Difference between revisions of "Isotopy (in topology)"
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''This term may also have other meanings, see [[Isotopy]]''. | ''This term may also have other meanings, see [[Isotopy]]''. | ||
− | A [[Homotopy|homotopy]] of a topological space <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i0529401.png" /> with respect to a topological space <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i0529402.png" /> is a continuous family | + | A [[Homotopy|homotopy]] of a topological space <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i0529401.png" /> with respect to a topological space <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i0529402.png" /> is a continuous family (indexed by $t$) |
− | <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i0529403.png" /> of [[Homeomorphism|homeomorphism]] ( | + | <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i0529403.png" /> of [[Homeomorphism|homeomorphism]] ( here and throughout, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i0529404.png" />) from <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i0529407.png" /> onto a subset of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i0529408.png" />. Analogously, an isotopy is a fibrewise-continuous mapping <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i0529409.png" /> such that <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294010.png" /> takes the fibre <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294011.png" /> homeomorphically onto a subset of the fibre <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294012.png" />. An isotopy <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294013.png" /> for which <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294014.png" /> for each <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294015.png" /> is called an isotopy of the space <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294016.png" />. |
By a covering (or enveloping) isotopy for an isotopy <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294017.png" /> one understands an isotopy <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294018.png" /> such that <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294019.png" />. Two imbeddings <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294020.png" /> of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294021.png" /> into <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294022.png" /> are said to be isotopic if there exist a covering isotopy <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294023.png" /> for which <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294024.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294025.png" />. Two spaces <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294026.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294027.png" /> are said to be isotopy equivalent if there exist imbeddings <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294028.png" /> and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294029.png" /> such that the composites <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294030.png" /> and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294031.png" /> are isotopic to the identity mapping. Isotopy-equivalent spaces are also called spaces of the same isotopy type (by analogy with the homotopy type). If two spaces are homeomorphic, then they are isotopy equivalent; however, there are non-homeomorphic spaces of the same isotopy type, for example, an <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294032.png" />-dimensional ball and the same ball with a line segment glued to it (at its ends). Any homotopy invariant is an isotopy invariant, but there exist isotopy invariants, for example dimension, that are not homotopy invariants. | By a covering (or enveloping) isotopy for an isotopy <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294017.png" /> one understands an isotopy <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294018.png" /> such that <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294019.png" />. Two imbeddings <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294020.png" /> of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294021.png" /> into <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294022.png" /> are said to be isotopic if there exist a covering isotopy <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294023.png" /> for which <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294024.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294025.png" />. Two spaces <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294026.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294027.png" /> are said to be isotopy equivalent if there exist imbeddings <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294028.png" /> and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294029.png" /> such that the composites <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294030.png" /> and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294031.png" /> are isotopic to the identity mapping. Isotopy-equivalent spaces are also called spaces of the same isotopy type (by analogy with the homotopy type). If two spaces are homeomorphic, then they are isotopy equivalent; however, there are non-homeomorphic spaces of the same isotopy type, for example, an <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/i/i052/i052940/i05294032.png" />-dimensional ball and the same ball with a line segment glued to it (at its ends). Any homotopy invariant is an isotopy invariant, but there exist isotopy invariants, for example dimension, that are not homotopy invariants. |
Revision as of 13:27, 15 May 2014
This term may also have other meanings, see Isotopy.
A homotopy of a topological space with respect to a topological space
is a continuous family (indexed by $t$)
of homeomorphism ( here and throughout,
) from
onto a subset of
. Analogously, an isotopy is a fibrewise-continuous mapping
such that
takes the fibre
homeomorphically onto a subset of the fibre
. An isotopy
for which
for each
is called an isotopy of the space
.
By a covering (or enveloping) isotopy for an isotopy one understands an isotopy
such that
. Two imbeddings
of
into
are said to be isotopic if there exist a covering isotopy
for which
,
. Two spaces
,
are said to be isotopy equivalent if there exist imbeddings
and
such that the composites
and
are isotopic to the identity mapping. Isotopy-equivalent spaces are also called spaces of the same isotopy type (by analogy with the homotopy type). If two spaces are homeomorphic, then they are isotopy equivalent; however, there are non-homeomorphic spaces of the same isotopy type, for example, an
-dimensional ball and the same ball with a line segment glued to it (at its ends). Any homotopy invariant is an isotopy invariant, but there exist isotopy invariants, for example dimension, that are not homotopy invariants.
The fundamental problem in isotopy theory is the isotopy extension problem, that is, the problem of the existence of an isotopy covering a given isotopy
. This problem, like the general problem of finding a complete system of isotopy invariants for imbeddings, is most often considered in the category of topological manifolds and its subcategories of piecewise-linear or differentiable manifolds.
A topological isotopy of a manifold
with respect to a manifold
,
, can be extended to a covering isotopy
if and only if the corresponding fibrewise imbedding
is locally flat (cf. Locally flat imbedding); here
is a subinterval of
. If
and
, then the isotopy
is covered by an isotopy
provided that the imbedding
is locally flat for any
. This is not true in codimension 2 (for example, "tying a knot" on a circle in
), and therefore additional homotopy hypotheses are required for the existence of a covering isotopy. Sufficiently locally close flat imbeddings are isotopic for
.
The existence theorem for a piecewise-linear isotopy is formulated in similar fashion in the general case (under the natural condition that the corresponding fibrewise imbeddings be locally flat in the piecewise-linear sense). If , then a piecewise-linear isotopy can always be extended, since in these codimensions a piecewise-linear imbedding is locally flat in the piecewise-linear sense. For
or 1 it is necessary to additionally suppose that the imbeddings
be locally flat in the piecewise-linear sense, since in these codimensions, a piecewise-linear imbedding need not to be locally flat even in the topological sense, for example, a cone over a knot.
A differentiable isotopy can always be extended to a differentiable covering isotopy.
The problem of finding a complete system of isotopy invariants for imbeddings of a manifold in
has only been solved in a few particular cases. Thus, every locally flat (in the topological sense) imbedding of spheres
for
or for
,
, is isotopic to the standard sphere, while if
,
, then a locally flat sphere
in
is isotopic to the standard sphere if and only if the complement
has the homotopy type of the circle (the Stallings–Brown theorem). In codimension 2 there can exist non-isotopic knots. In precisely the same way the Zeeman–Stallings theorem on the piecewise-linear isotopy (unknottedness) of piecewise-linear spheres can be stated.
An invariant of piecewise-linear isotopy is finer than an invariant of topological isotopy. Thus, the problem of topological isotopy of an arbitrary homeomorphism of to the identity has been solved in the positive sense for
, and under the same restriction the isotopy has been proved of any two orientation-preserving homeomorphism of the sphere
onto itself. In the piecewise-linear case, these statements can be proved by elementary methods without any restrictions. Sufficiently close homeomorphisms of a topological manifold onto itself are isotopic; on the other hand, there exist arbitrarily close, piecewise-linear non-isotopic, piecewise-linear homeomorphisms of piecewise-linear manifolds, for example, of the
-dimensional tori for
.
In contrast with the topological and piecewise-linear cases, it is by no means true that any two diffeomorphisms of an -sphere onto itself are differentiably isotopic. The isotopy classes of differentiable imbeddings of a sphere
into
have been studied in detail for any
. If
, then there exist a topological space
,
, such that the homotopy groups
are in one-to-one correspondence with the imbedding classes of
into
. Here
for
, while
is
or
depending on
being even or odd. Thus, the standard
-sphere
, imbedded in
, can for
be knotted in the differentiable sense, that is, there exist imbeddings
that are not differentiably isotopic to the standard imbedding. These knots are called Haefliger knots. If
, then the differentiable knots
can be knotted in the topological sense; however, there are considerably more of these than of the topological or piecewise-linear ones; for odd
they have been completely classified. If
,
, then any differentiable imbedding
is differentiably isotopic to the standard imbedding.
The fact that there exist diffeomorphisms of onto itself that are not isotopic to the identity leads to the existence of non-trivial differentiable structures on spheres of dimension
. Although every homeomorphism of
,
, onto itself can can be approximated by a diffeomorphism, not all close diffeomorphisms of a sphere are differentiably isotopic, that is, a diffeomorphism of a sphere onto itself can by an infinitesimal perturbation be transformed in one not isotopic to it.
References
[1] | L.V. Keldysh, "Topological imbeddings in Euclidean space" Proc. Steklov Inst. Math. , 81 (1968) Trudy Mat. Inst. Steklov. , 81 |
[2] | C.P. Rourke, B.J. Sanderson, "Introduction to piecewise-linear topology" , Springer (1972) |
[3] | S.P. Novikov, "Differentiable sphere bundles" Izv. Akad. Nauk SSSR Ser. Mat. , 29 : 1 (1965) pp. 71–96 (In Russian) |
[4] | A.V. Chernavskii, "Local contractibility of the group of homeomorphisms of a manifold" Math. USSR Sb. , 8 : 3 (1969) pp. 287–333 |
[5] | T. Rushing, "Topological embeddings" , Acad. Press (1973) |
[6] | L.C. Siebenmann, R.C. Kirby, "Foundational essays on topological manifolds, smoothings, and triangulations" , Princeton Univ. Press (1977) |
Comments
Isotopies are also very important in infinite-dimensional topology (cf. Infinite-dimensional space). For example, if and
are points in the Hilbert cube
, then there exists an isotopy
such that
and
.
References
[a1] | J. van Mill, "Infinite-dimensional topology, prerequisites and introduction" , North-Holland (1988) |
Isotopy (in topology). Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Isotopy_(in_topology)&oldid=32170