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{{Short description|Connects homology and cohomology groups for oriented closed manifolds}}
{{Short description|Connects homology and cohomology groups for oriented closed manifolds}}
In [[mathematics]], the '''Poincaré duality''' theorem, named after [[Henri Poincaré]], is a basic result on the structure of the [[homology (mathematics)|homology]] and [[cohomology]] [[group (mathematics)|group]]s of [[manifold]]s. It states that if ''M'' is an ''n''-dimensional [[Orientability|oriented]] [[closed manifold]] ([[Compact space|compact]] and without boundary), then the ''k''th cohomology group of ''M'' is [[Group isomorphism|isomorphic]] to the (<math>n-k</math>)th homology group of ''M'', for all integers ''k''
In [[mathematics]], the '''Poincaré duality''' theorem, named after [[Henri Poincaré]], is a basic result on the structure of the [[homology (mathematics)|homology]] and [[cohomology]] [[group (mathematics)|group]]s of [[manifold]]s. It states that if ''M'' is an ''n''-dimensional [[Orientability|oriented]] [[closed manifold]] ([[Compact space|compact]] and without boundary), then the ''k''th cohomology group of ''M'' is [[Group isomorphism|isomorphic]] to the {{nowrap|(''n'' − ''k'')}}th homology group of ''M'', for all integers ''k''
:<math>H^k(M) \cong H_{n-k}(M).</math>
: <math>H^k(M) \cong H_{n-k}(M).</math>


Poincaré duality holds for any coefficient [[ring (mathematics)|ring]], so long as one has taken an orientation with respect to that coefficient ring; in particular, since every manifold has a unique orientation mod 2, Poincaré duality holds mod 2 without any assumption of orientation.
Poincaré duality holds for any coefficient [[ring (mathematics)|ring]], so long as one has taken an orientation with respect to that coefficient ring; in particular, since every manifold has a unique orientation mod 2, Poincaré duality holds mod 2 without any assumption of orientation.


== History ==
== History ==
A form of Poincaré duality was first stated, without proof, by [[Henri Poincaré]] in 1893. It was stated in terms of [[Betti number]]s: The ''k''th and (<math>n-k</math>)th Betti numbers of a closed (i.e., compact and without boundary) orientable ''n''-manifold are equal. The ''cohomology'' concept was at that time about 40 years from being clarified. In his 1895 paper ''[[Analysis Situs (paper)|Analysis Situs]]'', Poincaré tried to prove the theorem using topological [[intersection theory]], which he had invented. Criticism of his work by [[Poul Heegaard]] led him to realize that his proof was seriously flawed. In the first two complements to ''Analysis Situs'', Poincaré gave a new proof in terms of dual triangulations.
A form of Poincaré duality was first stated, without proof, by [[Henri Poincaré]] in 1893. It was stated in terms of [[Betti number]]s: The ''k''th and {{nowrap|(''n'' − ''k'')}}th Betti numbers of a closed (i.e., compact and without boundary) orientable ''n''-manifold are equal. The ''cohomology'' concept was at that time about 40 years from being clarified. In his 1895 paper ''[[Analysis Situs (paper)|Analysis Situs]]'', Poincaré tried to prove the theorem using topological [[intersection theory]], which he had invented. Criticism of his work by [[Poul Heegaard]] led him to realize that his proof was seriously flawed. In the first two complements to ''Analysis Situs'', Poincaré gave a new proof in terms of dual triangulations.


Poincaré duality did not take on its modern form until the advent of cohomology in the 1930s, when [[Eduard Čech]] and [[Hassler Whitney]] invented the [[cup product|cup]] and [[cap product]]s and formulated Poincaré duality in these new terms.
Poincaré duality did not take on its modern form until the advent of cohomology in the 1930s, when [[Eduard Čech]] and [[Hassler Whitney]] invented the [[cup product|cup]] and [[cap product]]s and formulated Poincaré duality in these new terms.


== Modern formulation ==
== Modern formulation ==
The modern statement of the Poincaré duality theorem is in terms of homology and cohomology: if <math>M </math> is a closed oriented ''n''-manifold, then there is a canonically defined isomorphism <math>H^k(M, \Z) \to H_{n-k}(M, \Z)</math> for any integer <math>k</math>. To define such an isomorphism, one chooses a fixed [[fundamental class]] <math>[M]
The modern statement of the Poincaré duality theorem is in terms of homology and cohomology: if ''M'' is a closed oriented ''n''-manifold, then there is a canonically defined isomorphism <math>H^k(M, \Z) \to H_{n-k}(M, \Z)</math> for any integer ''k''. To define such an isomorphism, one chooses a fixed [[fundamental class]] [''M''] of ''M'', which will exist if <math>M</math> is oriented. Then the isomorphism is defined by mapping an element <math>\alpha \in H^k(M)</math> to the [[cap product]] <math>[M]\frown \alpha</math>.<ref>{{Cite book|first=Allen|last=Hatcher|authorlink=Allen Hatcher|url=https://pi.math.cornell.edu/~hatcher/AT/ATpage.html|title=Algebraic Topology|date=2002|publisher=[[Cambridge University Press]]|isbn=9780521795401|edition= 1st|location=Cambridge|language=English|mr=1867354}}</ref>
</math> of <math>M</math>, which will exist if <math>M</math> is oriented. Then the isomorphism is defined by mapping an element <math>\alpha \in H^k(M)</math> to the [[cap product]] <math>[M]\frown \alpha</math>.<ref>{{Cite book|first=Allen|last=Hatcher|authorlink=Allen Hatcher|url=https://www.math.cornell.edu/~hatcher/AT/ATpage.html|title=Algebraic Topology|date=2002|publisher=[[Cambridge University Press]]|isbn=9780521795401|edition= 1st|location=Cambridge|language=English|mr=1867354}}</ref>


Homology and cohomology groups are defined to be zero for negative degrees, so Poincaré duality in particular implies that the homology and cohomology groups of orientable closed ''n''-manifolds are zero for degrees bigger than ''n''.
Homology and cohomology groups are defined to be zero for negative degrees, so Poincaré duality in particular implies that the homology and cohomology groups of orientable closed ''n''-manifolds are zero for degrees bigger than ''n''.


Here, homology and cohomology are integral, but the isomorphism remains valid over any coefficient ring. In the case where an oriented manifold is not compact, one has to replace homology by [[Borel–Moore homology]]
Here, homology and cohomology are integral, but the isomorphism remains valid over any coefficient ring. In the case where an oriented manifold is not compact, one has to replace homology by [[Borel–Moore homology]]
: <math>H^i(X) \stackrel{\cong}{\to} H_{n-i}^{BM}(X),</math>

:<math>H^i(X) \stackrel{\cong}{\to} H_{n-i}^{BM}(X),</math>

or replace cohomology by [[cohomology with compact support]]
or replace cohomology by [[cohomology with compact support]]
: <math>H^i_c(X) \stackrel{\cong}{\to} H_{n-i}(X).</math>

:<math>H^i_c(X) \stackrel{\cong}{\to} H_{n-i}(X).</math>


== Dual cell structures ==
== Dual cell structures ==
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[[File:Dually007.png|thumb|350px|right|<math>\cup_{S \in T} \Delta \cap DS</math> – a picture of the parts of the dual-cells in a top-dimensional simplex.]]
[[File:Dually007.png|thumb|350px|right|<math>\cup_{S \in T} \Delta \cap DS</math> – a picture of the parts of the dual-cells in a top-dimensional simplex.]]


Precisely, let ''T'' be a triangulation of an ''n''-manifold ''M''. Let ''S'' be a simplex of ''T''. Let <math>\Delta</math> be a top-dimensional simplex of ''T'' containing ''S'', so we can think of ''S'' as a subset of the vertices of <math>\Delta</math>. Define the dual cell ''DS'' corresponding to ''S'' so that <math>\Delta \cap DS</math> is the convex hull in <math>\Delta</math> of the barycentres of all subsets of the vertices of <math>\Delta</math> that contain <math>S</math>. One can check that if ''S'' is ''i''-dimensional, then ''DS'' is an (<math>n-i</math>)-dimensional cell. Moreover, the dual cells to ''T'' form a CW-decomposition of ''M'', and the only (<math>n-i</math>)-dimensional dual cell that intersects an ''i''-cell ''S'' is ''DS''. Thus the pairing <math>C_i M \otimes C_{n-i} M \to \Z</math> given by taking intersections induces an isomorphism <math>C_i M \to C^{n-i} M</math>, where <math>C_i</math> is the cellular homology of the triangulation ''T'', and <math>C_{n-i} M</math> and <math>C^{n-i} M</math> are the cellular homologies and cohomologies of the dual polyhedral/CW decomposition the manifold respectively. The fact that this is an isomorphism of [[chain complex]]es is a proof of Poincaré duality. Roughly speaking, this amounts to the fact that the boundary relation for the triangulation ''T'' is the incidence relation for the dual polyhedral decomposition under the correspondence <math>S \longmapsto DS</math>.
Precisely, let <math>T</math> be a triangulation of an <math>n</math>-manifold <math>M</math>. Let <math>S</math> be a simplex of <math>T</math>. Let <math>\Delta</math> be a top-dimensional simplex of <math>T</math> containing <math>S</math>, so we can think of <math>S</math> as a subset of the vertices of <math>\Delta</math>. Define the dual cell <math>DS</math> corresponding to <math>S</math> so that <math>\Delta \cap DS</math> is the convex hull in <math>\Delta</math> of the barycentres of all subsets of the vertices of <math>\Delta</math> that contain <math>S</math>. One can check that if <math>S</math> is <math>i</math>-dimensional, then <math>DS</math> is an <math>(n-i)</math>-dimensional cell. Moreover, the dual cells to <math>T</math> form a CW-decomposition of <math>M</math>, and the only (<math>n-i</math>)-dimensional dual cell that intersects an <math>i</math>-cell <math>S</math> is <math>DS</math>. Thus the pairing <math>C_i M \otimes C_{n-i} M \to \Z</math> given by taking intersections induces an isomorphism <math>C_i M \to C^{\, n-i} M</math>, where <math>C_i</math> is the cellular homology of the triangulation <math>T</math>, and <math>C_{n-i} M</math> and <math>C^{\, n-i} M</math> are the cellular homologies and cohomologies of the dual polyhedral/CW decomposition the manifold respectively. The fact that this is an isomorphism of [[chain complex]]es is a proof of Poincaré duality. Roughly speaking, this amounts to the fact that the boundary relation for the triangulation <math>T</math> is the incidence relation for the dual polyhedral decomposition under the correspondence <math>S \longmapsto DS</math>.


=== Naturality ===
=== Naturality ===
Note that <math>H^k</math> is a [[contravariant functor]] while <math>H_{n-k}</math> is [[covariant functor|covariant]]. The family of isomorphisms
Note that <math>H^k</math> is a [[contravariant functor]] while <math>H_{n-k}</math> is [[covariant functor|covariant]]. The family of isomorphisms

: <math>D_M\colon H^k(M) \to H_{n-k}(M)</math>
: <math>D_M\colon H^k(M) \to H_{n-k}(M)</math>

is [[natural transformation|natural]] in the following sense: if
is [[natural transformation|natural]] in the following sense: if
: <math>f\colon M\to N</math>

:<math>f\colon M\to N</math>

is a [[continuous map]] between two oriented ''n''-manifolds which is compatible with orientation, i.e. which maps the fundamental class of ''M'' to the fundamental class of ''N'', then
is a [[continuous map]] between two oriented ''n''-manifolds which is compatible with orientation, i.e. which maps the fundamental class of ''M'' to the fundamental class of ''N'', then

: <math>D_N = f_{*} \circ D_M \circ f^{*} ,</math>
: <math>D_N = f_{*} \circ D_M \circ f^{*} ,</math>

where <math>f_{*}</math> and <math>f^{*}</math> are the maps induced by <math>f</math> in homology and cohomology, respectively.
where <math>f_{*}</math> and <math>f^{*}</math> are the maps induced by <math>f</math> in homology and cohomology, respectively.


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Assuming the manifold ''M'' is compact, boundaryless, and [[orientable manifold|orientable]], let
Assuming the manifold ''M'' is compact, boundaryless, and [[orientable manifold|orientable]], let
: <math>\tau H_i M</math>

:<math>\tau H_i M</math>

denote the [[torsion (algebra)|torsion]] subgroup of <math>H_i M</math> and let
denote the [[torsion (algebra)|torsion]] subgroup of <math>H_i M</math> and let
: <math>fH_i M = H_i M / \tau H_i M</math>

:<math>fH_i M = H_i M / \tau H_i M</math>

be the [[free group|free]] part – all homology groups taken with integer coefficients in this section. Then there are [[bilinear operator|bilinear maps]] which are [[duality pairing]]s (explained below).
be the [[free group|free]] part – all homology groups taken with integer coefficients in this section. Then there are [[bilinear operator|bilinear maps]] which are [[duality pairing]]s (explained below).
: <math>fH_i M \otimes fH_{n-i} M \to \Z</math>

:<math>fH_i M \otimes fH_{n-i} M \to \Z</math>

and
and
: <math>\tau H_i M \otimes \tau H_{n-i-1} M \to \Q/\Z</math>.


Here <math>\Q/\Z</math> is the quotient of the rationals by the integers, taken as an additive group. Notice that in the torsion linking form, there is a −1 in the dimension, so the paired dimensions add up to {{nowrap|''n'' − 1}}, rather than to ''n''.
:<math>\tau H_i M \otimes \tau H_{n-i-1} M \to \Q/\Z</math>.

Here <math>\Q/\Z</math> is the quotient of the rationals by the integers, taken as an additive group. Notice that in the torsion linking form, there is a <math>-1</math> in the dimension, so the paired dimensions add up to <math>n-1,</math> rather than to <math>n</math>.


The first form is typically called the ''[[intersection theory|intersection product]]'' and the 2nd the ''torsion linking form''.{{anchor|torsion linking form}} Assuming the manifold ''M'' is smooth, the intersection product is computed by perturbing the homology classes to be transverse and computing their oriented intersection number. For the torsion linking form, one computes the pairing of ''x'' and ''y'' by realizing ''nx'' as the boundary of some class ''z''. The form then takes the value equal to the fraction whose numerator is the transverse intersection number of ''z'' with ''y'', and whose denominator is ''n''.
The first form is typically called the ''[[intersection theory|intersection product]]'' and the 2nd the ''torsion linking form''.{{anchor|torsion linking form}} Assuming the manifold ''M'' is smooth, the intersection product is computed by perturbing the homology classes to be transverse and computing their oriented intersection number. For the torsion linking form, one computes the pairing of ''x'' and ''y'' by realizing ''nx'' as the boundary of some class ''z''. The form then takes the value equal to the fraction whose numerator is the transverse intersection number of ''z'' with ''y'', and whose denominator is ''n''.


The statement that the pairings are duality pairings means that the adjoint maps
The statement that the pairings are duality pairings means that the adjoint maps
:<math>fH_i M \to \mathrm{Hom}_{\Z}(fH_{n-i} M,\Z)</math>
: <math>fH_i M \to \mathrm{Hom}_{\Z}(fH_{n-i} M,\Z)</math>
and
and
:<math>\tau H_i M \to \mathrm{Hom}_{\Z}(\tau H_{n-i-1} M, \Q/\Z)</math>
: <math>\tau H_i M \to \mathrm{Hom}_{\Z}(\tau H_{n-i-1} M, \Q/\Z)</math>
are isomorphisms of groups.
are isomorphisms of groups.


This result is an application of Poincaré duality
This result is an application of Poincaré duality
: <math>H_i M \simeq H^{n-i} M</math>,

:<math>H_i M \simeq H^{n-i} M</math>,

together with the [[universal coefficient theorem]], which gives an identification
together with the [[universal coefficient theorem]], which gives an identification
:<math>fH^{n-i} M \equiv \mathrm{Hom}(H_{n-i} M; \Z)</math>
: <math>fH^{n-i} M \equiv \mathrm{Hom}(H_{n-i} M; \Z)</math>
and
and
:<math>\tau H^{n-i} M \equiv \mathrm{Ext}(H_{n-i-1} M; \Z) \equiv \mathrm{Hom}(\tau H_{n-i-1} M; \Q/\Z)</math>.
: <math>\tau H^{n-i} M \equiv \mathrm{Ext}(H_{n-i-1} M; \Z) \equiv \mathrm{Hom}(\tau H_{n-i-1} M; \Q/\Z)</math>.
Thus, Poincaré duality says that <math>fH_i M</math> and <math>fH_{n-i} M</math> are isomorphic, although there is no natural map giving the isomorphism, and similarly <math>\tau H_i M</math> and <math>\tau H_{n-i-1} M</math> are also isomorphic, though not naturally.
Thus, Poincaré duality says that <math>fH_i M</math> and <math>fH_{n-i} M</math> are isomorphic, although there is no natural map giving the isomorphism, and similarly <math>\tau H_i M</math> and <math>\tau H_{n-i-1} M</math> are also isomorphic, though not naturally.


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While for most dimensions, Poincaré duality induces a bilinear ''pairing'' between different homology groups, in the middle dimension it induces a [[bilinear form|bilinear ''form'']] on a single homology group. The resulting [[Intersection theory#Topological intersection form|intersection form]] is a very important topological invariant.
While for most dimensions, Poincaré duality induces a bilinear ''pairing'' between different homology groups, in the middle dimension it induces a [[bilinear form|bilinear ''form'']] on a single homology group. The resulting [[Intersection theory#Topological intersection form|intersection form]] is a very important topological invariant.


What is meant by "middle dimension" depends on parity. For even dimension <math>n = 2k,</math> which is more common, this is literally the middle dimension ''k,'' and there is a form on the free part of the middle homology:
What is meant by "middle dimension" depends on parity. For even dimension {{nowrap|1=''n'' = 2''k''}}, which is more common, this is literally the middle dimension ''k'', and there is a form on the free part of the middle homology:
:<math>fH_k M \otimes fH_k M \to \Z</math>
: <math>fH_k M \otimes fH_k M \to \Z</math>


By contrast, for odd dimension <math>n = 2k+1,</math> which is less commonly discussed, it is most simply the lower middle dimension ''k,'' and there is a form on the torsion part of the homology in that dimension:
By contrast, for odd dimension {{nowrap|1=''n'' = 2''k'' + 1}}, which is less commonly discussed, it is most simply the lower middle dimension ''k'', and there is a form on the torsion part of the homology in that dimension:
:<math>\tau H_k M \otimes \tau H_k M \to \Q/\Z.</math>
: <math>\tau H_k M \otimes \tau H_k M \to \Q/\Z.</math>
However, there is also a pairing between the free part of the homology in the lower middle dimension ''k'' and in the upper middle dimension <math>k+1</math>:
However, there is also a pairing between the free part of the homology in the lower middle dimension ''k'' and in the upper middle dimension {{nowrap|''k'' + 1}}:
:<math>fH_k M \otimes fH_{k+1} M \to \Z.</math>
: <math>fH_k M \otimes fH_{k+1} M \to \Z.</math>
The resulting groups, while not a single group with a bilinear form, are a simple chain complex and are studied in algebraic [[L-theory]].
The resulting groups, while not a single group with a bilinear form, are a simple chain complex and are studied in algebraic [[L-theory]].


;Applications
;Applications
This approach to Poincaré duality was used by [[Józef H. Przytycki|Józef Przytycki]] and Akira Yasuhara to give an elementary homotopy and diffeomorphism classification of 3-dimensional [[lens space]]s.<ref>
This approach to Poincaré duality was used by [[Józef H. Przytycki|Józef Przytycki]] and Akira Yasuhara to give an elementary homotopy and diffeomorphism classification of 3-dimensional [[lens space]]s.<ref>
{{citation|first1=Józef H.|last1=Przytycki|authorlink1=Józef H. Przytycki|first2=Akira|last2=Yasuhara|title=Symmetry of links and classification of lens spaces|journal=[[Geometriae Dedicata]] | volume=98|year=2003|issue=1|mr=1988423|doi=10.1023/A:1024008222682}}</ref>
{{citation|first1=Józef H.|last1=Przytycki|authorlink1=Józef H. Przytycki|first2=Akira|last2=Yasuhara|title=Symmetry of links and classification of lens spaces|journal=[[Geometriae Dedicata]] | volume=98|year=2003|issue=1|pages=57–61 |mr=1988423|doi=10.1023/A:1024008222682|s2cid=14601373 }}</ref>


== Application to Euler Characteristics ==
== Application to Euler Characteristics ==
An immediate result from Poincaré duality is that any closed odd-dimensional manifold M has [[Euler characteristic|Euler characteristic]] zero, which in turn gives that any manifold that bounds has even Euler characteristics.
An immediate result from Poincaré duality is that any closed odd-dimensional manifold ''M'' has [[Euler characteristic]] zero, which in turn gives that any manifold that bounds has even Euler characteristic.

== Thom isomorphism formulation ==
== Thom isomorphism formulation ==


Poincaré duality is closely related to the [[Thom space|Thom isomorphism theorem]], as we will explain here. For this exposition, let <math>M</math> be a compact, boundaryless oriented ''n''-manifold. Let <math>M \times M</math> be the product of <math>M</math> with itself, let <math>V</math> be an open tubular neighbourhood of the diagonal in <math>M \times M</math>. Consider the maps:
Poincaré duality is closely related to the [[Thom space|Thom isomorphism theorem]]. Let <math>M</math> be a compact, boundaryless oriented ''n''-manifold, and {{nowrap|''M'' × ''M''}} the product of ''M'' with itself. Let ''V'' be an open [[Tubular neighborhood|tubular neighbourhood]] of the diagonal in {{nowrap|''M'' × ''M''}}. Consider the maps:
:* <math> H_* M \otimes H_* M \to H_* (M \times M)</math> the [[Künneth theorem|Homology cross product]]

:* <math> H_* M \otimes H_* M \to H_* (M \times M)</math> the [[Künneth theorem|Homology cross [product]]

:* <math>H_* (M \times M) \to H_* \left(M \times M, (M \times M) \setminus V\right)</math> inclusion.
:* <math>H_* (M \times M) \to H_* \left(M \times M, (M \times M) \setminus V\right)</math> inclusion.

:* <math>H_* \left(M \times M, (M \times M) \setminus V\right) \to H_* (\nu M, \partial \nu M) </math> [[excision theorem|excision map]] where <math>\nu M</math> is the [[normal bundle|normal disc bundle]] of the diagonal in <math>M \times M</math>.
:* <math>H_* \left(M \times M, (M \times M) \setminus V\right) \to H_* (\nu M, \partial \nu M) </math> [[excision theorem|excision map]] where <math>\nu M</math> is the [[normal bundle|normal disc bundle]] of the diagonal in <math>M \times M</math>.

:* <math>H_* (\nu M, \partial \nu M) \to H_{*-n} M</math> the [[Thom space|Thom isomorphism]]. This map is well-defined as there is a standard identification <math>\nu M \equiv TM</math> which is an oriented bundle, so the Thom isomorphism applies.
:* <math>H_* (\nu M, \partial \nu M) \to H_{*-n} M</math> the [[Thom space|Thom isomorphism]]. This map is well-defined as there is a standard identification <math>\nu M \equiv TM</math> which is an oriented bundle, so the Thom isomorphism applies.


Combined, this gives a map <math>H_i M \otimes H_j M \to H_{i+j-n} M</math>, which is the ''intersection product''—strictly speaking it is a generalization of the intersection product above, but it is also called the intersection product. A similar argument with the [[Künneth theorem]] gives the ''torsion linking form''.
Combined, this gives a map <math>H_i M \otimes H_j M \to H_{i+j-n} M</math>, which is the ''intersection product'', generalizing the intersection product discussed above. A similar argument with the [[Künneth theorem]] gives the ''torsion linking form''.


This formulation of Poincaré duality has become quite popular<ref>{{cite book |last=Rudyak |first=Yuli |title=On Thom spectra, orientability, and cobordism |others=With a foreword by [[Haynes Miller]]|location=Berlin |series=Springer Monographs in Mathematics|publisher=Springer-Verlag |year=1998 |isbn=3-540-62043-5|mr=1627486 }}</ref> as it provides a means to define Poincaré duality for any [[generalized homology theory]] provided one has a Künneth theorem and a Thom isomorphism for that homology theory. A Thom isomorphism theorem for a homology theory is now accepted as the generalized notion of [[orientability]] for a homology theory. For example, a [[spin structure|spin<sup>'''C'''</sup>-structure]] on a manifold turns out to be precisely what is needed to be orientable in the sense of [[k-theory|complex topological k-theory]].
This formulation of Poincaré duality has become popular<ref>{{cite book |last=Rudyak |first=Yuli |title=On Thom spectra, orientability, and cobordism |others=With a foreword by [[Haynes Miller]]|location=Berlin |series=Springer Monographs in Mathematics|publisher=Springer-Verlag |year=1998 |isbn=3-540-62043-5|mr=1627486 }}</ref> as it defines Poincaré duality for any [[generalized homology theory]], given a Künneth theorem and a Thom isomorphism for that homology theory. A Thom isomorphism theorem for a homology theory is now viewed as the generalized notion of [[orientability]] for that theory. For example, a [[spin structure|spin<sup>'''C'''</sup>-structure]] on a manifold is a precise analog of an orientation within [[k-theory|complex topological k-theory]].


== Generalizations and related results ==
== Generalizations and related results ==
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* [[Weyl group]]
* [[Weyl group]]


==References==
== References ==
{{Reflist}}
{{Reflist}}


==Further reading==
== Further reading ==
*{{citation |first=Richard C. |last=Blanchfield |title=Intersection theory of manifolds with operators with applications to knot theory |journal=[[Annals of Mathematics]] |volume=65 |issue=2 |year=1957 |pages=340–356 |jstor=1969966 | doi = 10.2307/1969966|mr=0085512 }}
* {{citation |first=Richard C. |last=Blanchfield |title=Intersection theory of manifolds with operators with applications to knot theory |journal=[[Annals of Mathematics]] |volume=65 |issue=2 |year=1957 |pages=340–356 |jstor=1969966 | doi = 10.2307/1969966|mr=0085512 }}
* {{Citation | last1=Griffiths | first1=Phillip | author1-link= Phillip Griffiths | last2=Harris | first2=Joseph | author2-link= Joe Harris (mathematician) | title=Principles of algebraic geometry | publisher=Wiley | location=New York | series=Wiley Classics Library | isbn=978-0-471-05059-9 | mr=1288523 | year=1994}}
* {{Citation | last1=Griffiths | first1=Phillip | author1-link= Phillip Griffiths | last2=Harris | first2=Joseph | author2-link= Joe Harris (mathematician) | title=Principles of algebraic geometry | publisher=Wiley | location=New York | series=Wiley Classics Library | isbn=978-0-471-05059-9 | mr=1288523 | year=1994}}


== External links ==
== External links ==
*[http://www.map.mpim-bonn.mpg.de/Intersection_form Intersection form] at the Manifold Atlas
* [http://www.map.mpim-bonn.mpg.de/Intersection_form Intersection form] at the Manifold Atlas
*[http://www.map.mpim-bonn.mpg.de/Linking_form Linking form] at the Manifold Atlas
* [http://www.map.mpim-bonn.mpg.de/Linking_form Linking form] at the Manifold Atlas


{{DEFAULTSORT:Poincare duality}}
{{DEFAULTSORT:Poincare duality}}

Latest revision as of 08:59, 19 November 2024

In mathematics, the Poincaré duality theorem, named after Henri Poincaré, is a basic result on the structure of the homology and cohomology groups of manifolds. It states that if M is an n-dimensional oriented closed manifold (compact and without boundary), then the kth cohomology group of M is isomorphic to the (nk)th homology group of M, for all integers k

Poincaré duality holds for any coefficient ring, so long as one has taken an orientation with respect to that coefficient ring; in particular, since every manifold has a unique orientation mod 2, Poincaré duality holds mod 2 without any assumption of orientation.

History

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A form of Poincaré duality was first stated, without proof, by Henri Poincaré in 1893. It was stated in terms of Betti numbers: The kth and (nk)th Betti numbers of a closed (i.e., compact and without boundary) orientable n-manifold are equal. The cohomology concept was at that time about 40 years from being clarified. In his 1895 paper Analysis Situs, Poincaré tried to prove the theorem using topological intersection theory, which he had invented. Criticism of his work by Poul Heegaard led him to realize that his proof was seriously flawed. In the first two complements to Analysis Situs, Poincaré gave a new proof in terms of dual triangulations.

Poincaré duality did not take on its modern form until the advent of cohomology in the 1930s, when Eduard Čech and Hassler Whitney invented the cup and cap products and formulated Poincaré duality in these new terms.

Modern formulation

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The modern statement of the Poincaré duality theorem is in terms of homology and cohomology: if M is a closed oriented n-manifold, then there is a canonically defined isomorphism for any integer k. To define such an isomorphism, one chooses a fixed fundamental class [M] of M, which will exist if is oriented. Then the isomorphism is defined by mapping an element to the cap product .[1]

Homology and cohomology groups are defined to be zero for negative degrees, so Poincaré duality in particular implies that the homology and cohomology groups of orientable closed n-manifolds are zero for degrees bigger than n.

Here, homology and cohomology are integral, but the isomorphism remains valid over any coefficient ring. In the case where an oriented manifold is not compact, one has to replace homology by Borel–Moore homology

or replace cohomology by cohomology with compact support

Dual cell structures

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Given a triangulated manifold, there is a corresponding dual polyhedral decomposition. The dual polyhedral decomposition is a cell decomposition of the manifold such that the k-cells of the dual polyhedral decomposition are in bijective correspondence with the ()-cells of the triangulation, generalizing the notion of dual polyhedra.

– a picture of the parts of the dual-cells in a top-dimensional simplex.

Precisely, let be a triangulation of an -manifold . Let be a simplex of . Let be a top-dimensional simplex of containing , so we can think of as a subset of the vertices of . Define the dual cell corresponding to so that is the convex hull in of the barycentres of all subsets of the vertices of that contain . One can check that if is -dimensional, then is an -dimensional cell. Moreover, the dual cells to form a CW-decomposition of , and the only ()-dimensional dual cell that intersects an -cell is . Thus the pairing given by taking intersections induces an isomorphism , where is the cellular homology of the triangulation , and and are the cellular homologies and cohomologies of the dual polyhedral/CW decomposition the manifold respectively. The fact that this is an isomorphism of chain complexes is a proof of Poincaré duality. Roughly speaking, this amounts to the fact that the boundary relation for the triangulation is the incidence relation for the dual polyhedral decomposition under the correspondence .

Naturality

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Note that is a contravariant functor while is covariant. The family of isomorphisms

is natural in the following sense: if

is a continuous map between two oriented n-manifolds which is compatible with orientation, i.e. which maps the fundamental class of M to the fundamental class of N, then

where and are the maps induced by in homology and cohomology, respectively.

Note the very strong and crucial hypothesis that maps the fundamental class of M to the fundamental class of N. Naturality does not hold for an arbitrary continuous map , since in general is not an injection on cohomology. For example, if is a covering map then it maps the fundamental class of M to a multiple of the fundamental class of N. This multiple is the degree of the map .

Bilinear pairings formulation

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Assuming the manifold M is compact, boundaryless, and orientable, let

denote the torsion subgroup of and let

be the free part – all homology groups taken with integer coefficients in this section. Then there are bilinear maps which are duality pairings (explained below).

and

.

Here is the quotient of the rationals by the integers, taken as an additive group. Notice that in the torsion linking form, there is a −1 in the dimension, so the paired dimensions add up to n − 1, rather than to n.

The first form is typically called the intersection product and the 2nd the torsion linking form. Assuming the manifold M is smooth, the intersection product is computed by perturbing the homology classes to be transverse and computing their oriented intersection number. For the torsion linking form, one computes the pairing of x and y by realizing nx as the boundary of some class z. The form then takes the value equal to the fraction whose numerator is the transverse intersection number of z with y, and whose denominator is n.

The statement that the pairings are duality pairings means that the adjoint maps

and

are isomorphisms of groups.

This result is an application of Poincaré duality

,

together with the universal coefficient theorem, which gives an identification

and

.

Thus, Poincaré duality says that and are isomorphic, although there is no natural map giving the isomorphism, and similarly and are also isomorphic, though not naturally.

Middle dimension

While for most dimensions, Poincaré duality induces a bilinear pairing between different homology groups, in the middle dimension it induces a bilinear form on a single homology group. The resulting intersection form is a very important topological invariant.

What is meant by "middle dimension" depends on parity. For even dimension n = 2k, which is more common, this is literally the middle dimension k, and there is a form on the free part of the middle homology:

By contrast, for odd dimension n = 2k + 1, which is less commonly discussed, it is most simply the lower middle dimension k, and there is a form on the torsion part of the homology in that dimension:

However, there is also a pairing between the free part of the homology in the lower middle dimension k and in the upper middle dimension k + 1:

The resulting groups, while not a single group with a bilinear form, are a simple chain complex and are studied in algebraic L-theory.

Applications

This approach to Poincaré duality was used by Józef Przytycki and Akira Yasuhara to give an elementary homotopy and diffeomorphism classification of 3-dimensional lens spaces.[2]

Application to Euler Characteristics

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An immediate result from Poincaré duality is that any closed odd-dimensional manifold M has Euler characteristic zero, which in turn gives that any manifold that bounds has even Euler characteristic.

Thom isomorphism formulation

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Poincaré duality is closely related to the Thom isomorphism theorem. Let be a compact, boundaryless oriented n-manifold, and M × M the product of M with itself. Let V be an open tubular neighbourhood of the diagonal in M × M. Consider the maps:

  • the Homology cross product
  • inclusion.
  • excision map where is the normal disc bundle of the diagonal in .
  • the Thom isomorphism. This map is well-defined as there is a standard identification which is an oriented bundle, so the Thom isomorphism applies.

Combined, this gives a map , which is the intersection product, generalizing the intersection product discussed above. A similar argument with the Künneth theorem gives the torsion linking form.

This formulation of Poincaré duality has become popular[3] as it defines Poincaré duality for any generalized homology theory, given a Künneth theorem and a Thom isomorphism for that homology theory. A Thom isomorphism theorem for a homology theory is now viewed as the generalized notion of orientability for that theory. For example, a spinC-structure on a manifold is a precise analog of an orientation within complex topological k-theory.

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The Poincaré–Lefschetz duality theorem is a generalisation for manifolds with boundary. In the non-orientable case, taking into account the sheaf of local orientations, one can give a statement that is independent of orientability: see twisted Poincaré duality.

Blanchfield duality is a version of Poincaré duality which provides an isomorphism between the homology of an abelian covering space of a manifold and the corresponding cohomology with compact supports. It is used to get basic structural results about the Alexander module and can be used to define the signatures of a knot.

With the development of homology theory to include K-theory and other extraordinary theories from about 1955, it was realised that the homology could be replaced by other theories, once the products on manifolds were constructed; and there are now textbook treatments in generality. More specifically, there is a general Poincaré duality theorem for a generalized homology theory which requires a notion of orientation with respect to a homology theory, and is formulated in terms of a generalized Thom isomorphism theorem. The Thom isomorphism theorem in this regard can be considered as the germinal idea for Poincaré duality for generalized homology theories.

Verdier duality is the appropriate generalization to (possibly singular) geometric objects, such as analytic spaces or schemes, while intersection homology was developed by Robert MacPherson and Mark Goresky for stratified spaces, such as real or complex algebraic varieties, precisely so as to generalise Poincaré duality to such stratified spaces.

There are many other forms of geometric duality in algebraic topology, including Lefschetz duality, Alexander duality, Hodge duality, and S-duality.

More algebraically, one can abstract the notion of a Poincaré complex, which is an algebraic object that behaves like the singular chain complex of a manifold, notably satisfying Poincaré duality on its homology groups, with respect to a distinguished element (corresponding to the fundamental class). These are used in surgery theory to algebraicize questions about manifolds. A Poincaré space is one whose singular chain complex is a Poincaré complex. These are not all manifolds, but their failure to be manifolds can be measured by obstruction theory.

See also

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References

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  1. ^ Hatcher, Allen (2002). Algebraic Topology (1st ed.). Cambridge: Cambridge University Press. ISBN 9780521795401. MR 1867354.
  2. ^ Przytycki, Józef H.; Yasuhara, Akira (2003), "Symmetry of links and classification of lens spaces", Geometriae Dedicata, 98 (1): 57–61, doi:10.1023/A:1024008222682, MR 1988423, S2CID 14601373
  3. ^ Rudyak, Yuli (1998). On Thom spectra, orientability, and cobordism. Springer Monographs in Mathematics. With a foreword by Haynes Miller. Berlin: Springer-Verlag. ISBN 3-540-62043-5. MR 1627486.

Further reading

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