topology (point-set topology, point-free topology)
see also differential topology, algebraic topology, functional analysis and topological homotopy theory
Basic concepts
fiber space, space attachment
Extra stuff, structure, properties
Kolmogorov space, Hausdorff space, regular space, normal space
sequentially compact, countably compact, locally compact, sigma-compact, paracompact, countably paracompact, strongly compact
Examples
Basic statements
closed subspaces of compact Hausdorff spaces are equivalently compact subspaces
open subspaces of compact Hausdorff spaces are locally compact
compact spaces equivalently have converging subnet of every net
continuous metric space valued function on compact metric space is uniformly continuous
paracompact Hausdorff spaces equivalently admit subordinate partitions of unity
injective proper maps to locally compact spaces are equivalently the closed embeddings
locally compact and second-countable spaces are sigma-compact
Theorems
Analysis Theorems
synthetic differential geometry
Introductions
from point-set topology to differentiable manifolds
geometry of physics: coordinate systems, smooth spaces, manifolds, smooth homotopy types, supergeometry
Differentials
Tangency
The magic algebraic facts
Theorems
Axiomatics
(shape modality $\dashv$ flat modality $\dashv$ sharp modality)
$(ʃ \dashv \flat \dashv \sharp )$
dR-shape modality$\dashv$ dR-flat modality
$ʃ_{dR} \dashv \flat_{dR}$
(reduction modality $\dashv$ infinitesimal shape modality $\dashv$ infinitesimal flat modality)
$(\Re \dashv \Im \dashv \&)$
fermionic modality$\dashv$ bosonic modality $\dashv$ rheonomy modality
$(\rightrightarrows \dashv \rightsquigarrow \dashv Rh)$
\array{ && id &\dashv& id \ && \vee && \vee \ &\stackrel{fermionic}{}& \rightrightarrows &\dashv& \rightsquigarrow & \stackrel{bosonic}{} \ && \bot && \bot \ &\stackrel{bosonic}{} & \rightsquigarrow &\dashv& Rh & \stackrel{rheonomic}{} \ && \vee && \vee \ &\stackrel{reduced}{} & \Re &\dashv& \Im & \stackrel{infinitesimal}{} \ && \bot && \bot \ &\stackrel{infinitesimal}{}& \Im &\dashv& \& & \stackrel{\text{étale}}{} \ && \vee && \vee \ &\stackrel{cohesive}{}& ʃ &\dashv& \flat & \stackrel{discrete}{} \ && \bot && \bot \ &\stackrel{discrete}{}& \flat &\dashv& \sharp & \stackrel{continuous}{} \ && \vee && \vee \ && \emptyset &\dashv& \ast }
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Models
Models for Smooth Infinitesimal Analysis
smooth algebra ($C^\infty$-ring)
differential equations, variational calculus
Euler-Lagrange equation, de Donder-Weyl formalism?,
Chern-Weil theory, ∞-Chern-Weil theory
Cartan geometry (super, higher)
∞-Lie theory (higher geometry)
A holonomy groupoid is a (topological/Lie-) groupoid naturally associated with a foliation $\mathcal{F}$ of a manifold $X$. It is, in some sense, the smallest de-singularization of the leaf-space quotient $X/\mathcal{F}$ of the foliation, which is, in general, not a manifold itself. Every foliation groupoid of $\mathcal{F}$ has this de-singularization property, but the holonomy groupoid is, in some sense, minimal with respect to this property.
Explicitly, given a foliation $\mathcal{F}$ on a manifold $X$, the holonomy groupoid of $\mathcal{F}$ has as objects the points of $X$. Given points $x,y$ in the same leaf, a morphism between them is the equivalence class of a path in the leaf from $x$ to $y$, where two paths are identified if they induce the same germ of a holonomy transformation between small transversal sections through $x$ and $y$. If $x$ and $y$ are not in the same leaf, then there is no morphism between them.
This is naturally a topological groupoid and a Lie groupoid if done right.
The monodromy groupoid of the foliation is obtained from this by further dividing out the homotopy between paths in a leaf.
Let $(X,\mathcal{F})$ be a foliated manifold with $q = codim(\mathcal{F})$. Let $L$ be a leaf of $\mathcal{F}$; let $x,y \in L$ be two points; and let $S$ and $T$ be transversal sections through $x$ and $y$ respectively (i.e., $S$ and $T$ are sub-manifolds transversal to the leaves of $\mathcal{F}$).
To a path $\gamma: [0,1] \to L$ from $x$ to $y$, we assign the germ of a (partially defined) diffeomorphism
called the holonomy transformation of the path $\gamma$ with respect to $S$ and $T$, as follows:
If there exists a single foliation chart $U$ of $\mathcal{F}$ that contains the image of $\gamma$, then there exists a sufficiently small open neighborhood $A$ of $x$ in the space $S \cap U$ for which there exists a unique smooth map $f: A \to T$ satisfying the following conditions:
$f(x) = y$;
For every $a \in A$, the point $f(a)$ lies in the same plaque in $U$ as $a$. Observe that $f$ is a diffeomorphism onto its image.
Then define ${hol^{S,T}}(\gamma)$ to be the germ of this diffeomorphism at $x$:
In general, the image of $\gamma$ is not contained inside any single foliation chart $U$, but as it is a compact subspace of $X$, there exist finitely many foliation charts $U_{1},\ldots,U_{n+1}$ and numbers $t_{0},\ldots,t_{n+1}$ such that
$0 = t_{0} \lt t_{1} \lt \cdots \lt t_{n} \lt t_{n+1} = 1$ and
$\gamma([t_{i-1},t_{i}])$ is contained in $U_{i}$ for $i = 1,\ldots,n+1$.
Then arbitrarily choose transversal sections $T_{i}$ through $\gamma(t_{i})$ for $i = 1,\ldots,n$ and define
This definition is independent of the choice of $U_{i}$‘s, $t_{i}$’s and $T_{i}$’s. It only depends on the initial and final transversal sections $S$ and $T$.
Proposition
Two homotopic paths with the same endpoints induce the same holonomy. (Note, however, that the converse is not true. Two paths with the same endpoints inducing the same holonomy may not be homotopic.)
If $S,S'$ are two transversal sections through $x$ and $T,T'$ two transversal sections through $y$, then
Given a foliated manifold $(X,\mathcal{F})$, the monodromy groupoid is the disjoint union of the fundamental groupoids of the leaves of $\mathcal{F}$, which is the groupoid having the following properties:
Its objects are the points of $X$.
There are no morphisms between two points on different leaves.
The morphisms between two points on the same leaf are homotopy-classes of paths lying in the leaf joining those points.
The holonomy groupoid is defined analogously, where instead of identifying two paths if they are homotopic, they are identified if they induce the same holonomy as described above.
The holonomy groupoid appears in
and was studied extensively in
See also
Marius Crainic, Ieke Moerdijk, Foliation groupoids and their cyclic homology, arXiv:math/0003119
Ronnie Brown, Osman Mucuk, Foliations, locally Lie groupoids and holonomy, numdam
Applications to singular foliations and to Poisson manifolds in particular are in
Last revised on July 2, 2016 at 06:57:30. See the history of this page for a list of all contributions to it.