cases}
\]\[(71)\quad
\begin{cases}
\tilde d_i^{\omega} : P^{\omega} \to R_i^{\omega} \\
\tilde d_i'^{\omega} : P^{\omega} \to R_i^{\omega'} \\
a_i^{\omega} : R_i^{\omega} \to R_i^{\omega'}
\end{cases}\]
LaTeX source
\[
(71)\quad
\begin{cases}
\tilde d_i^{\omega} : P^{\omega} \to R_i^{\omega} \\
\tilde d_i'^{\omega} : P^{\omega} \to R_i^{\omega'} \\
a_i^{\omega} : R_i^{\omega} \to R_i^{\omega'}
\end{cases}
\]\[(72)\quad
\begin{cases}
(\tilde d_i'^{\omega})^{-1} a_i^{\omega} \tilde d_i^{\omega} = 1 \\
(\tilde d'^{\omega}_{\omega i})^{-1} \tilde d^{\omega'}_{\omega i} (\tilde d_i'^{\omega'})^{-1} \tilde d_i^{\omega} = 1
\end{cases}\]
LaTeX source
\[
(72)\quad
\begin{cases}
(\tilde d_i'^{\omega})^{-1} a_i^{\omega} \tilde d_i^{\omega} = 1 \\
(\tilde d'^{\omega}_{\omega i})^{-1} \tilde d^{\omega'}_{\omega i} (\tilde d_i'^{\omega'})^{-1} \tilde d_i^{\omega} = 1
\end{cases}
\]\[(73)\quad
\begin{cases}
u(\tilde d_i^{\omega}) = \varphi_i^{\omega}(\zeta_1)\, \tilde d_i^{\omega} \\
u(\tilde d_i'^{\omega}) = \varphi_i^{\omega'}(\zeta')\, \tilde d_i'^{\omega} \\
u(a_i^{\omega}) = a_i^{\omega} \varphi_i^{\omega}(\lambda)
\end{cases}
\qquad \zeta', \zeta_1, \lambda \in \widehat{\Pi}_{0,3}\]
LaTeX source
\[
(73)\quad
\begin{cases}
u(\tilde d_i^{\omega}) = \varphi_i^{\omega}(\zeta_1)\, \tilde d_i^{\omega} \\
u(\tilde d_i'^{\omega}) = \varphi_i^{\omega'}(\zeta')\, \tilde d_i'^{\omega} \\
u(a_i^{\omega}) = a_i^{\omega} \varphi_i^{\omega}(\lambda)
\end{cases}
\qquad \zeta', \zeta_1, \lambda \in \widehat{\Pi}_{0,3}
\]\[(74)\quad \zeta' = \varepsilon_0(\lambda\zeta_1) \qquad \text{i.e.} \qquad \zeta_1 = \lambda^{-1} \cdot \varepsilon_0^{-1}(\zeta')\]
LaTeX source
\[
(74)\quad \zeta' = \varepsilon_0(\lambda\zeta_1) \qquad \text{i.e.} \qquad \zeta_1 = \lambda^{-1} \cdot \varepsilon_0^{-1}(\zeta')
\]\[(75)\quad \beta\, \zeta_1 = \beta' \sigma_\infty(\zeta')\]
LaTeX source
\[ (75)\quad \beta\, \zeta_1 = \beta' \sigma_\infty(\zeta') \]
\[(75)\quad
\begin{aligned}
\beta' &= \zeta_1 \sigma_\infty(\zeta')^{-1} = \text{\struck{$\varepsilon_0(\lambda\zeta_1)$}}\ \zeta_1 (\sigma_\infty\varepsilon_0)(\lambda\zeta_1)^{-1} \\
&= \lambda^{-1} \cdot \varepsilon_0^{-1}(\zeta')\, \sigma_\infty(\zeta')^{-1}.
\end{aligned}\]
LaTeX source
\[
(75)\quad
\begin{aligned}
\beta' &= \zeta_1 \sigma_\infty(\zeta')^{-1} = \text{\struck{$\varepsilon_0(\lambda\zeta_1)$}}\ \zeta_1 (\sigma_\infty\varepsilon_0)(\lambda\zeta_1)^{-1} \\
&= \lambda^{-1} \cdot \varepsilon_0^{-1}(\zeta')\, \sigma_\infty(\zeta')^{-1}.
\end{aligned}
\]\[(75')\quad \sigma_\infty(\beta') = \sigma_\infty(\zeta_1)\, \zeta'^{-1} = \sigma_\infty(\zeta_1)\, \varepsilon_0(\lambda\zeta_1)^{-1}
= \sigma_\infty(\lambda)^{-1} \overbrace{\rho(\zeta')\, \zeta'^{-1}}^{\alpha'^{-1}}\]
LaTeX source
\[
(75')\quad \sigma_\infty(\beta') = \sigma_\infty(\zeta_1)\, \zeta'^{-1} = \sigma_\infty(\zeta_1)\, \varepsilon_0(\lambda\zeta_1)^{-1}
= \sigma_\infty(\lambda)^{-1} \overbrace{\rho(\zeta')\, \zeta'^{-1}}^{\alpha'^{-1}}
\]\[\text{\struck{$\beta' \sigma_\infty(\beta') = 1$}}\]
LaTeX source
\[
\text{\struck{$\beta' \sigma_\infty(\beta') = 1$}}
\]\[(77)\quad \sigma_\infty(\beta')^{-1} = \alpha' \sigma_\infty(\lambda).\]
LaTeX source
\[
(77)\quad \sigma_\infty(\beta')^{-1} = \alpha' \sigma_\infty(\lambda).
\]\[(78)\quad \beta' \sigma_\infty(\beta') = 1 \qquad \text{ou encore} \quad \sigma_\infty(\beta')^{-1} = \beta'\]
LaTeX source
\[
(78)\quad \beta' \sigma_\infty(\beta') = 1 \qquad \text{ou encore} \quad \sigma_\infty(\beta')^{-1} = \beta'
\]\[\beta_1 = \sigma_\infty(\beta')^{-1} = \alpha' \sigma_\infty(\lambda)\]
LaTeX source
\[
\beta_1 = \sigma_\infty(\beta')^{-1} = \alpha' \sigma_\infty(\lambda)
\]\[(\ast\ast)\quad \beta_1 \sigma_\infty(\beta_1) = 1\]
LaTeX source
\[ (\ast\ast)\quad \beta_1 \sigma_\infty(\beta_1) = 1 \]
\[(78)\quad \beta' = \alpha' \sigma_\infty(\lambda) \qquad \text{où} \quad \alpha' = \zeta' \rho(\zeta')^{-1}\]
LaTeX source
\[
(78)\quad \beta' = \alpha' \sigma_\infty(\lambda) \qquad \text{où} \quad \alpha' = \zeta' \rho(\zeta')^{-1}
\]\[J \subset \Sigma, \qquad J = (R_i)_{i \in J}\]
LaTeX source
\[
J \subset \Sigma, \qquad J = (R_i)_{i \in J}
\]\[\Gamma_{\Sigma,J} = \Gamma \simeq \mathfrak{S}_J \times \{1, \tau\}\]
LaTeX source
\[
\Gamma_{\Sigma,J} = \Gamma \simeq \mathfrak{S}_J \times \{1, \tau\}
\]\[(3)\quad
\left\{
\begin{array}{ll}
\boldsymbol{\varpi} = \Omega(\Sigma) \simeq \Omega(E_3)
& \text{ens. des deux orientations} \\
& \text{de } \Sigma \text{, ou de } E \\
\boldsymbol{\omega} = \Omega(J) \simeq \Omega(\Sigma_{\mathbf{R}}) & \\
\boldsymbol{\varepsilon} = \pi_0(\Sigma \setminus \Sigma_{\mathbf{R}})
= \pi_0(E \setminus V) = \pi_0\big((E/V)^{*}\big) &
\end{array}
\right.\]
LaTeX source
\[
(3)\quad
\left\{
\begin{array}{ll}
\boldsymbol{\varpi} = \Omega(\Sigma) \simeq \Omega(E_3)
& \text{ens. des deux orientations} \\
& \text{de } \Sigma \text{, ou de } E \\
\boldsymbol{\omega} = \Omega(J) \simeq \Omega(\Sigma_{\mathbf{R}}) & \\
\boldsymbol{\varepsilon} = \pi_0(\Sigma \setminus \Sigma_{\mathbf{R}})
= \pi_0(E \setminus V) = \pi_0\big((E/V)^{*}\big) &
\end{array}
\right.
\]\[\Sigma_{\mathbf{R}} = \Sigma \cap V
\qquad \text{cercle euclidien du plan euclidien } V .\]
LaTeX source
\[
\Sigma_{\mathbf{R}} = \Sigma \cap V
\qquad \text{cercle euclidien du plan euclidien } V .
\]\[(4)\quad \sum_{j \in J} R_j = 0\]
LaTeX source
\[
(4)\quad \sum_{j \in J} R_j = 0
\]\[(5)\quad V \simeq V_J(\mathbf{R})
= \operatorname{Ker}\big(\mathbf{R}^J \xrightarrow{\ \text{somme}\ } \mathbf{R}\big)\]
LaTeX source
\[
(5)\quad V \simeq V_J(\mathbf{R})
= \operatorname{Ker}\big(\mathbf{R}^J \xrightarrow{\ \text{somme}\ } \mathbf{R}\big)
\]\[(6)\quad \Delta = V^{\perp} \simeq \mathbf{R}(\boldsymbol{\varepsilon})\]
LaTeX source
\[
(6)\quad \Delta = V^{\perp} \simeq \mathbf{R}(\boldsymbol{\varepsilon})
\]\[(7)\quad E \simeq V_J(\mathbf{R}) \oplus \mathbf{R}(\boldsymbol{\varepsilon})
\qquad \text{isom. d'espaces euclidiens}\]
LaTeX source
\[
(7)\quad E \simeq V_J(\mathbf{R}) \oplus \mathbf{R}(\boldsymbol{\varepsilon})
\qquad \text{isom. d'espaces euclidiens}
\]\[q(R_j) = 1\]
LaTeX source
\[ q(R_j) = 1 \]
\[(8)\quad g_E = \underbrace{g_{V_J(\mathbf{R})}}_{\text{tautol.}}
\oplus \operatorname{sg}(g)\, \mathrm{id}_{\Delta}\]
LaTeX source
\[
(8)\quad g_E = \underbrace{g_{V_J(\mathbf{R})}}_{\text{tautol.}}
\oplus \operatorname{sg}(g)\, \mathrm{id}_{\Delta}
\]\[(9)\quad \tau_E = \mathrm{id}_{V_J(\mathbf{R})} \oplus (-\mathrm{id}_{\Delta})\]
LaTeX source
\[
(9)\quad \tau_E = \mathrm{id}_{V_J(\mathbf{R})} \oplus (-\mathrm{id}_{\Delta})
\]\[(10)\quad \Sigma^{*} = \Sigma \setminus J = \Sigma - \{R_i \mid i \in I\}\]
LaTeX source
\[
(10)\quad \Sigma^{*} = \Sigma \setminus J = \Sigma - \{R_i \mid i \in I\}
\]\[(11)\quad \Sigma'_{R_i} \simeq P(T_{\Sigma,R_i})\]
LaTeX source
\[
(11)\quad \Sigma'_{R_i} \simeq P(T_{\Sigma,R_i})
\]\[\chi_!(\Sigma) - 3\chi_!(\text{rondelle ouverte})
+ 3\big(\underbrace{\chi_!(\text{ruban Möbius})}_{0}\big)
= 2 - 3 = -1 = 1 - g ,\]
LaTeX source
\[
\chi_!(\Sigma) - 3\chi_!(\text{rondelle ouverte})
+ 3\big(\underbrace{\chi_!(\text{ruban Möbius})}_{0}\big)
= 2 - 3 = -1 = 1 - g ,
\]\[(12)\quad \partial\widetilde{\Sigma} \simeq \coprod_{i \in I} TU_{\Sigma,R_i}\]
LaTeX source
\[
(12)\quad \partial\widetilde{\Sigma} \simeq \coprod_{i \in I} TU_{\Sigma,R_i}
\]\[(13)\quad
\operatorname{Rev\,et}(\widetilde{\Sigma})
\xrightarrow[\text{équiv}]{\ \approx\ }
\operatorname{Rev\,et}(\widetilde{\Sigma}^{\circ})
\xrightarrow[\text{iso}]{\ \sim\ }
\operatorname{Rev\,et}(\Sigma^{*})\]
LaTeX source
\[
(13)\quad
\operatorname{Rev\,et}(\widetilde{\Sigma})
\xrightarrow[\text{équiv}]{\ \approx\ }
\operatorname{Rev\,et}(\widetilde{\Sigma}^{\circ})
\xrightarrow[\text{iso}]{\ \sim\ }
\operatorname{Rev\,et}(\Sigma^{*})
\]\[\widetilde{\Sigma}^{\circ}
\overset{\mathrm{def}}{=} \widetilde{\Sigma} \setminus \partial\widetilde{\Sigma}
= \widetilde{\Sigma} \,|\, \Sigma^{*} \hookrightarrow \widetilde{\Sigma}\]
LaTeX source
\[
\widetilde{\Sigma}^{\circ}
\overset{\mathrm{def}}{=} \widetilde{\Sigma} \setminus \partial\widetilde{\Sigma}
= \widetilde{\Sigma} \,|\, \Sigma^{*} \hookrightarrow \widetilde{\Sigma}
\]\[\widetilde{\Sigma}^{\circ} \xrightarrow{\ \sim\ } \Sigma^{*},\]
LaTeX source
\[
\widetilde{\Sigma}^{\circ} \xrightarrow{\ \sim\ } \Sigma^{*},
\]\[(14)\quad \Pi_1(\widetilde{\Sigma}) \longrightarrow \Pi_1(\Sigma^{*})\]
LaTeX source
\[
(14)\quad \Pi_1(\widetilde{\Sigma}) \longrightarrow \Pi_1(\Sigma^{*})
\]\[\Pi_1(U_i) \longrightarrow \Pi_1(\widetilde{\Sigma})\]
LaTeX source
\[
\Pi_1(U_i) \longrightarrow \Pi_1(\widetilde{\Sigma})
\]\[(15)\quad \Pi_1\Big(\coprod U_i\Big) \longrightarrow \Pi_1(\Sigma^{*}) .\]
LaTeX source
\[
(15)\quad \Pi_1\Big(\coprod U_i\Big) \longrightarrow \Pi_1(\Sigma^{*}) .
\]\[\widetilde{\Sigma} \longrightarrow \Sigma, \qquad J \subset \Sigma\]
LaTeX source
\[
\widetilde{\Sigma} \longrightarrow \Sigma, \qquad J \subset \Sigma
\]\[(16)\quad
\left\{
\begin{array}{ll}
Q_i \ (i \in J) & \text{antipodique de } R_i \ (= -R_i) \\
R_i^{\omega} \in U_i & (i \in J,\ \omega \in \boldsymbol{\omega}) \\
P_{\varepsilon} & (\varepsilon \in \boldsymbol{\varepsilon}
= \pi_0(\Sigma \setminus \Sigma_{\mathbf{R}})) \\
S_i^{\varepsilon} &
\end{array}
\right.\]
LaTeX source
\[
(16)\quad
\left\{
\begin{array}{ll}
Q_i \ (i \in J) & \text{antipodique de } R_i \ (= -R_i) \\
R_i^{\omega} \in U_i & (i \in J,\ \omega \in \boldsymbol{\omega}) \\
P_{\varepsilon} & (\varepsilon \in \boldsymbol{\varepsilon}
= \pi_0(\Sigma \setminus \Sigma_{\mathbf{R}})) \\
S_i^{\varepsilon} &
\end{array}
\right.
\]\[(17)\quad \{P_\varepsilon\} = \Delta \cap (\Sigma - \Sigma_{\mathbf{R}})_\varepsilon\]
LaTeX source
\[
(17)\quad \{P_\varepsilon\} = \Delta \cap (\Sigma - \Sigma_{\mathbf{R}})_\varepsilon
\]\[(18)\quad
U_{i\mathbf{R}} \overset{\mathrm{def}}{=}
\underbrace{U_i \cap T_{\Sigma_{\mathbf{R}},R_i}}_{TU_{\Sigma_{\mathbf{R}},R_i}}
\simeq \boldsymbol{\omega}\]
LaTeX source
\[
(18)\quad
U_{i\mathbf{R}} \overset{\mathrm{def}}{=}
\underbrace{U_i \cap T_{\Sigma_{\mathbf{R}},R_i}}_{TU_{\Sigma_{\mathbf{R}},R_i}}
\simeq \boldsymbol{\omega}
\]\[(19)\quad S_i^{\varepsilon} \in U_i \cap T_{\Sigma_i} = TU_{\Sigma_i}\]
LaTeX source
\[
(19)\quad S_i^{\varepsilon} \in U_i \cap T_{\Sigma_i} = TU_{\Sigma_i}
\]\[J = \{0, 1, \infty\}, \qquad \boldsymbol{\omega} = \{+1, -1\}\]
LaTeX source
\[
J = \{0, 1, \infty\}, \qquad \boldsymbol{\omega} = \{+1, -1\}
\]\[\boldsymbol{\varpi} \simeq \{+1, -1\}, \quad \text{d'où} \quad
\boldsymbol{\varepsilon} \simeq \{+1, -1\} .\]
LaTeX source
\[
\boldsymbol{\varpi} \simeq \{+1, -1\}, \quad \text{d'où} \quad
\boldsymbol{\varepsilon} \simeq \{+1, -1\} .
\]\[\text{\struck{(19)}}\qquad
\boldsymbol{\varpi} \simeq \{\pm 1\}\]
LaTeX source
\[
\text{\struck{(19)}}\qquad
\boldsymbol{\varpi} \simeq \{\pm 1\}
\]\[(20)\quad
\overset{12}{a_i^{\omega,\varepsilon}},\quad
\overset{6}{b_i^{\omega}},\quad
\overset{6}{c_i^{\varepsilon}},\quad
\overset{6}{d_i^{\varepsilon}},
\qquad i \in J,\ \omega \in \boldsymbol{\omega},\ \varepsilon \in \boldsymbol{\varepsilon}\]
LaTeX source
\[
(20)\quad
\overset{12}{a_i^{\omega,\varepsilon}},\quad
\overset{6}{b_i^{\omega}},\quad
\overset{6}{c_i^{\varepsilon}},\quad
\overset{6}{d_i^{\varepsilon}},
\qquad i \in J,\ \omega \in \boldsymbol{\omega},\ \varepsilon \in \boldsymbol{\varepsilon}
\]\[(22)\quad
\tau a_i^{\omega,\varepsilon} = a_i^{\omega,\varepsilon'}, \quad
\tau b_i^{\omega} = b_i^{\omega}, \quad
\tau c_i^{\varepsilon} = c_i^{\varepsilon'}, \quad
\tau d_i^{\varepsilon} = d_i^{\varepsilon'} .\]
LaTeX source
\[
(22)\quad
\tau a_i^{\omega,\varepsilon} = a_i^{\omega,\varepsilon'}, \quad
\tau b_i^{\omega} = b_i^{\omega}, \quad
\tau c_i^{\varepsilon} = c_i^{\varepsilon'}, \quad
\tau d_i^{\varepsilon} = d_i^{\varepsilon'} .
\]\[(23)\quad a_i^{\omega\varepsilon} : S_i^{\varepsilon} \longrightarrow R_i^{\omega}
\quad \text{sur } U_i\]
LaTeX source
\[
(23)\quad a_i^{\omega\varepsilon} : S_i^{\varepsilon} \longrightarrow R_i^{\omega}
\quad \text{sur } U_i
\]\[(24)\quad b_i^{\omega} : Q_i \longrightarrow R_{\omega' i}^{\omega'}
\quad \text{sur } \widetilde{\Sigma}_{\mathbf{R}} \simeq \operatorname{Dic}(\Sigma_{\mathbf{R}}, J)\]
LaTeX source
\[
(24)\quad b_i^{\omega} : Q_i \longrightarrow R_{\omega' i}^{\omega'}
\quad \text{sur } \widetilde{\Sigma}_{\mathbf{R}} \simeq \operatorname{Dic}(\Sigma_{\mathbf{R}}, J)
\]\[(25)\quad c_i^{\omega} : P^{\omega} \longrightarrow Q_i
\qquad \text{suivant un arc de grand cercle}\]
LaTeX source
\[
(25)\quad c_i^{\omega} : P^{\omega} \longrightarrow Q_i
\qquad \text{suivant un arc de grand cercle}
\]\[(26)\quad d_i^{\omega} : P^{\omega} \longrightarrow S_i^{\omega}
\qquad \text{suivant un arc de grand cercle}\]
LaTeX source
\[
(26)\quad d_i^{\omega} : P^{\omega} \longrightarrow S_i^{\omega}
\qquad \text{suivant un arc de grand cercle}
\]\[(27)\quad b_i : R_{\omega i}^{\omega'} \longrightarrow R_{\omega' i}^{\omega'}, \qquad
\widetilde{b}_i^{\omega} = b_i^{\omega} (b_i^{\omega'})^{-1}\]
LaTeX source
\[
(27)\quad b_i : R_{\omega i}^{\omega'} \longrightarrow R_{\omega' i}^{\omega'}, \qquad
\widetilde{b}_i^{\omega} = b_i^{\omega} (b_i^{\omega'})^{-1}
\]\[(27)\quad
\left\{
\begin{array}{ll}
\widetilde{\Sigma}_\varepsilon = \widetilde{\Sigma} \setminus
\bigcup_{i \in J} \operatorname{supp} d_i^{\varepsilon}
& \varepsilon \in \boldsymbol{\varepsilon} \\[4pt]
\widetilde{\Sigma}_i = \widetilde{\Sigma} \setminus
\bigcup_{j \in J \setminus \{i\}} b_j &
\end{array}
\right.\]
LaTeX source
\[
(27)\quad
\left\{
\begin{array}{ll}
\widetilde{\Sigma}_\varepsilon = \widetilde{\Sigma} \setminus
\bigcup_{i \in J} \operatorname{supp} d_i^{\varepsilon}
& \varepsilon \in \boldsymbol{\varepsilon} \\[4pt]
\widetilde{\Sigma}_i = \widetilde{\Sigma} \setminus
\bigcup_{j \in J \setminus \{i\}} b_j &
\end{array}
\right.
\]\[(28)\quad
\left\{
\begin{array}{l}
\Pi_\varepsilon = \pi_1(\widetilde{\Sigma}, \widetilde{\Sigma}_\varepsilon)
\simeq \pi_1(\Sigma^{*}, \Sigma^{*}_\varepsilon)
\simeq \pi_1(\Sigma^{*}, P_\varepsilon) \\[4pt]
\Pi_i = \pi_1(\widetilde{\Sigma}, \widetilde{\Sigma}_i)
= \pi_1(\Sigma^{*}, \Sigma^{*}_i)
\simeq \pi_1(\Sigma^{*}, Q_i)
\end{array}
\right.\]
LaTeX source
\[
(28)\quad
\left\{
\begin{array}{l}
\Pi_\varepsilon = \pi_1(\widetilde{\Sigma}, \widetilde{\Sigma}_\varepsilon)
\simeq \pi_1(\Sigma^{*}, \Sigma^{*}_\varepsilon)
\simeq \pi_1(\Sigma^{*}, P_\varepsilon) \\[4pt]
\Pi_i = \pi_1(\widetilde{\Sigma}, \widetilde{\Sigma}_i)
= \pi_1(\Sigma^{*}, \Sigma^{*}_i)
\simeq \pi_1(\Sigma^{*}, Q_i)
\end{array}
\right.
\]\[(29)\quad
\left\{
\begin{array}{ll}
\varphi_{\varepsilon,x} \text{ ou } \varphi_\omega :
\Pi_\varepsilon \xrightarrow{\ \sim\ } \pi_1(\widetilde{\Sigma}, x)
& \big(\simeq \pi_1(\Sigma^{*}, x) \text{ si } x \in \Sigma^{*}\big) \\[4pt]
\varphi_{i,x} \text{ ou } \varphi_i :
\Pi_i \xrightarrow{\ \sim\ } \pi_1(\widetilde{\Sigma}, x)
& \text{—}
\end{array}
\right.\]
LaTeX source
\[
(29)\quad
\left\{
\begin{array}{ll}
\varphi_{\varepsilon,x} \text{ ou } \varphi_\omega :
\Pi_\varepsilon \xrightarrow{\ \sim\ } \pi_1(\widetilde{\Sigma}, x)
& \big(\simeq \pi_1(\Sigma^{*}, x) \text{ si } x \in \Sigma^{*}\big) \\[4pt]
\varphi_{i,x} \text{ ou } \varphi_i :
\Pi_i \xrightarrow{\ \sim\ } \pi_1(\widetilde{\Sigma}, x)
& \text{—}
\end{array}
\right.
\]\[(30)\quad
\left\{
\begin{array}{ll}
\varphi_{i\varepsilon} : \Pi_\omega \longrightarrow \Pi_i
& \text{défini par } c_i^{\varepsilon} : P_\varepsilon \to Q_i \\[4pt]
\varphi_{\varepsilon i} : \Pi_i \longrightarrow \Pi_\omega
& \text{---\ } (c_i^{\varepsilon})^{-1} : Q_i \to P_\varepsilon
\end{array}
\right.\]
LaTeX source
\[
(30)\quad
\left\{
\begin{array}{ll}
\varphi_{i\varepsilon} : \Pi_\omega \longrightarrow \Pi_i
& \text{défini par } c_i^{\varepsilon} : P_\varepsilon \to Q_i \\[4pt]
\varphi_{\varepsilon i} : \Pi_i \longrightarrow \Pi_\omega
& \text{---\ } (c_i^{\varepsilon})^{-1} : Q_i \to P_\varepsilon
\end{array}
\right.
\]\[(31)\quad
\left\{
\begin{array}{ll}
\varphi_{R_i^{\omega},\, \omega i} : \Pi_{\omega i} \xrightarrow{\ \sim\ }
\pi_1(\widetilde{\Sigma}, R_i^{\omega})
& \text{ou } \varphi_{\omega i} \\[4pt]
\varphi_{S_i^{\varepsilon},\, \varepsilon} : \Pi_\varepsilon \xrightarrow{\ \sim\ }
\pi_1(\widetilde{\Sigma}, S_i^{\varepsilon})
& \text{ou } \varphi^{\varepsilon} \text{ ou } d_i^{\varepsilon}
\end{array}
\right.\]
LaTeX source
\[
(31)\quad
\left\{
\begin{array}{ll}
\varphi_{R_i^{\omega},\, \omega i} : \Pi_{\omega i} \xrightarrow{\ \sim\ }
\pi_1(\widetilde{\Sigma}, R_i^{\omega})
& \text{ou } \varphi_{\omega i} \\[4pt]
\varphi_{S_i^{\varepsilon},\, \varepsilon} : \Pi_\varepsilon \xrightarrow{\ \sim\ }
\pi_1(\widetilde{\Sigma}, S_i^{\varepsilon})
& \text{ou } \varphi^{\varepsilon} \text{ ou } d_i^{\varepsilon}
\end{array}
\right.
\]\[\text{\struck{$a_i^{\omega} = a_i^{\omega-} a_i^{\omega+}$, \quad $a_i^{\omega+} : R_i^{\omega} \to S_i^{\omega}$, \quad $a_i^{\omega-} : S_i^{\omega} \to R_i^{\omega'}$}}\]
LaTeX source
\[
\text{\struck{$a_i^{\omega} = a_i^{\omega-} a_i^{\omega+}$, \quad $a_i^{\omega+} : R_i^{\omega} \to S_i^{\omega}$, \quad $a_i^{\omega-} : S_i^{\omega} \to R_i^{\omega'}$}}
\]\[(32)\quad
\Pi_{0,3} = \pi_1\big(\mathbf{P}^1_{\mathbf{C}} \setminus \{0,1,\infty\}
\,[= U_{0,3}(\mathbf{C})],\ P^{+}\big)
= \{\, l_0, l_1, l_\infty \mid l_\infty l_1 l_0 = 1 \,\}\]
LaTeX source
\[
(32)\quad
\Pi_{0,3} = \pi_1\big(\mathbf{P}^1_{\mathbf{C}} \setminus \{0,1,\infty\}
\,[= U_{0,3}(\mathbf{C})],\ P^{+}\big)
= \{\, l_0, l_1, l_\infty \mid l_\infty l_1 l_0 = 1 \,\}
\]\[\subset \widetilde{\Pi}_{0,3}
= \pi_1\big(U_{0,3}(\mathbf{C}),\ \mathfrak{S}_3 \times \{1,\tau\},\ P^{+}\big)\]
LaTeX source
\[
\subset \widetilde{\Pi}_{0,3}
= \pi_1\big(U_{0,3}(\mathbf{C}),\ \mathfrak{S}_3 \times \{1,\tau\},\ P^{+}\big)
\]\[= \{\, \rho, \sigma_\infty, \widetilde{\sigma}_\infty \mid
\rho^3 = \sigma_\infty^2 = \widetilde{\sigma}_\infty^2 = 1,\
\sigma_\infty(\rho) = \rho^{-1},\
\widetilde{\sigma}_\infty(\sigma_\infty) = 1 \,\}\]
LaTeX source
\[
= \{\, \rho, \sigma_\infty, \widetilde{\sigma}_\infty \mid
\rho^3 = \sigma_\infty^2 = \widetilde{\sigma}_\infty^2 = 1,\
\sigma_\infty(\rho) = \rho^{-1},\
\widetilde{\sigma}_\infty(\sigma_\infty) = 1 \,\}
\]\[\text{[i.e. } (\sigma_\infty \widetilde{\sigma}_\infty)^2 = 1 \text{]}
\qquad \simeq \mathrm{GL}(2,\mathbf{Z})/\{\pm 1\}\]
LaTeX source
\[
\text{[i.e. } (\sigma_\infty \widetilde{\sigma}_\infty)^2 = 1 \text{]}
\qquad \simeq \mathrm{GL}(2,\mathbf{Z})/\{\pm 1\}
\]\[(33)\quad
\left\{
\begin{array}{l}
\varepsilon_0 \overset{\mathrm{def}}{=} \sigma_\infty \rho, \quad
\varepsilon_1 \overset{\mathrm{def}}{=} \rho(\varepsilon_0)
\ (= \rho\, \varepsilon_0 \rho^{-1}), \\[4pt]
\varepsilon_\infty \overset{\mathrm{def}}{=} \rho(\varepsilon_1)
= \rho^2(\varepsilon_0) = \rho^{-1}(\varepsilon_0) \\[4pt]
l_0 \overset{\mathrm{def}}{=} \varepsilon_0^2, \quad
l_1 \overset{\mathrm{def}}{=} \varepsilon_1^2, \quad
l_\infty \overset{\mathrm{def}}{=} \varepsilon_\infty^2, \quad
l_\infty l_1 l_0 = 1 \\[4pt]
\rho(l_i) = l_{\rho(i)}
\ \ \{\rho(l_0) = l_1,\ \rho(l_1) = l_\infty,\ \rho(l_\infty) = l_0\}, \quad
\rho(\varepsilon_i) = \varepsilon_{\rho(i)}
\end{array}
\right.\]
LaTeX source
\[
(33)\quad
\left\{
\begin{array}{l}
\varepsilon_0 \overset{\mathrm{def}}{=} \sigma_\infty \rho, \quad
\varepsilon_1 \overset{\mathrm{def}}{=} \rho(\varepsilon_0)
\ (= \rho\, \varepsilon_0 \rho^{-1}), \\[4pt]
\varepsilon_\infty \overset{\mathrm{def}}{=} \rho(\varepsilon_1)
= \rho^2(\varepsilon_0) = \rho^{-1}(\varepsilon_0) \\[4pt]
l_0 \overset{\mathrm{def}}{=} \varepsilon_0^2, \quad
l_1 \overset{\mathrm{def}}{=} \varepsilon_1^2, \quad
l_\infty \overset{\mathrm{def}}{=} \varepsilon_\infty^2, \quad
l_\infty l_1 l_0 = 1 \\[4pt]
\rho(l_i) = l_{\rho(i)}
\ \ \{\rho(l_0) = l_1,\ \rho(l_1) = l_\infty,\ \rho(l_\infty) = l_0\}, \quad
\rho(\varepsilon_i) = \varepsilon_{\rho(i)}
\end{array}
\right.
\]\[(33)\quad
\left\{
\begin{array}{l}
\tau_\infty \overset{\mathrm{def}}{=} \sigma_\infty \widetilde{\sigma}_\infty
= \widetilde{\sigma}_\infty \sigma_\infty, \quad \tau_\infty^2 = 1 \\[4pt]
\tau_\infty(l_0) = l_0^{-1}, \quad \tau_\infty(l_1) = l_1^{-1}, \quad
\tau_\infty(l_\infty) = l_0^{-1} l_\infty^{-1} l_0 \\[4pt]
\widetilde{\sigma}_\infty(l_0) = l_1^{-1}, \quad
\widetilde{\sigma}_\infty(l_1) = l_0^{-1}, \quad
\widetilde{\sigma}_\infty(l_\infty) = l_\infty^{-1} \\[4pt]
\sigma_\infty(l_0) = l_1, \quad \sigma_\infty(l_1) = l_0, \quad
\sigma_\infty(l_\infty) = l_1^{-1} l_0^{-1}
\end{array}
\right.\]
LaTeX source
\[
(33)\quad
\left\{
\begin{array}{l}
\tau_\infty \overset{\mathrm{def}}{=} \sigma_\infty \widetilde{\sigma}_\infty
= \widetilde{\sigma}_\infty \sigma_\infty, \quad \tau_\infty^2 = 1 \\[4pt]
\tau_\infty(l_0) = l_0^{-1}, \quad \tau_\infty(l_1) = l_1^{-1}, \quad
\tau_\infty(l_\infty) = l_0^{-1} l_\infty^{-1} l_0 \\[4pt]
\widetilde{\sigma}_\infty(l_0) = l_1^{-1}, \quad
\widetilde{\sigma}_\infty(l_1) = l_0^{-1}, \quad
\widetilde{\sigma}_\infty(l_\infty) = l_\infty^{-1} \\[4pt]
\sigma_\infty(l_0) = l_1, \quad \sigma_\infty(l_1) = l_0, \quad
\sigma_\infty(l_\infty) = l_1^{-1} l_0^{-1}
\end{array}
\right.
\]\[(34)\quad
\left\{
\begin{array}{l}
\psi_\varepsilon^{i,\omega} : \Pi_{0,3} \xrightarrow{\ \sim\ } \Pi_\varepsilon \\[4pt]
\psi_i^{\omega,\varepsilon} : \Pi_{0,3} \xrightarrow{\ \sim\ } \Pi_i
\end{array}
\right.\]
LaTeX source
\[
(34)\quad
\left\{
\begin{array}{l}
\psi_\varepsilon^{i,\omega} : \Pi_{0,3} \xrightarrow{\ \sim\ } \Pi_\varepsilon \\[4pt]
\psi_i^{\omega,\varepsilon} : \Pi_{0,3} \xrightarrow{\ \sim\ } \Pi_i
\end{array}
\right.
\]\[\text{\struck{(35)}}\quad
\psi_r = \psi_{\varepsilon}^{i,\omega} : \Pi_{0,3} \xrightarrow{\ \sim\ } \Pi_\varepsilon
\qquad r = (i, \omega, \varpi)\]
LaTeX source
\[
\text{\struck{(35)}}\quad
\psi_r = \psi_{\varepsilon}^{i,\omega} : \Pi_{0,3} \xrightarrow{\ \sim\ } \Pi_\varepsilon
\qquad r = (i, \omega, \varpi)
\]\[(36)\quad
\psi_\varepsilon^{i,\omega} = \pi_1(u_{i,\omega,\varepsilon} ; P^{+}),
\quad \text{où } u_r = u_{i,\omega,\varepsilon} = u_\varepsilon^{i,\omega} :\]
LaTeX source
\[
(36)\quad
\psi_\varepsilon^{i,\omega} = \pi_1(u_{i,\omega,\varepsilon} ; P^{+}),
\quad \text{où } u_r = u_{i,\omega,\varepsilon} = u_\varepsilon^{i,\omega} :
\]\[\big(U_{0,3}(\mathbf{C}), P^{+}\big) \longrightarrow (\Sigma^{*}, P_\omega)\]
LaTeX source
\[
\big(U_{0,3}(\mathbf{C}), P^{+}\big) \longrightarrow (\Sigma^{*}, P_\omega)
\]\[\psi_r : \Pi_{0,3} \xrightarrow{\ \sim\ } \Pi_\omega, \qquad
r \in \operatorname{Rep}(J, \boldsymbol{\varpi})
\simeq \operatorname{Isom}\big((\Sigma_0^{*}, P_{+}), (\Sigma^{*}, P_{+})\big)\]
LaTeX source
\[
\psi_r : \Pi_{0,3} \xrightarrow{\ \sim\ } \Pi_\omega, \qquad
r \in \operatorname{Rep}(J, \boldsymbol{\varpi})
\simeq \operatorname{Isom}\big((\Sigma_0^{*}, P_{+}), (\Sigma^{*}, P_{+})\big)
\]\[g \in \widetilde{\mathfrak{S}}_J \subset \Gamma = \check{\mathfrak{S}}_J\]
LaTeX source
\[
g \in \widetilde{\mathfrak{S}}_J \subset \Gamma = \check{\mathfrak{S}}_J
\]\[\Gamma_{P_\varepsilon}
= \{\, (g, \tau^{\alpha}) \in \mathfrak{S}_J \times \mathbf{Z}/2\mathbf{Z} \mid
\alpha = 0 \text{ si } \operatorname{sg} g = 1,\
\alpha = 1 \text{ si } \operatorname{sg} g = -1 \,\}\]
LaTeX source
\[
\Gamma_{P_\varepsilon}
= \{\, (g, \tau^{\alpha}) \in \mathfrak{S}_J \times \mathbf{Z}/2\mathbf{Z} \mid
\alpha = 0 \text{ si } \operatorname{sg} g = 1,\
\alpha = 1 \text{ si } \operatorname{sg} g = -1 \,\}
\]\[= \{\, g \in \Gamma \mid g(\varepsilon) = \varepsilon \,\}\]
LaTeX source
\[
= \{\, g \in \Gamma \mid g(\varepsilon) = \varepsilon \,\}
\]\[(37)\qquad
\pi_1(g) \text{ par transport de structure}\]
LaTeX source
\[
(37)\qquad
\pi_1(g) \text{ par transport de structure}
\]\[u_r : \widetilde{\mathfrak{S}}_3 \xrightarrow{\ \sim\ } \widetilde{\mathfrak{S}}_3\]
LaTeX source
\[
u_r : \widetilde{\mathfrak{S}}_3 \xrightarrow{\ \sim\ } \widetilde{\mathfrak{S}}_3
\]\[r' = r g_0 \quad \text{avec } g_0 \in \widetilde{\mathfrak{S}}_3\]
LaTeX source
\[
r' = r g_0 \quad \text{avec } g_0 \in \widetilde{\mathfrak{S}}_3
\]\[(38)\quad \text{i.e. } u_{r'} = u_r u_{g_0}
\qquad (\text{avec } u_r(g_0) = g \text{ mais peu importe})\]
LaTeX source
\[
(38)\quad \text{i.e. } u_{r'} = u_r u_{g_0}
\qquad (\text{avec } u_r(g_0) = g \text{ mais peu importe})
\]\[(39)\quad \psi_{r'} = \psi_r \circ \pi_1(g_0, P_{+})
\qquad \text{si } r' = r \circ g_0\]
LaTeX source
\[
(39)\quad \psi_{r'} = \psi_r \circ \pi_1(g_0, P_{+})
\qquad \text{si } r' = r \circ g_0
\]\[g_0 = \rho \quad \text{donc} \quad
r' = r\rho = (\omega i, \omega, \varpi) \quad \text{si } r = (i, \omega, \varpi)\]
LaTeX source
\[
g_0 = \rho \quad \text{donc} \quad
r' = r\rho = (\omega i, \omega, \varpi) \quad \text{si } r = (i, \omega, \varpi)
\]\[(40)\quad
\psi_\varepsilon^{\omega i, \omega}
= \overbrace{\psi_\varepsilon^{i,\omega} \circ \rho}^{\rho_\omega \circ \psi_\varepsilon^{i,\omega} =}\]
LaTeX source
\[
(40)\quad
\psi_\varepsilon^{\omega i, \omega}
= \overbrace{\psi_\varepsilon^{i,\omega} \circ \rho}^{\rho_\omega \circ \psi_\varepsilon^{i,\omega} =}
\]\[\widetilde{\sigma}_\infty : \quad
0 \mapsto 1, \quad 1 \mapsto 0, \quad \infty \mapsto \infty,
\qquad \varpi \mapsto \varpi'\]
LaTeX source
\[
\widetilde{\sigma}_\infty : \quad
0 \mapsto 1, \quad 1 \mapsto 0, \quad \infty \mapsto \infty,
\qquad \varpi \mapsto \varpi'
\]\[g_0 = \widetilde{\sigma}_\infty, \qquad
r' = r \sigma_\infty = (\omega' i, \omega', \varpi')\]
LaTeX source
\[
g_0 = \widetilde{\sigma}_\infty, \qquad
r' = r \sigma_\infty = (\omega' i, \omega', \varpi')
\]\[(41)\quad
\psi_\varepsilon^{\omega' i, \omega'}
= \overbrace{\psi_\varepsilon^{i,\omega} \circ \widetilde{\sigma}_\infty}^{\widetilde{\sigma}_{?} \circ \psi_\varepsilon^{i,\omega} =}\]
LaTeX source
\[
(41)\quad
\psi_\varepsilon^{\omega' i, \omega'}
= \overbrace{\psi_\varepsilon^{i,\omega} \circ \widetilde{\sigma}_\infty}^{\widetilde{\sigma}_{?} \circ \psi_\varepsilon^{i,\omega} =}
\]\[\psi_r = \psi_i^{\omega,\varepsilon}
= \pi_1(\underbrace{u_{i,\omega,\varepsilon}}_{u_r} ; Q_\infty)\]
LaTeX source
\[
\psi_r = \psi_i^{\omega,\varepsilon}
= \pi_1(\underbrace{u_{i,\omega,\varepsilon}}_{u_r} ; Q_\infty)
\]\[(\infty,\ \omega_0 = +1,\ \varpi_0 = +1 \text{ donc } \varepsilon = \omega_0 \wedge \varpi_0 = +1)\]
LaTeX source
\[
(\infty,\ \omega_0 = +1,\ \varpi_0 = +1 \text{ donc } \varepsilon = \omega_0 \wedge \varpi_0 = +1)
\]\[\psi_{r'} = \psi_r \circ \pi_1(g_0 ; Q_\infty) \qquad \text{si } r' = r \circ g_0\]
LaTeX source
\[
\psi_{r'} = \psi_r \circ \pi_1(g_0 ; Q_\infty) \qquad \text{si } r' = r \circ g_0
\]\[(39)\quad
\left\{
\begin{array}{l}
\psi_i^{\omega,\varepsilon'} = \tau \circ \psi_i^{\omega,\varepsilon}
= \psi_i^{\omega,\varepsilon} \circ \tau_\infty \\[4pt]
\psi_i^{\omega',\varepsilon'} = \sigma_i \circ \psi_i^{\omega,\varepsilon}
= \psi_i^{\omega,\varepsilon} \circ \sigma_\infty
\end{array}
\right.\]
LaTeX source
\[
(39)\quad
\left\{
\begin{array}{l}
\psi_i^{\omega,\varepsilon'} = \tau \circ \psi_i^{\omega,\varepsilon}
= \psi_i^{\omega,\varepsilon} \circ \tau_\infty \\[4pt]
\psi_i^{\omega',\varepsilon'} = \sigma_i \circ \psi_i^{\omega,\varepsilon}
= \psi_i^{\omega,\varepsilon} \circ \sigma_\infty
\end{array}
\right.
\]\[(40)\quad
\psi_i^{\omega',\varepsilon}
= \widetilde{\sigma}_i \circ \psi_i^{\omega,\varepsilon}
= \psi_i^{\omega,\varepsilon} \circ \widetilde{\sigma}_\infty\]
LaTeX source
\[
(40)\quad
\psi_i^{\omega',\varepsilon}
= \widetilde{\sigma}_i \circ \psi_i^{\omega,\varepsilon}
= \psi_i^{\omega,\varepsilon} \circ \widetilde{\sigma}_\infty
\]\[\widetilde{\Sigma}_r = \widetilde{\Sigma}_i^{\omega,\varepsilon}\]
LaTeX source
\[
\widetilde{\Sigma}_r = \widetilde{\Sigma}_i^{\omega,\varepsilon}
\]\[P_\varepsilon Q_{\omega' i} R_i^{\omega} S_i^{\varepsilon}
\simeq P_{+} Q_\infty R_0^{+} S_0^{+} .\]
LaTeX source
\[
P_\varepsilon Q_{\omega' i} R_i^{\omega} S_i^{\varepsilon}
\simeq P_{+} Q_\infty R_0^{+} S_0^{+} .
\]\[\tau(\Sigma_r), \quad \widetilde{\sigma}_i(\Sigma_r), \quad
\widetilde{\sigma}_{\omega i}(\Sigma_r)\]
LaTeX source
\[
\tau(\Sigma_r), \quad \widetilde{\sigma}_i(\Sigma_r), \quad
\widetilde{\sigma}_{\omega i}(\Sigma_r)
\]\[(41)\quad
\widetilde{\Sigma}_r = \widetilde{\Sigma}_i^{\omega,\varepsilon}
= \widetilde{D}_r \cup \tau(\widetilde{D}_r) \cup \widetilde{\sigma}_i(\widetilde{D}_r)
\cup \widetilde{\sigma}_{\omega i}(\Sigma_r)\]
LaTeX source
\[
(41)\quad
\widetilde{\Sigma}_r = \widetilde{\Sigma}_i^{\omega,\varepsilon}
= \widetilde{D}_r \cup \tau(\widetilde{D}_r) \cup \widetilde{\sigma}_i(\widetilde{D}_r)
\cup \widetilde{\sigma}_{\omega i}(\Sigma_r)
\]\[P_\varepsilon Q_{\omega' i} R_{\omega' i}^{\omega} S_i^{\varepsilon} \ldots
P_{\varepsilon'} \ldots Q_i R_{\omega' i}^{\omega'} S_{\omega' i}^{\varepsilon} P_\varepsilon\]
LaTeX source
\[
P_\varepsilon Q_{\omega' i} R_{\omega' i}^{\omega} S_i^{\varepsilon} \ldots
P_{\varepsilon'} \ldots Q_i R_{\omega' i}^{\omega'} S_{\omega' i}^{\varepsilon} P_\varepsilon
\]\[P_+\,Q_1\,R_0^-\,S_0^+\,R_0^+\,S_0^-\,P_-\,Q_\infty\,R_1^-\,S_1^+\,P_+ .\]
LaTeX source
\[ P_+\,Q_1\,R_0^-\,S_0^+\,R_0^+\,S_0^-\,P_-\,Q_\infty\,R_1^-\,S_1^+\,P_+ . \]
\[\Pi_r = \Pi_i^{\omega,\varepsilon} = \pi_1(\widetilde{\Sigma};\widetilde{\Sigma}_r) = \pi_1(\Sigma^{*};\Sigma^{*}_r)\]
LaTeX source
\[
\Pi_r = \Pi_i^{\omega,\varepsilon} = \pi_1(\widetilde{\Sigma};\widetilde{\Sigma}_r) = \pi_1(\Sigma^{*};\Sigma^{*}_r)
\]\[\text{(42)}\qquad \Psi_r : \Pi_{0,3} \longrightarrow \Pi_r = \Pi_i^{\omega,i} = \pi_1(\widetilde{\Sigma};\widetilde{\Sigma}_r)\]
LaTeX source
\[
\text{(42)}\qquad \Psi_r : \Pi_{0,3} \longrightarrow \Pi_r = \Pi_i^{\omega,i} = \pi_1(\widetilde{\Sigma};\widetilde{\Sigma}_r)
\]\[\text{(43)}\qquad \Psi_i^{\omega} : \Pi_{0,3} \xrightarrow{\ \sim\ } \pi_1(\widetilde{\Sigma},R_i^{\omega})\]
LaTeX source
\[
\text{(43)}\qquad \Psi_i^{\omega} : \Pi_{0,3} \xrightarrow{\ \sim\ } \pi_1(\widetilde{\Sigma},R_i^{\omega})
\]\[\text{(44)}\]
LaTeX source
\[\text{(44)}\]\[\Pi_i^{\omega} = \pi_1(\widetilde{\Sigma},R^{\omega}_{\omega i}) \quad\text{à}\quad \Pi_i^{\omega'} = \pi_1(\widetilde{\Sigma},R^{\omega'}_{\omega' i}),\]
LaTeX source
\[
\Pi_i^{\omega} = \pi_1(\widetilde{\Sigma},R^{\omega}_{\omega i}) \quad\text{à}\quad \Pi_i^{\omega'} = \pi_1(\widetilde{\Sigma},R^{\omega'}_{\omega' i}),
\]\[\text{(45)}\qquad \widetilde{b}_i^{\omega}\bigl(\Psi_i^{\omega}(x)\bigr) = \Psi_i^{\omega'}\bigl(\sigma_\infty(x)\bigr) .\]
LaTeX source
\[
\text{(45)}\qquad \widetilde{b}_i^{\omega}\bigl(\Psi_i^{\omega}(x)\bigr) = \Psi_i^{\omega'}\bigl(\sigma_\infty(x)\bigr) .
\]\[\text{(1)}\qquad \Pi_1(X) \longrightarrow \widehat{\Pi}_1(X)\]
LaTeX source
\[
\text{(1)}\qquad \Pi_1(X) \longrightarrow \widehat{\Pi}_1(X)
\]\[\text{(2)}\qquad
\underbrace{\operatorname{Aut}_{\Pi_1(X)}(x)}_{\overset{\text{déf}}{=}\ \pi_1(X,x)} \longrightarrow \underbrace{\operatorname{Aut}_{\widehat{\Pi}_1(X)}(x)}_{\overset{\text{déf}}{=}\ \widehat{\pi}_1(X_{\mathrm{sch}},x)}\]
LaTeX source
\[
\text{(2)}\qquad
\underbrace{\operatorname{Aut}_{\Pi_1(X)}(x)}_{\overset{\text{déf}}{=}\ \pi_1(X,x)} \longrightarrow \underbrace{\operatorname{Aut}_{\widehat{\Pi}_1(X)}(x)}_{\overset{\text{déf}}{=}\ \widehat{\pi}_1(X_{\mathrm{sch}},x)}
\]\[\text{(3)}\qquad \pi_1(X_{\mathrm{sch}},x) \simeq \widehat{\pi}_1(X,x) .\]
LaTeX source
\[
\text{(3)}\qquad \pi_1(X_{\mathrm{sch}},x) \simeq \widehat{\pi}_1(X,x) .
\]\[\operatorname{Hom}_{\Pi_1(X)}(x,y) \longrightarrow \operatorname{Hom}_{\widehat{\Pi}_1(X)}(x,y)\]
LaTeX source
\[
\operatorname{Hom}_{\Pi_1(X)}(x,y) \longrightarrow \operatorname{Hom}_{\widehat{\Pi}_1(X)}(x,y)
\]\[\pi_1(X,y) \to \widehat{\pi}_1(X,y), \qquad \pi_1(X,x) \to \widehat{\pi}_1(X,x)\]
LaTeX source
\[
\pi_1(X,y) \to \widehat{\pi}_1(X,y), \qquad \pi_1(X,x) \to \widehat{\pi}_1(X,x)
\]\[\text{(5)}\qquad \Gamma = \Gamma_K \overset{\text{déf}}{=} \operatorname{Aut}_{K\text{-cat}}(\mathbb{C}),\]
LaTeX source
\[
\text{(5)}\qquad \Gamma = \Gamma_K \overset{\text{déf}}{=} \operatorname{Aut}_{K\text{-cat}}(\mathbb{C}),
\]\[{}^{u}\lambda : {}^{u}x \longrightarrow {}^{u}y \quad\text{si}\quad \lambda : x \to y \ \ (\text{dans } \widehat{\Pi}_1(X)) .\]
LaTeX source
\[
{}^{u}\lambda : {}^{u}x \longrightarrow {}^{u}y \quad\text{si}\quad \lambda : x \to y \ \ (\text{dans } \widehat{\Pi}_1(X)) .
\]\[\text{(6)}\qquad
\begin{cases}
u(\mathrm{id}_x) = \mathrm{id}_{{}^{u}x} & (x \in X)\\
u(\mu\lambda) = {}^{u}\mu\,{}^{u}\lambda & \Bigl(\begin{array}{l} x \xrightarrow{\lambda} y \xrightarrow{\mu} z \\ {}^{u}x \xrightarrow{{}^{u}\lambda} {}^{u}y \xrightarrow{{}^{u}\mu} {}^{u}z \end{array}\Bigr)
\end{cases}\]
LaTeX source
\[
\text{(6)}\qquad
\begin{cases}
u(\mathrm{id}_x) = \mathrm{id}_{{}^{u}x} & (x \in X)\\
u(\mu\lambda) = {}^{u}\mu\,{}^{u}\lambda & \Bigl(\begin{array}{l} x \xrightarrow{\lambda} y \xrightarrow{\mu} z \\ {}^{u}x \xrightarrow{{}^{u}\lambda} {}^{u}y \xrightarrow{{}^{u}\mu} {}^{u}z \end{array}\Bigr)
\end{cases}
\]\[\text{(7)}\qquad \overline{\Gamma} = \operatorname{Aut}_{K\text{-cat}}(\overline{K}) = \operatorname{Gal}_{\overline{K}/K} ,\]
LaTeX source
\[
\text{(7)}\qquad \overline{\Gamma} = \operatorname{Aut}_{K\text{-cat}}(\overline{K}) = \operatorname{Gal}_{\overline{K}/K} ,
\]\[\text{(*)}\qquad {}^{u}l : {}^{u}x = x \longrightarrow {}^{u}y = y ,\]
LaTeX source
\[
\text{(*)}\qquad {}^{u}l : {}^{u}x = x \longrightarrow {}^{u}y = y ,
\]\[\text{(8)}\qquad
\begin{cases}
{}^{u}l = g_l(u)\circ l = l \circ f_l(u) \\
g_l(u) \in \widehat{\pi}_1(X,y) \\
f_l(u) \in \widehat{\pi}_1(X,x)
\end{cases}\]
LaTeX source
\[
\text{(8)}\qquad
\begin{cases}
{}^{u}l = g_l(u)\circ l = l \circ f_l(u) \\
g_l(u) \in \widehat{\pi}_1(X,y) \\
f_l(u) \in \widehat{\pi}_1(X,x)
\end{cases}
\]\[\text{(9)}\qquad
\begin{cases}
f_l(u) = l^{-1}\cdot{}^{u}l , & g_l(u) = {}^{u}l\cdot l^{-1} \\
g_l(u) = l\bigl(f_l(u)\bigr) , & f_l(u) = l^{-1}\bigl(g_l(u)\bigr)
\end{cases}\]
LaTeX source
\[
\text{(9)}\qquad
\begin{cases}
f_l(u) = l^{-1}\cdot{}^{u}l , & g_l(u) = {}^{u}l\cdot l^{-1} \\
g_l(u) = l\bigl(f_l(u)\bigr) , & f_l(u) = l^{-1}\bigl(g_l(u)\bigr)
\end{cases}
\]\[x \xrightarrow{\ l'\ } y \xrightarrow{\ l\ } z\]
LaTeX source
\[
x \xrightarrow{\ l'\ } y \xrightarrow{\ l\ } z
\]\[\text{(10)}\qquad g_{ll'}(u) = g_l(u)\cdot l\bigl(g_{l'}(u)\bigr) \quad\text{soit}\quad g_u(ll') = g_u(l)\cdot l\bigl(g_u(l')\bigr)\]
LaTeX source
\[
\text{(10)}\qquad g_{ll'}(u) = g_l(u)\cdot l\bigl(g_{l'}(u)\bigr) \quad\text{soit}\quad g_u(ll') = g_u(l)\cdot l\bigl(g_u(l')\bigr)
\]\[\text{(11)}\qquad f_{ll'}(u) = l'^{-1}\bigl(f_l(u)\bigr)\cdot f_{l'}(u) \quad\text{i.e.}\quad f_u(ll') = l'^{-1}f_u(l)\cdot f_u(l')\]
LaTeX source
\[
\text{(11)}\qquad f_{ll'}(u) = l'^{-1}\bigl(f_l(u)\bigr)\cdot f_{l'}(u) \quad\text{i.e.}\quad f_u(ll') = l'^{-1}f_u(l)\cdot f_u(l')
\]\[\text{(12)}\qquad \text{\struck{$g_l : \Gamma \longrightarrow \widehat{\pi}_1(X,y)$}}\]
LaTeX source
\[
\text{(12)}\qquad \text{\struck{$g_l : \Gamma \longrightarrow \widehat{\pi}_1(X,y)$}}
\]\[x_0 \xrightarrow{\ l_1\ } x_1 \xrightarrow{\ l_2\ } \cdots \; x_{n-1} \xrightarrow{\ l_n\ } x_n\]
LaTeX source
\[
x_0 \xrightarrow{\ l_1\ } x_1 \xrightarrow{\ l_2\ } \cdots \; x_{n-1} \xrightarrow{\ l_n\ } x_n
\]\[\text{(12)}\qquad g_{l_n l_{n-1}\cdots l_1}(u) = g_{l_n}(u)\cdot l_n\bigl(g_{l_{n-1}}(u)\bigr)\cdot l_n l_{n-1}\bigl(g_{l_{n-2}}(u)\bigr)\cdots\]
LaTeX source
\[
\text{(12)}\qquad g_{l_n l_{n-1}\cdots l_1}(u) = g_{l_n}(u)\cdot l_n\bigl(g_{l_{n-1}}(u)\bigr)\cdot l_n l_{n-1}\bigl(g_{l_{n-2}}(u)\bigr)\cdots
\]\[\cdots (l_n\cdots l_2)\,g_{l_1}(u) .\]
LaTeX source
\[
\cdots (l_n\cdots l_2)\,g_{l_1}(u) .
\]\[\text{(13)}\qquad p : T \longrightarrow X\]
LaTeX source
\[
\text{(13)}\qquad p : T \longrightarrow X
\]\[\text{(14)}\qquad \text{\struck{$\Pi_1(X;$}}\ \pi_1(X;T) = \pi\]
LaTeX source
\[
\text{(14)}\qquad \text{\struck{$\Pi_1(X;$}}\ \pi_1(X;T) = \pi
\]\[\text{(15)}\qquad \varphi_x : \pi \xrightarrow{\ \sim\ } \pi_1\bigl(X,p(x)\bigr)\]
LaTeX source
\[
\text{(15)}\qquad \varphi_x : \pi \xrightarrow{\ \sim\ } \pi_1\bigl(X,p(x)\bigr)
\]\[\text{(16)}\qquad l_{y,x} : p(x) \longrightarrow p(y) \quad\text{dans } \Pi_1(X)\]
LaTeX source
\[
\text{(16)}\qquad l_{y,x} : p(x) \longrightarrow p(y) \quad\text{dans } \Pi_1(X)
\]\[\text{(17)}\qquad g^{T/X}_{y,x}(u) = g^{p}_{y,x}(u) = \varphi_y^{-1}\bigl(g_{l_{y,x}}(u)\bigr) = \varphi_x^{-1}\bigl(f_{l_{y,x}}(u)\bigr) \qquad \bigl(\in \widehat{\pi},\ \pi = \pi_1(X;T)\bigr) .\]
LaTeX source
\[
\text{(17)}\qquad g^{T/X}_{y,x}(u) = g^{p}_{y,x}(u) = \varphi_y^{-1}\bigl(g_{l_{y,x}}(u)\bigr) = \varphi_x^{-1}\bigl(f_{l_{y,x}}(u)\bigr) \qquad \bigl(\in \widehat{\pi},\ \pi = \pi_1(X;T)\bigr) .
\]\[\text{(18)}\qquad g_{zy}(u)\,g_{yx}(u) = g_{zx}(u) \qquad x,y,z \in T_K\]
LaTeX source
\[
\text{(18)}\qquad g_{zy}(u)\,g_{yx}(u) = g_{zx}(u) \qquad x,y,z \in T_K
\]\[\text{(19)}\qquad g_{x_n,x_0} = g_{x_n,x_{n-1}}\,g_{x_{n-1},x_{n-2}}\cdots g_{x_1,x_0}\]
LaTeX source
\[
\text{(19)}\qquad g_{x_n,x_0} = g_{x_n,x_{n-1}}\,g_{x_{n-1},x_{n-2}}\cdots g_{x_1,x_0}
\]\[\text{(20)}\qquad f_l(u) = \varphi_x\bigl(g^{T}_{y_0,x_0}(u)\bigr), \qquad g_l(u) = \varphi_y\bigl(g^{T}_{y_0,x_0}(u)\bigr)\]
LaTeX source
\[
\text{(20)}\qquad f_l(u) = \varphi_x\bigl(g^{T}_{y_0,x_0}(u)\bigr), \qquad g_l(u) = \varphi_y\bigl(g^{T}_{y_0,x_0}(u)\bigr)
\]\[\text{\struck{$x_0 = 0 \in T$, $y_0$}} \quad x_0 = 0,\ y_0 = 1 \in T = [0,1] .\]
LaTeX source
\[
\text{\struck{$x_0 = 0 \in T$, $y_0$}} \quad x_0 = 0,\ y_0 = 1 \in T = [0,1] .
\]\[\text{(21)}\]
LaTeX source
\[\text{(21)}\]\[f_K : T_K \longrightarrow T'_K ,\]
LaTeX source
\[ f_K : T_K \longrightarrow T'_K , \]
\[\text{(22)}\qquad \pi = \pi_1(X;T/X) \xrightarrow{\ \psi = \pi_1(f)\ } \pi' = \pi_1(X,T'/X)\]
LaTeX source
\[
\text{(22)}\qquad \pi = \pi_1(X;T/X) \xrightarrow{\ \psi = \pi_1(f)\ } \pi' = \pi_1(X,T'/X)
\]\[\text{(23)}\qquad g^{T'}_{y',x'}(u) = \psi\bigl(g^{T}_{y,x}(u)\bigr)\]
LaTeX source
\[
\text{(23)}\qquad g^{T'}_{y',x'}(u) = \psi\bigl(g^{T}_{y,x}(u)\bigr)
\]\[\bigl(x' = f(x),\ y' = f(y),\ \psi = \pi_1(f)\bigr)\]
LaTeX source
\[ \bigl(x' = f(x),\ y' = f(y),\ \psi = \pi_1(f)\bigr) \]
\[\text{\struck{$g^{\alpha} : T_{\alpha K} \times T_{\alpha K} \to$}}\]
LaTeX source
\[
\text{\struck{$g^{\alpha} : T_{\alpha K} \times T_{\alpha K} \to$}}
\]\[\text{(24)}\qquad \pi_\alpha \overset{\text{déf}}{=} \pi_1(X, T_\alpha)\]
LaTeX source
\[
\text{(24)}\qquad \pi_\alpha \overset{\text{déf}}{=} \pi_1(X, T_\alpha)
\]\[\text{(25)}\qquad
\left\{
\begin{array}{l}
T_{\alpha K} \times T_{\alpha K} \times \Gamma \longrightarrow \widehat{\pi}_\alpha \\
(x,y,u) \longmapsto g^{T_\alpha}_{y,x}(u) \overset{\text{déf}}{=} g^{\alpha}_{y,x}(u)
\end{array}
\right.\]
LaTeX source
\[
\text{(25)}\qquad
\left\{
\begin{array}{l}
T_{\alpha K} \times T_{\alpha K} \times \Gamma \longrightarrow \widehat{\pi}_\alpha \\
(x,y,u) \longmapsto g^{T_\alpha}_{y,x}(u) \overset{\text{déf}}{=} g^{\alpha}_{y,x}(u)
\end{array}
\right.
\]\[\text{(26)}\qquad \text{\struck{$\ill{}$}}\ \ \varphi_{\beta\alpha} : \pi_\beta \longrightarrow \pi_\alpha\]
LaTeX source
\[
\text{(26)}\qquad \text{\struck{$\ill{}$}}\ \ \varphi_{\beta\alpha} : \pi_\beta \longrightarrow \pi_\alpha
\]\[\text{(27)}\qquad g^{\beta}_{y,x}(u) = \varphi_{\beta\alpha}\bigl(g^{\alpha}_{y,x}(u)\bigr) \qquad x, y \in T_{\alpha K},\ u \in \Gamma\]
LaTeX source
\[
\text{(27)}\qquad g^{\beta}_{y,x}(u) = \varphi_{\beta\alpha}\bigl(g^{\alpha}_{y,x}(u)\bigr) \qquad x, y \in T_{\alpha K},\ u \in \Gamma
\]\[\text{(28)}\qquad \forall \alpha, \beta \in I,\ \ T_\alpha \cap T_\beta = \bigcup_{\gamma \leq \alpha,\beta} T_\gamma\]
LaTeX source
\[
\text{(28)}\qquad \forall \alpha, \beta \in I,\ \ T_\alpha \cap T_\beta = \bigcup_{\gamma \leq \alpha,\beta} T_\gamma
\]\[\text{\struck{$i_0 = i,\ i_1, \ldots, i_n = j$}}\]
LaTeX source
\[
\text{\struck{$i_0 = i,\ i_1, \ldots, i_n = j$}}
\]\[g^{\alpha}_{y,x}(u) \in \widehat{\pi}_\alpha \qquad (\alpha \in A,\ y, x \in T_\alpha)\]
LaTeX source
\[
g^{\alpha}_{y,x}(u) \in \widehat{\pi}_\alpha \qquad (\alpha \in A,\ y, x \in T_\alpha)
\]\[I_\alpha \subset T_\alpha \quad \text{partie de } T_\alpha \ (\text{\uncertain{non vide}, \uncertain{finie}}),\]
LaTeX source
\[
I_\alpha \subset T_\alpha \quad \text{partie de } T_\alpha \ (\text{\uncertain{non vide}, \uncertain{finie}}),
\]\[\text{(28)}\qquad {}^{uv}l = {}^{u}({}^{v}l) \qquad u, v \in \Gamma,\ l : x \to y \ \text{chemin dans } \Pi_1(X)\]
LaTeX source
\[
\text{(28)}\qquad {}^{uv}l = {}^{u}({}^{v}l) \qquad u, v \in \Gamma,\ l : x \to y \ \text{chemin dans } \Pi_1(X)
\]\[{}^{v}l = g_l(v)\cdot l\]
LaTeX source
\[
{}^{v}l = g_l(v)\cdot l
\]\[{}^{u}({}^{v}l) = {}^{u}\{g_l(v)\}\cdot\underbrace{{}^{u}l}_{g_l(u)\cdot l} = {}^{u}g_l(v)\,g_l(u)\cdot l\]
LaTeX source
\[
{}^{u}({}^{v}l) = {}^{u}\{g_l(v)\}\cdot\underbrace{{}^{u}l}_{g_l(u)\cdot l} = {}^{u}g_l(v)\,g_l(u)\cdot l
\]\[\text{(29)}\qquad
\left|\begin{array}{l}
g_l(uv) = {}^{u}g_l(v)\cdot g_l(u) \quad\text{soit}\\
g_l^{-1}(uv) = g_l^{-1}(u)\cdot{}^{u}g_l^{-1}(v)
\end{array}\right.\]
LaTeX source
\[
\text{(29)}\qquad
\left|\begin{array}{l}
g_l(uv) = {}^{u}g_l(v)\cdot g_l(u) \quad\text{soit}\\
g_l^{-1}(uv) = g_l^{-1}(u)\cdot{}^{u}g_l^{-1}(v)
\end{array}\right.
\]\[\text{(30)}\qquad f_l(uv) = f_l(u)\cdot{}^{u}f_l(v)\]
LaTeX source
\[
\text{(30)}\qquad f_l(uv) = f_l(u)\cdot{}^{u}f_l(v)
\]\[\widehat{\pi}_1(X,x) \xrightarrow{\ \pi_1(l)\ } \widehat{\pi}_1(X,y) \quad \text{induit par } l \ldots\]
LaTeX source
\[
\widehat{\pi}_1(X,x) \xrightarrow{\ \pi_1(l)\ } \widehat{\pi}_1(X,y) \quad \text{induit par } l \ldots
\]\[l' = la = bl \qquad a \in \pi_1(X,x),\ b \in \pi_1(X,y)\]
LaTeX source
\[ l' = la = bl \qquad a \in \pi_1(X,x),\ b \in \pi_1(X,y) \]
\[\text{(31)}\qquad
\left\{
\begin{array}{l}
f_{l'}(u) = \operatorname{int}(a^{-1})\,f_l(u)\,\underbrace{f_a(u)}_{a^{-1}\cdot{}^{u}a} = a^{-1}\cdot f_l(u)\cdot{}^{u}a \\[1ex]
g_{l'}(u) = \underbrace{g_b(u)}_{{}^{u}b\cdot b^{-1}}\,\operatorname{int}(b)\,g_l(u) = {}^{u}b\,g_l(u)\,b^{-1}
\end{array}
\right.\]
LaTeX source
\[
\text{(31)}\qquad
\left\{
\begin{array}{l}
f_{l'}(u) = \operatorname{int}(a^{-1})\,f_l(u)\,\underbrace{f_a(u)}_{a^{-1}\cdot{}^{u}a} = a^{-1}\cdot f_l(u)\cdot{}^{u}a \\[1ex]
g_{l'}(u) = \underbrace{g_b(u)}_{{}^{u}b\cdot b^{-1}}\,\operatorname{int}(b)\,g_l(u) = {}^{u}b\,g_l(u)\,b^{-1}
\end{array}
\right.
\]\[\bigl(\text{i.e.}\ \ g^{-1}_{l'}(u) = b\,g^{-1}_l(u)\,{}^{u}b^{-1}\bigr)\]
LaTeX source
\[
\bigl(\text{i.e.}\ \ g^{-1}_{l'}(u) = b\,g^{-1}_l(u)\,{}^{u}b^{-1}\bigr)
\]\[\text{(32)}\qquad
\left\{
\begin{array}{l}
g_{y,x} \in H^1\bigl(\Gamma, \widehat{\pi}_1(X,y)\bigr) \\
f_{y,x} \in H^1_{\mathrm{dr}}\bigl(\Gamma, \widehat{\pi}_1(X,x)\bigr)
\end{array}
\right.\]
LaTeX source
\[
\text{(32)}\qquad
\left\{
\begin{array}{l}
g_{y,x} \in H^1\bigl(\Gamma, \widehat{\pi}_1(X,y)\bigr) \\
f_{y,x} \in H^1_{\mathrm{dr}}\bigl(\Gamma, \widehat{\pi}_1(X,x)\bigr)
\end{array}
\right.
\]\[\widehat{\pi}_1(X,x) \xrightarrow[\text{ext}]{\ \text{isom}\ } \widehat{\pi}_1(Y,y)\]
LaTeX source
\[
\widehat{\pi}_1(X,x) \xrightarrow[\text{ext}]{\ \text{isom}\ } \widehat{\pi}_1(Y,y)
\]\[\text{(33)}\qquad
\left\{
\begin{array}{l}
f_l : \Gamma \longrightarrow \widehat{\pi}_1(X,x) \\
g_l : \Gamma \longrightarrow \widehat{\pi}_1(Y,y)
\end{array}
\right.
\qquad l : x \to y \ \ (\text{dans } \Pi_1(X))\]
LaTeX source
\[
\text{(33)}\qquad
\left\{
\begin{array}{l}
f_l : \Gamma \longrightarrow \widehat{\pi}_1(X,x) \\
g_l : \Gamma \longrightarrow \widehat{\pi}_1(Y,y)
\end{array}
\right.
\qquad l : x \to y \ \ (\text{dans } \Pi_1(X))
\]\[f_{x_0,x} \in H^1_{\mathrm{dr}}\bigl(\Gamma, \underbrace{\widehat{\pi}_1(X,x_0)}_{\widehat{\pi}(x_0)}\bigr),\]
LaTeX source
\[
f_{x_0,x} \in H^1_{\mathrm{dr}}\bigl(\Gamma, \underbrace{\widehat{\pi}_1(X,x_0)}_{\widehat{\pi}(x_0)}\bigr),
\]\[f_l : \Gamma \longrightarrow \widehat{\pi}(x_0)\]
LaTeX source
\[
f_l : \Gamma \longrightarrow \widehat{\pi}(x_0)
\]\[(34) \qquad (f_{x_0, x})_{\mathrm{ab}} \in H^1\bigl(\Gamma, \hat{\pi}_1(X, x_0)_{\mathrm{ab}}\bigr),\]
LaTeX source
\[
(34) \qquad (f_{x_0, x})_{\mathrm{ab}} \in H^1\bigl(\Gamma, \hat{\pi}_1(X, x_0)_{\mathrm{ab}}\bigr),
\]\[(35) \qquad U_{0,3} = \mathbb{P}^1 \setminus \{0, 1, \infty\}.\]
LaTeX source
\[
(35) \qquad U_{0,3} = \mathbb{P}^1 \setminus \{0, 1, \infty\}.
\]\[(36) \qquad f : X \to Y ;\]
LaTeX source
\[ (36) \qquad f : X \to Y ; \]
\[(37) \qquad \Pi_1(X) \xrightarrow{\; f_{*} = \Pi_1(f) \;} \Pi_1(Y),\]
LaTeX source
\[
(37) \qquad \Pi_1(X) \xrightarrow{\; f_{*} = \Pi_1(f) \;} \Pi_1(Y),
\]\[(38) \qquad \hat{\Pi}_1(X) \xrightarrow{\; \hat{f} = \hat{\Pi}_1(f) \;} \hat{\Pi}_1(Y),\]
LaTeX source
\[
(38) \qquad \hat{\Pi}_1(X) \xrightarrow{\; \hat{f} = \hat{\Pi}_1(f) \;} \hat{\Pi}_1(Y),
\]\[(39) \qquad \hat{f}({}^{u}\ell) = {}^{u}(\hat{f}\ell)\]
LaTeX source
\[
(39) \qquad \hat{f}({}^{u}\ell) = {}^{u}(\hat{f}\ell)
\]\[(40) \qquad
\begin{cases}
\hat{f}\bigl(f_{\ell}(u)\bigr) = f_{\hat{f}(\ell)}(u) \\
\hat{f}\bigl(g_{\ell}(u)\bigr) = g_{\hat{f}(\ell)}(u) .
\end{cases}\]
LaTeX source
\[
(40) \qquad
\begin{cases}
\hat{f}\bigl(f_{\ell}(u)\bigr) = f_{\hat{f}(\ell)}(u) \\
\hat{f}\bigl(g_{\ell}(u)\bigr) = g_{\hat{f}(\ell)}(u) .
\end{cases}
\]\[(41) \qquad \boxed{\mathrm{Hom}_{\hat{\Pi}_1(X, I)}(x_0, x_i)}, \qquad i \in I,\]
LaTeX source
\[
(41) \qquad \boxed{\mathrm{Hom}_{\hat{\Pi}_1(X, I)}(x_0, x_i)}, \qquad i \in I,
\]\[(42) \qquad f_{\ell_i}(u), \qquad i \in I,\ u \in \Gamma,\]
LaTeX source
\[
(42) \qquad f_{\ell_i}(u), \qquad i \in I,\ u \in \Gamma,
\]\[(43) \qquad f_{\lambda_j}(u) \ \text{ou}\ g_{\lambda_j}(u), \qquad j \in J,\ u \in \Gamma .\]
LaTeX source
\[
(43) \qquad f_{\lambda_j}(u) \ \text{ou}\ g_{\lambda_j}(u), \qquad j \in J,\ u \in \Gamma .
\]\[\mathrm{Hom}_{\hat{\Pi}_1(C)}(x, y) \longrightarrow \mathrm{Hom}_{\hat{\Pi}_1(U_{0,3})}(x, y)\]
LaTeX source
\[
\mathrm{Hom}_{\hat{\Pi}_1(C)}(x, y) \longrightarrow \mathrm{Hom}_{\hat{\Pi}_1(U_{0,3})}(x, y)
\]\[\hat{\Pi}_1(C, I) \longrightarrow \hat{\Pi}_1(X, I),\]
LaTeX source
\[
\hat{\Pi}_1(C, I) \longrightarrow \hat{\Pi}_1(X, I),
\]\[\hat{\pi}_1(C, x_0) \subset \hat{\pi}_1\bigl(U_{0,3}, f(x_0)\bigr)\]
LaTeX source
\[
\hat{\pi}_1(C, x_0) \subset \hat{\pi}_1\bigl(U_{0,3}, f(x_0)\bigr)
\]\[\hat{\pi}_1(C, x_0) \longrightarrow \hat{\pi}_1(X, x_0) ;\]
LaTeX source
\[
\hat{\pi}_1(C, x_0) \longrightarrow \hat{\pi}_1(X, x_0) ;
\]\[(45) \qquad \mathcal{C}' \longrightarrow \tilde{\mathcal{C}}'\]
LaTeX source
\[
(45) \qquad \mathcal{C}' \longrightarrow \tilde{\mathcal{C}}'
\]\[\pi_1(\tilde{\mathcal{C}}, x_0') \hookrightarrow \pi_1(\mathcal{C}, x_0) = \Pi_0,\]
LaTeX source
\[
\pi_1(\tilde{\mathcal{C}}, x_0') \hookrightarrow \pi_1(\mathcal{C}, x_0) = \Pi_0,
\]\[(45) \qquad \mathrm{Ob}\,\tilde{\mathcal{C}}_{x_i} = H_{x_i, x_0} \wedge^{\Pi_0} \Pi_0/\Pi_0'\]
LaTeX source
\[
(45) \qquad \mathrm{Ob}\,\tilde{\mathcal{C}}_{x_i} = H_{x_i, x_0} \wedge^{\Pi_0} \Pi_0/\Pi_0'
\]\[(46) \qquad \tilde{\Theta}_0(g \cdot x') = \Theta(g)\, \tilde{\Theta}_0(x')\]
LaTeX source
\[
(46) \qquad \tilde{\Theta}_0(g \cdot x') = \Theta(g)\, \tilde{\Theta}_0(x')
\]\[(47) \qquad E_0 \simeq \Pi_0/\Pi_0' ;\]
LaTeX source
\[ (47) \qquad E_0 \simeq \Pi_0/\Pi_0' ; \]
\[(48) \qquad \mathrm{int}\, g\,(\Pi_0') = \Theta(\Pi_0'),\]
LaTeX source
\[
(48) \qquad \mathrm{int}\, g\,(\Pi_0') = \Theta(\Pi_0'),
\]\[(49) \qquad \mathrm{Transp}_{\Pi_0}\bigl(\Pi_0', \Theta(\Pi_0')\bigr)/\Pi_0'\]
LaTeX source
\[
(49) \qquad \mathrm{Transp}_{\Pi_0}\bigl(\Pi_0', \Theta(\Pi_0')\bigr)/\Pi_0'
\]\[\mathcal{C} = \hat{\Pi}_1(X_{\bar K}, I), \qquad I \subset X_K,\]
LaTeX source
\[
\mathcal{C} = \hat{\Pi}_1(X_{\bar K}, I), \qquad I \subset X_K,
\]\[(*) \qquad \hat{\pi}_1(X', x') \longrightarrow \hat{\pi}_1\bigl(Y, f(x')\bigr)\]
LaTeX source
\[
(*) \qquad \hat{\pi}_1(X', x') \longrightarrow \hat{\pi}_1\bigl(Y, f(x')\bigr)
\]\[(50) \qquad
\begin{aligned}
E_0 &\longrightarrow \text{Ens.\ des s-groupes de } \Pi, \\
x' &\longmapsto \text{stabilisateur } \Pi_{x'},
\end{aligned}\]
LaTeX source
\[
(50) \qquad
\begin{aligned}
E_0 &\longrightarrow \text{Ens.\ des s-groupes de } \Pi, \\
x' &\longmapsto \text{stabilisateur } \Pi_{x'},
\end{aligned}
\]\[(51) \qquad E_0/\Pi_0 \overset{\mathrm{def}}{=} \pi_0(E_0) \longrightarrow \Sigma = \mathrm{Ssgr}(\Pi)/\Pi\]
LaTeX source
\[
(51) \qquad E_0/\Pi_0 \overset{\mathrm{def}}{=} \pi_0(E_0) \longrightarrow \Sigma = \mathrm{Ssgr}(\Pi)/\Pi
\]\[(52) \qquad \pi_0(\tilde{\Theta}_0) : \pi_0(E_0) \xrightarrow{\;\sim\;} \pi_0(E_0)\]
LaTeX source
\[
(52) \qquad \pi_0(\tilde{\Theta}_0) : \pi_0(E_0) \xrightarrow{\;\sim\;} \pi_0(E_0)
\]\[\hat{\pi}_1(X', x) \longrightarrow \hat{\pi}_1\bigl(Y, f(x)\bigr) .\]
LaTeX source
\[
\hat{\pi}_1(X', x) \longrightarrow \hat{\pi}_1\bigl(Y, f(x)\bigr) .
\]\[\text{\struck{$I'_1 \cap f^{-1}(I'_2) \longrightarrow$}} \quad
\hat{\Pi}_1(X'_1, J) \longrightarrow \hat{\Pi}_1(X'_2, I'_2)\]
LaTeX source
\[
\text{\struck{$I'_1 \cap f^{-1}(I'_2) \longrightarrow$}} \quad
\hat{\Pi}_1(X'_1, J) \longrightarrow \hat{\Pi}_1(X'_2, I'_2)
\]\[X'_1 \xrightarrow{\;f_1\;} Y, \qquad X'_2 \xrightarrow{\;f_2\;} Y\]
LaTeX source
\[
X'_1 \xrightarrow{\;f_1\;} Y, \qquad X'_2 \xrightarrow{\;f_2\;} Y
\]\[\begin{equation*}
\tag{53} u\, l^{T}_{y';x'} \;=\; g^{T}_{x,y}(u)\; l^{T}_{u(y'),u(x')}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{53} u\, l^{T}_{y';x'} \;=\; g^{T}_{x,y}(u)\; l^{T}_{u(y'),u(x')}
\end{equation*}\[g^{T}_{x',y'}(u) \in \hat\pi_1\bigl(X',\, T(u(x'),u(y'))\bigr)\]
LaTeX source
\[
g^{T}_{x',y'}(u) \in \hat\pi_1\bigl(X',\, T(u(x'),u(y'))\bigr)
\]\[\begin{equation*}
\tag{54} \hat f\bigl(\underbrace{g^{T}_{y';x'}(u)}_{\in\, \hat\pi_1(X,T)}\bigr) \;=\; g^{T}_{y,x}(u)
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{54} \hat f\bigl(\underbrace{g^{T}_{y';x'}(u)}_{\in\, \hat\pi_1(X,T)}\bigr) \;=\; g^{T}_{y,x}(u)
\end{equation*}\[\hat\varphi_\alpha : \hat\pi_1(X'_{\bar K}, T_\alpha) \longrightarrow \hat\pi_1(X, T)\]
LaTeX source
\[
\hat\varphi_\alpha : \hat\pi_1(X'_{\bar K}, T_\alpha) \longrightarrow \hat\pi_1(X, T)
\]\[g^{T}_{y,x}(u) \in \bigcap_{\alpha \in \pi_0(X'_T)} \operatorname{Im} \hat\varphi_\alpha
\qquad \forall u \in \Gamma = \Gamma_{\bar K/K}\]
LaTeX source
\[
g^{T}_{y,x}(u) \in \bigcap_{\alpha \in \pi_0(X'_T)} \operatorname{Im} \hat\varphi_\alpha
\qquad \forall u \in \Gamma = \Gamma_{\bar K/K}
\]\[z \mapsto -z, \qquad z \mapsto \frac{1}{z}, \qquad \text{\struck{\ill{}}}\]
LaTeX source
\[
z \mapsto -z, \qquad z \mapsto \frac{1}{z}, \qquad \text{\struck{\ill{}}}
\]\[1 \longrightarrow \mathbb{F}_2^{\,2} \longrightarrow \mathfrak{A}_4 \longrightarrow \mathbb{Z}/3\mathbb{Z} \longrightarrow 1\]
LaTeX source
\[
1 \longrightarrow \mathbb{F}_2^{\,2} \longrightarrow \mathfrak{A}_4 \longrightarrow \mathbb{Z}/3\mathbb{Z} \longrightarrow 1
\]\[l_\infty\, l_1\, l_0\, l_{-1} = 1\]
LaTeX source
\[
l_\infty\, l_1\, l_0\, l_{-1} = 1
\]\[E_0 \;\text{---}\; \pi_0(E_0) \;\text{\struck{$\simeq E_0/\pi \;\mathrm{Ssgr}($}}\]
LaTeX source
\[
E_0 \;\text{---}\; \pi_0(E_0) \;\text{\struck{$\simeq E_0/\pi \;\mathrm{Ssgr}($}}
\]\[\Sigma \;(= \Gamma \cdot \pi) \supset \pi \;\text{---}\; E_0 \longrightarrow \mathrm{Ssgr}(\pi)/\pi,
\qquad \Sigma/\pi = \Gamma\]
LaTeX source
\[
\Sigma \;(= \Gamma \cdot \pi) \supset \pi \;\text{---}\; E_0 \longrightarrow \mathrm{Ssgr}(\pi)/\pi,
\qquad \Sigma/\pi = \Gamma
\]\[\Sigma_J = \mathbb{P}\bigl(V(J)\bigr) \simeq \check{\mathbb{P}}\bigl(V(J)\bigr)\]
LaTeX source
\[
\Sigma_J = \mathbb{P}\bigl(V(J)\bigr) \simeq \check{\mathbb{P}}\bigl(V(J)\bigr)
\]\[F(1) \simeq \mathcal{O}(\omega)\]
LaTeX source
\[
F(1) \simeq \mathcal{O}(\omega)
\]\[\check{\mathcal{O}}(1) \simeq \check F(\omega)\]
LaTeX source
\[
\check{\mathcal{O}}(1) \simeq \check F(\omega)
\]\[\Omega^1_\Sigma \simeq F(-1) \simeq \mathcal{O}(-2)(\omega), \qquad
\check\Omega^1_\Sigma \simeq \mathcal{O}(2)(\omega) \quad \text{fibré tangent à } \Sigma\]
LaTeX source
\[
\Omega^1_\Sigma \simeq F(-1) \simeq \mathcal{O}(-2)(\omega), \qquad
\check\Omega^1_\Sigma \simeq \mathcal{O}(2)(\omega) \quad \text{fibré tangent à } \Sigma
\]\[\Gamma\bigl(\Sigma_J, \mathcal{O}_\Sigma(1)\bigr) \simeq V(J)
\qquad \text{\struck{$e_j - e_k$ section $\omega_{j,k}$}}\]
LaTeX source
\[
\Gamma\bigl(\Sigma_J, \mathcal{O}_\Sigma(1)\bigr) \simeq V(J)
\qquad \text{\struck{$e_j - e_k$ section $\omega_{j,k}$}}
\]\[\varphi_{jk} = e_k - e_j \in \Gamma\bigl(\Sigma, \mathcal{O}_\Sigma(1)\bigr) \quad \text{nulle en } R_i,
\qquad \varphi_{kj} = -\varphi_{jk}\]
LaTeX source
\[
\varphi_{jk} = e_k - e_j \in \Gamma\bigl(\Sigma, \mathcal{O}_\Sigma(1)\bigr) \quad \text{nulle en } R_i,
\qquad \varphi_{kj} = -\varphi_{jk}
\]\[\varphi_{jk}(R_i) = 0 \qquad
\boxed{\varphi_{jk}(R_k) = \tilde R_k, \quad \varphi_{jk}(R_j) = -\tilde R_j}\]
LaTeX source
\[
\varphi_{jk}(R_i) = 0 \qquad
\boxed{\varphi_{jk}(R_k) = \tilde R_k, \quad \varphi_{jk}(R_j) = -\tilde R_j}
\]\[\tilde Q_i = \varphi_{jk}(Q_i), \qquad \tilde Q'_i = -\varphi_{jk}(Q_i) = \varphi_{kj}(Q_i)\]
LaTeX source
\[
\tilde Q_i = \varphi_{jk}(Q_i), \qquad \tilde Q'_i = -\varphi_{jk}(Q_i) = \varphi_{kj}(Q_i)
\]\[\boxed{Q^\omega_{i} = \varphi_{\omega i, \omega' i}(Q_i)}\]
LaTeX source
\[
\boxed{Q^\omega_{i} = \varphi_{\omega i, \omega' i}(Q_i)}
\]\[\Sigma_n^{\ast\ast} = \Sigma_n \setminus \bigl\{ S(\Sigma_n) \cup A(\Sigma_n) \cup F(\Sigma_n) \bigr\}\]
LaTeX source
\[
\Sigma_n^{\ast\ast} = \Sigma_n \setminus \bigl\{ S(\Sigma_n) \cup A(\Sigma_n) \cup F(\Sigma_n) \bigr\}
\]\[\Sigma_n^{\ast\ast} \xrightarrow{\ \deg n\ } \Sigma_1^{\ast\ast} = \mathbb{P}_1 \setminus \{\underbrace{0, \infty}_{\text{« pôles »}}, 1, -1\}
\xrightarrow{\ \deg 2\ } \Sigma_3^{\ast\cdot} = U_{0,3}\]
LaTeX source
\[
\Sigma_n^{\ast\ast} \xrightarrow{\ \deg n\ } \Sigma_1^{\ast\ast} = \mathbb{P}_1 \setminus \{\underbrace{0, \infty}_{\text{« pôles »}}, 1, -1\}
\xrightarrow{\ \deg 2\ } \Sigma_3^{\ast\cdot} = U_{0,3}
\]\[\Sigma_n^{\ast\ast} \simeq \Sigma_1^{\ast\ast}/D_n \;\; \text{\uncertain{(sic)}}\]
LaTeX source
\[
\Sigma_n^{\ast\ast} \simeq \Sigma_1^{\ast\ast}/D_n \;\; \text{\uncertain{(sic)}}
\]\[\Sigma_{2n}^{\ast\cdot} \longrightarrow \Sigma_1^{\ast\cdot} \xrightarrow{\ 2\ } \Sigma_1^{\ast\cdot} \simeq U_0^3\]
LaTeX source
\[
\Sigma_{2n}^{\ast\cdot} \longrightarrow \Sigma_1^{\ast\cdot} \xrightarrow{\ 2\ } \Sigma_1^{\ast\cdot} \simeq U_0^3
\]\[\Sigma_n^{\ast\ast} \xrightarrow{\ D_n^+\ } \Sigma_1^{\ast\cdot} \simeq U_0^3\]
LaTeX source
\[
\Sigma_n^{\ast\ast} \xrightarrow{\ D_n^+\ } \Sigma_1^{\ast\cdot} \simeq U_0^3
\]\[Q^\omega_i = R_j - R_k \longmapsto R_j - \zeta R_k = P^\omega_i \;\text{\struck{\ill{}}}\; = P^{\omega,\zeta}_i\]
LaTeX source
\[
Q^\omega_i = R_j - R_k \longmapsto R_j - \zeta R_k = P^\omega_i \;\text{\struck{\ill{}}}\; = P^{\omega,\zeta}_i
\]\[P^{\omega,\zeta}_i = R_{\omega i} \;\text{\struck{$\zeta$}}\; - \zeta R_{\omega^2 i} \;\equiv\; -P^{\omega,\zeta}_{\omega^2 i}\]
LaTeX source
\[
P^{\omega,\zeta}_i = R_{\omega i} \;\text{\struck{$\zeta$}}\; - \zeta R_{\omega^2 i} \;\equiv\; -P^{\omega,\zeta}_{\omega^2 i}
\]\[P^{\omega',\zeta'}_i = R_{\omega' i} - \zeta' R_{\omega i} = R_k - \zeta^2 R_j = -\zeta' P^{\omega,\zeta}_i\]
LaTeX source
\[
P^{\omega',\zeta'}_i = R_{\omega' i} - \zeta' R_{\omega i} = R_k - \zeta^2 R_j = -\zeta' P^{\omega,\zeta}_i
\]\[S = S_0 \sqcup S_1 \sqcup S_\infty \subset \mathcal{X}\]
LaTeX source
\[
S = S_0 \sqcup S_1 \sqcup S_\infty \subset \mathcal{X}
\]\[\tau_0(r),\ \tau_1(r),\ \tau_\infty(r),\]
LaTeX source
\[ \tau_0(r),\ \tau_1(r),\ \tau_\infty(r), \]
\[\begin{equation*}
\tag{1}
\begin{cases}
\tau_1(\tau_0(r)) = \rho_\infty(r) \\
\tau_0(\tau_1(r)) = \rho_\infty^{-1}(r)
\end{cases}
\qquad \text{(face conservée)}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{1}
\begin{cases}
\tau_1(\tau_0(r)) = \rho_\infty(r) \\
\tau_0(\tau_1(r)) = \rho_\infty^{-1}(r)
\end{cases}
\qquad \text{(face conservée)}
\end{equation*}\[\begin{equation*}
\tag{2}
\begin{cases}
\tau_\infty \tau_1(r) = \rho_0(r) \\
\tau_1 \tau_\infty(r) = \rho_0^{-1}(r)
\end{cases}
\qquad \text{(sommet conservé)}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{2}
\begin{cases}
\tau_\infty \tau_1(r) = \rho_0(r) \\
\tau_1 \tau_\infty(r) = \rho_0^{-1}(r)
\end{cases}
\qquad \text{(sommet conservé)}
\end{equation*}\[\begin{equation*}
\tag{3}
\tau_0 \tau_\infty(r) = \tau_\infty \tau_0(r) \overset{\text{def}}{=} \rho_1(r)
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{3}
\tau_0 \tau_\infty(r) = \tau_\infty \tau_0(r) \overset{\text{def}}{=} \rho_1(r)
\end{equation*}\[\begin{equation*}
\tag{4}
\tau_0^2 = \tau_1^2 = \tau_\infty^2 = (\tau_0 \tau_\infty)^2 = 1
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{4}
\tau_0^2 = \tau_1^2 = \tau_\infty^2 = (\tau_0 \tau_\infty)^2 = 1
\end{equation*}\[\begin{equation*}
\tag{5}
\begin{cases}
\rho_\infty = \tau_1 \tau_0 \\
\rho_0 = \tau_\infty \tau_1 \\
\rho_1 = \tau_0 \tau_\infty
\end{cases}
\qquad \rho_\infty \rho_1 \rho_0 \;\text{\struck{$\rho_\infty$}}\; = 1
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{5}
\begin{cases}
\rho_\infty = \tau_1 \tau_0 \\
\rho_0 = \tau_\infty \tau_1 \\
\rho_1 = \tau_0 \tau_\infty
\end{cases}
\qquad \rho_\infty \rho_1 \rho_0 \;\text{\struck{$\rho_\infty$}}\; = 1
\end{equation*}\[\begin{equation*}
\tag{6} R^{i,j}_r \qquad r \in \mathcal{R},\ (i,j) \in \mathrm{Rep}\{0,1,\infty\}
\quad \text{i.e.\ } i,j \in \{0,1,\infty\},\ i \neq j
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{6} R^{i,j}_r \qquad r \in \mathcal{R},\ (i,j) \in \mathrm{Rep}\{0,1,\infty\}
\quad \text{i.e.\ } i,j \in \{0,1,\infty\},\ i \neq j
\end{equation*}\[\begin{equation*}
\tag{7} \boxed{R^{i,j}_r = R^{i,j}_{\tau_k(r)}, \quad k \notin \{i,j\}}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{7} \boxed{R^{i,j}_r = R^{i,j}_{\tau_k(r)}, \quad k \notin \{i,j\}}
\end{equation*}\[\begin{equation*}
\tag{8} \lambda^i_r : R^{i,i+1}_r \longrightarrow R^{i,i+2}_r \qquad r \in \mathcal{R},\ i \in \{0,1,\infty\}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{8} \lambda^i_r : R^{i,i+1}_r \longrightarrow R^{i,i+2}_r \qquad r \in \mathcal{R},\ i \in \{0,1,\infty\}
\end{equation*}\[\begin{equation*}
\tag{9} a^i_r : R^{i+1,i}_r \;\text{\struck{\ill{}}}\; \longrightarrow R^{i+1,i+2}_r \qquad r \in \mathcal{R},\ i \in \{0,1,\infty\}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{9} a^i_r : R^{i+1,i}_r \;\text{\struck{\ill{}}}\; \longrightarrow R^{i+1,i+2}_r \qquad r \in \mathcal{R},\ i \in \{0,1,\infty\}
\end{equation*}\[\begin{equation*}
\tag{10} \boxed{a^i_r = a^i_{\tau_i(r)}}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{10} \boxed{a^i_r = a^i_{\tau_i(r)}}
\end{equation*}\[\begin{equation*}
\tag{11} \tilde X^{\ast\ast} \longrightarrow X
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{11} \tilde X^{\ast\ast} \longrightarrow X
\end{equation*}\[\begin{equation*}
\tag{12}
\boxed{\underbrace{(\lambda^0_r)^{-1} a^1_r}_{\overset{\text{def}}{=}\, b^\infty_r}\;
\underbrace{(\lambda^\infty_r)^{-1} a^0_r}_{b^1_r}\;
\underbrace{(\lambda^1_r)^{-1} a^\infty_r}_{b^0_r} = 1}
\qquad \text{lacet en } R^{1\infty}_r
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{12}
\boxed{\underbrace{(\lambda^0_r)^{-1} a^1_r}_{\overset{\text{def}}{=}\, b^\infty_r}\;
\underbrace{(\lambda^\infty_r)^{-1} a^0_r}_{b^1_r}\;
\underbrace{(\lambda^1_r)^{-1} a^\infty_r}_{b^0_r} = 1}
\qquad \text{lacet en } R^{1\infty}_r
\end{equation*}\[\text{\struck{\ill{}}} \qquad (\tau_0 \tau_\infty)^2 = 1 \quad \text{i.e.} \quad \rho_1^2 = 1\]
LaTeX source
\[
\text{\struck{\ill{}}} \qquad (\tau_0 \tau_\infty)^2 = 1 \quad \text{i.e.} \quad \rho_1^2 = 1
\]\[\tau_0 \tau_\infty(r) = \tau_\infty \tau_0(r) \qquad \text{pour tout } r.\]
LaTeX source
\[
\tau_0 \tau_\infty(r) = \tau_\infty \tau_0(r) \qquad \text{pour tout } r.
\]\[\begin{equation*}
\tag{13}
\begin{cases}
\Lambda^i_r = (\lambda^i_{\tau_{i+1}(r)})^{-1} \lambda^i_r : R^{i,i+1}_r \longrightarrow R^{i,i+1}_{\tau_{i+1}(r)} \\
\Lambda'^i_r = \lambda^i_{\tau_{i-1}(r)} (\lambda^i_r)^{-1} : R^{i,i-1}_r \longrightarrow R^{i,i-1}_{\tau_{i-1}(r)}
\end{cases}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{13}
\begin{cases}
\Lambda^i_r = (\lambda^i_{\tau_{i+1}(r)})^{-1} \lambda^i_r : R^{i,i+1}_r \longrightarrow R^{i,i+1}_{\tau_{i+1}(r)} \\
\Lambda'^i_r = \lambda^i_{\tau_{i-1}(r)} (\lambda^i_r)^{-1} : R^{i,i-1}_r \longrightarrow R^{i,i-1}_{\tau_{i-1}(r)}
\end{cases}
\end{equation*}\[\begin{equation*}
\tag{14}
\boxed{\Lambda^i_r \Lambda^i_{\tau_{i+1}(r)} = 1} \qquad
\boxed{\Lambda'^i_r \Lambda'^i_{\tau_{i-1}(r)} = 1}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{14}
\boxed{\Lambda^i_r \Lambda^i_{\tau_{i+1}(r)} = 1} \qquad
\boxed{\Lambda'^i_r \Lambda'^i_{\tau_{i-1}(r)} = 1}
\end{equation*}\[\begin{equation*}
\tag{14} \{R^{ij}_r\} \quad
\begin{cases}
r \in \mathcal{R} \\
i \text{ ou } j \text{ est égal à } 1 \text{ i.e.\ } \{i,j\} \neq \{0,\infty\}
\end{cases}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{14} \{R^{ij}_r\} \quad
\begin{cases}
r \in \mathcal{R} \\
i \text{ ou } j \text{ est égal à } 1 \text{ i.e.\ } \{i,j\} \neq \{0,\infty\}
\end{cases}
\end{equation*}\[\begin{equation*}
\tag{15}
\begin{cases}
\lambda^1_r & r \in \mathcal{R} \\
\Lambda^0_r,\ \Lambda^\infty_r & r \in \mathcal{R},\ \text{\struck{\ill{}}} \\
a^i_r & r \in \mathcal{R},\ i \in \{0, \infty\}
\end{cases}
\qquad \Lambda^0_r \Lambda^0_{\tau_1 r} =
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{15}
\begin{cases}
\lambda^1_r & r \in \mathcal{R} \\
\Lambda^0_r,\ \Lambda^\infty_r & r \in \mathcal{R},\ \text{\struck{\ill{}}} \\
a^i_r & r \in \mathcal{R},\ i \in \{0, \infty\}
\end{cases}
\qquad \Lambda^0_r \Lambda^0_{\tau_1 r} =
\end{equation*}\[\begin{equation*}
\tag{16}
\text{\struck{$\Lambda^\infty_{\tau_1 r} (a_{\tau_1 r})^{-1} \lambda^1_{\tau_1 r} (a^\infty_{\tau_1 r})^{-1} \Lambda^0_r a^\infty_r \lambda^1_r a^0_r = 1$}}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{16}
\text{\struck{$\Lambda^\infty_{\tau_1 r} (a_{\tau_1 r})^{-1} \lambda^1_{\tau_1 r} (a^\infty_{\tau_1 r})^{-1} \Lambda^0_r a^\infty_r \lambda^1_r a^0_r = 1$}}
\end{equation*}\[\begin{equation*}
\tag{16}
\boxed{\Lambda'^\infty_{\tau_1(r)}
\underbrace{\bigl(a^0_{\tau_1 r} (\lambda^1_{\tau_1 r})^{-1} a^\infty_{\tau_1 r}\bigr)}_{\beta^1_{\tau_1(r)}}{}^{\!-1}
\Lambda^0_r
\underbrace{\bigl((a^\infty_r)^{-1} \lambda^1_r (a^0_r)^{-1}\bigr)}_{\beta^{1\,-1}_r} = 1}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{16}
\boxed{\Lambda'^\infty_{\tau_1(r)}
\underbrace{\bigl(a^0_{\tau_1 r} (\lambda^1_{\tau_1 r})^{-1} a^\infty_{\tau_1 r}\bigr)}_{\beta^1_{\tau_1(r)}}{}^{\!-1}
\Lambda^0_r
\underbrace{\bigl((a^\infty_r)^{-1} \lambda^1_r (a^0_r)^{-1}\bigr)}_{\beta^{1\,-1}_r} = 1}
\end{equation*}\[\begin{equation*}
\tag{17} R^{ij}_r \quad
\begin{cases}
r \in \mathcal{R} \\
\{i, j\} = \{0, 1\}
\end{cases}
\qquad\quad
\boxed{
\begin{cases}
R^{0,1}_r = R^{0,1}_{\tau_\infty r} \\
R^{1,0}_r = R^{1,0}_{\tau_\infty(r)}
\end{cases}}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{17} R^{ij}_r \quad
\begin{cases}
r \in \mathcal{R} \\
\{i, j\} = \{0, 1\}
\end{cases}
\qquad\quad
\boxed{
\begin{cases}
R^{0,1}_r = R^{0,1}_{\tau_\infty r} \\
R^{1,0}_r = R^{1,0}_{\tau_\infty(r)}
\end{cases}}
\end{equation*}\[\begin{equation*}
\tag{18}
\begin{cases}
a^\infty_r : R^{0,1}_r \;\text{\struck{\ill{}}}\; \longrightarrow R^{1,0}_r & (r \in \mathcal{R}) \\
\Lambda^0_r \;\text{\struck{$\Lambda^1_r$}} : R^{01}_r \longrightarrow R^{01}_{\tau_1(r)} \\
\Lambda'^1_r : R^{10}_r \longrightarrow R^{1,0}_{\tau_0(r)}
\end{cases}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{18}
\begin{cases}
a^\infty_r : R^{0,1}_r \;\text{\struck{\ill{}}}\; \longrightarrow R^{1,0}_r & (r \in \mathcal{R}) \\
\Lambda^0_r \;\text{\struck{$\Lambda^1_r$}} : R^{01}_r \longrightarrow R^{01}_{\tau_1(r)} \\
\Lambda'^1_r : R^{10}_r \longrightarrow R^{1,0}_{\tau_0(r)}
\end{cases}
\end{equation*}\[\begin{equation*}
\tag{19}
\boxed{
\begin{aligned}
\Lambda^0_r \Lambda^0_{\tau_1(r)} &= 1 \\
\Lambda'^1_r \Lambda'^1_{\tau_0(r)} &= 1
\end{aligned}}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{19}
\boxed{
\begin{aligned}
\Lambda^0_r \Lambda^0_{\tau_1(r)} &= 1 \\
\Lambda'^1_r \Lambda'^1_{\tau_0(r)} &= 1
\end{aligned}}
\end{equation*}\[\begin{equation*}
\tag{20} R^{0,1}_r \qquad r \in \mathcal{R}
\qquad\quad
\boxed{R^{0,1}_r = R^{0,1}_{\tau_\infty r}}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{20} R^{0,1}_r \qquad r \in \mathcal{R}
\qquad\quad
\boxed{R^{0,1}_r = R^{0,1}_{\tau_\infty r}}
\end{equation*}\[\begin{equation*}
\tag{21}
\begin{cases}
A^{0,1}_r \overset{\text{def}}{=} (a^\infty_{\tau_0 r})^{-1} \;\text{\struck{\ill{}}}\; (\Lambda'^1_r)^{-1} a^\infty_r : R^{0,1}_r \longrightarrow R^{0,1}_{\tau_0(r)} \\
\Lambda^0_r : R^{0,1}_r \longrightarrow R^{0,1}_{\tau_1 r} & (r \in \mathcal{R})
\end{cases}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{21}
\begin{cases}
A^{0,1}_r \overset{\text{def}}{=} (a^\infty_{\tau_0 r})^{-1} \;\text{\struck{\ill{}}}\; (\Lambda'^1_r)^{-1} a^\infty_r : R^{0,1}_r \longrightarrow R^{0,1}_{\tau_0(r)} \\
\Lambda^0_r : R^{0,1}_r \longrightarrow R^{0,1}_{\tau_1 r} & (r \in \mathcal{R})
\end{cases}
\end{equation*}\[\begin{equation*}
\tag{22}
\boxed{
\begin{cases}
\Lambda^0_r \Lambda^0_{\tau_1(r)} = 1 & r \in \mathcal{R} \\
A^{0,1}_r A^{0,1}_{\tau_0(r)} = 1 & r \in \mathcal{R}
\end{cases}}
\end{equation*}\]
LaTeX source
\begin{equation*}
\tag{22}
\boxed{
\begin{cases}
\Lambda^0_r \Lambda^0_{\tau_1(r)} = 1 & r \in \mathcal{R} \\
A^{0,1}_r A^{0,1}_{\tau_0(r)} = 1 & r \in \mathcal{R}
\end{cases}}
\end{equation*}