Cote n° 158 · pages 1–83
· 180 displayed formulas · [Autour des Dérivateurs] : notes manuscrites (s.d.).
Inventory dating : [vers 1990-1991]
Édition de démonstration
\[\mathrm{Hom}(G, F^{I}) = \mathrm{Hom}\bigl(I, \mathrm{Hom}(G,F)\bigr)\]
LaTeX source
\[
\mathrm{Hom}(G, F^{I}) = \mathrm{Hom}\bigl(I, \mathrm{Hom}(G,F)\bigr)
\]\[\mathrm{P}(b,E) \times \mathrm{P}(b',E')
= \coprod_{(z,z') \in E \times E'} \widetilde{z} \times \widetilde{z}'\]
LaTeX source
\[
\mathrm{P}(b,E) \times \mathrm{P}(b',E')
= \coprod_{(z,z') \in E \times E'} \widetilde{z} \times \widetilde{z}'
\]\[u(F) \subset F' \quad \Longleftrightarrow \quad F \subset u^{-1}(F')\]
LaTeX source
\[
u(F) \subset F' \quad \Longleftrightarrow \quad F \subset u^{-1}(F')
\]\[\coprod_{z \in E} z \ \times \coprod_{z' \in E'} z'
= \coprod_{(z,z') \in E \times E'} z \times z'\]
LaTeX source
\[
\coprod_{z \in E} z \ \times \coprod_{z' \in E'} z'
= \coprod_{(z,z') \in E \times E'} z \times z'
\]\[\mathrm{Hom}_{C}\bigl((b,E),(b',E')\bigr) \hookrightarrow \mathrm{Hom}_{B}(b,b')\]
LaTeX source
\[
\mathrm{Hom}_{C}\bigl((b,E),(b',E')\bigr) \hookrightarrow \mathrm{Hom}_{B}(b,b')
\]\[\{\, u : b \to b' \ \mid \ \widetilde{\pi}(u)(E) \subset E' \,\}\]
LaTeX source
\[
\{\, u : b \to b' \ \mid \ \widetilde{\pi}(u)(E) \subset E' \,\}
\]\[\widetilde{\pi}\backslash B \ \simeq \ B/\widetilde{\pi} \ = \ C,
\qquad \pi\backslash B \ = \ Z\]
LaTeX source
\[
\widetilde{\pi}\backslash B \ \simeq \ B/\widetilde{\pi} \ = \ C,
\qquad \pi\backslash B \ = \ Z
\]\[C \longrightarrow Z^{\wedge}, \qquad (b,E) \longmapsto \coprod_{z \in E} z\]
LaTeX source
\[
C \longrightarrow Z^{\wedge}, \qquad (b,E) \longmapsto \coprod_{z \in E} z
\]\[u^{E,E'}_{*} : \widetilde{E} \longrightarrow \widetilde{E}',
\qquad \widetilde{E} = \coprod_{z \in E} z, \qquad z \longmapsto \widetilde{z}'\]
LaTeX source
\[
u^{E,E'}_{*} : \widetilde{E} \longrightarrow \widetilde{E}',
\qquad \widetilde{E} = \coprod_{z \in E} z, \qquad z \longmapsto \widetilde{z}'
\]\[(b,E) \times (b',E') = \bigl(b \times b',\ p_{1}^{*}(E) \cap p_{2}^{*}(E')\bigr)\]
LaTeX source
\[
(b,E) \times (b',E') = \bigl(b \times b',\ p_{1}^{*}(E) \cap p_{2}^{*}(E')\bigr)
\]\[F \in \mathrm{Ob}\,X^{\wedge}/U \simeq (X/U)^{\wedge} = Y^{\wedge},\]
LaTeX source
\[
F \in \mathrm{Ob}\,X^{\wedge}/U \simeq (X/U)^{\wedge} = Y^{\wedge},
\]\[\widetilde{\Delta}_{n} = [0,n] \cap \mathbf{Z}\]
LaTeX source
\[
\widetilde{\Delta}_{n} = [0,n] \cap \mathbf{Z}
\]\[\pi(I) = \pi_{0}(F^{I}), \qquad \text{i.e.} \qquad
\pi(\widetilde{\Delta}_{n}) = \pi_{0}(F^{\,n+1}).\]
LaTeX source
\[
\pi(I) = \pi_{0}(F^{I}), \qquad \text{i.e.} \qquad
\pi(\widetilde{\Delta}_{n}) = \pi_{0}(F^{\,n+1}).
\]\[\varphi : (\widetilde{\Delta}_{/\pi})^{\circ} \longrightarrow Y^{\wedge}
\simeq (X/U)^{\wedge} \simeq X^{\wedge}/U .\]
LaTeX source
\[
\varphi : (\widetilde{\Delta}_{/\pi})^{\circ} \longrightarrow Y^{\wedge}
\simeq (X/U)^{\wedge} \simeq X^{\wedge}/U .
\]\[\varphi(\widetilde{\Delta}_{n}, \alpha) = \alpha \subset F^{\,n+1}\]
LaTeX source
\[
\varphi(\widetilde{\Delta}_{n}, \alpha) = \alpha \subset F^{\,n+1}
\]\[\widetilde{\Delta}^{\wedge} \longrightarrow (X/U)^{\wedge} \simeq X^{\wedge}/U\]
LaTeX source
\[
\widetilde{\Delta}^{\wedge} \longrightarrow (X/U)^{\wedge} \simeq X^{\wedge}/U
\]\[f^{*}(G^{\Psi}) = f^{*}(G)^{\,f^{*}(\Psi)}\]
LaTeX source
\[
f^{*}(G^{\Psi}) = f^{*}(G)^{\,f^{*}(\Psi)}
\]\[\varphi(\rho) : \beta \longrightarrow \alpha,
\qquad \beta = \varphi(\widetilde{\Delta}_{m}, \beta),
\qquad \alpha = \varphi(\widetilde{\Delta}_{n}, \alpha).\]
LaTeX source
\[
\varphi(\rho) : \beta \longrightarrow \alpha,
\qquad \beta = \varphi(\widetilde{\Delta}_{m}, \beta),
\qquad \alpha = \varphi(\widetilde{\Delta}_{n}, \alpha).
\]\[\Phi : \bigl((\widetilde{\Delta}_{/\pi})^{\circ}\bigr)^{\wedge}
\longrightarrow Y^{\wedge},
\qquad
\bigl((\widetilde{\Delta}_{/\pi})^{\circ}\bigr)^{\wedge}
= (\widetilde{\Delta}_{/\pi})^{\wedge} = Z^{\wedge},\]
LaTeX source
\[
\Phi : \bigl((\widetilde{\Delta}_{/\pi})^{\circ}\bigr)^{\wedge}
\longrightarrow Y^{\wedge},
\qquad
\bigl((\widetilde{\Delta}_{/\pi})^{\circ}\bigr)^{\wedge}
= (\widetilde{\Delta}_{/\pi})^{\wedge} = Z^{\wedge},
\]\[f : Y^{\wedge} \longrightarrow Z^{\wedge}
\qquad \bigl(\text{où } Z \overset{\text{déf}}{=} (\widetilde{\Delta}_{/\pi})^{\circ}\bigr).\]
LaTeX source
\[
f : Y^{\wedge} \longrightarrow Z^{\wedge}
\qquad \bigl(\text{où } Z \overset{\text{déf}}{=} (\widetilde{\Delta}_{/\pi})^{\circ}\bigr).
\]\[Z = (A_{/\pi})^{\circ} \simeq \pi\backslash A^{\circ} = \pi\backslash B,
\qquad \pi : A^{\circ} \longrightarrow (\mathrm{Ens}), \quad B = A^{\circ}.\]
LaTeX source
\[
Z = (A_{/\pi})^{\circ} \simeq \pi\backslash A^{\circ} = \pi\backslash B,
\qquad \pi : A^{\circ} \longrightarrow (\mathrm{Ens}), \quad B = A^{\circ}.
\]\[\widetilde{E} = \coprod_{a \in E} a
\qquad \text{(somme prise dans } Z^{\wedge}\text{)}.\]
LaTeX source
\[
\widetilde{E} = \coprod_{a \in E} a
\qquad \text{(somme prise dans } Z^{\wedge}\text{)}.
\]\[u_{*} = \pi(u) : Z_{b} \longrightarrow Z_{b'},
\qquad Z_{b} = \pi(b), \quad Z_{b'} = \pi(b'),\]
LaTeX source
\[
u_{*} = \pi(u) : Z_{b} \longrightarrow Z_{b'},
\qquad Z_{b} = \pi(b), \quad Z_{b'} = \pi(b'),
\]\[u^{E,E'}_{*} : \widetilde{E} \longrightarrow \widetilde{E}' .\]
LaTeX source
\[
u^{E,E'}_{*} : \widetilde{E} \longrightarrow \widetilde{E}' .
\]\[\widetilde{\pi}(u)(E) \subset E' \qquad \text{(et non } \widetilde{\pi}(u)(E) = E').\]
LaTeX source
\[
\widetilde{\pi}(u)(E) \subset E' \qquad \text{(et non } \widetilde{\pi}(u)(E) = E').
\]\[\widetilde{\pi}\backslash B \longrightarrow (\pi\backslash B)^{\wedge} = Z^{\wedge},
\qquad
(b,E) \longmapsto \widetilde{E} = \coprod_{a \in E} a \ \subset
\coprod_{a \in Z_{b}} a,\]
LaTeX source
\[
\widetilde{\pi}\backslash B \longrightarrow (\pi\backslash B)^{\wedge} = Z^{\wedge},
\qquad
(b,E) \longmapsto \widetilde{E} = \coprod_{a \in E} a \ \subset
\coprod_{a \in Z_{b}} a,
\]\[\widetilde{\pi}\backslash B \ \simeq \ \pi\backslash B \ \simeq \ B,\]
LaTeX source
\[
\widetilde{\pi}\backslash B \ \simeq \ \pi\backslash B \ \simeq \ B,
\]\[u_{*} = \widetilde{\pi}(u) : \widetilde{\pi}(b) \longrightarrow
\widetilde{\pi}(b'),
\qquad
\mathfrak{P}^{*}(\pi(b)) \longrightarrow \mathfrak{P}^{*}(\pi(b')),
\qquad E \longmapsto \pi(u)(E),\]
LaTeX source
\[
u_{*} = \widetilde{\pi}(u) : \widetilde{\pi}(b) \longrightarrow
\widetilde{\pi}(b'),
\qquad
\mathfrak{P}^{*}(\pi(b)) \longrightarrow \mathfrak{P}^{*}(\pi(b')),
\qquad E \longmapsto \pi(u)(E),
\]\[\Delta(E) = \text{groupe engendré par les } [x,y], \quad (x,y) \in E^{2},\]
LaTeX source
\[
\Delta(E) = \text{groupe engendré par les } [x,y], \quad (x,y) \in E^{2},
\]\[[x,x] = 1, \qquad [x,y][y,x] = 1, \qquad [x,y][y,z] = [x,z].\]
LaTeX source
\[ [x,x] = 1, \qquad [x,y][y,x] = 1, \qquad [x,y][y,z] = [x,z]. \]
\[g_{i} = [i, i+1] \qquad \text{pour } i \in [1, n-1].\]
LaTeX source
\[
g_{i} = [i, i+1] \qquad \text{pour } i \in [1, n-1].
\]\[\begin{cases}
[i,j] = g_{i}\,g_{i+1} \cdots g_{j-1} \\
[j,i] = [i,j]^{-1} = g_{j-1}^{-1} \cdots g_{i+1}^{-1} g_{i}^{-1}
\end{cases}\]
LaTeX source
\[
\begin{cases}
[i,j] = g_{i}\,g_{i+1} \cdots g_{j-1} \\
[j,i] = [i,j]^{-1} = g_{j-1}^{-1} \cdots g_{i+1}^{-1} g_{i}^{-1}
\end{cases}
\]\[[\alpha v, \alpha u] = [\beta v, \beta u],
\qquad \text{i.e.} \qquad [\alpha v, \alpha u]\,[\beta v, \beta u]^{-1} = 1 .\]
LaTeX source
\[
[\alpha v, \alpha u] = [\beta v, \beta u],
\qquad \text{i.e.} \qquad [\alpha v, \alpha u]\,[\beta v, \beta u]^{-1} = 1 .
\]\[H_{m,n} \times H_{n,p} \longrightarrow H_{m,p}\]
LaTeX source
\[
H_{m,n} \times H_{n,p} \longrightarrow H_{m,p}
\]\[fu = gv, \qquad gv' = gw, \qquad fuv_{1} = gwv_{1} = gv'v'_{1} = gw\,v'_{1}\]
LaTeX source
\[
fu = gv, \qquad gv' = gw, \qquad fuv_{1} = gwv_{1} = gv'v'_{1} = gw\,v'_{1}
\]\[H_{x} = x/R_{x}\]
LaTeX source
\[
H_{x} = x/R_{x}
\]\[M = \mathrm{End}_{X}(e) = \mathrm{End}_{X_{0}}(e)\]
LaTeX source
\[
M = \mathrm{End}_{X}(e) = \mathrm{End}_{X_{0}}(e)
\]\[uu' = vv',\]
LaTeX source
\[ uu' = vv', \]
\[[v,u] \overset{\text{déf}}{=} v'u'^{-1} \in G = \pi_{1}(X_{0}, e).\]
LaTeX source
\[
[v,u] \overset{\text{déf}}{=} v'u'^{-1} \in G = \pi_{1}(X_{0}, e).
\]\[[v,u] = v_{1}^{-1} u_{1} .\]
LaTeX source
\[
[v,u] = v_{1}^{-1} u_{1} .
\]\[G = \pi_{1}(X_{0}, e) \longrightarrow \pi_{1}(X, e)\]
LaTeX source
\[
G = \pi_{1}(X_{0}, e) \longrightarrow \pi_{1}(X, e)
\]\[[w, gv]\,[v, fu]\,[w, gfu]^{-1} .\]
LaTeX source
\[
[w, gv]\,[v, fu]\,[w, gfu]^{-1} .
\]\[\pi_{1}(X_{0}, e) \ \xrightarrow{\ \sim\ }\ G
\ \xrightarrow{\ \sim\ }\ \pi_{1}(X,e) \qquad \text{iso !}\]
LaTeX source
\[
\pi_{1}(X_{0}, e) \ \xrightarrow{\ \sim\ }\ G
\ \xrightarrow{\ \sim\ }\ \pi_{1}(X,e) \qquad \text{iso !}
\]\[u \sim_{R} v \quad \Longleftrightarrow \quad \exists\, p, q \in M\]
LaTeX source
\[
u \sim_{R} v \quad \Longleftrightarrow \quad \exists\, p, q \in M
\]\[Y = B_{M}, \qquad \varphi \in M, \qquad \varphi f u = \varphi g v ,\]
LaTeX source
\[
Y = B_{M}, \qquad \varphi \in M, \qquad \varphi f u = \varphi g v ,
\]\[X = Y/F .\]
LaTeX source
\[ X = Y/F . \]
\[\mathrm{Hom}(x,y) \simeq \{\, u \in M \mid x = yu \,\},\]
LaTeX source
\[
\mathrm{Hom}(x,y) \simeq \{\, u \in M \mid x = yu \,\},
\]\[x = \dot{u} = au .\]
LaTeX source
\[
x = \dot{u} = au .
\]\[M_0 = \mathrm{End}_X(e) = \{\, f \in M \mid ef = e,\ \text{i.e. } a\psi f = a\psi,
\ \text{i.e. } \psi f \overset{R}{\sim} \psi \,\}.\]
LaTeX source
\[
M_0 = \mathrm{End}_X(e) = \{\, f \in M \mid ef = e,\ \text{i.e. } a\psi f = a\psi,
\ \text{i.e. } \psi f \overset{R}{\sim} \psi \,\}.
\]\[f \in M_0 \iff \forall\, p,q \in \mathbb{N} \quad \varphi^{p}\psi f = \varphi^{q}\psi .\]
LaTeX source
\[
f \in M_0 \iff \forall\, p,q \in \mathbb{N} \quad \varphi^{p}\psi f = \varphi^{q}\psi .
\]\[\delta(f) \overset{\text{déf}}{=} q - p\]
LaTeX source
\[
\delta(f) \overset{\text{déf}}{=} q - p
\]\[\begin{cases}
\varphi^{p}\psi f = \varphi^{q}\psi \\
\varphi^{p'}\psi f = \varphi^{q'}\psi
\end{cases}\]
LaTeX source
\[
\begin{cases}
\varphi^{p}\psi f = \varphi^{q}\psi \\
\varphi^{p'}\psi f = \varphi^{q'}\psi
\end{cases}
\]\[\varphi^{p+p'}\psi f =
\begin{cases}
\varphi^{p'+q}\psi \\
\varphi^{p+q'}\psi
\end{cases}\]
LaTeX source
\[
\varphi^{p+p'}\psi f =
\begin{cases}
\varphi^{p'+q}\psi \\
\varphi^{p+q'}\psi
\end{cases}
\]\[\varphi^{p'+q}\psi = \varphi^{p+q'}\psi .\]
LaTeX source
\[
\varphi^{p'+q}\psi = \varphi^{p+q'}\psi .
\]\[M_0 \xrightarrow{\ \delta\ } \mathbb{Z} ,\]
LaTeX source
\[
M_0 \xrightarrow{\ \delta\ } \mathbb{Z} ,
\]\[\begin{cases}
\varphi^{p}\psi f = \varphi^{q}\psi \\
\varphi^{p'}\psi g = \varphi^{q'}\psi
\end{cases}\]
LaTeX source
\[
\begin{cases}
\varphi^{p}\psi f = \varphi^{q}\psi \\
\varphi^{p'}\psi g = \varphi^{q'}\psi
\end{cases}
\]\[\varphi^{p+p'}\psi fg = \varphi^{q+p'}\psi g
= \varphi^{q}\bigl(\underbrace{\varphi^{p'}\psi g}_{\varphi^{q'}\psi}\bigr)
= \varphi^{q+q'}\psi\]
LaTeX source
\[
\varphi^{p+p'}\psi fg = \varphi^{q+p'}\psi g
= \varphi^{q}\bigl(\underbrace{\varphi^{p'}\psi g}_{\varphi^{q'}\psi}\bigr)
= \varphi^{q+q'}\psi
\]\[M_0 \xrightarrow{\ \mathrm{can}\ } G_0 \xrightarrow{\ \delta_0\ } \mathbb{Z} .\]
LaTeX source
\[
M_0 \xrightarrow{\ \mathrm{can}\ } G_0 \xrightarrow{\ \delta_0\ } \mathbb{Z} .
\]\[\begin{cases}
z = a\rho \\
y = a\rho g \\
x = a\rho g f
\end{cases}
\qquad\text{donc}\qquad
\begin{cases}
e = xu = a\rho g f u \\
e = yv = a\rho g v \\
e = zw = a\rho w
\end{cases}\]
LaTeX source
\[
\begin{cases}
z = a\rho \\
y = a\rho g \\
x = a\rho g f
\end{cases}
\qquad\text{donc}\qquad
\begin{cases}
e = xu = a\rho g f u \\
e = yv = a\rho g v \\
e = zw = a\rho w
\end{cases}
\]\[(\ast\ast) \qquad
\boxed{\ \rho g f u \overset{R}{\sim} \rho g v \overset{R}{\sim} \rho w \overset{R}{\sim} \psi\ }\]
LaTeX source
\[
(\ast\ast) \qquad
\boxed{\ \rho g f u \overset{R}{\sim} \rho g v \overset{R}{\sim} \rho w \overset{R}{\sim} \psi\ }
\]\[\boxed{\ \varphi^{p}(\rho g f u) = \varphi^{q}(\rho g v) = \varphi^{r}(\rho w) = \varphi^{s}\psi\ }\]
LaTeX source
\[
\boxed{\ \varphi^{p}(\rho g f u) = \varphi^{q}(\rho g v) = \varphi^{r}(\rho w) = \varphi^{s}\psi\ }
\]\[\boxed{\ [w,\, gv]\,[v,\, fu]\,[w,\, gfu]^{-1} = 1\ } ,\]
LaTeX source
\[
\boxed{\ [w,\, gv]\,[v,\, fu]\,[w,\, gfu]^{-1} = 1\ } ,
\]\[\boxed{\ \sigma\lambda \overset{R}{\sim} \sigma\mu \overset{R}{\sim} \psi\ } ,\]
LaTeX source
\[
\boxed{\ \sigma\lambda \overset{R}{\sim} \sigma\mu \overset{R}{\sim} \psi\ } ,
\]\[\eta =
\begin{cases}
e\lambda' = a\sigma\lambda\lambda' = a\sigma\pi \\
e\mu' = a\sigma\mu\mu' = a\sigma\pi
\end{cases}\]
LaTeX source
\[
\eta =
\begin{cases}
e\lambda' = a\sigma\lambda\lambda' = a\sigma\pi \\
e\mu' = a\sigma\mu\mu' = a\sigma\pi
\end{cases}
\]\[\boxed{\ \sigma\pi\nu \overset{R}{\sim} \psi\ }
\qquad\text{où } \pi = \lambda\lambda' = \mu\mu' .\]
LaTeX source
\[
\boxed{\ \sigma\pi\nu \overset{R}{\sim} \psi\ }
\qquad\text{où } \pi = \lambda\lambda' = \mu\mu' .
\]\[\begin{cases}
\lambda'\nu,\ \mu'\nu \in M_0 \\
\lambda(\lambda'\nu) = \mu(\mu'\nu)
\end{cases}\]
LaTeX source
\[
\begin{cases}
\lambda'\nu,\ \mu'\nu \in M_0 \\
\lambda(\lambda'\nu) = \mu(\mu'\nu)
\end{cases}
\]\[[\mu,\lambda] = (\mu'\nu)(\lambda'\nu)^{-1} .\]
LaTeX source
\[
[\mu,\lambda] = (\mu'\nu)(\lambda'\nu)^{-1} .
\]\[[\mu,\lambda] = \bigl(\mu'\,\theta(\sigma\pi)\bigr)\bigl(\lambda'\,\theta(\sigma\pi)\bigr)^{-1}\]
LaTeX source
\[
[\mu,\lambda] = \bigl(\mu'\,\theta(\sigma\pi)\bigr)\bigl(\lambda'\,\theta(\sigma\pi)\bigr)^{-1}
\]\[u\,\theta(u) = \psi \qquad \text{(plus seulement } \overset{R}{\sim} \psi\text{)} ;\]
LaTeX source
\[
u\,\theta(u) = \psi \qquad \text{(plus seulement } \overset{R}{\sim} \psi\text{)} ;
\]\[[\mu,\lambda] = \bigl(\underbrace{\theta(\mu)\,\theta(\sigma\psi)}_{\in M_0}\bigr)
\bigl(\underbrace{\theta(\lambda)\,\theta(\sigma\psi)}_{\in M_0}\bigr)^{-1}\]
LaTeX source
\[
[\mu,\lambda] = \bigl(\underbrace{\theta(\mu)\,\theta(\sigma\psi)}_{\in M_0}\bigr)
\bigl(\underbrace{\theta(\lambda)\,\theta(\sigma\psi)}_{\in M_0}\bigr)^{-1}
\]\[\begin{array}{l}
[w,\, gv] = \bigl(\theta(w)\,\theta(\rho\psi)\bigr)\bigl(\theta(gv)\,\theta(\rho\psi)\bigr)^{-1} \\
{}[v,\, fu] = \bigl(\theta(v)\,\theta(\rho g\psi)\bigr)\bigl(\theta(fu)\,\theta(\rho g\psi)\bigr)^{-1} \\
{}[w,\, gfu] = \bigl(\theta(w)\,\theta(\rho\psi)\bigr)\bigl(\theta(gfu)\,\theta(\rho\psi)\bigr)^{-1}
\end{array}\]
LaTeX source
\[
\begin{array}{l}
[w,\, gv] = \bigl(\theta(w)\,\theta(\rho\psi)\bigr)\bigl(\theta(gv)\,\theta(\rho\psi)\bigr)^{-1} \\
{}[v,\, fu] = \bigl(\theta(v)\,\theta(\rho g\psi)\bigr)\bigl(\theta(fu)\,\theta(\rho g\psi)\bigr)^{-1} \\
{}[w,\, gfu] = \bigl(\theta(w)\,\theta(\rho\psi)\bigr)\bigl(\theta(gfu)\,\theta(\rho\psi)\bigr)^{-1}
\end{array}
\]\[\boxed{\ \bigl(\theta(gv)\,\theta(\rho\psi)\bigr)^{-1}
\bigl(\theta(v)\,\theta(\rho g\psi)\bigr)
\bigl(\theta(fu)\,\theta(\rho g\psi)\bigr)^{-1}
\bigl(\theta(gfu)^{-1}\,\theta(\rho\psi)\bigr) = 1\ }\]
LaTeX source
\[
\boxed{\ \bigl(\theta(gv)\,\theta(\rho\psi)\bigr)^{-1}
\bigl(\theta(v)\,\theta(\rho g\psi)\bigr)
\bigl(\theta(fu)\,\theta(\rho g\psi)\bigr)^{-1}
\bigl(\theta(gfu)^{-1}\,\theta(\rho\psi)\bigr) = 1\ }
\]\[\rho g f u \overset{R}{\sim} \rho g v \overset{R}{\sim} \rho w \overset{R}{\sim} \psi\]
LaTeX source
\[
\rho g f u \overset{R}{\sim} \rho g v \overset{R}{\sim} \rho w \overset{R}{\sim} \psi
\]\[\rho g f u \overset{R}{\sim} \rho g v \overset{R}{\sim} \rho w \overset{R}{\sim} 1\]
LaTeX source
\[
\rho g f u \overset{R}{\sim} \rho g v \overset{R}{\sim} \rho w \overset{R}{\sim} 1
\]\[\boxed{\ \rho g f u,\ \rho g v,\ \rho w \in M_0\ }\]
LaTeX source
\[
\boxed{\ \rho g f u,\ \rho g v,\ \rho w \in M_0\ }
\]\[\underbrace{\rho g f u}_{\overset{\text{déf}}{=}\ \pi},\qquad
\underbrace{\rho g v}_{\overset{\text{déf}}{=}\ \pi'} \ \in M_0 ,\]
LaTeX source
\[
\underbrace{\rho g f u}_{\overset{\text{déf}}{=}\ \pi},\qquad
\underbrace{\rho g v}_{\overset{\text{déf}}{=}\ \pi'} \ \in M_0 ,
\]\[\pi\bigl(\underbrace{\theta(gv)\,\theta(\rho\psi)}_{c_1}\bigr)
= \pi\bigl(\underbrace{\theta(v)\,\theta(\rho g\psi)}_{c_2}\bigr) = \psi\]
LaTeX source
\[
\pi\bigl(\underbrace{\theta(gv)\,\theta(\rho\psi)}_{c_1}\bigr)
= \pi\bigl(\underbrace{\theta(v)\,\theta(\rho g\psi)}_{c_2}\bigr) = \psi
\]\[\pi'\bigl(\underbrace{\theta(fu)\,\theta(\rho g\psi)}_{c_3}\bigr)
= \pi'\bigl(\underbrace{\theta(gfu)\,\theta(\rho\psi)}_{c_4}\bigr) = \psi\]
LaTeX source
\[
\pi'\bigl(\underbrace{\theta(fu)\,\theta(\rho g\psi)}_{c_3}\bigr)
= \pi'\bigl(\underbrace{\theta(gfu)\,\theta(\rho\psi)}_{c_4}\bigr) = \psi
\]\[\begin{array}{l}
\delta(c_1) = \delta(c_2) = \delta(\psi) - \delta(\pi) \\
\delta(c_3) = \delta(c_4) = \delta(\psi) - \delta(\pi')
\end{array}\]
LaTeX source
\[
\begin{array}{l}
\delta(c_1) = \delta(c_2) = \delta(\psi) - \delta(\pi) \\
\delta(c_3) = \delta(c_4) = \delta(\psi) - \delta(\pi')
\end{array}
\]\[\delta_0\bigl(c_1 c_2^{-1} c_3 c_4^{-1}\bigr)
= \underbrace{\bigl(\delta(c_1) - \delta(c_2)\bigr)}_{0}
+ \underbrace{\bigl(\delta(c_3) - \delta(c_4)\bigr)}_{0} = 0\]
LaTeX source
\[
\delta_0\bigl(c_1 c_2^{-1} c_3 c_4^{-1}\bigr)
= \underbrace{\bigl(\delta(c_1) - \delta(c_2)\bigr)}_{0}
+ \underbrace{\bigl(\delta(c_3) - \delta(c_4)\bigr)}_{0} = 0
\]\[\delta'_0 : \pi_1(X,e) \longrightarrow \mathbb{Z} .\]
LaTeX source
\[
\delta'_0 : \pi_1(X,e) \longrightarrow \mathbb{Z} .
\]\[\bigl(u \overset{R_\varphi}{\sim} v \iff \exists\, p,q \in \mathbb{N}
\ \ill{}\ \varphi^{p}u = \varphi^{q}v\bigr),\]
LaTeX source
\[
\bigl(u \overset{R_\varphi}{\sim} v \iff \exists\, p,q \in \mathbb{N}
\ \ill{}\ \varphi^{p}u = \varphi^{q}v\bigr),
\]\[\pi_1(X,e) \longrightarrow \mathbb{Z} ,\]
LaTeX source
\[
\pi_1(X,e) \longrightarrow \mathbb{Z} ,
\]\[uv = 1 ;\]
LaTeX source
\[ uv = 1 ; \]
\[p \overset{\text{déf}}{=} vu = 1 ,\]
LaTeX source
\[
p \overset{\text{déf}}{=} vu = 1 ,
\]\[\bigl[\ \bar{u}\bar{f} = \bar{v}\bar{f} \Longrightarrow \bar{u} = \bar{v}\ \bigr],\]
LaTeX source
\[
\bigl[\ \bar{u}\bar{f} = \bar{v}\bar{f} \Longrightarrow \bar{u} = \bar{v}\ \bigr],
\]\[R_0 : \qquad u \overset{R_0}{\sim} v \iff u\psi = v\psi\]
LaTeX source
\[
R_0 : \qquad u \overset{R_0}{\sim} v \iff u\psi = v\psi
\]\[\begin{array}{rcl}
M &\longrightarrow& \mathrm{Ep}(M_0) \\
u &\longmapsto& u_{M_0} = \bigl(\lambda \mapsto u\lambda : M_0 \to M_0\bigr)
\end{array}\]
LaTeX source
\[
\begin{array}{rcl}
M &\longrightarrow& \mathrm{Ep}(M_0) \\
u &\longmapsto& u_{M_0} = \bigl(\lambda \mapsto u\lambda : M_0 \to M_0\bigr)
\end{array}
\]\[u \overset{R_\varphi}{\sim} v \iff \exists\, p,q \in \mathbb{N}
\ \text{avec}\ \varphi^{p}u = \varphi^{q}v ,\]
LaTeX source
\[
u \overset{R_\varphi}{\sim} v \iff \exists\, p,q \in \mathbb{N}
\ \text{avec}\ \varphi^{p}u = \varphi^{q}v ,
\]\[M_0 = \{\, f \in M \mid \psi f \overset{R_\varphi}{\sim} \psi \,\} ,\]
LaTeX source
\[
M_0 = \{\, f \in M \mid \psi f \overset{R_\varphi}{\sim} \psi \,\} ,
\]\[\pi_1(M_0) = G_0 \xrightarrow{\ \delta_0\ } \mathbb{Z}\]
LaTeX source
\[
\pi_1(M_0) = G_0 \xrightarrow{\ \delta_0\ } \mathbb{Z}
\]\[\delta(f) = q - p \qquad \text{si } \varphi^{p}\psi f = \varphi^{q}\psi .\]
LaTeX source
\[
\delta(f) = q - p \qquad \text{si } \varphi^{p}\psi f = \varphi^{q}\psi .
\]\[\mathbb{N} \times e \longrightarrow e \times e ,\qquad
(n,u) \longmapsto (\varphi^{n}u,\, u)\]
LaTeX source
\[
\mathbb{N} \times e \longrightarrow e \times e ,\qquad
(n,u) \longmapsto (\varphi^{n}u,\, u)
\]\[\pi_1(X_0, e) \;\simeq\; \pi_1(M) \twoheadrightarrow \Gamma .\]
LaTeX source
\[ \pi_1(X_0, e) \;\simeq\; \pi_1(M) \twoheadrightarrow \Gamma . \]
\[(*) \qquad u p \;\struck{= up}\; = p , \qquad
\text{(en particulier } p^2 = p\text{)},\]
LaTeX source
\[
(*) \qquad u p \;\struck{= up}\; = p , \qquad
\text{(en particulier } p^2 = p\text{)},
\]\[p \;=\; u_i v_i .\]
LaTeX source
\[ p \;=\; u_i v_i . \]
\[(**) \qquad p \;=\; u\, v(u) ,\]
LaTeX source
\[ (**) \qquad p \;=\; u\, v(u) , \]
\[\mathrm{Im}\, p \;\subset\; \mathrm{Im}\, u \qquad \forall u \in M,\]
LaTeX source
\[
\mathrm{Im}\, p \;\subset\; \mathrm{Im}\, u \qquad \forall u \in M,
\]\[u(E_0) \;=\; u\, p(E) \;=\; \mathrm{Im}(up) \;\supset\; E_0 ,\]
LaTeX source
\[
u(E_0) \;=\; u\, p(E) \;=\; \mathrm{Im}(up) \;\supset\; E_0 ,
\]\[u \longmapsto u_{E_0} \;:\; M \longrightarrow \mathrm{Aut}(E_0)\]
LaTeX source
\[
u \longmapsto u_{E_0} \;:\; M \longrightarrow \mathrm{Aut}(E_0)
\]\[E_0 \;=\; \text{ens. des pts fixes de } M \text{ opérant dans } E,\]
LaTeX source
\[
E_0 \;=\; \text{ens. des pts fixes de } M \text{ opérant dans } E,
\]\[u\, p(x) \;=\; p(x) \quad \forall x \in E, \qquad \text{i.e.}\]
LaTeX source
\[
u\, p(x) \;=\; p(x) \quad \forall x \in E, \qquad \text{i.e.}
\]\[up \;=\; p \qquad \forall u \in M,\]
LaTeX source
\[ up \;=\; p \qquad \forall u \in M, \]
\[p \;:\; e \longrightarrow a .\]
LaTeX source
\[ p \;:\; e \longrightarrow a . \]
\[e \xrightarrow{\;p_b\;} b .\]
LaTeX source
\[
e \xrightarrow{\;p_b\;} b .
\]\[u \;:\; b \longrightarrow a\]
LaTeX source
\[ u \;:\; b \longrightarrow a \]
\[uq = p, \qquad \struck{\ill{}} \text{ avec } q \text{ comme } p,
\qquad \text{donc } uq = q\]
LaTeX source
\[
uq = p, \qquad \struck{\ill{}} \text{ avec } q \text{ comme } p,
\qquad \text{donc } uq = q
\]\[\underbrace{u\,q}_{q} \;=\; \underbrace{v\,q'}_{q'} \;=\; p\]
LaTeX source
\[
\underbrace{u\,q}_{q} \;=\; \underbrace{v\,q'}_{q'} \;=\; p
\]\[up = q, \qquad p = v\,\overline{v}, \qquad p = q\,q', \qquad
q = v\,\struck{\ill{}}\]
LaTeX source
\[
up = q, \qquad p = v\,\overline{v}, \qquad p = q\,q', \qquad
q = v\,\struck{\ill{}}
\]\[H_y \;=\; f \cdot H_x .\]
LaTeX source
\[ H_y \;=\; f \cdot H_x . \]
\[\lambda \longmapsto f\lambda \;:\; H_x \xrightarrow{\ \sim\ } H_y\]
LaTeX source
\[
\lambda \longmapsto f\lambda \;:\; H_x \xrightarrow{\ \sim\ } H_y
\]\[u \longmapsto fu \;:\; H_e \longrightarrow H_x\]
LaTeX source
\[ u \longmapsto fu \;:\; H_e \longrightarrow H_x \]
\[fu \;=\; gu \qquad \text{pour } u \in H_e, \quad
f, g : e \rightrightarrows x .\]
LaTeX source
\[
fu \;=\; gu \qquad \text{pour } u \in H_e, \quad
f, g : e \rightrightarrows x .
\]\[M \;=\; \mathrm{Ep}(E)\]
LaTeX source
\[
M \;=\; \mathrm{Ep}(E)
\]\[\struck{p}\, w \;=\; u\, w_u\]
LaTeX source
\[
\struck{p}\, w \;=\; u\, w_u
\]\[w \;=\; u\, w_u \qquad \text{avec } w, w_u \text{ minimaux}\]
LaTeX source
\[
w \;=\; u\, w_u \qquad \text{avec } w, w_u \text{ minimaux}
\]\[M \;=\; \mathrm{Mon}(E)\]
LaTeX source
\[
M \;=\; \mathrm{Mon}(E)
\]\[w \;=\; w\, u , \qquad
\mathrm{card}\bigl(E - w(E)\bigr) \;=\; \pi\]
LaTeX source
\[
w \;=\; w\, u , \qquad
\mathrm{card}\bigl(E - w(E)\bigr) \;=\; \pi
\]\[R(a,b) \;:\; X_{/\!/a} \cap X_{/\!/b} \neq \emptyset\]
LaTeX source
\[
R(a,b) \;:\; X_{/\!/a} \cap X_{/\!/b} \neq \emptyset
\]\[\mathrm{Ob}\, X \longrightarrow \pi_0(X) .\]
LaTeX source
\[
\mathrm{Ob}\, X \longrightarrow \pi_0(X) .
\]\[\varphi u = \varphi v \quad \text{avec } u, v, \varphi \ \uncertain{surj.}
\quad \Longrightarrow \quad u = v\]
LaTeX source
\[
\varphi u = \varphi v \quad \text{avec } u, v, \varphi \ \uncertain{surj.}
\quad \Longrightarrow \quad u = v
\]\[\varphi u = \varphi \quad \Longrightarrow \quad u = \mathrm{id}\ ?
\qquad \uncertain{\mathrm{Mon}}\]
LaTeX source
\[
\varphi u = \varphi \quad \Longrightarrow \quad u = \mathrm{id}\ ?
\qquad \uncertain{\mathrm{Mon}}
\]\[M \;=\; \mathrm{Ep}(E)\]
LaTeX source
\[
M \;=\; \mathrm{Ep}(E)
\]\[u f = v f \quad \Longrightarrow \quad u = v .\]
LaTeX source
\[ u f = v f \quad \Longrightarrow \quad u = v . \]
\[f u = f v , \qquad u \neq v\]
LaTeX source
\[ f u = f v , \qquad u \neq v \]
\[\mathrm{Hom}(e,x) \;\simeq\; \pi_0\bigl(e \backslash \Psi / x\bigr)
\;\simeq\; \pi_0\bigl(S/x\bigr)\]
LaTeX source
\[
\mathrm{Hom}(e,x) \;\simeq\; \pi_0\bigl(e \backslash \Psi / x\bigr)
\;\simeq\; \pi_0\bigl(S/x\bigr)
\]\[\varinjlim_{x \in X} \pi_0\bigl(S/x\bigr)\]
LaTeX source
\[
\varinjlim_{x \in X} \pi_0\bigl(S/x\bigr)
\]\[\pi_{0}(S_{/x}) \rightrightarrows \pi_{0}(S_{/a})\]
LaTeX source
\[
\pi_{0}(S_{/x}) \rightrightarrows \pi_{0}(S_{/a})
\]\[\pi_{0}(E_{/x}) \simeq\]
LaTeX source
\[
\pi_{0}(E_{/x}) \simeq
\]\[B\times C = \emptyset \quad\text{dans } X^{\wedge},\]
LaTeX source
\[
B\times C = \emptyset \quad\text{dans } X^{\wedge},
\]\[\beta\times\gamma = \emptyset \quad\text{dans } X^{\vee},\]
LaTeX source
\[
\beta\times\gamma = \emptyset \quad\text{dans } X^{\vee},
\]\[\mathrm{Hom}(a,x) = \emptyset\]
LaTeX source
\[
\mathrm{Hom}(a,x) = \emptyset
\]\[(u,\beta) \in \mathrm{Hom}(a,x)\times E\]
LaTeX source
\[
(u,\beta) \in \mathrm{Hom}(a,x)\times E
\]\[\pi_{0}(S_{/x}) \simeq I(x) \amalg \bigl(J(x)\times E\bigr)\]
LaTeX source
\[
\pi_{0}(S_{/x}) \simeq I(x) \amalg \bigl(J(x)\times E\bigr)
\]\[I(x) = \mathrm{Im}\bigl(\mathrm{Hom}(\beta,x)\amalg\mathrm{Hom}(\gamma,x)
\longrightarrow \mathrm{Hom}(a,x)\bigr)\]
LaTeX source
\[
I(x) = \mathrm{Im}\bigl(\mathrm{Hom}(\beta,x)\amalg\mathrm{Hom}(\gamma,x)
\longrightarrow \mathrm{Hom}(a,x)\bigr)
\]\[J(x) = \mathrm{Hom}(a,x)\setminus I(x)\]
LaTeX source
\[
J(x) = \mathrm{Hom}(a,x)\setminus I(x)
\]\[\pi_{0}(S_{/x}) = \emptyset \quad\text{si } \mathrm{Hom}(a,x) = \emptyset\]
LaTeX source
\[
\pi_{0}(S_{/x}) = \emptyset \quad\text{si } \mathrm{Hom}(a,x) = \emptyset
\]\[X' \sim \Sigma^{1} Z\]
LaTeX source
\[
X' \sim \Sigma^{1} Z
\]\[\beta/\!/Z \simeq {}_{a}\backslash X\]
LaTeX source
\[
\beta/\!/Z \simeq {}_{a}\backslash X
\]\[T = b_{0}/\!/X_{0} \ \cup\ c_{0}/\!/X_{0}\]
LaTeX source
\[
T = b_{0}/\!/X_{0} \ \cup\ c_{0}/\!/X_{0}
\]\[X_{0} \simeq \beta/\!/\tilde X \simeq \gamma/\!/\tilde X\]
LaTeX source
\[
X_{0} \simeq \beta/\!/\tilde X \simeq \gamma/\!/\tilde X
\]\[\tilde X \sim \Sigma^{1}T \qquad X' \sim \Sigma^{2}T \qquad
X' \simeq \Sigma^{1}\tilde X\]
LaTeX source
\[
\tilde X \sim \Sigma^{1}T \qquad X' \sim \Sigma^{2}T \qquad
X' \simeq \Sigma^{1}\tilde X
\]\[\Sigma^{1}X\]
LaTeX source
\[
\Sigma^{1}X
\]\[X\times Y \qquad X \longrightarrow X\times I \qquad x_{0}\times I\]
LaTeX source
\[
X\times Y \qquad X \longrightarrow X\times I \qquad x_{0}\times I
\]\[\Longrightarrow\ \exists\, X \longrightarrow X' \text{ cofinal},\]
LaTeX source
\[
\Longrightarrow\ \exists\, X \longrightarrow X' \text{ cofinal},
\]\[H^{2}(X') \simeq H^{2}(S^{2}) ;\]
LaTeX source
\[
H^{2}(X') \simeq H^{2}(S^{2}) ;
\]\[f^{*} : H^{2}(T,\underline{k}) \xrightarrow{\ \sim\ } H^{2}(S,\underline{k})\]
LaTeX source
\[
f^{*} : H^{2}(T,\underline{k}) \xrightarrow{\ \sim\ } H^{2}(S,\underline{k})
\]\[\xi \qquad \xi' \qquad H^{p}(S',\xi') \longrightarrow H^{p}(S,\xi)\]
LaTeX source
\[
\xi \qquad \xi' \qquad H^{p}(S',\xi') \longrightarrow H^{p}(S,\xi)
\]\[S\times T \longleftarrow S'\times T\]
LaTeX source
\[ S\times T \longleftarrow S'\times T \]
\[X_{/e} \simeq X_{/F}\]
LaTeX source
\[
X_{/e} \simeq X_{/F}
\]\[X \longrightarrow Y \quad \text{cocofinal},\]
LaTeX source
\[
X \longrightarrow Y \quad \text{cocofinal},
\]\[\tilde X \sim \Sigma(T), \quad\text{si } \beta/\!/\tilde X,\ \gamma/\!/\tilde X
\ \text{asph. (à vérifier)}\]
LaTeX source
\[
\tilde X \sim \Sigma(T), \quad\text{si } \beta/\!/\tilde X,\ \gamma/\!/\tilde X
\ \text{asph. (à vérifier)}
\]\[X' \sim \Sigma(\tilde X)\]
LaTeX source
\[ X' \sim \Sigma(\tilde X) \]
\[(vu_{1},\alpha) \sim (vu_{2},\beta)\]
LaTeX source
\[
(vu_{1},\alpha) \sim (vu_{2},\beta)
\]\[(vu_{1},\alpha) \sim (vu_{2},\beta)\]
LaTeX source
\[
(vu_{1},\alpha) \sim (vu_{2},\beta)
\]\[(v,\alpha) \sim (w,\beta)\]
LaTeX source
\[ (v,\alpha) \sim (w,\beta) \]
\[S = \bigl(\, a \to \xi \to b \ ;\ a \to \xi' \to b \,\bigr)\]
LaTeX source
\[ S = \bigl(\, a \to \xi \to b \ ;\ a \to \xi' \to b \,\bigr) \]
\[B = (u_{1},\alpha) \sim (u_{2},\beta)\]
LaTeX source
\[
B = (u_{1},\alpha) \sim (u_{2},\beta)
\]\[C = (u_{2},\alpha) \sim (u_{1},\beta)\]
LaTeX source
\[
C = (u_{2},\alpha) \sim (u_{1},\beta)
\]\[B \longrightarrow \xi\]
LaTeX source
\[ B \longrightarrow \xi \]
\[\xi = (vu_{1},\alpha) = (vu_{2},\beta)\]
LaTeX source
\[
\xi = (vu_{1},\alpha) = (vu_{2},\beta)
\]\[\xi = (vu_{2},\alpha) = (vu_{1},\beta)\]
LaTeX source
\[
\xi = (vu_{2},\alpha) = (vu_{1},\beta)
\]\[\xi = (v,\alpha) = (w,\beta)\]
LaTeX source
\[ \xi = (v,\alpha) = (w,\beta) \]
\[\mathrm{Hom}_{X'\supset X}(x,e) \simeq \pi_{0}\bigl({}_{x}\backslash S_{/e}\bigr)
\simeq \pi_{0}\bigl({}_{x}\backslash S\bigr)\]
LaTeX source
\[
\mathrm{Hom}_{X'\supset X}(x,e) \simeq \pi_{0}\bigl({}_{x}\backslash S_{/e}\bigr)
\simeq \pi_{0}\bigl({}_{x}\backslash S\bigr)
\]\[\simeq \varinjlim \Bigl(\mathrm{Hom}(x,a) \to \mathrm{Hom}(x,\xi)
\leftarrow \mathrm{Hom}(x,b) \to \mathrm{Hom}(x,\xi') \leftarrow \Bigr)\]
LaTeX source
\[
\simeq \varinjlim \Bigl(\mathrm{Hom}(x,a) \to \mathrm{Hom}(x,\xi)
\leftarrow \mathrm{Hom}(x,b) \to \mathrm{Hom}(x,\xi') \leftarrow \Bigr)
\]\[\simeq \underbrace{\bigl(\mathrm{Hom}(x,\xi)\amalg\mathrm{Hom}(x,\xi')\bigr)}_{E(x)}
\big/ R_{(x)},\]
LaTeX source
\[
\simeq \underbrace{\bigl(\mathrm{Hom}(x,\xi)\amalg\mathrm{Hom}(x,\xi')\bigr)}_{E(x)}
\big/ R_{(x)},
\]\[(*) \quad
\begin{cases}
\lambda v \sim \lambda' v & v : x \to a \\
\mu w \sim \mu' w & w : x \to b
\end{cases}\]
LaTeX source
\[
(*) \quad
\begin{cases}
\lambda v \sim \lambda' v & v : x \to a \\
\mu w \sim \mu' w & w : x \to b
\end{cases}
\]\[\mathrm{Hom}(b,\xi) \rightrightarrows \mathrm{Hom}(a,\cdot)\]
LaTeX source
\[
\mathrm{Hom}(b,\xi) \rightrightarrows \mathrm{Hom}(a,\cdot)
\]\[\tilde X = \tilde X_{/\!/\tilde\xi} \ \cup\ \tilde X_{/\!/\tilde\xi'}\]
LaTeX source
\[
\tilde X = \tilde X_{/\!/\tilde\xi} \ \cup\ \tilde X_{/\!/\tilde\xi'}
\]\[\tilde X_{/\!/\tilde\xi} \ \cap\ \tilde X_{/\!/\tilde\xi'}
= \tilde X_{/\!/\tilde a} \ \cup\ \tilde X_{/\!/\tilde b}\]
LaTeX source
\[
\tilde X_{/\!/\tilde\xi} \ \cap\ \tilde X_{/\!/\tilde\xi'}
= \tilde X_{/\!/\tilde a} \ \cup\ \tilde X_{/\!/\tilde b}
\]\[\mathrm{Hom}(e,x) \simeq \pi_{0}\bigl({}_{e}\backslash D_{/x}\bigr)
\simeq \pi_{0}\bigl(D_{/x}\bigr)
\simeq \varinjlim \bigl(\mathrm{Hom}(b,x) \rightrightarrows \mathrm{Hom}(a,x)\bigr)\]
LaTeX source
\[
\mathrm{Hom}(e,x) \simeq \pi_{0}\bigl({}_{e}\backslash D_{/x}\bigr)
\simeq \pi_{0}\bigl(D_{/x}\bigr)
\simeq \varinjlim \bigl(\mathrm{Hom}(b,x) \rightrightarrows \mathrm{Hom}(a,x)\bigr)
\]\[u \in \mathrm{Hom}(x,\xi) \subset \mathrm{Hom}(x,\xi)\amalg\mathrm{Hom}(x,\xi')
\overset{\text{déf}}{=} E(x)\]
LaTeX source
\[
u \in \mathrm{Hom}(x,\xi) \subset \mathrm{Hom}(x,\xi)\amalg\mathrm{Hom}(x,\xi')
\overset{\text{déf}}{=} E(x)
\]\[u' \in \mathrm{Hom}(x,\xi') \subset E(x)\]
LaTeX source
\[
u' \in \mathrm{Hom}(x,\xi') \subset E(x)
\]\[f_{0} = u,\ f_{1},\ f_{2},\ \ldots\ f_{n} = u'\]
LaTeX source
\[
f_{0} = u,\ f_{1},\ f_{2},\ \ldots\ f_{n} = u'
\]\[X' \simeq \Sigma^{1}_{W}(X) \simeq \Sigma^{2}_{W}(\tilde X)
\simeq \Sigma^{3}(T)\]
LaTeX source
\[
X' \simeq \Sigma^{1}_{W}(X) \simeq \Sigma^{2}_{W}(\tilde X)
\simeq \Sigma^{3}(T)
\]\[T \neq \emptyset .\]
LaTeX source
\[ T \neq \emptyset . \]
\[\underbrace{\lambda v,\; \mu w}_{\mathrm{Hom}(m,\xi)}
\qquad
\underbrace{\lambda' v,\; \mu' w}_{\mathrm{Hom}(a,\xi')}\]
LaTeX source
\[
\underbrace{\lambda v,\; \mu w}_{\mathrm{Hom}(m,\xi)}
\qquad
\underbrace{\lambda' v,\; \mu' w}_{\mathrm{Hom}(a,\xi')}
\]\[v^{*}(\tilde a) = w^{*}(\tilde b)\]
LaTeX source
\[
v^{*}(\tilde a) = w^{*}(\tilde b)
\]\[\boxed{\;\lambda v \sim \mu w\;}\]
LaTeX source
\[
\boxed{\;\lambda v \sim \mu w\;}
\]\[\widetilde{X}_{/\!/(\tilde a,\tilde b)} \neq \emptyset\]
LaTeX source
\[
\widetilde{X}_{/\!/(\tilde a,\tilde b)} \neq \emptyset
\]