Cote n° 161-6 · pages 3–33
· 138 displayed formulas · Graphes, icosaèdre [etc.] : notes manuscrites (s.d.).
Inventory dating : [à partir de 1973-vers 1977]
Édition de démonstration
\[x(u,v;\alpha) = u \cos\alpha + v \sin\alpha \qquad \alpha \text{ défini mod } 2\pi\mathbb{Z}.\]
LaTeX source
\[
x(u,v;\alpha) = u \cos\alpha + v \sin\alpha \qquad \alpha \text{ défini mod } 2\pi\mathbb{Z}.
\]\[v' = v \cos\theta + w \sin\theta .\]
LaTeX source
\[ v' = v \cos\theta + w \sin\theta . \]
\[\begin{cases}
\|x(u,v;\alpha) - u\|^2 \underset{\text{par raison de sym.}}{=} \|x(u,v';\alpha) - u\|^2 \\ \qquad = (\cos\alpha - 1)^2 + \sin^2\alpha = 2(1 - \cos\alpha) = 4 \sin^2 \frac{\alpha}{2} \\[1ex]
\|x(u,v,\alpha) - x(u,v',\alpha)\|^2 = \sin^2\alpha \, \|v - v'\|^2 \\ \qquad = \sin^2\alpha \; 4 \sin^2 \frac{\theta}{2} = \Bigl(4 \sin^2 \frac{\alpha}{2} \cos^2 \frac{\alpha}{2}\Bigr)\Bigl(4 \sin^2 \frac{\theta}{2}\Bigr)
\end{cases}\]
LaTeX source
\[
\begin{cases}
\|x(u,v;\alpha) - u\|^2 \underset{\text{par raison de sym.}}{=} \|x(u,v';\alpha) - u\|^2 \\ \qquad = (\cos\alpha - 1)^2 + \sin^2\alpha = 2(1 - \cos\alpha) = 4 \sin^2 \frac{\alpha}{2} \\[1ex]
\|x(u,v,\alpha) - x(u,v',\alpha)\|^2 = \sin^2\alpha \, \|v - v'\|^2 \\ \qquad = \sin^2\alpha \; 4 \sin^2 \frac{\theta}{2} = \Bigl(4 \sin^2 \frac{\alpha}{2} \cos^2 \frac{\alpha}{2}\Bigr)\Bigl(4 \sin^2 \frac{\theta}{2}\Bigr)
\end{cases}
\]\[\text{(1)} \qquad \cos\frac{\alpha}{2} = \pm \frac{1}{2 \sin \theta/2} .\]
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\[
\text{(1)} \qquad \cos\frac{\alpha}{2} = \pm \frac{1}{2 \sin \theta/2} .
\]\[\text{(1')} \qquad \cos\alpha = \frac{1}{2\sin^2\theta/2} - 1 = \frac{1 - 2\sin^2\theta/2}{2\sin^2\theta/2} = \frac{\cos\theta}{2\sin^2\theta/2} = \frac{\cos\theta}{1 - \cos\theta}\]
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\[
\text{(1')} \qquad \cos\alpha = \frac{1}{2\sin^2\theta/2} - 1 = \frac{1 - 2\sin^2\theta/2}{2\sin^2\theta/2} = \frac{\cos\theta}{2\sin^2\theta/2} = \frac{\cos\theta}{1 - \cos\theta}
\]\[\text{(2)} \qquad \theta = \frac{2\pi}{5}\]
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\[
\text{(2)} \qquad \theta = \frac{2\pi}{5}
\]\[\text{(3)} \qquad v_i = v \cos i\theta + w \sin i\theta \qquad i \in \mathbb{Z}/5\mathbb{Z}\]
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\[
\text{(3)} \qquad v_i = v \cos i\theta + w \sin i\theta \qquad i \in \mathbb{Z}/5\mathbb{Z}
\]\[\text{(4)} \qquad x_i = x(u, v_i, \alpha) = u\cos\alpha + v_i \sin\alpha = u\cos\alpha + v\cos i\theta \sin\alpha + w \sin i\theta \sin\alpha \qquad (i \in \mathbb{Z}/5\mathbb{Z})\]
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\[
\text{(4)} \qquad x_i = x(u, v_i, \alpha) = u\cos\alpha + v_i \sin\alpha = u\cos\alpha + v\cos i\theta \sin\alpha + w \sin i\theta \sin\alpha \qquad (i \in \mathbb{Z}/5\mathbb{Z})
\]\[\text{(5)} \qquad x'_i = -x_i , \quad u' = -u \qquad (i \in \mathbb{Z}/5\mathbb{Z})\]
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\[
\text{(5)} \qquad x'_i = -x_i , \quad u' = -u \qquad (i \in \mathbb{Z}/5\mathbb{Z})
\]\[\text{(4)} \qquad \ell = 2 \sin\frac{\alpha}{2}\]
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\[
\text{(4)} \qquad \ell = 2 \sin\frac{\alpha}{2}
\]\[\text{(4')} \qquad \ell' = 2 \cos\frac{\alpha}{2}\]
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\[
\text{(4')} \qquad \ell' = 2 \cos\frac{\alpha}{2}
\]\[\gamma u = x_0 , \quad \gamma x_0 = x'_{2} , \quad \gamma x_1 = x'_{-2} , \quad \gamma x_2 = x_1 , \quad \gamma x_3 = u , \quad \gamma x_4 = x_{-1}\]
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\[
\gamma u = x_0 , \quad \gamma x_0 = x'_{2} , \quad \gamma x_1 = x'_{-2} , \quad \gamma x_2 = x_1 , \quad \gamma x_3 = u , \quad \gamma x_4 = x_{-1}
\]\[\begin{align*}
\gamma u &= \gamma^{w}_{\alpha}(u) = u\cos\alpha + v\sin\alpha \\
\gamma v &= \gamma^{w}_{\alpha}\Bigl(v\cos\frac{\theta}{2} - w\sin\frac{\theta}{2}\Bigr) = (-u\sin\alpha + v\cos\alpha)\cos\frac{\theta}{2} - w\sin\frac{\theta}{2} \\
&= -u\sin\alpha\cos\frac{\theta}{2} + v\cos\alpha\cos\frac{\theta}{2} - w\sin\frac{\theta}{2} \\
\gamma w &= \gamma^{w}_{\alpha}\Bigl(+v\sin\frac{\theta}{2} + w\cos\frac{\theta}{2}\Bigr) = (-u\sin\alpha + v\cos\alpha)\sin\frac{\theta}{2} + w\cos\frac{\theta}{2} \\
&= -u\sin\alpha\sin\frac{\theta}{2} + v\cos\alpha\sin\frac{\theta}{2} + w\cos\frac{\theta}{2}
\end{align*}\]
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\begin{align*}
\gamma u &= \gamma^{w}_{\alpha}(u) = u\cos\alpha + v\sin\alpha \\
\gamma v &= \gamma^{w}_{\alpha}\Bigl(v\cos\frac{\theta}{2} - w\sin\frac{\theta}{2}\Bigr) = (-u\sin\alpha + v\cos\alpha)\cos\frac{\theta}{2} - w\sin\frac{\theta}{2} \\
&= -u\sin\alpha\cos\frac{\theta}{2} + v\cos\alpha\cos\frac{\theta}{2} - w\sin\frac{\theta}{2} \\
\gamma w &= \gamma^{w}_{\alpha}\Bigl(+v\sin\frac{\theta}{2} + w\cos\frac{\theta}{2}\Bigr) = (-u\sin\alpha + v\cos\alpha)\sin\frac{\theta}{2} + w\cos\frac{\theta}{2} \\
&= -u\sin\alpha\sin\frac{\theta}{2} + v\cos\alpha\sin\frac{\theta}{2} + w\cos\frac{\theta}{2}
\end{align*}\[\gamma = \begin{pmatrix}
\cos\alpha & -\sin\alpha\cos\frac{\theta}{2} & -\sin\alpha\sin\frac{\theta}{2} \\
\sin\alpha & \cos\alpha\cos\frac{\theta}{2} & \cos\alpha\sin\frac{\theta}{2} \\
0 & -\sin\frac{\theta}{2} & \cos\frac{\theta}{2}
\end{pmatrix}\]
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\[
\gamma = \begin{pmatrix}
\cos\alpha & -\sin\alpha\cos\frac{\theta}{2} & -\sin\alpha\sin\frac{\theta}{2} \\
\sin\alpha & \cos\alpha\cos\frac{\theta}{2} & \cos\alpha\sin\frac{\theta}{2} \\
0 & -\sin\frac{\theta}{2} & \cos\frac{\theta}{2}
\end{pmatrix}
\]\[\begin{align*}
\gamma u &= u\cos\alpha + v\sin\alpha = x_0 \qquad \text{OK} \\
\gamma x_0 &= \gamma u \cos\alpha + \gamma v \sin\alpha = u\Bigl(\cos^2\alpha - \sin^2\alpha\cos\frac{\theta}{2}\Bigr) + v\Bigl(\sin\alpha\cos\alpha + \sin\alpha\cos\alpha\cos\frac{\theta}{2}\Bigr) \\
&\qquad - w\Bigl(\sin\alpha\sin\frac{\theta}{2}\Bigr)
\end{align*}\]
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\begin{align*}
\gamma u &= u\cos\alpha + v\sin\alpha = x_0 \qquad \text{OK} \\
\gamma x_0 &= \gamma u \cos\alpha + \gamma v \sin\alpha = u\Bigl(\cos^2\alpha - \sin^2\alpha\cos\frac{\theta}{2}\Bigr) + v\Bigl(\sin\alpha\cos\alpha + \sin\alpha\cos\alpha\cos\frac{\theta}{2}\Bigr) \\
&\qquad - w\Bigl(\sin\alpha\sin\frac{\theta}{2}\Bigr)
\end{align*}\[\begin{cases}
-\cos\alpha = \cos^2\alpha - \sin^2\alpha\cos\frac{\theta}{2} \\
-\cos 2\theta \struck{\sin\alpha} = \struck{\sin\alpha}\cos\alpha\Bigl(1 + \cos\frac{\theta}{2}\Bigr) \\
\struck{\ill{}} \sin 2\theta = \struck{\sin\alpha} \sin\frac{\theta}{2}
\end{cases}\]
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\[
\begin{cases}
-\cos\alpha = \cos^2\alpha - \sin^2\alpha\cos\frac{\theta}{2} \\
-\cos 2\theta \struck{\sin\alpha} = \struck{\sin\alpha}\cos\alpha\Bigl(1 + \cos\frac{\theta}{2}\Bigr) \\
\struck{\ill{}} \sin 2\theta = \struck{\sin\alpha} \sin\frac{\theta}{2}
\end{cases}
\]\[\gamma x_1 = \gamma u \cos\alpha + \gamma v \sin\alpha\cos\theta + w\sin\alpha\sin\theta\]
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\[ \gamma x_1 = \gamma u \cos\alpha + \gamma v \sin\alpha\cos\theta + w\sin\alpha\sin\theta \]
\[\Gamma \simeq \mu_2 \times \Gamma'\]
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\[ \Gamma \simeq \mu_2 \times \Gamma' \]
\[\begin{cases}
(u, x_i), & \struck{\ill{}} \; (u', x'_i) \\
(x_i, x_{i+1}), & (x'_i, x'_{i+1}) \qquad i \in \mathbb{Z}/5\mathbb{Z} \\
(x_i, x'_{i-2}) & (x'_i, x_{i-2})
\end{cases}\]
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\[
\begin{cases}
(u, x_i), & \struck{\ill{}} \; (u', x'_i) \\
(x_i, x_{i+1}), & (x'_i, x'_{i+1}) \qquad i \in \mathbb{Z}/5\mathbb{Z} \\
(x_i, x'_{i-2}) & (x'_i, x_{i-2})
\end{cases}
\]\[\begin{array}{lll}
(u, x_i, x_{i+1}) & (u', x'_i, x'_{i+1}) & i \in \mathbb{Z}/5\mathbb{Z} \\
(x_i, x'_{i-2}, \underset{\textstyle x_{i+1}}{\underset{\shortparallel}{x_{i-4}}}) & (x'_i, x_{i-2}, \underset{\textstyle x'_{i+1}}{\underset{\shortparallel}{x'_{i-4}}}) &
\end{array}\]
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\[
\begin{array}{lll}
(u, x_i, x_{i+1}) & (u', x'_i, x'_{i+1}) & i \in \mathbb{Z}/5\mathbb{Z} \\
(x_i, x'_{i-2}, \underset{\textstyle x_{i+1}}{\underset{\shortparallel}{x_{i-4}}}) & (x'_i, x_{i-2}, \underset{\textstyle x'_{i+1}}{\underset{\shortparallel}{x'_{i-4}}}) &
\end{array}
\]\[\zeta^{3} + \zeta^{-1} + \zeta + \zeta^{-3} = \zeta + \zeta^{2} + \zeta^{3} + \zeta^{4} = -1\]
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\[
\zeta^{3} + \zeta^{-1} + \zeta + \zeta^{-3} = \zeta + \zeta^{2} + \zeta^{3} + \zeta^{4} = -1
\]\[\boxed{\gamma^{2} + \gamma - 1 = 0}\]
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\[
\boxed{\gamma^{2} + \gamma - 1 = 0}
\]\[\uncertain{\mathfrak{D}}_5 = \mathbb{Z}[\tfrac{1}{5}][t]/(t^{2} + t - 1)\]
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\[
\uncertain{\mathfrak{D}}_5 = \mathbb{Z}[\tfrac{1}{5}][t]/(t^{2} + t - 1)
\]\[\boxed{\gamma = (-1 \pm \sqrt{5})/2}\]
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\[
\boxed{\gamma = (-1 \pm \sqrt{5})/2}
\]\[2\cos\frac{2\pi}{5} = (\sqrt{5} - 1)/2 \qquad (2\gamma + 1)^{2} = 5 \qquad \struck{4\gamma^{2} + 4\gamma = 4}\]
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\[
2\cos\frac{2\pi}{5} = (\sqrt{5} - 1)/2 \qquad (2\gamma + 1)^{2} = 5 \qquad \struck{4\gamma^{2} + 4\gamma = 4}
\]\[\cos\frac{2\pi}{5} = \frac{\sqrt{5} - 1}{4} \qquad \cos\frac{4\pi}{5} = \frac{-\sqrt{5} - 1}{4} \qquad c^{2} + c - 1\]
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\[
\cos\frac{2\pi}{5} = \frac{\sqrt{5} - 1}{4} \qquad \cos\frac{4\pi}{5} = \frac{-\sqrt{5} - 1}{4} \qquad c^{2} + c - 1
\]\[(-1 + \sqrt{5})/2 = \bigl((-1 - \sqrt{5})/2\bigr)^{2} - 2 = \frac{1 + 5 + 2\sqrt{5}}{4} - 2 = -\frac{1}{2} + \frac{1}{2}\sqrt{5}\]
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\[
(-1 + \sqrt{5})/2 = \bigl((-1 - \sqrt{5})/2\bigr)^{2} - 2 = \frac{1 + 5 + 2\sqrt{5}}{4} - 2 = -\frac{1}{2} + \frac{1}{2}\sqrt{5}
\]\[\zeta \longmapsto \zeta^{2} \qquad \zeta \longmapsto \zeta^{3} \qquad \text{si } \zeta + \zeta^{-1} = t\]
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\[
\zeta \longmapsto \zeta^{2} \qquad \zeta \longmapsto \zeta^{3} \qquad \text{si } \zeta + \zeta^{-1} = t
\]\[\struck{\cos' D, D} \qquad \cos'_{\ill{}}(D, \zeta D) = \operatorname{Tr} \zeta^{2} = \zeta^{2} + \zeta^{-2} = t^{2} - 2\]
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\[
\struck{\cos' D, D} \qquad \cos'_{\ill{}}(D, \zeta D) = \operatorname{Tr} \zeta^{2} = \zeta^{2} + \zeta^{-2} = t^{2} - 2
\]\[t', t'' \qquad t'' = t'^{2} - 2 = (t''^{2} - 2)^{2} - 2 \qquad t' = t''^{2} - 2\]
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\[
t', t'' \qquad t'' = t'^{2} - 2 = (t''^{2} - 2)^{2} - 2 \qquad t' = t''^{2} - 2
\]\[\begin{array}{cccc}
\zeta & \zeta^{2} & \zeta^{3} & \zeta^{4} \\
& & \shortparallel & \shortparallel \\
& & \zeta^{-2} & \zeta^{-1} \\[1ex]
\zeta + \zeta^{-1} & \zeta^{2} + \zeta^{-2} & \zeta^{3} + \zeta^{-3} & \zeta^{4} + \zeta^{-4} \\
\shortparallel & \shortparallel & \shortparallel & \shortparallel \\
\eta = \eta_1 & \eta_2 & \uncertain{\eta_2} & \eta_1
\end{array}\]
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\[
\begin{array}{cccc}
\zeta & \zeta^{2} & \zeta^{3} & \zeta^{4} \\
& & \shortparallel & \shortparallel \\
& & \zeta^{-2} & \zeta^{-1} \\[1ex]
\zeta + \zeta^{-1} & \zeta^{2} + \zeta^{-2} & \zeta^{3} + \zeta^{-3} & \zeta^{4} + \zeta^{-4} \\
\shortparallel & \shortparallel & \shortparallel & \shortparallel \\
\eta = \eta_1 & \eta_2 & \uncertain{\eta_2} & \eta_1
\end{array}
\]\[\begin{aligned}
&= \sup_{\ill{}} [\bar\alpha(U) \wedge \bar\beta(V)] \wedge [\bar\alpha(U') \wedge \bar\beta(V')] \\
&= \bigl(\sup \bar\alpha(U) \wedge \bar\beta(V)\bigr) \wedge \bigl(\sup \bar\alpha(U') \wedge \bar\beta(V')\bigr) \\
&= \bar\gamma(W) \wedge \bar\gamma(W') , \qquad \text{ok}
\end{aligned}\]
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\[
\begin{aligned}
&= \sup_{\ill{}} [\bar\alpha(U) \wedge \bar\beta(V)] \wedge [\bar\alpha(U') \wedge \bar\beta(V')] \\
&= \bigl(\sup \bar\alpha(U) \wedge \bar\beta(V)\bigr) \wedge \bigl(\sup \bar\alpha(U') \wedge \bar\beta(V')\bigr) \\
&= \bar\gamma(W) \wedge \bar\gamma(W') , \qquad \text{ok}
\end{aligned}
\]\[\bar\gamma(\underbrace{\struck{\ill{}}\sup W_i}_{W}) \geq \sup\bigl(\bar\gamma(W_i)\bigr) \quad \text{clair, prouvons } \leq\]
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\[
\bar\gamma(\underbrace{\struck{\ill{}}\sup W_i}_{W}) \geq \sup\bigl(\bar\gamma(W_i)\bigr) \quad \text{clair, prouvons } \leq
\]\[\bar\gamma(W) = \sup_{\gamma(U \times V) \subset \sup_i W_i} \bar\alpha(U) \wedge \bar\beta(V)\]
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\[
\bar\gamma(W) = \sup_{\gamma(U \times V) \subset \sup_i W_i} \bar\alpha(U) \wedge \bar\beta(V)
\]\[\begin{array}{l} U = \sup U_j \\ V = \sup V_k \end{array} \;\Big|\; \forall\, j, k \ \exists\, i \text{ avec } \gamma(U_j \times V_k) \leq W_i\]
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\[
\begin{array}{l} U = \sup U_j \\ V = \sup V_k \end{array} \;\Big|\; \forall\, j, k \ \exists\, i \text{ avec } \gamma(U_j \times V_k) \leq W_i
\]\[\bar\alpha(U) \wedge \bar\beta(V) = \bigl(\sup_j \bar\alpha(U_j)\bigr) \wedge \bigl(\sup_k \bar\beta(V_k)\bigr) = \sup_{j,k} \bar\alpha(U_j) \wedge \bar\beta(V_k) \qquad \Bigl(\overset{?}{\leq} \sup_i \bar\gamma(W_i)\Bigr)\]
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\[
\bar\alpha(U) \wedge \bar\beta(V) = \bigl(\sup_j \bar\alpha(U_j)\bigr) \wedge \bigl(\sup_k \bar\beta(V_k)\bigr) = \sup_{j,k} \bar\alpha(U_j) \wedge \bar\beta(V_k) \qquad \Bigl(\overset{?}{\leq} \sup_i \bar\gamma(W_i)\Bigr)
\]\[\bar\alpha(U_j) \wedge \bar\beta(V_k) \leq \bar\gamma(W_i) \leq \sup_{i'} \bar\gamma(W_{i'}) \qquad \text{qfd}\]
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\[
\bar\alpha(U_j) \wedge \bar\beta(V_k) \leq \bar\gamma(W_i) \leq \sup_{i'} \bar\gamma(W_{i'}) \qquad \text{qfd}
\]\[(I_\lambda)_{\lambda \in \Lambda} \qquad I_\lambda \in \operatorname{Ob}(\uncertain{\mathrm{OM}})\]
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\[
(I_\lambda)_{\lambda \in \Lambda} \qquad I_\lambda \in \operatorname{Ob}(\uncertain{\mathrm{OM}})
\]\[\alpha^{0}_{\mu} : I_\mu \longrightarrow \prod{}' I_\lambda \qquad \alpha^{0}_{\mu}(x)_\lambda = \begin{cases} x & \text{si } \lambda = \mu \\ 1_{I_\lambda} & \text{si } \lambda \neq \mu \end{cases} \qquad \text{appl. cr.}\]
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\[
\alpha^{0}_{\mu} : I_\mu \longrightarrow \prod{}' I_\lambda \qquad \alpha^{0}_{\mu}(x)_\lambda = \begin{cases} x & \text{si } \lambda = \mu \\ 1_{I_\lambda} & \text{si } \lambda \neq \mu \end{cases} \qquad \text{appl. cr.}
\]\[\gamma : \prod{}' I_\lambda \longrightarrow K \quad \text{flèche dans } (\uncertain{\mathrm{OM}})\]
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\[
\gamma : \prod{}' I_\lambda \longrightarrow K \quad \text{flèche dans } (\uncertain{\mathrm{OM}})
\]\[\alpha_\mu = \gamma \circ \alpha^{0}_{\mu} : I_\mu \to K \quad \text{appl. cr.}\]
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\[
\alpha_\mu = \gamma \circ \alpha^{0}_{\mu} : I_\mu \to K \quad \text{appl. cr.}
\]\[\Gamma = (\mathbb{Z}/5\mathbb{Z})^{*} \simeq \mathbb{Z}/4\mathbb{Z}
\qquad
\begin{array}{ccc}
\mu_5 & \supset & \mu_5^{*} \\
| & & | \\
\operatorname{Spec} \mathbb{Z} & \longleftarrow & \mathbb{Z}[\frac{1}{5}]
\end{array}\]
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\[
\Gamma = (\mathbb{Z}/5\mathbb{Z})^{*} \simeq \mathbb{Z}/4\mathbb{Z}
\qquad
\begin{array}{ccc}
\mu_5 & \supset & \mu_5^{*} \\
| & & | \\
\operatorname{Spec} \mathbb{Z} & \longleftarrow & \mathbb{Z}[\frac{1}{5}]
\end{array}
\]\[\struck{\ill{}}\; \tau = \mu_5^{*}/\beta \quad \text{engendré par } \struck{\zeta}\, \zeta + \bar\zeta = \zeta + \zeta^{-1} = \eta\]
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\[
\struck{\ill{}}\; \tau = \mu_5^{*}/\beta \quad \text{engendré par } \struck{\zeta}\, \zeta + \bar\zeta = \zeta + \zeta^{-1} = \eta
\]\[\zeta \mapsto \zeta^{2} \text{ ou } \zeta \mapsto \zeta^{-2} = \zeta^{3} \text{ resp.} \qquad \zeta \mapsto \zeta^{-1} = \zeta^{4} \qquad \zeta \mapsto \zeta\]
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\[
\zeta \mapsto \zeta^{2} \text{ ou } \zeta \mapsto \zeta^{-2} = \zeta^{3} \text{ resp.} \qquad \zeta \mapsto \zeta^{-1} = \zeta^{4} \qquad \zeta \mapsto \zeta
\]\[\begin{array}{c} B \supset B^{\Gamma} \\ | \\ A \end{array}
\qquad
B = A[\zeta] \struck{\ill{}} = A[T]/(1 + T + T^{2} + T^{3} + T^{4})
\qquad T \longmapsto T^{4}\]
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\[
\begin{array}{c} B \supset B^{\Gamma} \\ | \\ A \end{array}
\qquad
B = A[\zeta] \struck{\ill{}} = A[T]/(1 + T + T^{2} + T^{3} + T^{4})
\qquad T \longmapsto T^{4}
\]\[\begin{aligned}
\beta(T) &= T^{-1} = T^{4} = -(1 + T + T^{2} + T^{3}) \\
\beta(T^{2}) &= T^{-2} = T^{3} \\
\beta(T^{3}) &= T^{-3} = T^{2} \\
\beta(T^{4}) &-
\end{aligned}
\qquad\qquad 1 = T^{0} \mid T \quad T^{2} \quad T^{3}\]
LaTeX source
\[
\begin{aligned}
\beta(T) &= T^{-1} = T^{4} = -(1 + T + T^{2} + T^{3}) \\
\beta(T^{2}) &= T^{-2} = T^{3} \\
\beta(T^{3}) &= T^{-3} = T^{2} \\
\beta(T^{4}) &-
\end{aligned}
\qquad\qquad 1 = T^{0} \mid T \quad T^{2} \quad T^{3}
\]\[\begin{aligned}
\beta(c_0 + c_1 T + c_2 T^{2} + c_3 T^{3}) \struck{\ill{}}
&= c_0 \mathbin{\ill{}} c_1(\uncertain{-1} + T + T^{2} + T^{3}) + c_2 T^{3} + c_3 T^{2} \\
&= (c_0 - c_1) - c_1 T + (c_3 - c_1) T^{2} + (c_2 - c_1) T^{3} \\
&\overset{?}{=} c_0 + c_1 T + c_2 T^{2} + c_3 T^{3}
\end{aligned}\]
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\[
\begin{aligned}
\beta(c_0 + c_1 T + c_2 T^{2} + c_3 T^{3}) \struck{\ill{}}
&= c_0 \mathbin{\ill{}} c_1(\uncertain{-1} + T + T^{2} + T^{3}) + c_2 T^{3} + c_3 T^{2} \\
&= (c_0 - c_1) - c_1 T + (c_3 - c_1) T^{2} + (c_2 - c_1) T^{3} \\
&\overset{?}{=} c_0 + c_1 T + c_2 T^{2} + c_3 T^{3}
\end{aligned}
\]\[c_1 = 0 \qquad c_2 = c_3 \qquad\qquad c_0 + c_2 (T^{2} + T^{3})\]
LaTeX source
\[
c_1 = 0 \qquad c_2 = c_3 \qquad\qquad c_0 + c_2 (T^{2} + T^{3})
\]\[\begin{array}{c} \mu_n \\ \cup \\ \mu_n^{*} \\ \downarrow \\ S \end{array}
\quad (\mathbb{Z}/n\mathbb{Z})^{*} \qquad \zeta \longmapsto \zeta^{-1}\]
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\[
\begin{array}{c} \mu_n \\ \cup \\ \mu_n^{*} \\ \downarrow \\ S \end{array}
\quad (\mathbb{Z}/n\mathbb{Z})^{*} \qquad \zeta \longmapsto \zeta^{-1}
\]\[\varphi(n) = \prod \bigl(p_i^{\alpha_i} - p_i^{\alpha_i - 1}\bigr) \qquad \text{pas gros} \qquad p^{n} - p^{n-1} = p^{n-1}(p - 1) \qquad (\mathbb{Z}/n\mathbb{Z})^{*} \ni -1\]
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\[
\varphi(n) = \prod \bigl(p_i^{\alpha_i} - p_i^{\alpha_i - 1}\bigr) \qquad \text{pas gros} \qquad p^{n} - p^{n-1} = p^{n-1}(p - 1) \qquad (\mathbb{Z}/n\mathbb{Z})^{*} \ni -1
\]\[\begin{array}{ccccc}
\mu_n^{T} & \subset & \mathcal{U} & & \\
\cup & & & & \\
\mu_n^{*T} & \subset & \mathcal{U} & & \zeta + \bar\zeta \\
\Big\downarrow{\scriptstyle \text{étale rang } 2} & & \Big\downarrow{\scriptstyle \operatorname{Tr}_{K/\mathbb{Q}}} & & \\
\vartheta_n^{T} = \mathcal{V}_n & \subset & \mathcal{O} & & \\
\Big\downarrow{\scriptstyle \text{étale rang } \uncertain{\varphi(n)/2}} & & & & \\
S & & & &
\end{array}\]
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\[
\begin{array}{ccccc}
\mu_n^{T} & \subset & \mathcal{U} & & \\
\cup & & & & \\
\mu_n^{*T} & \subset & \mathcal{U} & & \zeta + \bar\zeta \\
\Big\downarrow{\scriptstyle \text{étale rang } 2} & & \Big\downarrow{\scriptstyle \operatorname{Tr}_{K/\mathbb{Q}}} & & \\
\vartheta_n^{T} = \mathcal{V}_n & \subset & \mathcal{O} & & \\
\Big\downarrow{\scriptstyle \text{étale rang } \uncertain{\varphi(n)/2}} & & & & \\
S & & & &
\end{array}
\]\[\begin{array}{ccc}
\mu_n & \subset & \mathbb{G}_m \\[1ex]
\mu_n^{*} & \subset & \mathbb{G}_m \\
\downarrow & & \downarrow{\scriptstyle \rho} \\
\vartheta_n & \subset & \mathbb{E}^{1}
\end{array}
\qquad \rho(\lambda) = \lambda + \lambda^{-1}\]
LaTeX source
\[
\begin{array}{ccc}
\mu_n & \subset & \mathbb{G}_m \\[1ex]
\mu_n^{*} & \subset & \mathbb{G}_m \\
\downarrow & & \downarrow{\scriptstyle \rho} \\
\vartheta_n & \subset & \mathbb{E}^{1}
\end{array}
\qquad \rho(\lambda) = \lambda + \lambda^{-1}
\]\[\zeta + \zeta^{-1} \;\Big|\; \begin{array}{l} \frac{p - 1}{2} = 2 \\ \cos \end{array}\]
LaTeX source
\[
\zeta + \zeta^{-1} \;\Big|\; \begin{array}{l} \frac{p - 1}{2} = 2 \\ \cos \end{array}
\]\[1 + \zeta + \zeta^{2} + \zeta^{3} + \zeta^{4} = 0 \qquad \zeta + \zeta^{-1} = \gamma\]
LaTeX source
\[
1 + \zeta + \zeta^{2} + \zeta^{3} + \zeta^{4} = 0 \qquad \zeta + \zeta^{-1} = \gamma
\]\[\begin{aligned}
\operatorname{Tr} \gamma &= \gamma + \gamma^{\alpha} = \zeta + \zeta^{-1} + \zeta^{2} + \zeta^{-2} = \zeta + \zeta^{2} + \zeta^{3} + \zeta^{4} = -1 \\
\operatorname{N} \gamma &= \gamma\gamma^{\alpha} = (\zeta + \zeta^{-1})(\zeta^{2} + \zeta^{-2}) =
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
\operatorname{Tr} \gamma &= \gamma + \gamma^{\alpha} = \zeta + \zeta^{-1} + \zeta^{2} + \zeta^{-2} = \zeta + \zeta^{2} + \zeta^{3} + \zeta^{4} = -1 \\
\operatorname{N} \gamma &= \gamma\gamma^{\alpha} = (\zeta + \zeta^{-1})(\zeta^{2} + \zeta^{-2}) =
\end{aligned}
\]\[\struck{\ill{}} \qquad \operatorname{Hom}_{\mathrm{OM}}(K, L) \longrightarrow \operatorname{Hom}_{\mathrm{OM}}(I, L) \times \operatorname{Hom}_{\mathrm{OM}}(J, L) \qquad \varphi \longmapsto (\varphi \circ \alpha, \varphi \circ \beta)\]
LaTeX source
\[
\struck{\ill{}} \qquad \operatorname{Hom}_{\mathrm{OM}}(K, L) \longrightarrow \operatorname{Hom}_{\mathrm{OM}}(I, L) \times \operatorname{Hom}_{\mathrm{OM}}(J, L) \qquad \varphi \longmapsto (\varphi \circ \alpha, \varphi \circ \beta)
\]\[\bar\alpha : I \longrightarrow L \qquad \bar\beta : J \longrightarrow L \qquad \text{dans } (\mathrm{OM})\]
LaTeX source
\[
\bar\alpha : I \longrightarrow L \qquad \bar\beta : J \longrightarrow L \qquad \text{dans } (\mathrm{OM})
\]\[\bar\gamma : K \longrightarrow L\]
LaTeX source
\[ \bar\gamma : K \longrightarrow L \]
\[\bar\gamma(W) = \sup_{\substack{U \in I \\ V \in J \\ \gamma(U \times V) \subset W}} \bar\alpha(U) \wedge \bar\beta(V)\]
LaTeX source
\[
\bar\gamma(W) = \sup_{\substack{U \in I \\ V \in J \\ \gamma(U \times V) \subset W}} \bar\alpha(U) \wedge \bar\beta(V)
\]\[\bar\gamma \circ \alpha = \bar\alpha , \qquad \bar\gamma \circ \beta = \bar\beta\]
LaTeX source
\[ \bar\gamma \circ \alpha = \bar\alpha , \qquad \bar\gamma \circ \beta = \bar\beta \]
\[(\bar\gamma \circ \alpha)(U') = \bar\gamma(U' \times 1) = \sup_{\gamma(U \times V) \leq \gamma(U' \times 1)} \bar\alpha(U) \wedge \bar\beta(V)\]
LaTeX source
\[
(\bar\gamma \circ \alpha)(U') = \bar\gamma(U' \times 1) = \sup_{\gamma(U \times V) \leq \gamma(U' \times 1)} \bar\alpha(U) \wedge \bar\beta(V)
\]\[\bar\gamma(1_K) \struck{\ill{}} \overset{\text{def}}{=} \bar\alpha(1_I) \wedge \bar\beta(1_J) = 1_K\]
LaTeX source
\[
\bar\gamma(1_K) \struck{\ill{}} \overset{\text{def}}{=} \bar\alpha(1_I) \wedge \bar\beta(1_J) = 1_K
\]\[\bar\gamma(W \wedge W') = \sup_{\gamma(U \times V) \subset W \wedge W'} \bar\alpha(U) \wedge \bar\beta(V) = \sup_{\substack{\gamma(U \times V) \subset W \\ \gamma(U' \times V') \subset W'}} \bar\alpha(U \wedge U') \wedge \bar\beta(V \wedge V')\]
LaTeX source
\[
\bar\gamma(W \wedge W') = \sup_{\gamma(U \times V) \subset W \wedge W'} \bar\alpha(U) \wedge \bar\beta(V) = \sup_{\substack{\gamma(U \times V) \subset W \\ \gamma(U' \times V') \subset W'}} \bar\alpha(U \wedge U') \wedge \bar\beta(V \wedge V')
\]\[\underline{X} \longrightarrow (\mathrm{Ens}) \qquad \underline{\hat X} \longrightarrow (\mathrm{Ens}) ,\]
LaTeX source
\[
\underline{X} \longrightarrow (\mathrm{Ens}) \qquad \underline{\hat X} \longrightarrow (\mathrm{Ens}) ,
\]\[x \subset e \qquad x \quad y \qquad z \to x \cap y\]
LaTeX source
\[ x \subset e \qquad x \quad y \qquad z \to x \cap y \]
\[4 \longrightarrow 3 \longrightarrow 2 \longrightarrow 1 \longrightarrow 0\]
LaTeX source
\[ 4 \longrightarrow 3 \longrightarrow 2 \longrightarrow 1 \longrightarrow 0 \]
\[X_1 \longleftarrow X_0 \qquad y \leq x \qquad U_x \subset U_y \qquad F(y) \longrightarrow F(x)\]
LaTeX source
\[ X_1 \longleftarrow X_0 \qquad y \leq x \qquad U_x \subset U_y \qquad F(y) \longrightarrow F(x) \]
\[\operatorname{Hom}_G(X, E) \subset \operatorname{Hom}_G(P_S, E) \simeq E\]
LaTeX source
\[
\operatorname{Hom}_G(X, E) \subset \operatorname{Hom}_G(P_S, E) \simeq E
\]\[\struck{\ill{}} + v \cos i\frac{2\pi}{5} + w \sin i\frac{2\pi}{5} = \rho_i \qquad \boxed{0 \leqslant i \leqslant 4}\]
LaTeX source
\[
\struck{\ill{}} + v \cos i\frac{2\pi}{5} + w \sin i\frac{2\pi}{5} = \rho_i \qquad \boxed{0 \leqslant i \leqslant 4}
\]\[\begin{cases}
u \\
u\cos\alpha + \rho_i \sin\alpha \\
-u\cos\alpha - \rho_i \sin\alpha \\
-u
\end{cases}\]
LaTeX source
\[
\begin{cases}
u \\
u\cos\alpha + \rho_i \sin\alpha \\
-u\cos\alpha - \rho_i \sin\alpha \\
-u
\end{cases}
\]\[\frac{4\pi}{5} < \frac{2\pi}{3} \qquad \frac{\pi}{3} < \qquad \frac{4\pi}{5} \to \frac{\pi}{6} \;? \qquad \frac{4\pi}{5} \leqslant \frac{5\pi}{6}\]
LaTeX source
\[
\frac{4\pi}{5} < \frac{2\pi}{3} \qquad \frac{\pi}{3} < \qquad \frac{4\pi}{5} \to \frac{\pi}{6} \;? \qquad \frac{4\pi}{5} \leqslant \frac{5\pi}{6}
\]\[\begin{array}{l} u \perp v' \\ u \perp w' \end{array} \qquad v'w' = \cos\frac{2\pi}{5}\]
LaTeX source
\[
\begin{array}{l} u \perp v' \\ u \perp w' \end{array} \qquad v'w' = \cos\frac{2\pi}{5}
\]\[\begin{aligned}
x(\alpha) &= u\cos\alpha + v'\sin\alpha \\
y(\alpha) &= u\cos\alpha + w'\sin\alpha
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
x(\alpha) &= u\cos\alpha + v'\sin\alpha \\
y(\alpha) &= u\cos\alpha + w'\sin\alpha
\end{aligned}
\]\[x(\alpha) - u = u(\cos\alpha - 1) + v'\sin\alpha\]
LaTeX source
\[ x(\alpha) - u = u(\cos\alpha - 1) + v'\sin\alpha \]
\[\begin{aligned}
\|x(\alpha) - u\|^{2} = \|y(\alpha) - u\|^{2} &= (\cos\alpha - 1)^{2} + \sin^{2}\alpha = 2 - 2\cos\alpha \\
&= 4\sin^{2}\frac{\alpha}{2} \qquad \Bigl(1 - \cos\alpha = 2\sin^{2}\frac{\alpha}{2}\Bigr)
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
\|x(\alpha) - u\|^{2} = \|y(\alpha) - u\|^{2} &= (\cos\alpha - 1)^{2} + \sin^{2}\alpha = 2 - 2\cos\alpha \\
&= 4\sin^{2}\frac{\alpha}{2} \qquad \Bigl(1 - \cos\alpha = 2\sin^{2}\frac{\alpha}{2}\Bigr)
\end{aligned}
\]\[\|x(\alpha) - u\| = 2\sin\frac{\alpha}{2}\]
LaTeX source
\[
\|x(\alpha) - u\| = 2\sin\frac{\alpha}{2}
\]\[\begin{aligned}
\|x(\alpha) - y(\alpha)\|^{2} &= \|v'\sin\alpha - w'\sin\alpha\|^{2} \\
&= \sin^{2}\alpha \, \|v' - w'\|^{2} = \sin^{2}\alpha \Bigl(2 - 2\cos\frac{2\pi}{5}\Bigr) \\
&\struck{= \sin^{2}\alpha + \sin^{2}\alpha - 2\cos\frac{2\pi}{5}\sin^{2}\alpha} \\
&= 4\sin^{2}\alpha \sin^{2}\frac{\pi}{5} \struck{= \ill{}}
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
\|x(\alpha) - y(\alpha)\|^{2} &= \|v'\sin\alpha - w'\sin\alpha\|^{2} \\
&= \sin^{2}\alpha \, \|v' - w'\|^{2} = \sin^{2}\alpha \Bigl(2 - 2\cos\frac{2\pi}{5}\Bigr) \\
&\struck{= \sin^{2}\alpha + \sin^{2}\alpha - 2\cos\frac{2\pi}{5}\sin^{2}\alpha} \\
&= 4\sin^{2}\alpha \sin^{2}\frac{\pi}{5} \struck{= \ill{}}
\end{aligned}
\]\[\|x(\alpha) - y(\alpha)\| = 2\sin\alpha \sin\frac{\pi}{5} = 4\sin\frac{\alpha}{2}\cos\frac{\alpha}{2}\sin\frac{\pi}{5}\]
LaTeX source
\[
\|x(\alpha) - y(\alpha)\| = 2\sin\alpha \sin\frac{\pi}{5} = 4\sin\frac{\alpha}{2}\cos\frac{\alpha}{2}\sin\frac{\pi}{5}
\]\[\|x(\alpha) - u\| = \|y(\alpha) - u\| = \|x(\alpha) - y(\alpha)\|\]
LaTeX source
\[ \|x(\alpha) - u\| = \|y(\alpha) - u\| = \|x(\alpha) - y(\alpha)\| \]
\[\Longleftrightarrow \quad 2\cos\frac{\alpha}{2}\sin\frac{\pi}{5} = 1 \quad \text{i.e.} \quad \boxed{\cos\frac{\alpha}{2} = \frac{1}{2\sin\pi/5}}\]
LaTeX source
\[
\Longleftrightarrow \quad 2\cos\frac{\alpha}{2}\sin\frac{\pi}{5} = 1 \quad \text{i.e.} \quad \boxed{\cos\frac{\alpha}{2} = \frac{1}{2\sin\pi/5}}
\]\[\begin{aligned}
(AB, A'B') &= P \\
(EC', CE') &= Q = \alpha(P) \\
(SD, S'D') &= R = \alpha(Q) = \alpha^{2}(P) \\
(AB, A'B') &= \uncertain{\alpha(R)} = \alpha^{2}(Q) = \alpha^{3}(P)
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
(AB, A'B') &= P \\
(EC', CE') &= Q = \alpha(P) \\
(SD, S'D') &= R = \alpha(Q) = \alpha^{2}(P) \\
(AB, A'B') &= \uncertain{\alpha(R)} = \alpha^{2}(Q) = \alpha^{3}(P)
\end{aligned}
\]\[\alpha D \longrightarrow D \qquad \begin{array}{cc} 30 & 15 \\ \uncertain{\alpha^{!}}? & \alpha \end{array}\]
LaTeX source
\[
\alpha D \longrightarrow D \qquad \begin{array}{cc} 30 & 15 \\ \uncertain{\alpha^{!}}? & \alpha \end{array}
\]\[G/\mathfrak{F}_2 \longrightarrow G/\mathfrak{F}_4 \qquad 2, 4, 3, 1\]
LaTeX source
\[
G/\mathfrak{F}_2 \longrightarrow G/\mathfrak{F}_4 \qquad 2, 4, 3, 1
\]\[\frac{\pi}{\uncertain{3}} \leqslant \frac{2\pi}{5} \leqslant \frac{5\pi}{6}
\qquad
\cos\alpha = \cos^{2}\frac{\alpha}{2} - \sin^{2}\frac{\alpha}{2} = 2\cos^{2}\frac{\alpha}{2} - 1 = \frac{1}{2\sin^{2}\theta} - 1 = 1 - 2\sin^{2}\theta = \cos 2\theta\]
LaTeX source
\[
\frac{\pi}{\uncertain{3}} \leqslant \frac{2\pi}{5} \leqslant \frac{5\pi}{6}
\qquad
\cos\alpha = \cos^{2}\frac{\alpha}{2} - \sin^{2}\frac{\alpha}{2} = 2\cos^{2}\frac{\alpha}{2} - 1 = \frac{1}{2\sin^{2}\theta} - 1 = 1 - 2\sin^{2}\theta = \cos 2\theta
\]\[u \to u\cos\alpha + v\sin\alpha \qquad v \to u(-\sin\alpha) + v\cos\alpha\]
LaTeX source
\[ u \to u\cos\alpha + v\sin\alpha \qquad v \to u(-\sin\alpha) + v\cos\alpha \]
\[\frac{1\,2\,3\,4\,\struck{0}}{2,4,1,3,0} \qquad \frac{}{3,1,4,2,0} \qquad \zeta \quad \zeta^{2}\]
LaTeX source
\[
\frac{1\,2\,3\,4\,\struck{0}}{2,4,1,3,0} \qquad \frac{}{3,1,4,2,0} \qquad \zeta \quad \zeta^{2}
\]\[u, 2u, 3u, 4u, 0 \qquad \zeta^{i} \qquad e^{i\theta} \qquad u^{2} + w^{2} = 1 \qquad \theta^{2} + \mu^{2} = 1 \qquad x^{2} - y^{2}\]
LaTeX source
\[
u, 2u, 3u, 4u, 0 \qquad \zeta^{i} \qquad e^{i\theta} \qquad u^{2} + w^{2} = 1 \qquad \theta^{2} + \mu^{2} = 1 \qquad x^{2} - y^{2}
\]\[g(\sigma . i) \qquad \rho(g)(\sigma . i) = \bigl(\rho(g)\ldots\bigr)\bigl(\rho(\ldots)\bigr) \qquad g(\sigma i) = g\sigma g^{-1}\, gi\]
LaTeX source
\[
g(\sigma . i) \qquad \rho(g)(\sigma . i) = \bigl(\rho(g)\ldots\bigr)\bigl(\rho(\ldots)\bigr) \qquad g(\sigma i) = g\sigma g^{-1}\, gi
\]\[G/H = X \ni e \qquad y e = a . e = a \qquad y x = y g e = g \uncertain{u} e = g' a e = \ill{}\]
LaTeX source
\[
G/H = X \ni e \qquad y e = a . e = a \qquad y x = y g e = g \uncertain{u} e = g' a e = \ill{}
\]\[b' = b h \qquad b^{-1} b' \in H \quad \Longrightarrow \quad (ba)^{-1} b' a \in H \quad \text{i.e.} \quad a^{-1} b^{-1} b' a \in H \quad \text{i.e.} \quad a^{-1} H a \subset H\]
LaTeX source
\[
b' = b h \qquad b^{-1} b' \in H \quad \Longrightarrow \quad (ba)^{-1} b' a \in H \quad \text{i.e.} \quad a^{-1} b^{-1} b' a \in H \quad \text{i.e.} \quad a^{-1} H a \subset H
\]\[\frac{N(H')}{\bigcap \operatorname{Conj} H} \qquad
N(H) \cap N(H') = N(\uncertain{H'}) \subset N(H) = \mathfrak{Z}_3 . \mathfrak{F}_2^{2}
\qquad
\begin{array}{ccc}
N(H') & \subset & N(H) \\
\cup & & \cup \\
H' & \subset & H \;\text{---}\; \mathfrak{F}_2^{2} \\
\cup & & \cup \\
K \cap H' = K'_0 & \subset & K' = 0
\end{array}\]
LaTeX source
\[
\frac{N(H')}{\bigcap \operatorname{Conj} H} \qquad
N(H) \cap N(H') = N(\uncertain{H'}) \subset N(H) = \mathfrak{Z}_3 . \mathfrak{F}_2^{2}
\qquad
\begin{array}{ccc}
N(H') & \subset & N(H) \\
\cup & & \cup \\
H' & \subset & H \;\text{---}\; \mathfrak{F}_2^{2} \\
\cup & & \cup \\
K \cap H' = K'_0 & \subset & K' = 0
\end{array}
\]\[\cos^{2}\alpha \cos\frac{2\pi}{5} = \cos\alpha \qquad 2\sin\frac{\alpha}{2}\sin\frac{2\pi}{5} = 1 \qquad \boxed{\cos\alpha = \frac{1}{2\sin\frac{2\pi}{\uncertain{10}}}}\]
LaTeX source
\[
\cos^{2}\alpha \cos\frac{2\pi}{5} = \cos\alpha \qquad 2\sin\frac{\alpha}{2}\sin\frac{2\pi}{5} = 1 \qquad \boxed{\cos\alpha = \frac{1}{2\sin\frac{2\pi}{\uncertain{10}}}}
\]\[1 + x + x^{2} + x^{3} + x^{4} = 0 \qquad \Bigl(2\sin\frac{\alpha}{2}\Bigr)\Bigl(2\sin^{2}\frac{\pi}{\uncertain{4}}\Bigr) \qquad \alpha = 60\,?\]
LaTeX source
\[
1 + x + x^{2} + x^{3} + x^{4} = 0 \qquad \Bigl(2\sin\frac{\alpha}{2}\Bigr)\Bigl(2\sin^{2}\frac{\pi}{\uncertain{4}}\Bigr) \qquad \alpha = 60\,?
\]\[\cos\frac{\alpha}{2} = \frac{\sqrt{3}}{2} \qquad \sqrt{3}\sin\frac{\pi}{5} = 1 \qquad \frac{\pi}{6}\]
LaTeX source
\[
\cos\frac{\alpha}{2} = \frac{\sqrt{3}}{2} \qquad \sqrt{3}\sin\frac{\pi}{5} = 1 \qquad \frac{\pi}{6}
\]\[\begin{array}{c}
\boldsymbol{\mu}_5 \\ \vert \\ \boldsymbol{\mu}_5^{*} \\ \vert \\ \mathbb{V}_5 \\ \vert \\ \mathbb{Z}[\tfrac{1}{4}]
\end{array}\]
LaTeX source
\[
\begin{array}{c}
\boldsymbol{\mu}_5 \\ \vert \\ \boldsymbol{\mu}_5^{*} \\ \vert \\ \mathbb{V}_5 \\ \vert \\ \mathbb{Z}[\tfrac{1}{4}]
\end{array}
\]\[\cos'(D_i, D_j)^2 + \cos'(D_i, D_j)\]
LaTeX source
\[ \cos'(D_i, D_j)^2 + \cos'(D_i, D_j) \]
\[1 - \gamma = \gamma^2, \qquad 2 - \gamma = 1 + \gamma^2, \qquad
\gamma^2 + \gamma - 1 = 0\]
LaTeX source
\[ 1 - \gamma = \gamma^2, \qquad 2 - \gamma = 1 + \gamma^2, \qquad \gamma^2 + \gamma - 1 = 0 \]
\[\cos\alpha = \frac{\struck{4}\gamma/2}{1 - \gamma/2} = \frac{\gamma}{2-\gamma}
= a + b\gamma = \frac{1}{5}(2\gamma + 1) = \frac{1}{\sqrt{5}}\]
LaTeX source
\[
\cos\alpha = \frac{\struck{4}\gamma/2}{1 - \gamma/2} = \frac{\gamma}{2-\gamma}
= a + b\gamma = \frac{1}{5}(2\gamma + 1) = \frac{1}{\sqrt{5}}
\]\[\begin{aligned}
\cos 2\alpha &= \cos^2\alpha - \sin^2\alpha = 2\cos^2\alpha - 1
= 2\,\frac{\gamma^2}{4 - 4\gamma + \gamma^2} - 1 \\
&= \frac{2(1-\gamma)}{4 - 4\gamma + 1 - \gamma} - 1
= \frac{2 - 2\gamma}{5(1-\gamma)} - 1 = \frac{2}{5} - 1 = -\frac{3}{5}
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
\cos 2\alpha &= \cos^2\alpha - \sin^2\alpha = 2\cos^2\alpha - 1
= 2\,\frac{\gamma^2}{4 - 4\gamma + \gamma^2} - 1 \\
&= \frac{2(1-\gamma)}{4 - 4\gamma + 1 - \gamma} - 1
= \frac{2 - 2\gamma}{5(1-\gamma)} - 1 = \frac{2}{5} - 1 = -\frac{3}{5}
\end{aligned}
\]\[\frac{2}{25}\,\underbrace{[4\gamma^2 + 4\gamma + 1]}_{4 - 4\gamma + 4\gamma + 1} - 1\]
LaTeX source
\[
\frac{2}{25}\,\underbrace{[4\gamma^2 + 4\gamma + 1]}_{4 - 4\gamma + 4\gamma + 1} - 1
\]\[\frac{B(x,y)^2}{Q(x)Q(y)} - 2 = -\frac{6}{5}
\qquad\qquad 2\cos 2\alpha = -\frac{6}{5}\]
LaTeX source
\[
\frac{B(x,y)^2}{Q(x)Q(y)} - 2 = -\frac{6}{5}
\qquad\qquad 2\cos 2\alpha = -\frac{6}{5}
\]\[\boxed{B(x,y)^2 = \frac{4}{5}\,Q(x)Q(y)}\]
LaTeX source
\[
\boxed{B(x,y)^2 = \frac{4}{5}\,Q(x)Q(y)}
\]\[2a + (2b - 1 \uncertain{-a})\gamma + b\gamma^2 = 0, \qquad
\gamma^2 + \Bigl(-2 + \frac{1}{b} + \frac{a}{b}\Bigr)\gamma - \frac{2a}{b} = 0\]
LaTeX source
\[
2a + (2b - 1 \uncertain{-a})\gamma + b\gamma^2 = 0, \qquad
\gamma^2 + \Bigl(-2 + \frac{1}{b} + \frac{a}{b}\Bigr)\gamma - \frac{2a}{b} = 0
\]\[-\frac{2a}{b} = -1, \quad \boxed{b = 2a}, \qquad
-2 + \frac{1}{2a} + \frac{1}{2} = 1, \qquad a = \frac{1}{5},\ b = \frac{2}{5}\]
LaTeX source
\[
-\frac{2a}{b} = -1, \quad \boxed{b = 2a}, \qquad
-2 + \frac{1}{2a} + \frac{1}{2} = 1, \qquad a = \frac{1}{5},\ b = \frac{2}{5}
\]\[\cos' 2\alpha = 2\cos 2\alpha = 2(2\cos^2\alpha - 1) = (2\cos\alpha)^2 - 2,
\qquad \frac{1}{2a} = \frac{5}{2}, \qquad a = \frac{1}{5}\]
LaTeX source
\[
\cos' 2\alpha = 2\cos 2\alpha = 2(2\cos^2\alpha - 1) = (2\cos\alpha)^2 - 2,
\qquad \frac{1}{2a} = \frac{5}{2}, \qquad a = \frac{1}{5}
\]\[\tfrac{1}{2}B = B' \qquad\qquad
\boxed{B'(x,y)^2 = \frac{1}{5}\,Q(x)Q(y)}\]
LaTeX source
\[
\tfrac{1}{2}B = B' \qquad\qquad
\boxed{B'(x,y)^2 = \frac{1}{5}\,Q(x)Q(y)}
\]\[\pi(f, g)^{*} = (u' \mapsto g^{*} \circ u' \circ f^{\circ}), \qquad
\pi(f, g)_{*} = (u' \mapsto g_{*} f_{*}^{(E)})\]
LaTeX source
\[
\pi(f, g)^{*} = (u' \mapsto g^{*} \circ u' \circ f^{\circ}), \qquad
\pi(f, g)_{*} = (u' \mapsto g_{*} f_{*}^{(E)})
\]\[\pi(f, g) : \pi(C, E) \longrightarrow \pi(\uncertain{C'}, E')\]
LaTeX source
\[
\pi(f, g) : \pi(C, E) \longrightarrow \pi(\uncertain{C'}, E')
\]\[\text{(1)}\qquad
\boxed{\gamma = \gamma(C, E) : \pi(C, E) \longrightarrow \hat{C} \times_{\mathrm{top}} E}\]
LaTeX source
\[
\text{(1)}\qquad
\boxed{\gamma = \gamma(C, E) : \pi(C, E) \longrightarrow \hat{C} \times_{\mathrm{top}} E}
\]\[\begin{aligned}
\gamma_1 &= \gamma_1(C, E) : \pi(C, E) \to \hat{C} \\
\gamma_2 &= \gamma_2(C, E) : \pi(C, E) \to E
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
\gamma_1 &= \gamma_1(C, E) : \pi(C, E) \to \hat{C} \\
\gamma_2 &= \gamma_2(C, E) : \pi(C, E) \to E
\end{aligned}
\]\[\gamma_1^{*} : \hat{C} \to \pi(C, E) \quad \text{défini par} \quad
F \mapsto [X \mapsto F(X)_E]\]
LaTeX source
\[
\gamma_1^{*} : \hat{C} \to \pi(C, E) \quad \text{défini par} \quad
F \mapsto [X \mapsto F(X)_E]
\]\[\gamma_2^{*} : E \to \pi(C, E), \qquad X \mapsto (i \mapsto X)\]
LaTeX source
\[
\gamma_2^{*} : E \to \pi(C, E), \qquad X \mapsto (i \mapsto X)
\]\[\omega(\varphi) = (\omega_x(\varphi))_{x \in X'_0} \in \prod_{x \in X'_0} \Omega_x(X)\]
LaTeX source
\[
\omega(\varphi) = (\omega_x(\varphi))_{x \in X'_0} \in \prod_{x \in X'_0} \Omega_x(X)
\]\[\mathrm{Pl}_{\mathrm{isot}}(X, S) \xrightarrow{\ \omega\ } \prod_{x \in X'_0} \Omega_x(X)
\overset{\mathrm{df}}{=} \Omega(X)\]
LaTeX source
\[
\mathrm{Pl}_{\mathrm{isot}}(X, S) \xrightarrow{\ \omega\ } \prod_{x \in X'_0} \Omega_x(X)
\overset{\mathrm{df}}{=} \Omega(X)
\]\[\mathrm{Pl}^{\alpha}_{\mathrm{isot}}(X, S) \longrightarrow
\mathrm{Pl}_{\mathrm{isot}}(\mathcal{U}_{\alpha}, S)\]
LaTeX source
\[
\mathrm{Pl}^{\alpha}_{\mathrm{isot}}(X, S) \longrightarrow
\mathrm{Pl}_{\mathrm{isot}}(\mathcal{U}_{\alpha}, S)
\]\[I \times S^1 \qquad (I = \pi_0(\mathcal{V}_{\alpha}))\]
LaTeX source
\[
I \times S^1 \qquad (I = \pi_0(\mathcal{V}_{\alpha}))
\]\[\mathcal{U}'_{\lambda} = S_g - \bigcup_{j \in I_{\lambda}} \mathring{D}_j - P_{\lambda}\]
LaTeX source
\[
\mathcal{U}'_{\lambda} = S_g - \bigcup_{j \in I_{\lambda}} \mathring{D}_j - P_{\lambda}
\]\[\begin{cases}
\alpha \in \Omega(X) & [\text{d'où } I = I(\alpha), \text{ à expliciter combinatoirement}] \\
\pi \text{ partition de } I \text{ en } (I_{\lambda})_{\lambda \in \Lambda} & \\
(g_{\lambda})_{\lambda \in \Lambda} \in \mathbb{N}^{\Lambda} & \\
(\beta_{\lambda})_{\lambda \in \Lambda} \in \mathbb{N}^{\Lambda} &
\end{cases}\]
LaTeX source
\[
\begin{cases}
\alpha \in \Omega(X) & [\text{d'où } I = I(\alpha), \text{ à expliciter combinatoirement}] \\
\pi \text{ partition de } I \text{ en } (I_{\lambda})_{\lambda \in \Lambda} & \\
(g_{\lambda})_{\lambda \in \Lambda} \in \mathbb{N}^{\Lambda} & \\
(\beta_{\lambda})_{\lambda \in \Lambda} \in \mathbb{N}^{\Lambda} &
\end{cases}
\]\[X \xrightarrow{\ \varphi_{\alpha, \pi, g, \beta}\ } S_{\alpha, \pi, g, \beta}\]
LaTeX source
\[
X \xrightarrow{\ \varphi_{\alpha, \pi, g, \beta}\ } S_{\alpha, \pi, g, \beta}
\]\[\mathrm{Pl}_{\mathrm{isot}}(X, S) \longrightarrow
\text{l'ensemble des systèmes } \alpha, \pi, g, \nu \text{ associés à } X\]
LaTeX source
\[
\mathrm{Pl}_{\mathrm{isot}}(X, S) \longrightarrow
\text{l'ensemble des systèmes } \alpha, \pi, g, \nu \text{ associés à } X
\]\[(*)\qquad
\mathrm{Isot}(S_{\rho}, S) \xrightarrow{\ r\ } \mathrm{Pl}_{\mathrm{isot}}(X, S; \rho)\]
LaTeX source
\[
(*)\qquad
\mathrm{Isot}(S_{\rho}, S) \xrightarrow{\ r\ } \mathrm{Pl}_{\mathrm{isot}}(X, S; \rho)
\]\[G = \mathrm{Isot}_{o}(S, S) \qquad [\simeq G_{\rho} = \mathrm{Isot}_{o}(S_{\rho}, S_{\rho})]\]
LaTeX source
\[
G = \mathrm{Isot}_{o}(S, S) \qquad [\simeq G_{\rho} = \mathrm{Isot}_{o}(S_{\rho}, S_{\rho})]
\]\[G \longrightarrow \mathrm{Autext}(\pi_1(S, s))\]
LaTeX source
\[
G \longrightarrow \mathrm{Autext}(\pi_1(S, s))
\]\[h\varphi \underset{\mathrm{isot}}{\simeq} \varphi \;\Longrightarrow\;
h\varphi \underset{\mathrm{homot}}{\simeq} \varphi\]
LaTeX source
\[
h\varphi \underset{\mathrm{isot}}{\simeq} \varphi \;\Longrightarrow\;
h\varphi \underset{\mathrm{homot}}{\simeq} \varphi
\]\[\pi_1(h) \circ c \simeq c \quad \text{mod automorphismes intérieurs}\]
LaTeX source
\[
\pi_1(h) \circ c \simeq c \quad \text{mod automorphismes intérieurs}
\]\[\pi_1(h \varphi_i) = \pi_1(h) \circ \pi_1(\varphi_i) \in
\struck{\ill{}}\ \mathrm{Homext}(\pi_1(X_i), \pi_1(S))\]
LaTeX source
\[
\pi_1(h \varphi_i) = \pi_1(h) \circ \pi_1(\varphi_i) \in
\struck{\ill{}}\ \mathrm{Homext}(\pi_1(X_i), \pi_1(S))
\]\[\mathcal{G}/\mathcal{H} \simeq \mathfrak{X} \qquad
\pi_1(\mathcal{H}) \to \pi_1(\mathcal{G}) \to \pi_1(\mathfrak{X}) \to
\pi_0(\mathcal{H}) \to \pi_0(\mathcal{G}) \to \pi_0(\mathfrak{X})\]
LaTeX source
\[
\mathcal{G}/\mathcal{H} \simeq \mathfrak{X} \qquad
\pi_1(\mathcal{H}) \to \pi_1(\mathcal{G}) \to \pi_1(\mathfrak{X}) \to
\pi_0(\mathcal{H}) \to \pi_0(\mathcal{G}) \to \pi_0(\mathfrak{X})
\]\[\mathcal{H} = \mathrm{Aut}(S / X)\]
LaTeX source
\[
\mathcal{H} = \mathrm{Aut}(S / X)
\]\[\text{Graphes}\quad
(S, A, A' \xrightarrow{\ \varphi = (\varphi_1, \varphi_2) = (\varphi_1, \varphi_1 \circ \sigma)\ } S \times S, \sigma)
\;\;\langle\simeq\rangle\;\;
(S, R \subset A \times A, L \to A, \sigma)\]
LaTeX source
\[
\text{Graphes}\quad
(S, A, A' \xrightarrow{\ \varphi = (\varphi_1, \varphi_2) = (\varphi_1, \varphi_1 \circ \sigma)\ } S \times S, \sigma)
\;\;\langle\simeq\rangle\;\;
(S, R \subset A \times A, L \to A, \sigma)
\]\[\mathrm{Aut}\,\Gamma = \mathrm{Perm}(S) \times \underbrace{\mathrm{Aut}(A, \sigma)}\]
LaTeX source
\[
\mathrm{Aut}\,\Gamma = \mathrm{Perm}(S) \times \underbrace{\mathrm{Aut}(A, \sigma)}
\]\[\varphi : A \longrightarrow S\]
LaTeX source
\[ \varphi : A \longrightarrow S \]
\[\left\{
\begin{array}{l}
\boxed{G \supset H' \supset H} \quad \text{et} \\
\boxed{\dot{\sigma} \in (H' \cap \mathrm{Norm}_G(H))/H \qquad \dot{\sigma}^2 = 1,\ \dot{\sigma} \neq 1}
\end{array}
\right.\]
LaTeX source
\[
\left\{
\begin{array}{l}
\boxed{G \supset H' \supset H} \quad \text{et} \\
\boxed{\dot{\sigma} \in (H' \cap \mathrm{Norm}_G(H))/H \qquad \dot{\sigma}^2 = 1,\ \dot{\sigma} \neq 1}
\end{array}
\right.
\]\[\bigcap_{g \in G} g H g^{-1} = \{1\}\]
LaTeX source
\[
\bigcap_{g \in G} g H g^{-1} = \{1\}
\]\[\underset{a}{A} \xrightarrow[\text{source}]{\ \varphi_1\ } \underset{s}{S}, \qquad
\left\{
\begin{array}{l}
\sigma : A \to A \\
\sigma^2 = \mathrm{id},\ \sigma \text{ ss pt fixe}
\end{array}
\right.\]
LaTeX source
\[
\underset{a}{A} \xrightarrow[\text{source}]{\ \varphi_1\ } \underset{s}{S}, \qquad
\left\{
\begin{array}{l}
\sigma : A \to A \\
\sigma^2 = \mathrm{id},\ \sigma \text{ ss pt fixe}
\end{array}
\right.
\]\[\boxed{G \supset \underset{G_a}{H'} \supset \underset{G_s}{H} \qquad
\dot{\sigma} \in \mathrm{Norm}_G(H)/H \qquad \dot{\sigma}^2 = 1 \qquad
\dot{\sigma} \neq 1}\]
LaTeX source
\[
\boxed{G \supset \underset{G_a}{H'} \supset \underset{G_s}{H} \qquad
\dot{\sigma} \in \mathrm{Norm}_G(H)/H \qquad \dot{\sigma}^2 = 1 \qquad
\dot{\sigma} \neq 1}
\]\[\boxed{\bigcap_{g \in G} g^{-1} H g = \{1\}}\]
LaTeX source
\[
\boxed{\bigcap_{g \in G} g^{-1} H g = \{1\}}
\]\[\begin{aligned}
G/H &\longrightarrow G/H' \times G/H' \\
gH &\longmapsto gH',\ g\sigma H'
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
G/H &\longrightarrow G/H' \times G/H' \\
gH &\longmapsto gH',\ g\sigma H'
\end{aligned}
\]\[\boxed{H' \cap \dot{\sigma}^{-1} H' \dot{\sigma} \subset H}\]
LaTeX source
\[
\boxed{H' \cap \dot{\sigma}^{-1} H' \dot{\sigma} \subset H}
\]