Cote n° 159 · pages 1–33
· 175 displayed formulas · Connexions projectives et uniformisation : notes manuscrites (s.d.).
Inventory dating : s.d.
Édition de démonstration
\[\mathrm{Aff}(r) \;=\; \mathrm{GL}(r)\cdot E^{r}\]
LaTeX source
\[
\mathrm{Aff}(r) \;=\; \mathrm{GL}(r)\cdot E^{r}
\]\[{\scriptstyle r+1}
\left\{
\begin{pmatrix} A & C \\ 0 & 1 \end{pmatrix}
\right\}
{\scriptstyle r}\]
LaTeX source
\[
{\scriptstyle r+1}
\left\{
\begin{pmatrix} A & C \\ 0 & 1 \end{pmatrix}
\right\}
{\scriptstyle r}
\]\[0 \longrightarrow \Omega \longrightarrow E \longrightarrow
\underline{O}_S \longrightarrow 0\]
LaTeX source
\[
0 \longrightarrow \Omega \longrightarrow E \longrightarrow
\underline{O}_S \longrightarrow 0
\]\[0 \longrightarrow \Omega \longrightarrow E \xrightarrow{\;p\;}
\underline{O}_S \longrightarrow 0\]
LaTeX source
\[
0 \longrightarrow \Omega \longrightarrow E \xrightarrow{\;p\;}
\underline{O}_S \longrightarrow 0
\]\[\widehat{S} = \underline{O}_{\widehat{P}}\]
LaTeX source
\[
\widehat{S} = \underline{O}_{\widehat{P}}
\]\[E^{\circ} \simeq \Omega \times \underline{O}_S\]
LaTeX source
\[
E^{\circ} \simeq \Omega \times \underline{O}_S
\]\[\widehat{P}(S') \;\simeq\; \text{Quotients inversibles } L' \text{ de } E,\]
LaTeX source
\[
\widehat{P}(S') \;\simeq\; \text{Quotients inversibles } L' \text{ de } E,
\]\[(x,\lambda) \longmapsto \varphi(x) + \lambda, \qquad
\varphi : \Omega \longrightarrow \underline{O}_S\]
LaTeX source
\[
(x,\lambda) \longmapsto \varphi(x) + \lambda, \qquad
\varphi : \Omega \longrightarrow \underline{O}_S
\]\[\widehat{P}^{\circ} = V(\Omega)^{\wedge} \quad
\text{(complété formel le long de la section nulle)}\]
LaTeX source
\[
\widehat{P}^{\circ} = V(\Omega)^{\wedge} \quad
\text{(complété formel le long de la section nulle)}
\]\[= \mathrm{Spf}\;\widehat{\mathrm{Sym}}(\Omega)
\;=\; \widehat{S}^{\circ}\]
LaTeX source
\[
= \mathrm{Spf}\;\widehat{\mathrm{Sym}}(\Omega)
\;=\; \widehat{S}^{\circ}
\]\[u_a(x,\lambda) = (x + \lambda a,\; \lambda)\]
LaTeX source
\[ u_a(x,\lambda) = (x + \lambda a,\; \lambda) \]
\[\widetilde{\varphi} \circ u_a : (x,\lambda) \longrightarrow
\varphi(x + \lambda a) + \lambda
= \varphi(x) + (1 + \varphi(a))\lambda
= (1 + \varphi(a))\left( \frac{\varphi}{1 + \varphi(a)}(x) + \lambda \right),\]
LaTeX source
\[
\widetilde{\varphi} \circ u_a : (x,\lambda) \longrightarrow
\varphi(x + \lambda a) + \lambda
= \varphi(x) + (1 + \varphi(a))\lambda
= (1 + \varphi(a))\left( \frac{\varphi}{1 + \varphi(a)}(x) + \lambda \right),
\]\[\varphi^a = u_a^{*}(\varphi) = \frac{\varphi}{1 + \varphi(a)}\]
LaTeX source
\[
\varphi^a = u_a^{*}(\varphi) = \frac{\varphi}{1 + \varphi(a)}
\]\[\varphi^a(\omega) = \frac{\varphi(\omega)}{1 + \varphi(a)}
= \varphi\Big( \sum_{n \geqslant 0} (-1)^n \omega a^n \Big),\]
LaTeX source
\[
\varphi^a(\omega) = \frac{\varphi(\omega)}{1 + \varphi(a)}
= \varphi\Big( \sum_{n \geqslant 0} (-1)^n \omega a^n \Big),
\]\[\varphi^a(\omega) = \varphi(u_a(\omega))\]
LaTeX source
\[ \varphi^a(\omega) = \varphi(u_a(\omega)) \]
\[u_a(\omega) = \struck{\ill{}} \frac{\omega}{1+a}
= \sum_{n \geqslant 0} (-1)^n \omega a^n\]
LaTeX source
\[
u_a(\omega) = \struck{\ill{}} \frac{\omega}{1+a}
= \sum_{n \geqslant 0} (-1)^n \omega a^n
\]\[E \otimes_{\underline{O}_S} \widehat{S} \longrightarrow \widehat{L}
\simeq \widehat{S}\]
LaTeX source
\[
E \otimes_{\underline{O}_S} \widehat{S} \longrightarrow \widehat{L}
\simeq \widehat{S}
\]\[\pi(\omega \otimes f,\, g) = \omega f + g,
\qquad \omega \in \Omega(S),\; f,g \in \widehat{S}(S).\]
LaTeX source
\[
\pi(\omega \otimes f,\, g) = \omega f + g,
\qquad \omega \in \Omega(S),\; f,g \in \widehat{S}(S).
\]\[\omega \otimes f + e \otimes g,
\qquad \omega \in \Omega(S),\;\; f,g \in \widehat{S}(S),\]
LaTeX source
\[
\omega \otimes f + e \otimes g,
\qquad \omega \in \Omega(S),\;\; f,g \in \widehat{S}(S),
\]\[u_{a*}^{\widehat{E}}(\omega \otimes f + e \otimes g)
= u_a(\omega) \otimes u_{a*}(f) + u_a(e) \otimes u_{a*}(g)\]
LaTeX source
\[
u_{a*}^{\widehat{E}}(\omega \otimes f + e \otimes g)
= u_a(\omega) \otimes u_{a*}(f) + u_a(e) \otimes u_{a*}(g)
\]\[= \omega \otimes u_{a*}(f) + (e + a) \otimes u_{a*}(g)\]
LaTeX source
\[
= \omega \otimes u_{a*}(f) + (e + a) \otimes u_{a*}(g)
\]\[= \big( \omega \otimes u_{a*}(f) + a \otimes u_{a*}(g) \big)
+ e \otimes u_{a*}(g)\]
LaTeX source
\[
= \big( \omega \otimes u_{a*}(f) + a \otimes u_{a*}(g) \big)
+ e \otimes u_{a*}(g)
\]\[\pi\big( u_{a*}^{\widehat{E}}(\omega \otimes f + e \otimes g) \big)
= \omega\, u_{a*}(f) + a\, u_{a*}(g) + u_{a*}(g)\]
LaTeX source
\[
\pi\big( u_{a*}^{\widehat{E}}(\omega \otimes f + e \otimes g) \big)
= \omega\, u_{a*}(f) + a\, u_{a*}(g) + u_{a*}(g)
\]\[= \omega\, u_{a*}(f) + (a+1)\, u_{a*}(g)\]
LaTeX source
\[
= \omega\, u_{a*}(f) + (a+1)\, u_{a*}(g)
\]\[\pi(\omega \otimes f + e \otimes g) = \omega f + g .\]
LaTeX source
\[ \pi(\omega \otimes f + e \otimes g) = \omega f + g . \]
\[u_{a*}^{\widehat{L}}(g) = (a+1)\, u_{a*}(g)
\qquad \Big( = \frac{g}{(1+a)^{\,n-1}} \;\text{ si } \deg g = n \Big)\]
LaTeX source
\[
u_{a*}^{\widehat{L}}(g) = (a+1)\, u_{a*}(g)
\qquad \Big( = \frac{g}{(1+a)^{\,n-1}} \;\text{ si } \deg g = n \Big)
\]\[u_{a*}^{\widehat{L}}\big( \pi(\omega \otimes f + e \otimes g) \big)
= (a+1)\, u_{a*}(\omega f + g)\]
LaTeX source
\[
u_{a*}^{\widehat{L}}\big( \pi(\omega \otimes f + e \otimes g) \big)
= (a+1)\, u_{a*}(\omega f + g)
\]\[= (a+1) \big( u_{a*}(\omega)\, u_{a*}(f) + u_{a*}(g) \big)\]
LaTeX source
\[
= (a+1) \big( u_{a*}(\omega)\, u_{a*}(f) + u_{a*}(g) \big)
\]\[= \omega\, u_{a*}(f) + (a+1)\, u_{a*}(g) \qquad \text{OK}\]
LaTeX source
\[
= \omega\, u_{a*}(f) + (a+1)\, u_{a*}(g) \qquad \text{OK}
\]\[\widehat{S} = \struck{\ill{}}\;
T \wedge^{(\Omega,\, u^{\widehat{L}}_{\Omega*})}
\widehat{\mathrm{Sym}}(\Omega)\]
LaTeX source
\[
\widehat{S} = \struck{\ill{}}\;
T \wedge^{(\Omega,\, u^{\widehat{L}}_{\Omega*})}
\widehat{\mathrm{Sym}}(\Omega)
\]\[\widehat{L} =
T \wedge^{(\Omega,\, u^{\widehat{L}}_{\Omega*})}
\widehat{\mathrm{Sym}}(\Omega)\]
LaTeX source
\[
\widehat{L} =
T \wedge^{(\Omega,\, u^{\widehat{L}}_{\Omega*})}
\widehat{\mathrm{Sym}}(\Omega)
\]\[\mathrm{gr}^1_{\widehat{J}}(\widehat{S}) \simeq \Omega\]
LaTeX source
\[
\mathrm{gr}^1_{\widehat{J}}(\widehat{S}) \simeq \Omega
\]\[\big( \mathrm{gr}_{\widehat{J}}(\widehat{S})
\simeq \widehat{\mathrm{Sym}}(\Omega) \big)\]
LaTeX source
\[
\big( \mathrm{gr}_{\widehat{J}}(\widehat{S})
\simeq \widehat{\mathrm{Sym}}(\Omega) \big)
\]\[f + g \;\longrightarrow\; \frac{f}{(1+a)^{n}} + \frac{g}{(1+a)^{n+1}}\]
LaTeX source
\[
f + g \;\longrightarrow\; \frac{f}{(1+a)^{n}} + \frac{g}{(1+a)^{n+1}}
\]\[f \;\longmapsto\; naf + g + \text{termes de degré } \geqslant n + 1\]
LaTeX source
\[
f \;\longmapsto\; naf + g + \text{termes de degré } \geqslant n + 1
\]\[\Omega \;\longrightarrow\; \mathrm{Hom}\big( \mathrm{Sym}^n \Omega,\;
\mathrm{Sym}^{n+1} \Omega \big)\]
LaTeX source
\[
\Omega \;\longrightarrow\; \mathrm{Hom}\big( \mathrm{Sym}^n \Omega,\;
\mathrm{Sym}^{n+1} \Omega \big)
\]\[v(a)(f) = af\]
LaTeX source
\[ v(a)(f) = af \]
\[T \times_{\Omega} \big[ \mathrm{Hom}\big( \mathrm{Sym}^n \Omega,\;
\mathrm{Sym}^{n+m} \Omega \big) \big]\]
LaTeX source
\[
T \times_{\Omega} \big[ \mathrm{Hom}\big( \mathrm{Sym}^n \Omega,\;
\mathrm{Sym}^{n+m} \Omega \big) \big]
\]\[0 \longrightarrow \Omega \longrightarrow E \longrightarrow
\underline{O}_X \longrightarrow 0\]
LaTeX source
\[
0 \longrightarrow \Omega \longrightarrow E \longrightarrow
\underline{O}_X \longrightarrow 0
\]\[P^n_{X/S} \;\simeq\; \underline{O}_{\widehat{P}}
\big/ \widehat{J}^{\,n+1}
\qquad \big( \simeq \underline{O}_X \otimes_{\Omega}
\mathrm{Sym}^{\bullet}(\Omega) \big)\]
LaTeX source
\[
P^n_{X/S} \;\simeq\; \underline{O}_{\widehat{P}}
\big/ \widehat{J}^{\,n+1}
\qquad \big( \simeq \underline{O}_X \otimes_{\Omega}
\mathrm{Sym}^{\bullet}(\Omega) \big)
\]\[(*) \qquad \Omega \;\simeq\; \Omega^1_{X/S}\]
LaTeX source
\[
(*) \qquad \Omega \;\simeq\; \Omega^1_{X/S}
\]\[\Omega \xrightarrow{\;-u_1\;}
\mathrm{Hom}\big( \Omega,\ \mathrm{Sym}^2(\Omega) \big)\]
LaTeX source
\[
\Omega \xrightarrow{\;-u_1\;}
\mathrm{Hom}\big( \Omega,\ \mathrm{Sym}^2(\Omega) \big)
\]\[\mathrm{Hom}\big( \Omega^1_{X/S},\ \mathrm{Sym}^2 \Omega^1_{X/S} \big)\]
LaTeX source
\[
\mathrm{Hom}\big( \Omega^1_{X/S},\ \mathrm{Sym}^2 \Omega^1_{X/S} \big)
\]\[P^{\infty}_{X/S} \simeq \underline{O}_S[[\delta f_1, \ldots]]\]
LaTeX source
\[
P^{\infty}_{X/S} \simeq \underline{O}_S[[\delta f_1, \ldots]]
\]\[\Delta : P^{\infty}_{X/S} \longrightarrow
P^{\infty}_{X/S} \otimes_S P^{\infty}_{X/S}
= P^{\infty}_{X/S}\big( P^{\infty}_{X/S} \big)
\simeq P^{\infty}_{X/X}[[\ldots\]
LaTeX source
\[
\Delta : P^{\infty}_{X/S} \longrightarrow
P^{\infty}_{X/S} \otimes_S P^{\infty}_{X/S}
= P^{\infty}_{X/S}\big( P^{\infty}_{X/S} \big)
\simeq P^{\infty}_{X/X}[[\ldots
\]\[\Delta(\delta f_i) = \delta(f_i) \otimes 1 + 1 \otimes \delta(f_i)
= \delta(f_i) + \delta f_i\]
LaTeX source
\[ \Delta(\delta f_i) = \delta(f_i) \otimes 1 + 1 \otimes \delta(f_i) = \delta(f_i) + \delta f_i \]
\[M \otimes P^n_{X/S} \longrightarrow P^n_{X/S} \otimes M\]
LaTeX source
\[
M \otimes P^n_{X/S} \longrightarrow P^n_{X/S} \otimes M
\]\[M \xrightarrow{\;\Delta\;} P^n_{X/S} \otimes M\]
LaTeX source
\[
M \xrightarrow{\;\Delta\;} P^n_{X/S} \otimes M
\]\[\Delta(m) = m + \Sigma\]
LaTeX source
\[ \Delta(m) = m + \Sigma \]
\[F_i \in \Gamma\, P^{\infty}_{X/S}
= \Gamma\, \underline{O}_S[[\delta f_1, \ldots, \delta f_n]],
\qquad 1 \leqslant i \leqslant n\]
LaTeX source
\[
F_i \in \Gamma\, P^{\infty}_{X/S}
= \Gamma\, \underline{O}_S[[\delta f_1, \ldots, \delta f_n]],
\qquad 1 \leqslant i \leqslant n
\]\[F_i = \delta f_i + G_i, \qquad G_i \text{ d'ordre } \geqslant 2\]
LaTeX source
\[
F_i = \delta f_i + G_i, \qquad G_i \text{ d'ordre } \geqslant 2
\]\[\Phi_i \in \Gamma\, \widehat{\mathrm{Sym}}\;
\underline{O}_S[[T_1, \ldots, T_n]],
\qquad 1 \leqslant i \leqslant n\]
LaTeX source
\[
\Phi_i \in \Gamma\, \widehat{\mathrm{Sym}}\;
\underline{O}_S[[T_1, \ldots, T_n]],
\qquad 1 \leqslant i \leqslant n
\]\[\Phi_i = T_i + \Psi_i \qquad (\Psi_i \text{ d'ordre } \geqslant 2)\]
LaTeX source
\[
\Phi_i = T_i + \Psi_i \qquad (\Psi_i \text{ d'ordre } \geqslant 2)
\]\[\underline{O}_S[[T_1, \struck{\delta f}]] = \widehat{S}
\xrightarrow{\;\Delta'\;} P^{\infty}_{X/S} \widehat{\otimes} \widehat{S}
= P^{\infty}_{X/S}(\widehat{S}) \simeq P^{\infty}_{X/S}[[T \ldots\]
LaTeX source
\[
\underline{O}_S[[T_1, \struck{\delta f}]] = \widehat{S}
\xrightarrow{\;\Delta'\;} P^{\infty}_{X/S} \widehat{\otimes} \widehat{S}
= P^{\infty}_{X/S}(\widehat{S}) \simeq P^{\infty}_{X/S}[[T \ldots
\]\[\Delta(\struck{\ill{}}\; \delta f_i + G_i) \in \Gamma\, P^{\infty}_{X/S}\]
LaTeX source
\[
\Delta(\struck{\ill{}}\; \delta f_i + G_i) \in \Gamma\, P^{\infty}_{X/S}
\]\[c_{\infty} : P^{\infty}_{X/S} \longrightarrow \widehat{S}.\]
LaTeX source
\[
c_{\infty} : P^{\infty}_{X/S} \longrightarrow \widehat{S}.
\]\[\Omega^1_{X/S} = \omega, \qquad f_*(\omega) = \Omega, \qquad
R^1 f_*\big( \Omega^{\bullet}_{X/k} \big) = DR\]
LaTeX source
\[
\Omega^1_{X/S} = \omega, \qquad f_*(\omega) = \Omega, \qquad
R^1 f_*\big( \Omega^{\bullet}_{X/k} \big) = DR
\]\[R^1 f_*(\underline{O}_X) \simeq \check{\Omega} \simeq \tau\]
LaTeX source
\[
R^1 f_*(\underline{O}_X) \simeq \check{\Omega} \simeq \tau
\]\[0 \longrightarrow \Omega \longrightarrow DR \longrightarrow
\check{\Omega} \longrightarrow 0\]
LaTeX source
\[
0 \longrightarrow \Omega \longrightarrow DR \longrightarrow
\check{\Omega} \longrightarrow 0
\]\[DR \times DR \xrightarrow{\;q\;} \underline{O}_S \qquad \text{alternée}\]
LaTeX source
\[
DR \times DR \xrightarrow{\;q\;} \underline{O}_S \qquad \text{alternée}
\]\[b = R^2 f_*\big( \Omega^{\bullet}_{X/S} \big)
\simeq R^1 f_*\big( \Omega^1_{X/S} \big)\]
LaTeX source
\[
b = R^2 f_*\big( \Omega^{\bullet}_{X/S} \big)
\simeq R^1 f_*\big( \Omega^1_{X/S} \big)
\]\[0 \longrightarrow \check{\Omega} \otimes \check{\Omega} \longrightarrow
\Sigma \longrightarrow \underline{O}_S \longrightarrow 0\]
LaTeX source
\[
0 \longrightarrow \check{\Omega} \otimes \check{\Omega} \longrightarrow
\Sigma \longrightarrow \underline{O}_S \longrightarrow 0
\]\[\Lambda^2 DR \xrightarrow{\;q\;} \underline{O}_S\]
LaTeX source
\[
\Lambda^2 DR \xrightarrow{\;q\;} \underline{O}_S
\]\[0 \longrightarrow \mathrm{Fil}^2 \longrightarrow \mathrm{Fil}^1
\longrightarrow \Lambda^2 DR\]
LaTeX source
\[
0 \longrightarrow \mathrm{Fil}^2 \longrightarrow \mathrm{Fil}^1
\longrightarrow \Lambda^2 DR
\]\[\begin{pmatrix} 0 & \pm\,\mathrm{id} \\ \mathrm{id} & \varphi_0 \end{pmatrix}\]
LaTeX source
\[
\begin{pmatrix} 0 & \pm\,\mathrm{id} \\ \mathrm{id} & \varphi_0 \end{pmatrix}
\]\[q'(t) = q(t) + u(t) \qquad \big( u : \check{\Omega} \to \Omega \big)\]
LaTeX source
\[
q'(t) = q(t) + u(t) \qquad \big( u : \check{\Omega} \to \Omega \big)
\]\[\varphi'_0(t,t') = \varphi\big( q(t) + u(t),\; q(t') + u(t') \big)\]
LaTeX source
\[ \varphi'_0(t,t') = \varphi\big( q(t) + u(t),\; q(t') + u(t') \big) \]
\[= \varphi_0(t,t') + \big( t,\, u(t') \big) - \big( t',\, u(t) \big)\]
LaTeX source
\[ = \varphi_0(t,t') + \big( t,\, u(t') \big) - \big( t',\, u(t) \big) \]
\[0 \longrightarrow \Lambda^2 \Omega \longrightarrow \Sigma \longrightarrow
\underline{O}_S \longrightarrow 0\]
LaTeX source
\[
0 \longrightarrow \Lambda^2 \Omega \longrightarrow \Sigma \longrightarrow
\underline{O}_S \longrightarrow 0
\]\[DR \longrightarrow DR \otimes \Omega^1_{S/T}\]
LaTeX source
\[
DR \longrightarrow DR \otimes \Omega^1_{S/T}
\]\[\Omega \longrightarrow \check{\Omega} \otimes \Omega^1_{S/T}\]
LaTeX source
\[
\Omega \longrightarrow \check{\Omega} \otimes \Omega^1_{S/T}
\]\[\Omega^1_{S/T} \longrightarrow \check{\Omega} \otimes \check{\Omega}\]
LaTeX source
\[
\Omega^1_{S/T} \longrightarrow \check{\Omega} \otimes \check{\Omega}
\]\[\Omega^1_{S/T} \longrightarrow \Lambda^2 \check{\Omega}\]
LaTeX source
\[
\Omega^1_{S/T} \longrightarrow \Lambda^2 \check{\Omega}
\]\[H^0(X, \Omega_X)\]
LaTeX source
\[ H^0(X, \Omega_X) \]
\[0 \longrightarrow \Omega^1_X \xrightarrow{\;\omega\;} \Omega_X
\xrightarrow{\;\det\;} \Omega^1_X \longrightarrow (DR)_X\]
LaTeX source
\[
0 \longrightarrow \Omega^1_X \xrightarrow{\;\omega\;} \Omega_X
\xrightarrow{\;\det\;} \Omega^1_X \longrightarrow (DR)_X
\]\[0 \longrightarrow \Gamma^2 \Omega \longrightarrow \Omega \otimes \Omega
\longrightarrow \Lambda^2 \Omega \longrightarrow 0\]
LaTeX source
\[ 0 \longrightarrow \Gamma^2 \Omega \longrightarrow \Omega \otimes \Omega \longrightarrow \Lambda^2 \Omega \longrightarrow 0 \]
\[f_*(\omega^2) \;\simeq\; \Omega^1_{S/T}\]
LaTeX source
\[
f_*(\omega^2) \;\simeq\; \Omega^1_{S/T}
\]\[\frac{g(g+1)}{2} - (3g-3) \;=\; \frac{1}{2}\big( g^2 - 5g + 6 \big)
\;=\; \frac{1}{2}(g-2)(g-3)\]
LaTeX source
\[
\frac{g(g+1)}{2} - (3g-3) \;=\; \frac{1}{2}\big( g^2 - 5g + 6 \big)
\;=\; \frac{1}{2}(g-2)(g-3)
\]\[\longrightarrow \underline{O}_X \longrightarrow P^1 \longrightarrow \omega
\longrightarrow 0\]
LaTeX source
\[
\longrightarrow \underline{O}_X \longrightarrow P^1 \longrightarrow \omega
\longrightarrow 0
\]\[E \otimes_{\underline{O}} P \longrightarrow E\]
LaTeX source
\[
E \otimes_{\underline{O}} P \longrightarrow E
\]\[2 - 2g\]
LaTeX source
\[ 2 - 2g \]
\[P^{\infty}_{X/S}, \qquad \Omega\quad \Omega^2\quad \Omega^3\]
LaTeX source
\[
P^{\infty}_{X/S}, \qquad \Omega\quad \Omega^2\quad \Omega^3
\]\[\omega^2 \longrightarrow P^{3+} \longrightarrow \omega \longrightarrow 0\]
LaTeX source
\[
\omega^2 \longrightarrow P^{3+} \longrightarrow \omega \longrightarrow 0
\]\[\longrightarrow f_*(\omega^2) \longrightarrow f_*\big( P^{3+}_{X\varphi}
\big) \longrightarrow f_*(\omega) \longrightarrow 0\]
LaTeX source
\[
\longrightarrow f_*(\omega^2) \longrightarrow f_*\big( P^{3+}_{X\varphi}
\big) \longrightarrow f_*(\omega) \longrightarrow 0
\]\[P^{\infty}\big( \widehat{\mathrm{Sym}}(\Omega) \big), \qquad
P^{\infty}(\omega^n), \qquad \omega \otimes P^{\infty},
\qquad P^{\infty} \otimes \omega\]
LaTeX source
\[
P^{\infty}\big( \widehat{\mathrm{Sym}}(\Omega) \big), \qquad
P^{\infty}(\omega^n), \qquad \omega \otimes P^{\infty},
\qquad P^{\infty} \otimes \omega
\]\[M \otimes P^{\infty}, \qquad R^1 f_*\big( M \otimes \omega^n \big) = 0
\quad \text{si } n \gg 1\]
LaTeX source
\[
M \otimes P^{\infty}, \qquad R^1 f_*\big( M \otimes \omega^n \big) = 0
\quad \text{si } n \gg 1
\]\[S^i = f_*\, P^{\infty}(\omega^n) = f_*\big( \omega^n \otimes P \big)\]
LaTeX source
\[
S^i = f_*\, P^{\infty}(\omega^n) = f_*\big( \omega^n \otimes P \big)
\]\[\mathrm{gr}\, S^{\bullet} \;\simeq\; \sum_{n \geqslant \ill{}}
f_*\big( \omega \otimes P \big).\]
LaTeX source
\[
\mathrm{gr}\, S^{\bullet} \;\simeq\; \sum_{n \geqslant \ill{}}
f_*\big( \omega \otimes P \big).
\]\[M_g^{\mathfrak{z}}(S) = \text{courbes algébriques}\]
LaTeX source
\[
M_g^{\mathfrak{z}}(S) = \text{courbes algébriques}
\]\[0 \longrightarrow \underline{O}_X \longrightarrow E \longrightarrow
\underline{O}_X \longrightarrow 0\]
LaTeX source
\[
0 \longrightarrow \underline{O}_X \longrightarrow E \longrightarrow
\underline{O}_X \longrightarrow 0
\]\[(*) \qquad H^0_{DR}(X, \mathfrak{g}) \simeq
H^2_{DR}(X, \mathfrak{g})^{\vee}\]
LaTeX source
\[
(*) \qquad H^0_{DR}(X, \mathfrak{g}) \simeq
H^2_{DR}(X, \mathfrak{g})^{\vee}
\]\[(**) \qquad \chi_{DR}(X, \mathfrak{g})
\overset{\text{déf}}{=} \sum (-1)^i \dim H^i_{DR}(X, \mathfrak{g})
\;=\; 3\, \chi_{DR}(X, \underline{O}_X)\]
LaTeX source
\[
(**) \qquad \chi_{DR}(X, \mathfrak{g})
\overset{\text{déf}}{=} \sum (-1)^i \dim H^i_{DR}(X, \mathfrak{g})
\;=\; 3\, \chi_{DR}(X, \underline{O}_X)
\]\[= \struck{6g} \; 6 - 6g\]
LaTeX source
\[
= \struck{6g} \; 6 - 6g
\]\[(\!*\!*\!*) \qquad \dim H^1_{DR}(X, \mathfrak{g})
= 2 \dim H^0_{DR}(X, \mathfrak{g}) + (6g - 6)\]
LaTeX source
\[
(\!*\!*\!*) \qquad \dim H^1_{DR}(X, \mathfrak{g})
= 2 \dim H^0_{DR}(X, \mathfrak{g}) + (6g - 6)
\]\[H^0_{DR}(X, \mathfrak{g}) \simeq \mathrm{Lie}\;
\mathrm{Aut}^{\mathfrak{z}}_{X/k}(P)\]
LaTeX source
\[
H^0_{DR}(X, \mathfrak{g}) \simeq \mathrm{Lie}\;
\mathrm{Aut}^{\mathfrak{z}}_{X/k}(P)
\]\[\dim H^1_{DR}(X, \mathfrak{g}) = 2 \dim
\mathrm{Aut}^{\mathfrak{z}}_{X/k}(P) + 6g - 6\]
LaTeX source
\[
\dim H^1_{DR}(X, \mathfrak{g}) = 2 \dim
\mathrm{Aut}^{\mathfrak{z}}_{X/k}(P) + 6g - 6
\]\[= 2 \Big( \dim \mathrm{Aut}^{\mathfrak{z}}_{X/k}(P) + 3g - 3 \Big)\]
LaTeX source
\[
= 2 \Big( \dim \mathrm{Aut}^{\mathfrak{z}}_{X/k}(P) + 3g - 3 \Big)
\]\[\pi \xrightarrow{\;\rho\;} \mathrm{PGL}(1, \mathbf{C}) = H,
\qquad \pi = \pi_1(X, x)\]
LaTeX source
\[
\pi \xrightarrow{\;\rho\;} \mathrm{PGL}(1, \mathbf{C}) = H,
\qquad \pi = \pi_1(X, x)
\]\[M_g^{\mathfrak{z}}(X) \;\simeq\;
\mathrm{Hom}_{\mathrm{gr.\,ana}}(\pi, H) \,\big/\, H\]
LaTeX source
\[
M_g^{\mathfrak{z}}(X) \;\simeq\;
\mathrm{Hom}_{\mathrm{gr.\,ana}}(\pi, H) \,\big/\, H
\]\[\rho \cdot u = \rho \circ u ;\]
LaTeX source
\[ \rho \cdot u = \rho \circ u ; \]
\[\rho \circ u = \mathrm{int}(\rho(g)) \circ u,\]
LaTeX source
\[
\rho \circ u = \mathrm{int}(\rho(g)) \circ u,
\]\[\pi_1(Y) \;\simeq\; \pi = \pi_1(X, x)\]
LaTeX source
\[ \pi_1(Y) \;\simeq\; \pi = \pi_1(X, x) \]
\[\rho_Y : \pi_1(Y) \longrightarrow H\]
LaTeX source
\[ \rho_Y : \pi_1(Y) \longrightarrow H \]
\[M_g(X) \hookrightarrow M_g^{\mathfrak{z}}(X)\]
LaTeX source
\[
M_g(X) \hookrightarrow M_g^{\mathfrak{z}}(X)
\]\[H^0\big( X, \omega^{\otimes 2}_{X/\mathbf{C}} \big), \ldots\]
LaTeX source
\[
H^0\big( X, \omega^{\otimes 2}_{X/\mathbf{C}} \big), \ldots
\]\[M_{\mathrm{ann}}(X) \longrightarrow M_g^{\mathfrak{z}}(X)\]
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\[
M_{\mathrm{ann}}(X) \longrightarrow M_g^{\mathfrak{z}}(X)
\]\[\lambda c = c \quad\text{i.e.}\quad (\lambda - 1)\, c = 0,\]
LaTeX source
\[
\lambda c = c \quad\text{i.e.}\quad (\lambda - 1)\, c = 0,
\]\[\mathrm{Aut}_X(P_X) \;\simeq\; H^0(X, \omega_X)\]
LaTeX source
\[
\mathrm{Aut}_X(P_X) \;\simeq\; H^0(X, \omega_X)
\]\[\mathcal{U} \simeq \omega + \underline{O}_X + \omega^{-1}\]
LaTeX source
\[
\mathcal{U} \simeq \omega + \underline{O}_X + \omega^{-1}
\]\[c_{D_t} : \mathcal{U} \longrightarrow \mathcal{U} \otimes \omega
\simeq \omega^2 + \omega + \underline{O}_X\]
LaTeX source
\[
c_{D_t} : \mathcal{U} \longrightarrow \mathcal{U} \otimes \omega
\simeq \omega^2 + \omega + \underline{O}_X
\]\[\begin{cases}
c_{D_t}(dt) = -2\, dt \\
c_{D_t}(1) = 1 \\
c_{D_t}\big( (dt)^{-1} \big) = 0
\end{cases}\]
LaTeX source
\[
\begin{cases}
c_{D_t}(dt) = -2\, dt \\
c_{D_t}(1) = 1 \\
c_{D_t}\big( (dt)^{-1} \big) = 0
\end{cases}
\]\[c_{D_t}\big( \lambda\, dt + \mu \cdot 1 + \nu\, (dt)^{-1} \big)
= \lambda'\, dt^2 + (\mu' - 2\lambda)\, dt + (\nu' \ldots\]
LaTeX source
\[
c_{D_t}\big( \lambda\, dt + \mu \cdot 1 + \nu\, (dt)^{-1} \big)
= \lambda'\, dt^2 + (\mu' - 2\lambda)\, dt + (\nu' \ldots
\]\[u_\omega = \exp \Theta_\omega : \mathcal{U} \longrightarrow \mathcal{U}\]
LaTeX source
\[
u_\omega = \exp \Theta_\omega : \mathcal{U} \longrightarrow \mathcal{U}
\]\[\exp \Theta_{-\omega}(1) = 1 + [-\omega,\, 1] = 1 + \omega\]
LaTeX source
\[
\exp \Theta_{-\omega}(1) = 1 + [-\omega,\, 1] = 1 + \omega
\]\[u_\omega(c_{D_t}) = \struck{\ill{}}\; u \circ c_{D_t} \circ u^{-1}
= \big( \exp \Theta_{-\omega} \big) \ldots\]
LaTeX source
\[
u_\omega(c_{D_t}) = \struck{\ill{}}\; u \circ c_{D_t} \circ u^{-1}
= \big( \exp \Theta_{-\omega} \big) \ldots
\]\[u_\omega(c_{D_t}) - c_{D_t} \;\equiv\; \varphi\]
LaTeX source
\[
u_\omega(c_{D_t}) - c_{D_t} \;\equiv\; \varphi
\]\[\varphi(dt) \;\struck{=}\; c_{D_t}(dt)
= \big( \mathrm{id} + \Theta_{-\omega} \big)
\big( \struck{D_t}(dt) \big) = -2\, dt + \ldots\]
LaTeX source
\[
\varphi(dt) \;\struck{=}\; c_{D_t}(dt)
= \big( \mathrm{id} + \Theta_{-\omega} \big)
\big( \struck{D_t}(dt) \big) = -2\, dt + \ldots
\]\[\varphi(1) = -2\,\omega\, dt\]
LaTeX source
\[ \varphi(1) = -2\,\omega\, dt \]
\[\varphi(1) + c_{D_t}(1) = \Big( \mathrm{id} + \Theta_{-\omega}
+ \tfrac{1}{2} \Theta_{-\omega}^{\,2} \Big)\,
c_{D_t}\big( 1 + [\omega,\, 1] \big)\]
LaTeX source
\[
\varphi(1) + c_{D_t}(1) = \Big( \mathrm{id} + \Theta_{-\omega}
+ \tfrac{1}{2} \Theta_{-\omega}^{\,2} \Big)\,
c_{D_t}\big( 1 + [\omega,\, 1] \big)
\]\[= 1 + [-\omega,\, 1] + \big[ -\omega,\, [-\omega,\, 1] \big] + \ldots\]
LaTeX source
\[ = 1 + [-\omega,\, 1] + \big[ -\omega,\, [-\omega,\, 1] \big] + \ldots \]
\[= 1 + (-2\omega) + 2\omega^2 - \lambda'\, dt^2 + 2\lambda\, dt + \ldots\]
LaTeX source
\[ = 1 + (-2\omega) + 2\omega^2 - \lambda'\, dt^2 + 2\lambda\, dt + \ldots \]
\[\varphi(1) = \big( -\lambda' + \struck{\ill{}} \big)\, dt^2
\;\struck{\ill{}}\]
LaTeX source
\[
\varphi(1) = \big( -\lambda' + \struck{\ill{}} \big)\, dt^2
\;\struck{\ill{}}
\]\[u_\omega(c_{D_t}) = c_{D_t} + d^1_{\omega/S}(\omega)\]
LaTeX source
\[
u_\omega(c_{D_t}) = c_{D_t} + d^1_{\omega/S}(\omega)
\]\[\boxed{\;u_\omega(c) = c + d^1_{\omega/S}(\omega)\;}\]
LaTeX source
\[
\boxed{\;u_\omega(c) = c + d^1_{\omega/S}(\omega)\;}
\]\[\ill{} \longrightarrow M \longrightarrow F \longrightarrow
\underline{O}_X \longrightarrow 0\]
LaTeX source
\[
\ill{} \longrightarrow M \longrightarrow F \longrightarrow
\underline{O}_X \longrightarrow 0
\]\[E \simeq F \otimes L,\]
LaTeX source
\[ E \simeq F \otimes L, \]
\[\underline{\omega} \hookrightarrow E \simeq F \otimes L \twoheadrightarrow L\]
LaTeX source
\[
\underline{\omega} \hookrightarrow E \simeq F \otimes L \twoheadrightarrow L
\]\[\pi_1(X^{\mathrm{an}}, x) \longrightarrow H(\mathbb{C})\]
LaTeX source
\[
\pi_1(X^{\mathrm{an}}, x) \longrightarrow H(\mathbb{C})
\]\[(P,\sigma) \quad\longleftrightarrow\quad 0 \to \Omega \to E \to \underline{O}_S \to 0\]
LaTeX source
\[
(P,\sigma) \quad\longleftrightarrow\quad 0 \to \Omega \to E \to \underline{O}_S \to 0
\]\[J/J^2 = \omega \;\xrightarrow{\ \omega\ }\; \Omega^1_{X/S}\]
LaTeX source
\[
J/J^2 = \omega \;\xrightarrow{\ \omega\ }\; \Omega^1_{X/S}
\]\[\widehat{S} \;\underset{\sim}{\overset{u}{\longleftrightarrow}}\; P\]
LaTeX source
\[
\widehat{S} \;\underset{\sim}{\overset{u}{\longleftrightarrow}}\; P
\]\[\widehat{S}/\widehat{J}^{\,4}_P \longrightarrow P/J^4\]
LaTeX source
\[
\widehat{S}/\widehat{J}^{\,4}_P \longrightarrow P/J^4
\]\[\Omega \longrightarrow \widehat{S} \otimes \Omega^1_{X/S},
\qquad
\prod_{i \geqslant 0} \Omega^{\otimes i} \otimes \Omega^1_{X/S},
\qquad g \in G(c)\]
LaTeX source
\[
\Omega \longrightarrow \widehat{S} \otimes \Omega^1_{X/S},
\qquad
\prod_{i \geqslant 0} \Omega^{\otimes i} \otimes \Omega^1_{X/S},
\qquad g \in G(c)
\]\[S = \mathrm{Sym}(\Omega) \;\xrightarrow{\ c\ }\; \widehat{S} \,\widehat{\otimes}\, \Omega^1_{X/S},
\qquad
\Omega \;\xrightarrow{\ c\ }\; \widehat{S} \,\widehat{\otimes}\, \Omega^1_{X/S}\]
LaTeX source
\[
S = \mathrm{Sym}(\Omega) \;\xrightarrow{\ c\ }\; \widehat{S} \,\widehat{\otimes}\, \Omega^1_{X/S},
\qquad
\Omega \;\xrightarrow{\ c\ }\; \widehat{S} \,\widehat{\otimes}\, \Omega^1_{X/S}
\]\[C(\omega_0) = \sum_{i \geqslant 0} \omega_0^{\,i} \otimes \varpi_i,
\qquad \varpi_i \in \Omega^1_{X/S}\]
LaTeX source
\[
C(\omega_0) = \sum_{i \geqslant 0} \omega_0^{\,i} \otimes \varpi_i,
\qquad \varpi_i \in \Omega^1_{X/S}
\]\[C(\lambda\omega_0) = \lambda\,C(\omega_0) + \omega_0\,d\lambda\]
LaTeX source
\[ C(\lambda\omega_0) = \lambda\,C(\omega_0) + \omega_0\,d\lambda \]
\[= 1 \otimes \lambda\varpi_0 + \omega_0 \otimes (\lambda\varpi_1 + d\lambda)
+ \omega_0^2 \otimes \lambda\varpi_2 + \cdots + \omega_0^{\,i} \otimes \lambda\varpi_i \cdots\]
LaTeX source
\[
= 1 \otimes \lambda\varpi_0 + \omega_0 \otimes (\lambda\varpi_1 + d\lambda)
+ \omega_0^2 \otimes \lambda\varpi_2 + \cdots + \omega_0^{\,i} \otimes \lambda\varpi_i \cdots
\]\[d(\lambda\omega) = \lambda\,d\omega + \struck{\omega\,d\lambda}\]
LaTeX source
\[
d(\lambda\omega) = \lambda\,d\omega + \struck{\omega\,d\lambda}
\]\[J^i \longrightarrow J^{i-1} \otimes \Omega^1_{X/S}\]
LaTeX source
\[
J^i \longrightarrow J^{i-1} \otimes \Omega^1_{X/S}
\]\[\lambda\omega^i \longrightarrow \struck{C(\ill{})}\ \omega^i \otimes d\lambda
+ \lambda\,\omega^{i-1} C(\omega)\]
LaTeX source
\[
\lambda\omega^i \longrightarrow \struck{C(\ill{})}\ \omega^i \otimes d\lambda
+ \lambda\,\omega^{i-1} C(\omega)
\]\[\struck{\Omega}\ \Omega^i \xrightarrow{\ \uncertain{h_i}\ } \Omega^{i-1} \otimes \Omega^1_{X/S}\]
LaTeX source
\[
\struck{\Omega}\ \Omega^i \xrightarrow{\ \uncertain{h_i}\ } \Omega^{i-1} \otimes \Omega^1_{X/S}
\]\[\lambda\omega^i \longrightarrow \lambda\,\omega^{i-1}\,\underline{C(\omega)},
\qquad
\lambda\omega_0^{\,i} \longrightarrow \lambda\,\omega_0^{\,i-1}\,C(\omega_0)\]
LaTeX source
\[
\lambda\omega^i \longrightarrow \lambda\,\omega^{i-1}\,\underline{C(\omega)},
\qquad
\lambda\omega_0^{\,i} \longrightarrow \lambda\,\omega_0^{\,i-1}\,C(\omega_0)
\]\[C(\omega_0^{\,u})^{u^{-1}} =
\left(\varpi_0 + \frac{\omega_0}{1+\sum \alpha_i \omega_0^{\,i}}\,\varpi_1
+ \left(\frac{\omega_0}{1+\sum \alpha_i \omega_0^{\,i}}\right)^{\!2}\varpi_2\right)
\left(1 + \sum (i+1)\alpha_i \left(\frac{\ill{}}{1 + \ill{}}\right)\right)\]
LaTeX source
\[
C(\omega_0^{\,u})^{u^{-1}} =
\left(\varpi_0 + \frac{\omega_0}{1+\sum \alpha_i \omega_0^{\,i}}\,\varpi_1
+ \left(\frac{\omega_0}{1+\sum \alpha_i \omega_0^{\,i}}\right)^{\!2}\varpi_2\right)
\left(1 + \sum (i+1)\alpha_i \left(\frac{\ill{}}{1 + \ill{}}\right)\right)
\]\[+ \sum \left(\frac{\omega_0}{\sum 1 + \alpha_j \omega_0^{\,j}}\right)^{\!\ill{}} \otimes\, d\alpha_i\]
LaTeX source
\[
+ \sum \left(\frac{\omega_0}{\sum 1 + \alpha_j \omega_0^{\,j}}\right)^{\!\ill{}} \otimes\, d\alpha_i
\]\[C(\omega_0^{\,u})^{u^{-1}} \equiv (\varpi_0 + \omega_0\varpi_1 + \omega_0^2\varpi_2)
\left[1 + \struck{\ill{}}\ 4\alpha_3\omega_0^3\right]\]
LaTeX source
\[
C(\omega_0^{\,u})^{u^{-1}} \equiv (\varpi_0 + \omega_0\varpi_1 + \omega_0^2\varpi_2)
\left[1 + \struck{\ill{}}\ 4\alpha_3\omega_0^3\right]
\]\[\sum_{i \geqslant 1} \Omega^i \otimes \Omega^1_{X/S}
\qquad = \struck{\ill{}}\ C(\omega_0) + 4\alpha_3\,\omega_0^3\,\varpi_0\]
LaTeX source
\[
\sum_{i \geqslant 1} \Omega^i \otimes \Omega^1_{X/S}
\qquad = \struck{\ill{}}\ C(\omega_0) + 4\alpha_3\,\omega_0^3\,\varpi_0
\]\[C(\omega_0^{\,u})^{u^{-1}} = (\varpi_0 + \omega_0\varpi_1 + \omega_0^2\varpi_2)
\bigl(1 + (n+1)\alpha_n\,\omega_0^{\,n}\bigr)\]
LaTeX source
\[
C(\omega_0^{\,u})^{u^{-1}} = (\varpi_0 + \omega_0\varpi_1 + \omega_0^2\varpi_2)
\bigl(1 + (n+1)\alpha_n\,\omega_0^{\,n}\bigr)
\]\[= \struck{\varpi_0}\ C(\omega_0) + \varpi_0\ \struck{\ill{}}\ (n+1)\alpha_n\,\omega_0^{\,n}\,\varpi_0\]
LaTeX source
\[
= \struck{\varpi_0}\ C(\omega_0) + \varpi_0\ \struck{\ill{}}\ (n+1)\alpha_n\,\omega_0^{\,n}\,\varpi_0
\]\[C(\omega_0^{\,u})^{u^{-1}} = (\varpi_0 + \omega_0\varpi_1 + \omega_0^2\varpi_2)
\bigl(1 + 3\alpha_2\,\omega_0^2\bigr)
= C(\omega_0) + 3\alpha_2\,\omega_0^2\,\varpi_0\]
LaTeX source
\[
C(\omega_0^{\,u})^{u^{-1}} = (\varpi_0 + \omega_0\varpi_1 + \omega_0^2\varpi_2)
\bigl(1 + 3\alpha_2\,\omega_0^2\bigr)
= C(\omega_0) + 3\alpha_2\,\omega_0^2\,\varpi_0
\]\[(c,u) \longmapsto \struck{\ill{}}\ u(\hat{c})\]
LaTeX source
\[
(c,u) \longmapsto \struck{\ill{}}\ u(\hat{c})
\]\[\mathrm{Conn}\,P \;(\times\, G_0) \longrightarrow \mathrm{Conn}_{\mathrm{Alg}}(\widehat{S})
\quad \struck{mod}\]
LaTeX source
\[
\mathrm{Conn}\,P \;(\times\, G_0) \longrightarrow \mathrm{Conn}_{\mathrm{Alg}}(\widehat{S})
\quad \struck{mod}
\]\[G \times \mathrm{Conn}(P), \qquad (g,c) \longmapsto g\cdot\hat{c}.\]
LaTeX source
\[
G \times \mathrm{Conn}(P), \qquad (g,c) \longmapsto g\cdot\hat{c}.
\]\[h \in G(c) \iff h\cdot\hat{c} \ \text{de la forme}\ \hat{c}\]
LaTeX source
\[
h \in G(c) \iff h\cdot\hat{c} \ \text{de la forme}\ \hat{c}
\]\[\struck{G(c) \times{}}\quad G_0 \times G(c) \longrightarrow G,
\qquad (g,h) \longmapsto g\cdot h\]
LaTeX source
\[
\struck{G(c) \times{}}\quad G_0 \times G(c) \longrightarrow G,
\qquad (g,h) \longmapsto g\cdot h
\]\[C(\omega^{\,u}) = \struck{\ill{}}\ C\omega + \sum_{i \geqslant 2} C(\omega)u_i
+ \omega\,C(u_i)
= C(\omega)\Bigl(1 + \sum u_i\Bigr) + \omega \sum C(u_i)\]
LaTeX source
\[
C(\omega^{\,u}) = \struck{\ill{}}\ C\omega + \sum_{i \geqslant 2} C(\omega)u_i
+ \omega\,C(u_i)
= C(\omega)\Bigl(1 + \sum u_i\Bigr) + \omega \sum C(u_i)
\]\[C(\lambda\,\omega^{\otimes i}) = \omega^{\otimes i} \otimes d\lambda
+ \lambda\,i\,\omega^{\otimes i-1}\,\ill{}\]
LaTeX source
\[
C(\lambda\,\omega^{\otimes i}) = \omega^{\otimes i} \otimes d\lambda
+ \lambda\,i\,\omega^{\otimes i-1}\,\ill{}
\]\[C\bigl((\lambda\omega_0)^{\,u}\bigr) =
\bigl(\lambda\,\add{C(\omega_0)} + \omega_0 \otimes d\lambda\bigr)
\Bigl(1 + \sum_{i \geqslant 2}\alpha_i\,\omega_0^{\,i}\Bigr)
+ \lambda\omega_0 \sum_{i \geqslant 2}
\bigl(\omega_0^{\,i} \otimes d\alpha_i + i\,\alpha_i\,\omega_0^{\,i-1}\,C(\omega_0)\bigr)\]
LaTeX source
\[
C\bigl((\lambda\omega_0)^{\,u}\bigr) =
\bigl(\lambda\,\add{C(\omega_0)} + \omega_0 \otimes d\lambda\bigr)
\Bigl(1 + \sum_{i \geqslant 2}\alpha_i\,\omega_0^{\,i}\Bigr)
+ \lambda\omega_0 \sum_{i \geqslant 2}
\bigl(\omega_0^{\,i} \otimes d\alpha_i + i\,\alpha_i\,\omega_0^{\,i-1}\,C(\omega_0)\bigr)
\]\[C(\omega_0) = \struck{\ill{}}\ \varpi_0 + \omega_0\varpi_1 + \omega_0^2\varpi_2,
\qquad \varpi_i \in \struck{\ill{}}\ \widehat{S} \otimes \Omega^1_{X/S}\]
LaTeX source
\[
C(\omega_0) = \struck{\ill{}}\ \varpi_0 + \omega_0\varpi_1 + \omega_0^2\varpi_2,
\qquad \varpi_i \in \struck{\ill{}}\ \widehat{S} \otimes \Omega^1_{X/S}
\]\[C(\struck{\lambda}\,\omega_0^{\,u}) = \struck{C(\omega_0}\ (\varpi_0 + \varpi_1 + \varpi_2)
\Bigl(1 + \sum_{i \geqslant 2}\alpha_i\,\omega_0^{\,i} + \ill{}\Bigr)\]
LaTeX source
\[
C(\struck{\lambda}\,\omega_0^{\,u}) = \struck{C(\omega_0}\ (\varpi_0 + \varpi_1 + \varpi_2)
\Bigl(1 + \sum_{i \geqslant 2}\alpha_i\,\omega_0^{\,i} + \ill{}\Bigr)
\]\[C(\omega_0^{\,u}) = C\Bigl(\omega_0\bigl(1 + \sum_{i \geqslant 2}\alpha_i\,\omega_0^{\,i}\bigr)\Bigr)
= C(\omega_0)\Bigl(1 + \sum \alpha_i\,\omega_0^{\,i}\Bigr)
+ \omega_0 \sum_{i \geqslant 2}\bigl(\omega_0^{\,i} \otimes d\alpha_i
+ i\,\alpha_i\,\omega_0^{\,i-1}\,C(\omega_0)\bigr)\]
LaTeX source
\[
C(\omega_0^{\,u}) = C\Bigl(\omega_0\bigl(1 + \sum_{i \geqslant 2}\alpha_i\,\omega_0^{\,i}\bigr)\Bigr)
= C(\omega_0)\Bigl(1 + \sum \alpha_i\,\omega_0^{\,i}\Bigr)
+ \omega_0 \sum_{i \geqslant 2}\bigl(\omega_0^{\,i} \otimes d\alpha_i
+ i\,\alpha_i\,\omega_0^{\,i-1}\,C(\omega_0)\bigr)
\]\[= C(\omega_0)\Bigl(1 + \sum_{i \geqslant 2}(i+1)\alpha_i\,\omega_0^{\,i}\Bigr)
+ \omega_0^2 \sum_{i \geqslant 2} \ill{}\]
LaTeX source
\[
= C(\omega_0)\Bigl(1 + \sum_{i \geqslant 2}(i+1)\alpha_i\,\omega_0^{\,i}\Bigr)
+ \omega_0^2 \sum_{i \geqslant 2} \ill{}
\]\[C(\omega_0^{\,u})^{u^{-1}} = \struck{\ill{}}
\Biggl(1 + \sum_{i \geqslant 2}(i+1)\alpha_i
\biggl(\frac{\omega_0}{1 + \sum_j \alpha_j\,\omega_0^{\,j}}\biggr)^{\!i}\Biggr)
+ \ill{} \sum_{i \geqslant 2}
\biggl(\frac{\omega_0}{1 + \sum_{j \geqslant 2} \alpha_j\,\omega_0^{\,j}}\biggr)^{\!i+1}
\otimes\, d\alpha_i\]
LaTeX source
\[
C(\omega_0^{\,u})^{u^{-1}} = \struck{\ill{}}
\Biggl(1 + \sum_{i \geqslant 2}(i+1)\alpha_i
\biggl(\frac{\omega_0}{1 + \sum_j \alpha_j\,\omega_0^{\,j}}\biggr)^{\!i}\Biggr)
+ \ill{} \sum_{i \geqslant 2}
\biggl(\frac{\omega_0}{1 + \sum_{j \geqslant 2} \alpha_j\,\omega_0^{\,j}}\biggr)^{\!i+1}
\otimes\, d\alpha_i
\]\[G_0 \times C_0 \;\xrightarrow{\ \sim\ }\; C, \qquad (h,c) \longmapsto h\cdot c\]
LaTeX source
\[
G_0 \times C_0 \;\xrightarrow{\ \sim\ }\; C, \qquad (h,c) \longmapsto h\cdot c
\]\[G(c) = \{\, g \in G \ \mid\ g\cdot c \in C_0 \,\}\]
LaTeX source
\[
G(c) = \{\, g \in G \ \mid\ g\cdot c \in C_0 \,\}
\]\[G_0 \times G(c) \;\xrightarrow{\ \sim\ }\; G, \qquad (h,g) \longmapsto h\,g\]
LaTeX source
\[
G_0 \times G(c) \;\xrightarrow{\ \sim\ }\; G, \qquad (h,g) \longmapsto h\,g
\]\[C : P \longrightarrow P \,\widehat{\otimes}\, \Omega^1_{X/S}\]
LaTeX source
\[
C : P \longrightarrow P \,\widehat{\otimes}\, \Omega^1_{X/S}
\]\[\begin{cases}
C(fg) = f\,C(g) + g\,C(f), & f, g \ \text{sections de}\ P \\
C(\lambda \cdot 1) = 1 \otimes d\lambda, & \lambda \ \text{section de}\ \underline{O}_X
\end{cases}\]
LaTeX source
\[
\begin{cases}
C(fg) = f\,C(g) + g\,C(f), & f, g \ \text{sections de}\ P \\
C(\lambda \cdot 1) = 1 \otimes d\lambda, & \lambda \ \text{section de}\ \underline{O}_X
\end{cases}
\]\[\Omega \longrightarrow \widehat{\mathrm{Sym}}(\Omega) \,\widehat{\otimes}\, \Omega^1_{X/S}
= \prod_{i \geqslant 0} \mathrm{Sym}^i(\Omega) \otimes \ill{}\]
LaTeX source
\[
\Omega \longrightarrow \widehat{\mathrm{Sym}}(\Omega) \,\widehat{\otimes}\, \Omega^1_{X/S}
= \prod_{i \geqslant 0} \mathrm{Sym}^i(\Omega) \otimes \ill{}
\]\[\begin{cases}
\varpi_i \in \struck{\ill{}}\ \Gamma\bigl(\Omega^{\otimes (i-1)} \otimes \Omega^1_{X/S}\bigr) & (i \neq 1) \\
\varpi_1 \ \text{une connexion sur}\ \Omega
\end{cases}\]
LaTeX source
\[
\begin{cases}
\varpi_i \in \struck{\ill{}}\ \Gamma\bigl(\Omega^{\otimes (i-1)} \otimes \Omega^1_{X/S}\bigr) & (i \neq 1) \\
\varpi_1 \ \text{une connexion sur}\ \Omega
\end{cases}
\]\[\mathrm{gr}^i(S) = J^i/J^{i+1} \simeq \Omega^i
\;\xrightarrow{\ \widetilde{c}\ }\;
\struck{\ill{}}\ \bigl(P \,\widehat{\otimes}\, \Omega^1_{X/S}\bigr)\]
LaTeX source
\[
\mathrm{gr}^i(S) = J^i/J^{i+1} \simeq \Omega^i
\;\xrightarrow{\ \widetilde{c}\ }\;
\struck{\ill{}}\ \bigl(P \,\widehat{\otimes}\, \Omega^1_{X/S}\bigr)
\]\[\widetilde{c}(\omega_0) = \omega_i \otimes \varpi_0\]
LaTeX source
\[
\widetilde{c}(\omega_0) = \omega_i \otimes \varpi_0
\]\[\varpi_0 \in \Gamma\bigl(\Omega^{-1} \otimes \Omega^1_{X/S}\bigr)
= \mathrm{Hom}\bigl(\Omega, \Omega^1_{X/S}\bigr)\]
LaTeX source
\[
\varpi_0 \in \Gamma\bigl(\Omega^{-1} \otimes \Omega^1_{X/S}\bigr)
= \mathrm{Hom}\bigl(\Omega, \Omega^1_{X/S}\bigr)
\]\[\mathrm{Conn}(P) \longrightarrow \mathrm{Conn}(\widehat{S})\]
LaTeX source
\[
\mathrm{Conn}(P) \longrightarrow \mathrm{Conn}(\widehat{S})
\]\[\mathrm{Conn}^{*}(P) \times G_0 \longrightarrow \mathrm{Conn}^{*}(\widehat{S}),
\qquad (c,g) \longmapsto g\cdot\hat{c}\]
LaTeX source
\[
\mathrm{Conn}^{*}(P) \times G_0 \longrightarrow \mathrm{Conn}^{*}(\widehat{S}),
\qquad (c,g) \longmapsto g\cdot\hat{c}
\]\[G(c) \;\xrightarrow{\ \sim\ }\; G/G_0 \simeq \Gamma(X, \Omega^{\otimes 2}).\]
LaTeX source
\[
G(c) \;\xrightarrow{\ \sim\ }\; G/G_0 \simeq \Gamma(X, \Omega^{\otimes 2}).
\]