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Difference between revisions of "Normal form (for singularities)"

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Any equivalence relation $\sim$ on a set of objects $\mathscr M$ defines the [[quotient set]] $\mathscr M/\sim$ whose elements are equivalence classes: the equivalence class of an element $M\in\mathscr M$ is denoted $[M]=\{M'\in\mathscr M:~M'\sim M\}$. Description of the quotient set is referred to as the ''classification problem'' for $\mathscr M$ with respect to the equivalence relation. The ''normal form'' of an object $M$ is a "selected representative" from the class $[M]$, usually possessing some nice properties (simplicity, integrability etc). Often (although not always) one requires that two ''distinct'' representatives ("normal forms") are ''not equivalent'' to each other: $M_1\ne M_2\iff M_1\not\sim M_2$.
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#REDIRECT [[Normal form]]
 
 
The most typical classification problems appear when there is a group $G$ acting on $\mathscr M$: then the natural equivalence relation arises, $M_1\sim M_2\iff \exists g\in G:~g\cdot M_1=M_2$. If both $\mathscr M$ and $G$ are finite-dimensional spaces, the classification problem is usually much easier than in the case of infinite-dimensional spaces.
 
 
 
Below  follows a list (very partial) of the most important classification problems in which normal forms are known and very useful.
 
 
 
==Finite-dimensional classification problems==
 
When  the objects of classification form a finite-dimensional variety, in  most cases it is a subvariety of matrices, with the equivalence relation  induced by transformations reflecting the change of basis.
 
===Linear maps between finite-dimensional linear spaces===
 
Let $\Bbbk$ be a field. A  linear map from $\Bbbk^m$ to $\Bbbk^n$ is represented by an $n\times m$  matrix over $\Bbbk$ ($m$ rows and $n$ columns). A different choice of  bases in the source and the target space results in a matrix $M$ being  replaced by another matrix $M'=HML$, where $H$ (resp., $L$) is an  ''invertible'' $m\times m$ (resp., $n\times n$) matrix of transition  between the bases,
 
$$
 
M\sim M'\iff\exists H\in\operatorname{GL}(m,\Bbbk),\ L\in \operatorname{GL}(n,\Bbbk):\quad M'=HML.
 
\tag{LR}
 
$$
 
 
 
Obviously,  this binary relation $\sim$ is an equivalence (symmetric, reflexive and  transitive), called ''left-right linear equivalence''. Each matrix $M$  is left-right equivalent to a matrix (of the same size) with  $k\leqslant\min(n,m)$ units on the diagonal and zeros everywhere else.  The number $k$ is a complete invariant of equivalence (matrices of  different ranks are not equivalent) and is called the [[rank]] of a  matrix.
 
 
 
A similar question may be posed about homomorphisms of finitely generated modules over rings. For some rings the normal form is known as the [[Normal_form_(for_matrices)#The_Smith_normal_form|Smith normal form]].
 
===Linear operators (self-maps)===
 
The  matrix of a linear operator of an $n$-dimensional space over $\Bbbk$  ''into itself'' is transformed by a change of basis in a more  restrictive way compared to (LR): if the source and the target spaces coincide, then necessarily $n=m$ and  $L=H^{-1}$. The  corresponding equivalence is called [[similarity]] (sometimes ''conjugacy'' or ''linear conjugacy'') of matrices,  and the normal form is known as the [[Jordan normal form]], see also [[Normal_form_(for_matrices)#The_Jordan_normal_form here]]. This normal form is characterized by a specific block diagonal structure and explicitly features the [[Eigen value|eigenvalues]] on the  diagonal. Note that this form holds only over an algebraically closed  field $\Bbbk$, e.g., $\Bbbk=\CC$.
 
===Quadrics in linear spaces===
 
A  quadratic form $Q\colon\Bbbk^n\Bbbk$, $(x_1,\dots,x_n)\mapsto \sum  a_{i,j}^n a_{ij}x_ix_j$ with a symmetric matrix $Q$ after a ''linear  invertible'' change of coordinates will have a new matrix $Q'=HQH^*$  (the asterisk means the transpose):
 
$$
 
Q'\sim Q\iff \exists H\in\operatorname{GL}(n,\Bbbk):\ Q'=HQH^*.\tag{QL}
 
$$
 
The normal form for this equivalence is diagonal, but the diagonal entries depend on the field:
 
*  Over $\RR$, the diagional entries can be all made $0$ or $\pm 1$. The  number of entries of each type is an invariant of classification, called  (or closely related) to the [[inertia index]].
 
* Over $\CC$, one  can keep only zeros and units (not signed). The number of units is  called the [[rank]] of a quadratic form; it is a complete invariant.
 
===Quadrics in Euclidean spaces===
 
This  classification deals with real symmetric matrices representing  quadratic forms, yet the condition (QL) is represented by a more  restrictive condition that the conjugacy matrix $H$ is orthogonal  (preserves the Euclidean scalar product):
 
$$
 
Q'\sim Q\iff \exists H\in\operatorname{O}(n,\RR)=\{H\in\operatorname{GL}(n,\RR):\ HH^*=E\}:\ Q'=HQH^*.\tag{QE}
 
$$
 
The normal form is diagonal, with the diagonal entries forming a complete system of invariants.
 
 
 
A similar set of normal forms exists for self-adjoint matrices conjugated by Hermitian matrices.
 
===Quadrics in the projective plane===
 
==Infinite-dimensional classification problems==
 

Latest revision as of 14:58, 22 April 2012

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Normal form (for singularities). Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Normal_form_(for_singularities)&oldid=24844