Cote n° 122 · pages 2–33
· 77 displayed formulas · Point singulier isolé de la fibre : notes manuscrites (s.d.).
Inventory dating : [vers 1968-1971]
Édition de démonstration
\[H^{*}(P, F) \longrightarrow H^{*}(\mathring{P}, F) \quad \text{un isom}
\qquad (\text{si } F \text{ loc. constant})\]
LaTeX source
\[
H^{*}(P, F) \longrightarrow H^{*}(\mathring{P}, F) \quad \text{un isom}
\qquad (\text{si } F \text{ loc. constant})
\]\[H^{*}_{\partial P}(P, F) = 0\]
LaTeX source
\[
H^{*}_{\partial P}(P, F) = 0
\]\[\underline{H}^{*}_{\partial P}(F) = 0 .\]
LaTeX source
\[
\underline{H}^{*}_{\partial P}(F) = 0 .
\]\[\cdots \longrightarrow H^{i}_{!}(\mathring{P}, F) \longrightarrow H^{i}(P, F)
\longrightarrow H^{i}(\partial P, F) \longrightarrow \cdots\]
LaTeX source
\[
\cdots \longrightarrow H^{i}_{!}(\mathring{P}, F) \longrightarrow H^{i}(P, F)
\longrightarrow H^{i}(\partial P, F) \longrightarrow \cdots
\]\[H^{i}_{!}(\mathring{P}, F) \simeq H^{n-i}(\mathring{P}, \check{F} \otimes T)^\vee
\simeq H^{n-i}(P, \check{F} \otimes T)^\vee\]
LaTeX source
\[
H^{i}_{!}(\mathring{P}, F) \simeq H^{n-i}(\mathring{P}, \check{F} \otimes T)^\vee
\simeq H^{n-i}(P, \check{F} \otimes T)^\vee
\]\[\varphi : H^{n-i}(P, \check{F} \otimes T)^\vee \longrightarrow H^{i}(P, F)\]
LaTeX source
\[
\varphi : H^{n-i}(P, \check{F} \otimes T)^\vee \longrightarrow H^{i}(P, F)
\]\[\varphi \in H^{i}(P, F) \otimes H^{n-i}(P, \check{F} \otimes T)\]
LaTeX source
\[
\varphi \in H^{i}(P, F) \otimes H^{n-i}(P, \check{F} \otimes T)
\]\[\widetilde{\partial P} \simeq \partial P \times D^{1} .\]
LaTeX source
\[
\widetilde{\partial P} \simeq \partial P \times D^{1} .
\]\[\begin{array}{ccccccc}
\to & H^{i}_{!}(P - \widetilde{\partial P}) & \to & H^{i}(P) & \to & H^{i}(\widetilde{\partial P}) & \to \cdots \\
& \downarrow & & \| & & \downarrow{\wr} & \\
\to & H^{i}_{!}(P - \partial P) & \to & H^{i}(P) & \to & H^{i}(\partial P) & \to \cdots
\end{array}\]
LaTeX source
\[
\begin{array}{ccccccc}
\to & H^{i}_{!}(P - \widetilde{\partial P}) & \to & H^{i}(P) & \to & H^{i}(\widetilde{\partial P}) & \to \cdots \\
& \downarrow & & \| & & \downarrow{\wr} & \\
\to & H^{i}_{!}(P - \partial P) & \to & H^{i}(P) & \to & H^{i}(\partial P) & \to \cdots
\end{array}
\]\[H^{i}_{!}(P - \widetilde{\partial P}) \simeq H^{i}(P - \partial P)\]
LaTeX source
\[
H^{i}_{!}(P - \widetilde{\partial P}) \simeq H^{i}(P - \partial P)
\]\[\begin{array}{ccccccc}
\to & H^{i}_{P'}(P, F) & \Longrightarrow & H^{i}(P, F) & \to & H^{i}(P - P', F) & \to \cdots \\
& \downarrow & & \| & & \updownarrow{\scriptstyle 2} & \\
\to & H^{i}(P, \partial P; F) & \longrightarrow & H^{i}(P, F) & \to & H^{i}(\partial P, F) & \to
\end{array}
\qquad
\begin{array}{c} (P, P - P') \\ \uparrow \\ (P, \partial P) \end{array}\]
LaTeX source
\[
\begin{array}{ccccccc}
\to & H^{i}_{P'}(P, F) & \Longrightarrow & H^{i}(P, F) & \to & H^{i}(P - P', F) & \to \cdots \\
& \downarrow & & \| & & \updownarrow{\scriptstyle 2} & \\
\to & H^{i}(P, \partial P; F) & \longrightarrow & H^{i}(P, F) & \to & H^{i}(\partial P, F) & \to
\end{array}
\qquad
\begin{array}{c} (P, P - P') \\ \uparrow \\ (P, \partial P) \end{array}
\]\[H^{i}_{P'}(P, F) \simeq H^{i}(P \bmod \partial P, F) \simeq H^{i}_{!}(\mathring{P}, F)\]
LaTeX source
\[
H^{i}_{P'}(P, F) \simeq H^{i}(P \bmod \partial P, F) \simeq H^{i}_{!}(\mathring{P}, F)
\]\[H^{i}_{P'}(P, F) \xrightarrow{\ \sim\ } H^{i}_{!}(\mathring{P}' \bmod \partial P', F)
\simeq H^{i}_{!}(\mathring{P}', F)\]
LaTeX source
\[
H^{i}_{P'}(P, F) \xrightarrow{\ \sim\ } H^{i}_{!}(\mathring{P}' \bmod \partial P', F)
\simeq H^{i}_{!}(\mathring{P}', F)
\]\[(P', \partial P') \to (P, P - P') .\]
LaTeX source
\[ (P', \partial P') \to (P, P - P') . \]
\[W = P \cup Q, \qquad P \cap Q = \partial P = \partial Q .\]
LaTeX source
\[ W = P \cup Q, \qquad P \cap Q = \partial P = \partial Q . \]
\[W - R = \mathring{P} \amalg \mathring{Q} .\]
LaTeX source
\[
W - R = \mathring{P} \amalg \mathring{Q} .
\]\[\cdots \to H^{i}(W, F) \to H^{i}(W - R, F) \to H^{i+1}(R, F \otimes \mathcal{T}_{R})
\to H^{i+1}(W, F)\]
LaTeX source
\[
\cdots \to H^{i}(W, F) \to H^{i}(W - R, F) \to H^{i+1}(R, F \otimes \mathcal{T}_{R})
\to H^{i+1}(W, F)
\]\[H^{i}(W - R) = H^{i}(\mathring{P}) \times H^{i}(\mathring{Q}) = H^{i}(P) \times H^{i}(Q)\]
LaTeX source
\[
H^{i}(W - R) = H^{i}(\mathring{P}) \times H^{i}(\mathring{Q}) = H^{i}(P) \times H^{i}(Q)
\]\[\cdots \to H^{i}_{!}(W - T, F) \to H^{i}_{!}(W, F) \to H^{i}_{!}(R, F) \to \cdots\]
LaTeX source
\[
\cdots \to H^{i}_{!}(W - T, F) \to H^{i}_{!}(W, F) \to H^{i}_{!}(R, F) \to \cdots
\]\[\begin{aligned}
H^{i}_{!}(W - T, F) &\simeq H^{i}_{!}(\mathring{P}, F) \times H^{i}_{!}(\mathring{Q}, F) \\
&\simeq H^{n-i}(\mathring{P}, \check{F} \otimes \mathcal{T}_W)^\vee \times
H^{n-i}(\mathring{Q}, \check{F} \otimes \mathcal{T}_W)^\vee \\
&\simeq H^{n-i}(P, \check{F} \otimes \mathcal{T}_W)^\vee \times
H^{n-i}(Q, \check{F} \otimes \mathcal{T}_W)^\vee
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
H^{i}_{!}(W - T, F) &\simeq H^{i}_{!}(\mathring{P}, F) \times H^{i}_{!}(\mathring{Q}, F) \\
&\simeq H^{n-i}(\mathring{P}, \check{F} \otimes \mathcal{T}_W)^\vee \times
H^{n-i}(\mathring{Q}, \check{F} \otimes \mathcal{T}_W)^\vee \\
&\simeq H^{n-i}(P, \check{F} \otimes \mathcal{T}_W)^\vee \times
H^{n-i}(Q, \check{F} \otimes \mathcal{T}_W)^\vee
\end{aligned}
\]\[\cdots \to H^{i}_{P}(W, F) \to H^{i}(W, F) \to H^{i}(W - P, F) \to \cdots\]
LaTeX source
\[
\cdots \to H^{i}_{P}(W, F) \to H^{i}(W, F) \to H^{i}(W - P, F) \to \cdots
\]\[H^{i}(W - P, F) \simeq H^{i}(\mathring{Q}, F) \xleftarrow{\ \sim\ } H^{i}(Q, F)\]
LaTeX source
\[
H^{i}(W - P, F) \simeq H^{i}(\mathring{Q}, F) \xleftarrow{\ \sim\ } H^{i}(Q, F)
\]\[H^{i}_{P}(\widetilde{P}, F) \xrightarrow{\ \sim\ }
H^{i}_{!}(\widetilde{P} \bmod \partial\widetilde{P}, F) \simeq H^{i}_{!}(\mathring{P}, F),
\qquad
H^{i}_{P}(\widetilde{P}, F) \simeq H^{i}_{P}(W, F) \ \ (\text{excision})\]
LaTeX source
\[
H^{i}_{P}(\widetilde{P}, F) \xrightarrow{\ \sim\ }
H^{i}_{!}(\widetilde{P} \bmod \partial\widetilde{P}, F) \simeq H^{i}_{!}(\mathring{P}, F),
\qquad
H^{i}_{P}(\widetilde{P}, F) \simeq H^{i}_{P}(W, F) \ \ (\text{excision})
\]\[\cdots \to H^{i}_{!}(\mathring{P}, F) \to H^{i}(W, F) \to H^{i}(Q, F) \to \cdots\]
LaTeX source
\[
\cdots \to H^{i}_{!}(\mathring{P}, F) \to H^{i}(W, F) \to H^{i}(Q, F) \to \cdots
\]\[H^{i}_{!}(\mathring{P}, F) \simeq H^{n-i}(P, \check{F} \otimes \mathcal{T}_W)^\vee\]
LaTeX source
\[
H^{i}_{!}(\mathring{P}, F) \simeq H^{n-i}(P, \check{F} \otimes \mathcal{T}_W)^\vee
\]\[\boxed{\begin{array}{ccc}
S_{!}(W, R) & \text{dual de} & S(W, R) \\
\uparrow & & \downarrow \\
S(W, P) \simeq S_{!}(W, Q) & \text{dual de} & S(W, Q) \simeq S_{!}(W, P) \\
\uparrow & & \downarrow \\
S(W, R) \simeq MV(W; P, Q) & \text{dual de} & S_{!}(W, R) \simeq MV_{!}(W, R)
\end{array}}\]
LaTeX source
\[
\boxed{\begin{array}{ccc}
S_{!}(W, R) & \text{dual de} & S(W, R) \\
\uparrow & & \downarrow \\
S(W, P) \simeq S_{!}(W, Q) & \text{dual de} & S(W, Q) \simeq S_{!}(W, P) \\
\uparrow & & \downarrow \\
S(W, R) \simeq MV(W; P, Q) & \text{dual de} & S_{!}(W, R) \simeq MV_{!}(W, R)
\end{array}}
\]\[\begin{gathered}
H^{i}_{Q}(W) \to H^{i}(W) \to H^{i}(W - Q) \simeq H^{i}(P) \\
H^{i}_{Q}(W) \simeq H^{i}_{!}(W - P) = H^{i}_{!}(Q - \partial Q)
\simeq \bigl(H^{n-i}(Q - \partial Q)\bigr)^\vee = H^{n-i}(Q)^\vee \\
H^{i}_{Q}(W) \times H^{n-i}(Q)
\end{gathered}\]
LaTeX source
\[
\begin{gathered}
H^{i}_{Q}(W) \to H^{i}(W) \to H^{i}(W - Q) \simeq H^{i}(P) \\
H^{i}_{Q}(W) \simeq H^{i}_{!}(W - P) = H^{i}_{!}(Q - \partial Q)
\simeq \bigl(H^{n-i}(Q - \partial Q)\bigr)^\vee = H^{n-i}(Q)^\vee \\
H^{i}_{Q}(W) \times H^{n-i}(Q)
\end{gathered}
\]\[\boxed{\begin{array}{c|l}
\begin{array}{ccc} & \Psi & \\ \swarrow & & \searrow \\ \Phi & & \Phi' \\ \searrow & & \swarrow \\ & \Psi' & \end{array}
&
\begin{array}{l}
\Psi : H(P), H(Q), H(T), H(W) \\
\Psi' : \ldots\ \text{dual} \\
\Phi : H(P)^\vee, H(Q), H(W) \\
\Phi' : H(P), H(Q)^\vee, H(W)
\end{array}
\end{array}}\]
LaTeX source
\[
\boxed{\begin{array}{c|l}
\begin{array}{ccc} & \Psi & \\ \swarrow & & \searrow \\ \Phi & & \Phi' \\ \searrow & & \swarrow \\ & \Psi' & \end{array}
&
\begin{array}{l}
\Psi : H(P), H(Q), H(T), H(W) \\
\Psi' : \ldots\ \text{dual} \\
\Phi : H(P)^\vee, H(Q), H(W) \\
\Phi' : H(P), H(Q)^\vee, H(W)
\end{array}
\end{array}}
\]\[\left.\begin{aligned}
\Phi &\simeq S(W, P) \simeq S_{!}(W, Q) \\
\Phi' &\simeq S(W, Q) \simeq S_{!}(W, P)
\end{aligned}\right\} (\Phi, \Phi' \text{ duals})
\qquad
\left.\begin{aligned}
\Psi &\simeq S(W, T) \simeq MV(W; P, Q) \\
\Psi' &\simeq S_{!}(W, T) \simeq MV_{!}(W; P, Q)
\end{aligned}\right\} (\Psi, \Psi' \text{ duals})\]
LaTeX source
\[
\left.\begin{aligned}
\Phi &\simeq S(W, P) \simeq S_{!}(W, Q) \\
\Phi' &\simeq S(W, Q) \simeq S_{!}(W, P)
\end{aligned}\right\} (\Phi, \Phi' \text{ duals})
\qquad
\left.\begin{aligned}
\Psi &\simeq S(W, T) \simeq MV(W; P, Q) \\
\Psi' &\simeq S_{!}(W, T) \simeq MV_{!}(W; P, Q)
\end{aligned}\right\} (\Psi, \Psi' \text{ duals})
\]\[P \cap Q = \partial P = \partial Q, \qquad P \cup Q = W\]
LaTeX source
\[ P \cap Q = \partial P = \partial Q, \qquad P \cup Q = W \]
\[\begin{array}{ccc}
P \longrightarrow S & \qquad & Q \longrightarrow T \\
\wr & & \uparrow \\
M & & N
\end{array}\]
LaTeX source
\[
\begin{array}{ccc}
P \longrightarrow S & \qquad & Q \longrightarrow T \\
\wr & & \uparrow \\
M & & N
\end{array}
\]\[\begin{array}{ccc}
\partial P \longrightarrow S & \qquad & \partial Q \longrightarrow T \\
\wr & & \uparrow \\
\partial M & & \partial N
\end{array}\]
LaTeX source
\[
\begin{array}{ccc}
\partial P \longrightarrow S & \qquad & \partial Q \longrightarrow T \\
\wr & & \uparrow \\
\partial M & & \partial N
\end{array}
\]\[\alpha : S \simeq \partial N \qquad \beta : T \simeq \partial M\]
LaTeX source
\[ \alpha : S \simeq \partial N \qquad \beta : T \simeq \partial M \]
\[\sigma : \partial P \simeq S \times \partial M \qquad
\tau : \partial Q \simeq T \times \partial N\]
LaTeX source
\[ \sigma : \partial P \simeq S \times \partial M \qquad \tau : \partial Q \simeq T \times \partial N \]
\[(\alpha, \sigma) : \partial P \simeq \partial N \times \partial M, \qquad
(\beta, \tau) : \partial Q \simeq \partial M \times \partial N\]
LaTeX source
\[ (\alpha, \sigma) : \partial P \simeq \partial N \times \partial M, \qquad (\beta, \tau) : \partial Q \simeq \partial M \times \partial N \]
\[\varphi : \partial P \simeq \partial Q .\]
LaTeX source
\[ \varphi : \partial P \simeq \partial Q . \]
\[W - Q = P - \partial P \hookrightarrow P\]
LaTeX source
\[ W - Q = P - \partial P \hookrightarrow P \]
\[W - P = Q - \partial Q \hookrightarrow Q .\]
LaTeX source
\[ W - P = Q - \partial Q \hookrightarrow Q . \]
\[\begin{array}{cccc}
W & P & Q & R \\
V' & X'_{\eta} = V_{\eta} & V'_{s} & V'_{s} \times \eta
\end{array}
\qquad\qquad
\begin{array}{ccc} & W & \\ P & & Q \\ & R & \end{array}\]
LaTeX source
\[
\begin{array}{cccc}
W & P & Q & R \\
V' & X'_{\eta} = V_{\eta} & V'_{s} & V'_{s} \times \eta
\end{array}
\qquad\qquad
\begin{array}{ccc} & W & \\ P & & Q \\ & R & \end{array}
\]\[\begin{array}{cccc}
M & N & T = \dot{M}, & S = \dot{N} \\
X'_{\eta} & e & V'_{s} & \eta \sim S^{1}
\end{array}\]
LaTeX source
\[
\begin{array}{cccc}
M & N & T = \dot{M}, & S = \dot{N} \\
X'_{\eta} & e & V'_{s} & \eta \sim S^{1}
\end{array}
\]\[H^{i}(Q) \times H^{n-i-1}(P) \longrightarrow H^{n-1}(R) \simeq \Lambda\]
LaTeX source
\[
H^{i}(Q) \times H^{n-i-1}(P) \longrightarrow H^{n-1}(R) \simeq \Lambda
\]\[H^{n-i}(P)^\vee \longrightarrow H^{i}(P)\]
LaTeX source
\[
H^{n-i}(P)^\vee \longrightarrow H^{i}(P)
\]\[\binom{5}{2} = \frac{5.4.3}{12.} = 10\]
LaTeX source
\[
\binom{5}{2} = \frac{5.4.3}{12.} = 10
\]\[\begin{array}{ccc}
123 & 234 & 345 \\
124 & 235 & \\
125 & 245 & \\
134 & & \\
135 & & \\
145 & &
\end{array}
\qquad 10 + 10 + 2\]
LaTeX source
\[
\begin{array}{ccc}
123 & 234 & 345 \\
124 & 235 & \\
125 & 245 & \\
134 & & \\
135 & & \\
145 & &
\end{array}
\qquad 10 + 10 + 2
\]\[\begin{array}{ccc}
\emptyset & T \sim S & R \\
5 + 5 & 2 + 2 & 2 \\
3 & 3 + 3 & \\
2 + 2 & 1 + 1 & \\
1 + 2 & 1 + 1 & \\ \hline
\boxed{20} & \boxed{14} & \boxed{2}
\end{array}
\qquad
\begin{array}{c}
M \sim N \\
2 + 2 \\ \hline
\boxed{4}
\end{array}\]
LaTeX source
\[
\begin{array}{ccc}
\emptyset & T \sim S & R \\
5 + 5 & 2 + 2 & 2 \\
3 & 3 + 3 & \\
2 + 2 & 1 + 1 & \\
1 + 2 & 1 + 1 & \\ \hline
\boxed{20} & \boxed{14} & \boxed{2}
\end{array}
\qquad
\begin{array}{c}
M \sim N \\
2 + 2 \\ \hline
\boxed{4}
\end{array}
\]\[L^{\bullet\pi} = \mathbb{R}\Gamma(W_0 \times S^{1}) \simeq
\mathbb{R}\Gamma(W_0) \overset{\mathbf{L}}{\otimes}_{\Lambda} \mathbb{R}\Gamma(S^{1})
\simeq \mathbb{R}\Gamma(W_0) \times \mathbb{R}\Gamma(W_0)(-1)\]
LaTeX source
\[
L^{\bullet\pi} = \mathbb{R}\Gamma(W_0 \times S^{1}) \simeq
\mathbb{R}\Gamma(W_0) \overset{\mathbf{L}}{\otimes}_{\Lambda} \mathbb{R}\Gamma(S^{1})
\simeq \mathbb{R}\Gamma(W_0) \times \mathbb{R}\Gamma(W_0)(-1)
\]\[\begin{aligned}
\mathbb{R}\Gamma(P) \simeq \mathbb{R}\Gamma(W - W_0) &\xrightarrow[\ \alpha\ ]{\text{compatible avec cup}} \mathbb{R}\Gamma(W_0) \\
\mathbb{R}\Gamma(P) \simeq \mathbb{R}\Gamma(W - W_0) &\xrightarrow{\ \beta\ } \mathbb{R}\Gamma(W_0)(-1)
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
\mathbb{R}\Gamma(P) \simeq \mathbb{R}\Gamma(W - W_0) &\xrightarrow[\ \alpha\ ]{\text{compatible avec cup}} \mathbb{R}\Gamma(W_0) \\
\mathbb{R}\Gamma(P) \simeq \mathbb{R}\Gamma(W - W_0) &\xrightarrow{\ \beta\ } \mathbb{R}\Gamma(W_0)(-1)
\end{aligned}
\]\[u_1 = \rho_0, \qquad u_2 = \mathrm{id}_1\]
LaTeX source
\[
u_1 = \rho_0, \qquad u_2 = \mathrm{id}_1
\]\[\mathbb{R}(\Gamma, \pi)_{!}(\mathring{M}) \simeq
\mathbb{R}\mathrm{Hom}_{\Lambda}(K^\bullet, \Lambda)[2n],
\qquad K^\bullet = \mathbb{R}(\Gamma, \pi)(M),\]
LaTeX source
\[
\mathbb{R}(\Gamma, \pi)_{!}(\mathring{M}) \simeq
\mathbb{R}\mathrm{Hom}_{\Lambda}(K^\bullet, \Lambda)[2n],
\qquad K^\bullet = \mathbb{R}(\Gamma, \pi)(M),
\]\[\boxed{\ u : \mathbb{R}\mathrm{Hom}_{\Lambda}(K^\bullet, \Lambda)[-2n] \longrightarrow K^\bullet\ }
\qquad \text{dans } D(\Lambda[\pi]),\]
LaTeX source
\[
\boxed{\ u : \mathbb{R}\mathrm{Hom}_{\Lambda}(K^\bullet, \Lambda)[-2n] \longrightarrow K^\bullet\ }
\qquad \text{dans } D(\Lambda[\pi]),
\]\[\xi \in H^{2n}\bigl(K^\bullet \overset{\mathbf{L}}{\otimes}_{\Lambda} K^\bullet\bigr).\]
LaTeX source
\[
\xi \in H^{2n}\bigl(K^\bullet \overset{\mathbf{L}}{\otimes}_{\Lambda} K^\bullet\bigr).
\]\[\boxed{\ u_1 : \mathbb{R}\Gamma(W - W_0)^\vee[-2n-1] \longrightarrow \mathbb{R}\Gamma(W - W_0)\ }\]
LaTeX source
\[
\boxed{\ u_1 : \mathbb{R}\Gamma(W - W_0)^\vee[-2n-1] \longrightarrow \mathbb{R}\Gamma(W - W_0)\ }
\]\[\boxed{\begin{aligned}
\lambda &: \mathbb{R}\Gamma(W_0) \times \mathbb{R}\Gamma(W - W_0) \longrightarrow \Lambda[-2n] \\
\mu &: \mathbb{R}\Gamma(W_0) \times \mathbb{R}\Gamma(W - W_0) \longrightarrow \Lambda[-(2n-1)]
\end{aligned}}\]
LaTeX source
\[
\boxed{\begin{aligned}
\lambda &: \mathbb{R}\Gamma(W_0) \times \mathbb{R}\Gamma(W - W_0) \longrightarrow \Lambda[-2n] \\
\mu &: \mathbb{R}\Gamma(W_0) \times \mathbb{R}\Gamma(W - W_0) \longrightarrow \Lambda[-(2n-1)]
\end{aligned}}
\]\[\begin{aligned}
\lambda &: H^{2n-i}(W_0) \times H^{i}(W - W_0) \longrightarrow \Lambda \\
\mu &: H^{2n-1-i}(W_0) \times H^{i}(W - W_0) \longrightarrow \Lambda
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
\lambda &: H^{2n-i}(W_0) \times H^{i}(W - W_0) \longrightarrow \Lambda \\
\mu &: H^{2n-1-i}(W_0) \times H^{i}(W - W_0) \longrightarrow \Lambda
\end{aligned}
\]\[\begin{aligned}
\lambda^i &: H^{i}(W - W_0) \longrightarrow H^{i-1}(W_0) && \text{je dis que c'est } \beta \\
\mu^i &: H^{i}(W - W_0) \longrightarrow H^{i}(W_0) && \text{je dis que c'est } \alpha
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
\lambda^i &: H^{i}(W - W_0) \longrightarrow H^{i-1}(W_0) && \text{je dis que c'est } \beta \\
\mu^i &: H^{i}(W - W_0) \longrightarrow H^{i}(W_0) && \text{je dis que c'est } \alpha
\end{aligned}
\]\[L^{\bullet\,\mathrm{triv}} \times K^\bullet \longrightarrow \Lambda[-2n+1]\]
LaTeX source
\[
L^{\bullet\,\mathrm{triv}} \times K^\bullet \longrightarrow \Lambda[-2n+1]
\]\[\boxed{\ \text{accoupl\supplied{ement}}\quad \mathbb{R}\Gamma(W_0)^{\mathrm{triv}} \times
\mathbb{R}(\Gamma, \pi)(M) \longrightarrow \Lambda[-(2n-1)]\ }\]
LaTeX source
\[
\boxed{\ \text{accoupl\supplied{ement}}\quad \mathbb{R}\Gamma(W_0)^{\mathrm{triv}} \times
\mathbb{R}(\Gamma, \pi)(M) \longrightarrow \Lambda[-(2n-1)]\ }
\]\[\mathbb{R}(\Gamma, \pi)(M) \longrightarrow
\mathbb{R}\Gamma(W_0)^\vee[-(2n-1)]^{\mathrm{triv}} \simeq \mathbb{R}\Gamma(W_0)^{\mathrm{triv}}\]
LaTeX source
\[
\mathbb{R}(\Gamma, \pi)(M) \longrightarrow
\mathbb{R}\Gamma(W_0)^\vee[-(2n-1)]^{\mathrm{triv}} \simeq \mathbb{R}\Gamma(W_0)^{\mathrm{triv}}
\]\[\cdots \longrightarrow H^{i-2}(W_0) \longrightarrow H^{i}(W) \longrightarrow
H^{i}(W - W_0) \longrightarrow H^{i-1}(W_0) \longrightarrow H^{i+1}(W)\]
LaTeX source
\[
\cdots \longrightarrow H^{i-2}(W_0) \longrightarrow H^{i}(W) \longrightarrow
H^{i}(W - W_0) \longrightarrow H^{i-1}(W_0) \longrightarrow H^{i+1}(W)
\]\[\begin{aligned}
&\underbrace{H^{2n}(W)}_{=0} \to H^{2n}(W - W_0) \xrightarrow{\ \mathrm{inj}\ }
\underbrace{H^{2n-1}(W_0)}_{\simeq \Lambda} \xrightarrow{\ \mathrm{surj}\ }
\underbrace{H^{2n+1}(W)}_{=\Lambda} \\
&\qquad \to \underbrace{H^{2n+1}(W - W_0)}_{=0}
\to \underbrace{H^{2n}(W_0)}_{=0} \to 0
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
&\underbrace{H^{2n}(W)}_{=0} \to H^{2n}(W - W_0) \xrightarrow{\ \mathrm{inj}\ }
\underbrace{H^{2n-1}(W_0)}_{\simeq \Lambda} \xrightarrow{\ \mathrm{surj}\ }
\underbrace{H^{2n+1}(W)}_{=\Lambda} \\
&\qquad \to \underbrace{H^{2n+1}(W - W_0)}_{=0}
\to \underbrace{H^{2n}(W_0)}_{=0} \to 0
\end{aligned}
\]\[\left\{\begin{aligned}
H^{2n}(W - W_0) &= H^{2n+1}(W - W_0) = 0 \\
\Lambda = H^{2n-1}(W_0) &\simeq H^{2n+1}(W) = \Lambda
\end{aligned}\right.\]
LaTeX source
\[
\left\{\begin{aligned}
H^{2n}(W - W_0) &= H^{2n+1}(W - W_0) = 0 \\
\Lambda = H^{2n-1}(W_0) &\simeq H^{2n+1}(W) = \Lambda
\end{aligned}\right.
\]\[\left\{\begin{aligned}
H^{i}(W) \longrightarrow H^{i}(W_0) \quad &\text{un isom pour } i \leq n-2 \\
&\text{un mono pour } i = n-1
\end{aligned}\right.\]
LaTeX source
\[
\left\{\begin{aligned}
H^{i}(W) \longrightarrow H^{i}(W_0) \quad &\text{un isom pour } i \leq n-2 \\
&\text{un mono pour } i = n-1
\end{aligned}\right.
\]\[\left\{\begin{aligned}
H^{i}_{!}(W_0) \longrightarrow H^{i+2}(W) \quad &\text{un isom si } i \geq n+1 \\
&\text{un épim si } i = n
\end{aligned}\right.\]
LaTeX source
\[
\left\{\begin{aligned}
H^{i}_{!}(W_0) \longrightarrow H^{i+2}(W) \quad &\text{un isom si } i \geq n+1 \\
&\text{un épim si } i = n
\end{aligned}\right.
\]\[\Bigl[\ H^{i}(W - W_0) = 0 \ \text{ si } i > n+1 \Bigr],
\qquad H^{i}(W - W_0) = H^{i}(P).\]
LaTeX source
\[
\Bigl[\ H^{i}(W - W_0) = 0 \ \text{ si } i > n+1 \Bigr],
\qquad H^{i}(W - W_0) = H^{i}(P).
\]\[\left\{\begin{aligned}
H^{i}(W - W_0) &= 0 \quad \text{si } i > n+1 \\
H^{i}(W_0) &= 0 \quad \text{si } i \neq n-1, n, 0, 2n-1
\end{aligned}\right.\]
LaTeX source
\[
\left\{\begin{aligned}
H^{i}(W - W_0) &= 0 \quad \text{si } i > n+1 \\
H^{i}(W_0) &= 0 \quad \text{si } i \neq n-1, n, 0, 2n-1
\end{aligned}\right.
\]\[0 \to H^{0}(W) \to H^{0}(W - W_0) \to 0, \qquad
0 \to H^{1}(W - W_0) \to H^{0}(W_0) \to 0\]
LaTeX source
\[
0 \to H^{0}(W) \to H^{0}(W - W_0) \to 0, \qquad
0 \to H^{1}(W - W_0) \to H^{0}(W_0) \to 0
\]\[\left\{\begin{aligned}
&0 \to H^{n}(W - W_0) \to H^{n-1}(W_0) \to 0 \\
&0 \to H^{n+1}(W - W_0) \to H^{n}(W_0) \to 0 \qquad (\text{si } n \neq 1) \\
&0 \to H^{2n-1}(W_0) \to H^{2n+1}(W) \to 0
\end{aligned}\right.\]
LaTeX source
\[
\left\{\begin{aligned}
&0 \to H^{n}(W - W_0) \to H^{n-1}(W_0) \to 0 \\
&0 \to H^{n+1}(W - W_0) \to H^{n}(W_0) \to 0 \qquad (\text{si } n \neq 1) \\
&0 \to H^{2n-1}(W_0) \to H^{2n+1}(W) \to 0
\end{aligned}\right.
\]\[\begin{aligned}
&0 \to H^{0}(W) \xrightarrow{\ \sim\ } H^{0}(W - W_0) \to 0 \\
&0 \to H^{1}(W - W_0) \to H^{0}(W_0) \to 0 \\
&0 \to H^{2}(W - W_0) \to H^{1}(W_0) \to H^{3}(W) \simeq \Lambda \to 0 \ ]
\end{aligned}\]
LaTeX source
\[
\begin{aligned}
&0 \to H^{0}(W) \xrightarrow{\ \sim\ } H^{0}(W - W_0) \to 0 \\
&0 \to H^{1}(W - W_0) \to H^{0}(W_0) \to 0 \\
&0 \to H^{2}(W - W_0) \to H^{1}(W_0) \to H^{3}(W) \simeq \Lambda \to 0 \ ]
\end{aligned}
\]\[\boxed{\ H^{i}(M, \Lambda) = 0 \quad \text{si } i > n\ }\]
LaTeX source
\[
\boxed{\ H^{i}(M, \Lambda) = 0 \quad \text{si } i > n\ }
\]\[\cdots \to H^{2n-i}(M)^\vee \to H^{i}(M) \to H^{i}(W_0) \to
H^{2n-i-1}(M)^\vee \to H^{i+1}(M) \to H^{i+1}(W_0)\]
LaTeX source
\[
\cdots \to H^{2n-i}(M)^\vee \to H^{i}(M) \to H^{i}(W_0) \to
H^{2n-i-1}(M)^\vee \to H^{i+1}(M) \to H^{i+1}(W_0)
\]\[\left\{\begin{aligned}
H^{i}(W_0) &\xrightarrow{\ \sim\ } H^{2n-i-1}(M)^\vee && \text{si } i \geq n+2
&& (\text{épim si } i = n+1) \quad (\text{donc } 2n-i-1 \leq n-3) \\
H^{i}(M) &\xrightarrow{\ \sim\ } H^{i}(W_0) && \text{si } i \leq n-2
&& (\text{mono si } i = n-1)
\end{aligned}\right.\]
LaTeX source
\[
\left\{\begin{aligned}
H^{i}(W_0) &\xrightarrow{\ \sim\ } H^{2n-i-1}(M)^\vee && \text{si } i \geq n+2
&& (\text{épim si } i = n+1) \quad (\text{donc } 2n-i-1 \leq n-3) \\
H^{i}(M) &\xrightarrow{\ \sim\ } H^{i}(W_0) && \text{si } i \leq n-2
&& (\text{mono si } i = n-1)
\end{aligned}\right.
\]\[\boxed{\begin{array}{c}
0 \to H^{n+1}(M)^\vee \xrightarrow{\ u\ } H^{n-1}(M) \to H^{n-1}(W_0) \to H^{n}(M)^\vee \\
\downarrow \\
0 \leftarrow H^{n+1}(M) \xleftarrow{\ {}^t u\ } H^{n-1}(M)^\vee \leftarrow H^{n}(W_0) \leftarrow H^{n}(M)
\end{array}}\]
LaTeX source
\[
\boxed{\begin{array}{c}
0 \to H^{n+1}(M)^\vee \xrightarrow{\ u\ } H^{n-1}(M) \to H^{n-1}(W_0) \to H^{n}(M)^\vee \\
\downarrow \\
0 \leftarrow H^{n+1}(M) \xleftarrow{\ {}^t u\ } H^{n-1}(M)^\vee \leftarrow H^{n}(W_0) \leftarrow H^{n}(M)
\end{array}}
\]\[\Updownarrow\]
LaTeX source
\[ \Updownarrow \]
\[\left\{\begin{aligned}
&H^{i}(V_\eta) \to H^{i-1}(V_s) \ \text{un \emph{isom} si } i \neq 0, 2n \\
&\emph{et}\ \left\{\begin{aligned}
&H^{0}(V_\eta) \simeq \Lambda \\
&H^{2n}(V_\eta) \to H^{2n-1}(V_s) \ \text{inj et conoyau} \simeq \Lambda \\
\end{aligned}\right. \qquad (\text{quand } n \geq 1)
\end{aligned}\right.\]
LaTeX source
\[
\left\{\begin{aligned}
&H^{i}(V_\eta) \to H^{i-1}(V_s) \ \text{un \emph{isom} si } i \neq 0, 2n \\
&\emph{et}\ \left\{\begin{aligned}
&H^{0}(V_\eta) \simeq \Lambda \\
&H^{2n}(V_\eta) \to H^{2n-1}(V_s) \ \text{inj et conoyau} \simeq \Lambda \\
\end{aligned}\right. \qquad (\text{quand } n \geq 1)
\end{aligned}\right.
\]\[\Bigl[\ 0 \to \underbrace{H^{2n}(V_\eta)}_{=0 \text{ si } n \geq 2} \to H^{2n-1}(V_s)
\to H^{2n+1}(V) \to \underbrace{H^{2n+1}(V_\eta)}_{=0 \text{ si } n \geq 1}
\to \underbrace{H^{2n}(V_s)}_{=0} \to 0 \ \Bigr]\]
LaTeX source
\[
\Bigl[\ 0 \to \underbrace{H^{2n}(V_\eta)}_{=0 \text{ si } n \geq 2} \to H^{2n-1}(V_s)
\to H^{2n+1}(V) \to \underbrace{H^{2n+1}(V_\eta)}_{=0 \text{ si } n \geq 1}
\to \underbrace{H^{2n}(V_s)}_{=0} \to 0 \ \Bigr]
\]\[\Downarrow \quad \text{si on suppose déjà que l'on a singularité « isolée »}\]
LaTeX source
\[
\Downarrow \quad \text{si on suppose déjà que l'on a singularité « isolée »}
\]\[H^{i}(V_s) = 0 \quad \text{si } i \neq 0, n-1, n\]
LaTeX source
\[
H^{i}(V_s) = 0 \quad \text{si } i \neq 0, n-1, n
\]