Seifert fibrations #
A Seifert fibration of a 3-manifold M is a decomposition of M into disjoint circles, the
fibres, such that every fibre has a neighbourhood which is a union of fibres and is isomorphic,
fibres to fibres, to a model fibred solid torus. Seifert-fibred pieces are, together with the
atoroidal ones, the pieces of the JSJ decomposition of a 3-manifold, and six of Thurston's eight
geometries are the geometries of Seifert-fibred spaces.
The model fibred solid torus V(p, q), for an integer q > 0 and an integer p coprime to q,
is the solid torus D² × S¹ decomposed into the orbits of the circle action
t • (z, w) = (t ^ p * z, t ^ q * w). The core {0} × S¹ is one fibre; every other fibre winds
q times around the core direction. Cutting along a meridian disc presents V(p, q) as
[0, 1] × D², decomposed into the segments [0, 1] × {x}, with its ends identified by the
rotation through 2πp/q; this is the description of Hatcher and Scott.
The decomposition is recorded as a Setoid M whose classes are the fibres. The local condition is
stated with open partial homeomorphisms onto open subsets of the closed model V(p, q), so that
fibres in the boundary of M (modelled on fibres in the boundary torus of V(p, q)) are allowed
and no separate model for boundary fibres is needed. Both the chart's source and its target are
required to be unions of fibres; it follows that every fibre is a circle
(TauCeti.IsSeifertFibration.nonempty_homeomorph_circle).
Only fibred solid tori occur as local models, as in Seifert's original definition. Scott also allows fibred solid Klein bottles, which are nonorientable; in an orientable 3-manifold, the case relevant to the JSJ decomposition and geometrization, the two definitions agree.
The predicate is a property of the decomposition alone. It forces M to be locally homeomorphic to
open subsets of D² × S¹, but separation and countability hypotheses are kept separate, as in
TauCeti.IsCompactConnectedThreeManifold.
Main definitions #
TauCeti.SolidTorus: the closed solid torusD² × S¹.TauCeti.SolidTorus.fiberSetoid p q: the fibres of the model fibred solid torusV(p, q).TauCeti.IsSeifertChart r p q e: the chartecarries the classes ofrin its source onto the fibres ofV(p, q)in its target.TauCeti.IsSeifertFibration r: the classes ofrform a Seifert fibration.TauCeti.IsSeifertFibered M:Madmits a Seifert fibration.
Main results #
TauCeti.IsSeifertFibration.nonempty_homeomorph_circle: every fibre of a Seifert fibration is homeomorphic to a circle.TauCeti.SolidTorus.isSeifertFibration_fiberSetoid: the modelV(p, q)is Seifert fibred.TauCeti.isSeifertFibration_ker_fst: for a boundaryless surfaceF, the circles{x} × S¹form a Seifert fibration ofF × S¹.Homeomorph.isSeifertFibered_iff: being Seifert fibred is invariant under homeomorphism.
References #
- H. Seifert, Topologie dreidimensionaler gefaserter Räume, Acta Math. 60 (1933), 147–238.
- P. Scott, The geometries of 3-manifolds, Bull. London Math. Soc. 15 (1983), 401–487, Section 3.
- A. Hatcher, Notes on Basic 3-Manifold Topology, Section 2.1.
The closed solid torus D² × S¹, where D² is the closed unit disc of ℂ.
Instances For
The solid torus identified with the product of the closed unit disc and the unit sphere
of ℂ, for use with APIs stated in terms of metric balls and spheres.
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The fibres of the model fibred solid torus V(p, q): two points of D² × S¹ lie in the same
fibre when they lie in the same orbit of the circle action t • (z, w) = (t ^ p * z, t ^ q * w).
For q ≠ 0 the core {0} × S¹ is a single fibre. When moreover p is coprime to q, every
other fibre winds q times around the core direction and p times around the meridian of the
torus {|z| = r} × S¹ containing it.
Instances For
The defining orbit condition of the fibres of V(p, q).
The fibres of V(0, 1) are the circles {z} × S¹ of the product fibration.
Every fibre of the model fibred solid torus V(p, q), for q ≠ 0 and p coprime to q, is
homeomorphic to a circle.
An open partial homeomorphism e from M to the solid torus is a Seifert chart of r
onto the model V(p, q) when its source is a union of classes of r, its target is a union of
fibres of V(p, q), and on its source e carries the classes of r onto fibres of V(p, q).
The source of the chart is a union of classes of
r.- target_saturated (a : SolidTorus) : a ∈ e.target → ∀ (b : SolidTorus), (SolidTorus.fiberSetoid p q) a b → b ∈ e.target
The target of the chart is a union of fibres of
V(p, q). - rel_iff (x : M) : x ∈ e.source → ∀ y ∈ e.source, r x y ↔ (SolidTorus.fiberSetoid p q) (↑e x) (↑e y)
On its source the chart carries the classes of
ronto the fibres ofV(p, q).
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A Seifert chart maps the class of a point of its source onto the fibre of V(p, q) through its
image.
An equivalence relation on M is a Seifert fibration when every point of M lies in the
source of a Seifert chart of r onto a model fibred solid torus V(p, q), with q > 0 and p
coprime to q. Its classes, the fibres, are then circles.
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The defining local condition of a Seifert fibration.
A space is Seifert fibred when it admits a Seifert fibration.
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The defining condition of a Seifert-fibred space.
Every fibre of a Seifert fibration is homeomorphic to a circle.
A Seifert fibration pulls back along a homeomorphism.
Being Seifert fibred is invariant under homeomorphism.
The model fibred solid torus V(p, q), for q > 0 and p coprime to q, is Seifert fibred.
The solid torus is Seifert fibred.
For a boundaryless surface F, the circles {x} × S¹ form a Seifert fibration of F × S¹:
near each fibre, a chart of F identifies it with the product fibration V(0, 1).
The product of a boundaryless surface with a circle is Seifert fibred.