<?xml version="1.0"?>
<feed xmlns="http://www.w3.org/2005/Atom" xml:lang="en">
	<id>https://en.formulasearchengine.com/index.php?action=history&amp;feed=atom&amp;title=Reversible_reference_system_propagation_algorithm</id>
	<title>Reversible reference system propagation algorithm - Revision history</title>
	<link rel="self" type="application/atom+xml" href="https://en.formulasearchengine.com/index.php?action=history&amp;feed=atom&amp;title=Reversible_reference_system_propagation_algorithm"/>
	<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/index.php?title=Reversible_reference_system_propagation_algorithm&amp;action=history"/>
	<updated>2026-05-06T01:32:47Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
	<generator>MediaWiki 1.43.0-wmf.28</generator>
	<entry>
		<id>https://en.formulasearchengine.com/index.php?title=Reversible_reference_system_propagation_algorithm&amp;diff=16872&amp;oldid=prev</id>
		<title>en&gt;RockMagnetist: −Category:Algorithms; −Category:Fundamental physics concepts; −Category:Ordinary differential equations; +Category:Hamiltonian mechanics using HotCat</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/index.php?title=Reversible_reference_system_propagation_algorithm&amp;diff=16872&amp;oldid=prev"/>
		<updated>2012-03-15T05:46:18Z</updated>

		<summary type="html">&lt;p&gt;−&lt;a href=&quot;/index.php?title=Category:Algorithms&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;Category:Algorithms (page does not exist)&quot;&gt;Category:Algorithms&lt;/a&gt;; −&lt;a href=&quot;/index.php?title=Category:Fundamental_physics_concepts&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;Category:Fundamental physics concepts (page does not exist)&quot;&gt;Category:Fundamental physics concepts&lt;/a&gt;; −&lt;a href=&quot;/index.php?title=Category:Ordinary_differential_equations&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;Category:Ordinary differential equations (page does not exist)&quot;&gt;Category:Ordinary differential equations&lt;/a&gt;; +&lt;a href=&quot;/index.php?title=Category:Hamiltonian_mechanics&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;Category:Hamiltonian mechanics (page does not exist)&quot;&gt;Category:Hamiltonian mechanics&lt;/a&gt; using &lt;a href=&quot;/index.php?title=WP:HC&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;WP:HC (page does not exist)&quot;&gt;HotCat&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;In [[mathematics]], the &amp;#039;&amp;#039;&amp;#039;Abel–Jacobi map&amp;#039;&amp;#039;&amp;#039; is a construction of [[algebraic geometry]] which relates an [[algebraic curve]] to its [[Jacobian variety]].  In [[Riemannian geometry]], it is a more general construction mapping a [[manifold]] to its Jacobi torus.&lt;br /&gt;
The name derives from the [[#Abel–Jacobi theorem|theorem]] of [[Niels Henrik Abel|Abel]] and [[Carl Gustav Jacob Jacobi|Jacobi]] that two [[effective divisor]]s are [[linearly equivalent]] if and only if they are indistinguishable under the Abel–Jacobi map.&lt;br /&gt;
&lt;br /&gt;
==Construction of the map==&lt;br /&gt;
&lt;br /&gt;
In [[complex algebraic geometry]], the Jacobian of a curve &amp;#039;&amp;#039;C&amp;#039;&amp;#039; is constructed using path integration.  Namely, suppose &amp;#039;&amp;#039;C&amp;#039;&amp;#039; has [[genus of a curve|genus]] &amp;#039;&amp;#039;g&amp;#039;&amp;#039;, which means topologically that&lt;br /&gt;
: &amp;lt;math&amp;gt;H_1(C, \mathbb{Z}) \cong \mathbb{Z}^{2g}.&amp;lt;/math&amp;gt;&lt;br /&gt;
Geometrically, this homology group consists of (homology classes of) &amp;#039;&amp;#039;cycles&amp;#039;&amp;#039; in &amp;#039;&amp;#039;C&amp;#039;&amp;#039;, or in other words, closed loops.  Therefore we can choose 2&amp;#039;&amp;#039;g&amp;#039;&amp;#039; loops &amp;lt;math&amp;gt;\gamma_1, \dots, \gamma_{2g}&amp;lt;/math&amp;gt; generating it.  On the other hand, another, more algebro-geometric way of saying that the genus of &amp;#039;&amp;#039;C&amp;#039;&amp;#039; is &amp;#039;&amp;#039;g&amp;#039;&amp;#039;, is that&lt;br /&gt;
: &amp;lt;math&amp;gt;H^0(C, K) \cong \mathbb{C}^g,&amp;lt;/math&amp;gt; where &amp;#039;&amp;#039;K&amp;#039;&amp;#039; is the [[canonical bundle]] on &amp;#039;&amp;#039;C&amp;#039;&amp;#039;.&lt;br /&gt;
By definition, this is the space of globally defined holomorphic [[differential form]]s on &amp;#039;&amp;#039;C&amp;#039;&amp;#039;, so we can choose &amp;#039;&amp;#039;g&amp;#039;&amp;#039; linearly independent forms &amp;lt;math&amp;gt;\omega_1, \dots, \omega_g&amp;lt;/math&amp;gt;.  Given forms and closed loops we can integrate, and we define 2&amp;#039;&amp;#039;g&amp;#039;&amp;#039; vectors&lt;br /&gt;
: &amp;lt;math&amp;gt;\Omega_j = \left(\int_{\gamma_j} \omega_1, \dots, \int_{\gamma_j} \omega_g\right) \in \mathbb{C}^g.&amp;lt;/math&amp;gt;&lt;br /&gt;
It follows from the [[Riemann bilinear relations]] that the &amp;lt;math&amp;gt;\Omega_j&amp;lt;/math&amp;gt; generate a nondegenerate [[lattice (group)|lattice]] &amp;lt;math&amp;gt;\Lambda&amp;lt;/math&amp;gt; (that is, they are a real basis for &amp;lt;math&amp;gt;\mathbb{C}^g \cong \mathbb{R}^{2g}&amp;lt;/math&amp;gt;), and the Jacobian is defined by&lt;br /&gt;
: &amp;lt;math&amp;gt;J(C) = \mathbb{C}^g/\Lambda.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;Abel–Jacobi map&amp;#039;&amp;#039;&amp;#039; is then defined as follows.  We pick some base point &amp;lt;math&amp;gt;p_0 \in C&amp;lt;/math&amp;gt; and, nearly mimicking the definition of &amp;lt;math&amp;gt;\Lambda&amp;lt;/math&amp;gt;, define the map&lt;br /&gt;
: &amp;lt;math&amp;gt;u \colon C \to J(C), u(p) = \left( \int_{p_0}^p \omega_1, \dots, \int_{p_0}^p \omega_g\right)  \bmod \Lambda.&amp;lt;/math&amp;gt;&lt;br /&gt;
Although this is seemingly dependent on a path from &amp;lt;math&amp;gt;p_0&amp;lt;/math&amp;gt; to &amp;lt;math&amp;gt;p,&amp;lt;/math&amp;gt; any two such paths define a closed loop in &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; and, therefore, an element of &amp;lt;math&amp;gt;H_1(C, \mathbb{Z}),&amp;lt;/math&amp;gt; so integration over it gives an element of &amp;lt;math&amp;gt;\Lambda.&amp;lt;/math&amp;gt;  Thus the difference is erased in the passage to the quotient by &amp;lt;math&amp;gt;\Lambda&amp;lt;/math&amp;gt;. Changing  base-point &amp;lt;math&amp;gt;p_0&amp;lt;/math&amp;gt;  does change the map, but only by a translation of the torus.&lt;br /&gt;
&lt;br /&gt;
==The Abel–Jacobi map of a Riemannian manifold==&lt;br /&gt;
&lt;br /&gt;
Let &amp;lt;math&amp;gt;M&amp;lt;/math&amp;gt; be a smooth compact [[manifold]].  Let &amp;lt;math&amp;gt;\pi=\pi_1(M)&amp;lt;/math&amp;gt; be its fundamental group.  Let  &amp;lt;math&amp;gt;f: \pi \to \pi^{ab}&amp;lt;/math&amp;gt; be its [[abelianisation]] map.  Let&lt;br /&gt;
&amp;lt;math&amp;gt;tor= tor(\pi^{ab})&amp;lt;/math&amp;gt; be the torsion subgroup of&lt;br /&gt;
&amp;lt;math&amp;gt;\pi^{ab}&amp;lt;/math&amp;gt;.  Let &amp;lt;math&amp;gt;g: \pi^{ab} \to \pi^{ab}/tor&amp;lt;/math&amp;gt;&lt;br /&gt;
be the quotient by torsion.  If &amp;lt;math&amp;gt;M&amp;lt;/math&amp;gt; is a surface, &amp;lt;math&amp;gt;\pi^{ab}/tor&amp;lt;/math&amp;gt; is non-canonically isomorphic to&lt;br /&gt;
&amp;lt;math&amp;gt;\mathbb{Z}^{2g}&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;g&amp;lt;/math&amp;gt; is the genus; more generally,  &amp;lt;math&amp;gt;\pi^{ab}/tor &amp;lt;/math&amp;gt; is non-canonically isomorphic to &amp;lt;math&amp;gt;\mathbb{Z}^b &amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;b&amp;lt;/math&amp;gt; is the first Betti number.  Let &amp;lt;math&amp;gt;\phi=g \circ f : \pi \to \mathbb{Z}^b &amp;lt;/math&amp;gt; be the composite homomorphism.&lt;br /&gt;
&lt;br /&gt;
Definition. The cover &amp;lt;math&amp;gt;\bar M&amp;lt;/math&amp;gt; of the manifold&lt;br /&gt;
&amp;lt;math&amp;gt;M&amp;lt;/math&amp;gt; corresponding the subgroup &amp;lt;math&amp;gt;\mathrm{Ker}(\phi)&lt;br /&gt;
\subset \pi&amp;lt;/math&amp;gt; is called the universal (or maximal) free abelian&lt;br /&gt;
cover.&lt;br /&gt;
&lt;br /&gt;
Now assume &amp;#039;&amp;#039;M&amp;#039;&amp;#039; has a [[Riemannian metric]].  Let &amp;lt;math&amp;gt;E&amp;lt;/math&amp;gt; be the space of harmonic &amp;lt;math&amp;gt;1&amp;lt;/math&amp;gt;-forms on&lt;br /&gt;
&amp;lt;math&amp;gt;M&amp;lt;/math&amp;gt;, with dual &amp;lt;math&amp;gt;E^*&amp;lt;/math&amp;gt; canonically identified with&lt;br /&gt;
&amp;lt;math&amp;gt;H_1(M,\mathbb{R})&amp;lt;/math&amp;gt;.  By integrating an integral&lt;br /&gt;
harmonic &amp;lt;math&amp;gt;1&amp;lt;/math&amp;gt;-form along paths from a basepoint &amp;lt;math&amp;gt;x_0\in&lt;br /&gt;
M&amp;lt;/math&amp;gt;, we obtain a map to the circle&lt;br /&gt;
&amp;lt;math&amp;gt;\mathbb{R}/\mathbb{Z}=S^1&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Similarly, in order to define a map &amp;lt;math&amp;gt;M\to H_1(M,\mathbb{R}) /&lt;br /&gt;
H_1(M,\mathbb{Z})_{\mathbb{R}}&amp;lt;/math&amp;gt; without choosing a basis for&lt;br /&gt;
cohomology, we argue as follows.  Let &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; be a point in the&lt;br /&gt;
[[universal cover]] &amp;lt;math&amp;gt;\tilde{M}&amp;lt;/math&amp;gt; of &amp;lt;math&amp;gt;M&amp;lt;/math&amp;gt;.  Thus&lt;br /&gt;
&amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; is represented by a point of &amp;lt;math&amp;gt;M&amp;lt;/math&amp;gt; together&lt;br /&gt;
with a path &amp;lt;math&amp;gt;c&amp;lt;/math&amp;gt; from &amp;lt;math&amp;gt;x_0&amp;lt;/math&amp;gt; to it.  By&lt;br /&gt;
integrating along the path &amp;lt;math&amp;gt;c&amp;lt;/math&amp;gt;, we obtain a linear form,&lt;br /&gt;
&amp;lt;math&amp;gt;h\to \int_c h&amp;lt;/math&amp;gt;, on &amp;lt;math&amp;gt;E&amp;lt;/math&amp;gt;.  We thus obtain a map&lt;br /&gt;
&amp;lt;math&amp;gt;\tilde{M}\to E^* = H_1(M,\mathbb{R})&amp;lt;/math&amp;gt;, which,&lt;br /&gt;
furthermore, descends to a map&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \overline{A}_M: \overline{M}\to E^*,\;\; c\mapsto \left(&lt;br /&gt;
h\mapsto \int_c h \right),&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\overline{M}&amp;lt;/math&amp;gt; is the universal free abelian cover.&lt;br /&gt;
&lt;br /&gt;
Definition. The Jacobi variety (Jacobi torus) of &amp;lt;math&amp;gt;M&amp;lt;/math&amp;gt; is the&lt;br /&gt;
torus&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;J_1(M)=H_1(M,\mathbb{R})/H_1(M,\mathbb{Z})_\mathbb{R}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Definition.  The &amp;#039;&amp;#039;Abel–Jacobi map&amp;#039;&amp;#039;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;A_M: M \to J_1(M),&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
is obtained from the map above by passing to quotients.&lt;br /&gt;
&lt;br /&gt;
The Abel–Jacobi map is unique up to translations of the Jacobi torus.  The map has applications in [[Systolic geometry]].&lt;br /&gt;
&lt;br /&gt;
==Abel–Jacobi theorem==&lt;br /&gt;
&lt;br /&gt;
The following theorem was proved by Abel: Suppose that&lt;br /&gt;
: &amp;lt;math&amp;gt;D = \sum_i n_i p_i\ &amp;lt;/math&amp;gt;&lt;br /&gt;
is a divisor (meaning a formal integer-linear combination of points of &amp;#039;&amp;#039;C&amp;#039;&amp;#039;).  We can define&lt;br /&gt;
: &amp;lt;math&amp;gt;u(D) = \sum_i n_i u(p_i)\ &amp;lt;/math&amp;gt;&lt;br /&gt;
and therefore speak of the value of the Abel–Jacobi map on divisors.  The theorem is then that if &amp;#039;&amp;#039;D&amp;#039;&amp;#039; and &amp;#039;&amp;#039;E&amp;#039;&amp;#039; are two &amp;#039;&amp;#039;effective&amp;#039;&amp;#039; divisors, meaning that the &amp;lt;math&amp;gt;n_i&amp;lt;/math&amp;gt; are all positive integers, then&lt;br /&gt;
: &amp;lt;math&amp;gt;u(D) = u(E)\ &amp;lt;/math&amp;gt; if and only if &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt; is [[linearly equivalent]] to &amp;lt;math&amp;gt;E.&amp;lt;/math&amp;gt; This implies that the Abel–Jacobi map induces an injective map (of abelian groups) from the space of divisor classes of degree zero to the Jacobian.&lt;br /&gt;
Jacobi proved that this map is also surjective, so the two groups are naturally isomorphic. &lt;br /&gt;
&lt;br /&gt;
The Abel–Jacobi theorem implies that the  [[Albanese variety]] of a compact complex curve (dual of holomorphic 1-forms modulo periods) is isomorphic to its [[Jacobian variety]] (divisors of degree 0 modulo equivalence).  For higher dimensional  compact projective varieties the Albanese variety and the Picard variety are dual but need not be isomorphic.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*{{cite book&lt;br /&gt;
 | author = E. Arbarello&lt;br /&gt;
 | coauthors = M. Cornalba, P. Griffiths, J. Harris&lt;br /&gt;
 | title = Geometry of Algebraic Curves, Vol. 1&lt;br /&gt;
 | year = 1985&lt;br /&gt;
 | series = Grundlehren der Mathematischen Wissenschaften&lt;br /&gt;
 | publisher = [[Springer-Verlag]]&lt;br /&gt;
 | isbn = 978-0-387-90997-4&lt;br /&gt;
 | chapter = 1.3, &amp;#039;&amp;#039;Abel&amp;#039;s Theorem&amp;#039;&amp;#039;&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
{{Algebraic curves navbox}}&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Abel-Jacobi map}}&lt;br /&gt;
[[Category:Algebraic curves]]&lt;br /&gt;
[[Category:Riemannian geometry]]&lt;br /&gt;
[[Category:Niels Henrik Abel]]&lt;/div&gt;</summary>
		<author><name>en&gt;RockMagnetist</name></author>
	</entry>
</feed>