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Rv. No, I believe it is actually power per unit wavelength. Imagine the total power being divided up into "bins" by wavelength (eg. 1 nm wide bins).
 
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In [[mathematics]], '''monodromy''' is the study of how objects from [[mathematical analysis]], [[algebraic topology]] and [[algebraic geometry|algebraic]] and [[differential geometry]] behave as they 'run round' a [[Mathematical singularity|singularity]]. As the name implies, the fundamental meaning  of ''monodromy'' comes from 'running round singly'. It is closely associated with [[covering map]]s and their degeneration into [[ramification]]; the aspect giving rise to monodromy phenomena is that certain [[function (mathematics)|function]]s we may wish to define fail to be ''single-valued'' as we 'run round' a path encircling a singularity. The failure of monodromy is best measured by defining a '''monodromy group''': a [[group (mathematics)|group]] of transformations acting on the data that encodes what does happen as we 'run round'.
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==Definition==
Let ''X'' be a connected and [[locally connected]] based [[topological space]] with base point ''x'', and let <math>p:\tilde{X}\to X</math> be a [[covering map|covering]] with [[Fiber_(mathematics)|fiber]] <math>F = p^{-1}(x)</math>. For a loop γ: [0, 1] → ''X'' based at ''x'', denote a [[homotopy lifting property|lift]] under the covering map (starting at a point <math>\tilde{x}\in F</math>) by <math>\tilde{\gamma}</math>. Finally, we denote by <math>\tilde{x}\cdot\gamma</math> the endpoint <math>\tilde{\gamma}(1)</math>, which is generally different from <math>\tilde{x}</math>. There are theorems which state that this construction gives a well-defined [[group action]] of the [[fundamental group]] π<sub>1</sub>(''X'', ''x'') on ''F'', and that the [[stabilizer (group theory)|stabilizer]] of <math>\tilde{x}</math> is exactly <math>p_{*}(\pi_1(\tilde{X},\tilde{x}))</math>, that is, an element [γ] fixes a point in ''F'' if and only if it is represented by the image of a loop in <math>\tilde{X}</math> based at <math>\tilde{x}</math>. This action is called the '''monodromy action''' and the corresponding [[group homomorphism|homomorphism]] π<sub>1</sub>(''X'', ''x'') → Aut(''F'') into the [[automorphism group]] on ''F'' is the '''monodromy'''. The image of this homomorphism is the '''monodromy group'''.
 
==Example==
These ideas were first made explicit in [[complex analysis]]. In the process of [[analytic continuation]], a function that is an [[analytic function]] ''F''(''z'') in some open subset ''E'' of the punctured complex plane '''C''' \ {0} may be continued back into ''E'', but with different values. For example take
 
::''F''(''z'') = log ''z''
::''E'' = {''z'' ∈ '''C''':  Re(''z'') > 0}
 
then analytic continuation anti-clockwise round the circle
 
::|''z''| = 0.5
 
will result in the return, not to ''F''(''z'') but
 
::''F''(''z'')+2&pi;''i''.
 
In this case the monodromy group is [[infinite cyclic]] and the covering space is the universal cover of the punctured complex plane. This cover can be visualized as the [[helicoid]] (as defined in the helicoid article) restricted to ρ > 0. The covering map is a vertical projection, in a sense collapsing the spiral in the obvious way to get a punctured plane.
 
==Differential equations in the complex domain==
One important application is to [[differential equation]]s, where a single solution may give further linearly independent solutions by [[analytic continuation]]. Linear differential equations defined in an open, connected set ''S'' in the complex plane have a monodromy group, which (more precisely) is a [[linear representation]] of the [[fundamental group]] of ''S'', summarising all the analytic continuations round loops within ''S''. The inverse problem, of constructing the equation (with [[regular singularity|regular singularities]]), given a representation, is called the [[Riemann–Hilbert problem]].
 
For a regular (and in particular Fuchsian) linear system one usually chooses as generators of the monodromy group the operators ''M<sub>j</sub>'' corresponding to loops each of which circumvents just one of the poles of the system counterclockwise. If the indices ''j'' are chosen in such a way that they increase from 1 to ''p'' + 1 when one circumvents the base point clockwise, then the only relation between the generators is the equality <math>M_1...M_{p+1}=id</math>. The [[Deligne–Simpson problem]] is the following realisation problem: For which tuples of conjugacy classes in GL(''n'', '''C''') do there exist irreducible tuples of matrices ''M<sub>j</sub>'' from these classes satisfying the above relation? The problem has been formulated by [[Pierre Deligne]] and [[Carlos Simpson]] was the first to obtain results towards its resolution. An additive version of the problem about residua of Fuchsian systems has been formulated and explored by [[Vladimir Kostov]]. The problem has been considered by other authors for matrix groups other than GL(''n'', '''C''') as well.<ref>{{Citation|author=V.P. Kostov|title=The Deligne–Simpson problem — a survey|journal=J. Algebra|volume=281|year=2004|issue=1|pages=83–108|mr=2091962}} and the references therein.</ref>
 
==Topological and geometric aspects==
In the case of a covering map, we look at it as a special case of a [[fibration]], and use the [[homotopy lifting property]] to 'follow' paths on the base space ''X'' (we assume it [[path-connected]] for simplicity) as they are lifted up into the cover ''C''. If we follow round a loop based at ''x'' in ''X'', which we lift to start at ''c'' above ''x'', we'll end at some ''c*'' again above ''x''; it is quite possible that ''c'' ≠ ''c*'', and to code this one considers the action of the [[fundamental group]] π<sub>1</sub>(''X'', ''x'') as a [[permutation group]] on the set of all ''c'', as a '''monodromy group''' in this context.
 
In differential geometry, an analogous role is played by [[parallel transport]]. In a [[principal bundle]] ''B'' over a [[smooth manifold]] ''M'', a [[connection (mathematics)|connection]] allows 'horizontal' movement from fibers above ''m'' in ''M'' to adjacent ones. The effect when applied to loops based at ''m'' is to define a '''[[holonomy]]''' group of translations of the fiber at ''m''; if the structure group of ''B'' is ''G'', it is a subgroup of ''G'' that measures the deviation of ''B'' from the product bundle ''M'' × ''G''.
 
===Monodromy groupoid and foliations===
Analogous to the [[Fundamental group#Fundamental groupoid|fundamental groupoid]] it is possible to get rid of the choice of a base point and to define a monodromy groupoid.  Here we consider (homotopy classes of) lifts of paths in the base space ''X'' of a fibration <math>p:\tilde X\to X</math>.  The result has the structure of a [[groupoid]] over the base space ''X''.  The advantage is that we can drop the condition of connectedness of ''X''.
 
Moreover the construction can also be generalized to [[foliation]]s:  Consider <math>(M,\mathcal{F})</math> a (possibly singular) foliation of ''M''.  Then for every path in a leaf of <math>\mathcal{F}</math> we can consider its induced diffeomorphism on local [[foliation#transversal section|transversal section]]s through the endpoints. Within a simply connected chart this diffeomorphism becomes unique and especially canonical between different transversal sections if we go over to the [[Germ (mathematics)|germ]] of the diffeomorphism around the endpoints. In this way it also becomes independent of the path (between fixed endpoints) within a simply connected chart and is therefore invariant under homotopy.
 
==Definition via Galois theory==
Let '''F'''(''x'') denote the field of the [[rational function]]s in the variable ''x'' over the [[field (mathematics)|field]] '''F''', which is the [[field of fractions]] of the [[polynomial ring]] '''F'''[''x'']. An element ''y'' = ''f''(''x'') of '''F'''(''x'') determines a finite [[field extension]] ['''F'''(''x'') : '''F'''(''y'')].
 
This extension is generally not Galois but has [[Galois closure]] ''L''(''f''). The associated [[Galois group]] of the extension [''L''(''f'') : '''F'''(''y'')] is called the monodromy group of the ''f''.  
 
In the case of '''F''' = '''C''' [[Riemann surface]] theory enters and allows for the geometric interpretation given above. In the case that the extension ['''C'''(''x'') : '''C'''(''y'')] is already Galois, the associated monodromy group is sometimes called a [[Covering map|group of deck transformations]]. 
 
This has connections with the [[Grothendieck's Galois theory|Galois theory of covering spaces]] leading to the [[Riemann existence theorem]].
 
==See also==
* [[Braid group]]
* [[Monodromy theorem]]
* [[Mapping class group]] (of a punctured disk)
 
==References==
{{Reflist}}
*{{springer|author=V.I. Danilov|title=Monodromy|id=M/m064700}}
*{{planetmath reference|id=4000|title=Monodromy}}
 
[[Category:Mathematical analysis]]
[[Category:Complex analysis]]
[[Category:Differential geometry]]
[[Category:Algebraic topology]]
[[Category:Homotopy theory]]

Latest revision as of 14:29, 30 October 2014

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