Algebraic equation: Difference between revisions

Revision as of 17:44, 10 January 2014

In ring theory and related areas of mathematics a central simple algebra (CSA) over a field K is a finite-dimensional associative algebra A, which is simple, and for which the center is exactly K. In other words, any simple algebra is a central simple algebra over its center.

For example, the complex numbers C form a CSA over themselves, but not over the real numbers R (the center of C is all of C, not just R). The quaternions H form a 4 dimensional CSA over R, and in fact represent the only non-trivial element of the Brauer group of the reals (see below).

Given two central simple algebras A ~ M(n,S) and B ~ M(m,T) over the same field F, A and B are called similar (or Brauer equivalent) if their division rings S and T are isomorphic. The set of all equivalence classes of central simple algebras over a given field F, under this equivalence relation, can be equipped with a group operation given by the tensor product of algebras. The resulting group is called the Brauer group Br(F) of the field F.^[1] It is always a torsion group.^[2]

Properties

According to the Artin–Wedderburn theorem a finite-dimensional simple algebra A is isomorphic to the matrix algebra M(n,S) for some division ring S. Hence, there is a unique division algebra in each Brauer equivalence class.^[3]
Every automorphism of a central simple algebra is an inner automorphism (follows from Skolem–Noether theorem).
The dimension of a central simple algebra as a vector space over its centre is always a square: the degree is the square root of this dimension. The Schur index of a central simple algebra is the degree of the equivalent division algebra:^[4] it depends only on the Brauer class of the algebra.^[5]
The period of a central simple algebra is the order of its Brauer class as an element of the Brauer group. It is a divisor of the index, and the two numbers are composed of the same prime factors.^[6]
If S is a simple subalgebra of a central simple algebra A then dim_F S divides dim_F A.
Every 4-dimensional central simple algebra over a field F is isomorphic to a quaternion algebra; in fact, it is either a two-by-two matrix algebra, or a division algebra.
If D is a central division algebra over K for which the index has prime factorisation

i n d (D) = \prod_{i = 1}^{r} p_{i}^{m_{i}}

then D has a tensor product decomposition

D = \otimes_{i = 1}^{r} D_{i}

where each component D_i is a central division algebra of index

p_{i}^{m_{i}}

, and the components are uniquely determined up to isomorphism.^[7]

Splitting field

We call a field E a splitting field for A over K if A⊗E is isomorphic to a matrix ring over E. Every finite dimensional CSA has a splitting field: indeed, in the case when A is a division algebra, then a maximal subfield of A is a splitting field. In general there is a splitting field which is a separable extension of K of degree equal to the index of A, and this splitting field is isomorphic to a subfield of A.^[8] As an example, the field C splits the quaternion algebra H over R with

t + x i + y j + z k \leftrightarrow (\begin{array}{c} t + x i & y + z i \\ - y + z i & t - x i \end{array}) .

We can use the existence of the splitting field to define reduced norm and reduced trace for a CSA A.^[9] Map A to a matrix ring over a splitting field and define the reduced norm and trace to be the composite of this map with determinant and trace respectively. For example, in the quaternion algebra H, the splitting above shows that the element t + x i + y j + z k has reduced norm t² + x² + y² + z² and reduced trace 2t.

The reduced norm is multiplicative and the reduced trace is additive. An element a of A is invertible if and only if its reduced norm in non-zero: hence a CSA is a division algebra if and only if the reduced norm is non-zero on the non-zero elements.^[10]

Generalization

CSAs over a field K are a non-commutative analog to extension fields over K – in both cases, they have no non-trivial 2-sided ideals, and have a distinguished field in their center, though a CSA can be non-commutative and need not have inverses (need not be a division algebra). This is of particular interest in noncommutative number theory as generalizations of number fields (extensions of the rationals Q); see noncommutative number field.

References

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+In [[ring theory]] and related areas of [[mathematics]] a '''central simple algebra''' ('''CSA''') over a [[field (mathematics)|field]] ''K'' is a finite-dimensional [[associative algebra]] ''A'', which is [[simple algebra|simple]], and for which the [[center of an algebra|center]] is exactly ''K''. In other words, any simple algebra is a central simple algebra over its center.
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+For example, the [[complex number]]s '''C''' form a CSA over themselves, but not over the [[real number]]s '''R''' (the center of '''C''' is all of '''C''', not just '''R'''). The [[quaternion]]s '''H''' form a 4 dimensional CSA over '''R''', and in fact represent the only non-trivial element of the [[Brauer group]] of the reals (see below).
+Given two central simple algebras ''A'' ~ ''M''(''n'',''S'') and ''B'' ~ ''M''(''m'',''T'') over the same field ''F'', ''A'' and ''B'' are called ''similar'' (or ''[[Brauer equivalent]]'') if their division rings ''S'' and ''T'' are isomorphic. The set of all [[equivalence class]]es of central simple algebras over a given field ''F'', under this equivalence relation, can be equipped with a [[group operation]] given by the [[tensor product of algebras]]. The resulting group is called the [[Brauer group]] Br(''F'') of the field ''F''.<ref name=L159>Lorenz (2008) p.159</ref>  It is always a [[torsion group]].<ref name=L194>Lorenz (2008) p.194</ref>
+== Properties ==
+* According to the [[Artin–Wedderburn theorem]] a finite-dimensional simple algebra ''A'' is isomorphic to the matrix algebra [[matrix ring|''M''(''n'',''S'')]] for some [[division ring]] ''S''. Hence, there is a unique division algebra in each Brauer equivalence class.<ref name=L160>Lorenz (2008) p.160</ref>
+* Every [[automorphism]] of a central simple algebra is an [[inner automorphism]] (follows from [[Skolem–Noether theorem]]).
+* The dimension of a central simple algebra as a vector space over its centre is always a square: the ''degree'' is the square root of this dimension.  The '''Schur index''' of a central simple algebra is the degree of the equivalent division algebra:<ref name=L163>Lorenz (2008) p.163</ref> it depends only on the [[Brauer class]] of the algebra.<ref name=GS100>Gille & Szamuely (2006) p.100</ref>
+* The ''period'' of a central simple algebra is the order of its Brauer class as an element of the Brauer group.  It is a divisor of the index, and the two numbers are composed of the same prime factors.<ref name=GS104>Gille & Szamuely (2006) p.104</ref>
+* If ''S'' is a simple [[subalgebra]] of a central simple algebra ''A'' then dim<sub>''F''</sub>&nbsp;''S'' divides dim<sub>''F''</sub>&nbsp;''A''.
+* Every 4-dimensional central simple algebra over a field ''F'' is isomorphic to a [[quaternion algebra]]; in fact, it is either a two-by-two [[matrix algebra]], or a [[division algebra]].
+* If ''D'' is a central division algebra over ''K'' for which the index has prime factorisation
+::<math>\mathrm{ind}(D) = \prod_{i=1}^r p_i^{m_i} \ </math>
+:then ''D'' has a tensor product decomposition
+::<math>D = \otimes_{i=1}^r D_i \ </math>
+:where each component ''D''<sub>''i''</sub> is a central division algebra of index <math>p_i^{m_i}</math>, and the components are uniquely determined up to isomorphism.<ref name=GS105>Gille & Szamuely (2006) p.105</ref>
+==Splitting field==
+We call a field ''E'' a ''splitting field'' for ''A'' over ''K'' if ''A''⊗''E'' is isomorphic to a matrix ring over ''E''.  Every finite dimensional CSA has a splitting field: indeed, in the case when ''A'' is a division algebra, then a maximal subfield of ''A'' is a splitting field.  In general there is a splitting field which is a [[separable extension]] of ''K'' of degree equal to the index of ''A'', and this splitting field is isomorphic to a subfield of ''A''.<ref name=GS101>Gille & Szamuely (2006) p.101</ref>  As an example, the field '''C''' splits the quaternion algebra '''H''' over '''R''' with
+:<math> t + x \mathbf{i} + y \mathbf{j} + z \mathbf{k} \leftrightarrow
+\left({\begin{array}{*{20}c} t + x i & y + z i \\ -y + z i & t - x i \end{array}}\right) . </math>
+We can use the existence of the splitting field to define '''reduced norm''' and '''reduced trace''' for a CSA ''A''.<ref name=GS378>Gille & Szamuely (2006) pp.37-38</ref>  Map ''A'' to a matrix ring over a splitting field and define the reduced norm and trace to be the composite of this map with determinant and trace respectively.  For example, in the quaternion algebra '''H''', the splitting above shows that the element ''t'' + ''x'' '''i''' + ''y'' '''j''' + ''z'' '''k''' has reduced norm ''t''<sup>2</sup> + ''x''<sup>2</sup> + ''y''<sup>2</sup> + ''z''<sup>2</sup> and reduced trace 2''t''.
+The reduced norm is multiplicative and the reduced trace is additive.  An element ''a'' of ''A'' is invertible if and only if its reduced norm in non-zero: hence a CSA is a division algebra if and only if the reduced norm is non-zero on the non-zero elements.<ref name=GS38>Gille & Szamuely (2006) p.38</ref>
+== Generalization ==
+CSAs over a field ''K'' are a non-commutative analog to [[extension field]]s over ''K'' – in both cases, they have no non-trivial 2-sided ideals, and have a distinguished field in their center, though a CSA can be non-commutative and need not have inverses (need not be a [[division algebra]]). This is of particular interest in [[noncommutative number theory]] as generalizations of [[number field]]s (extensions of the rationals '''Q'''); see [[noncommutative number field]].
+== See also ==
+* [[Azumaya algebra]], generalization of CSAs where the base field is replaced by a commutative local ring
+* [[Severi–Brauer variety]]
+==References==
+{{reflist}}
+* {{cite book | title=Further Algebra and Applications | first=P.M. | last=Cohn | authorlink=Paul Cohn | edition=2nd | publisher=Springer | year=2003 | isbn=1852336676 | zbl=1006.00001 }}
+* {{cite book | title=Introduction to Quadratic Forms over Fields | volume=67 | series=Graduate Studies in Mathematics | first=Tsit-Yuen | last=Lam | publisher=American Mathematical Society | year=2005 | isbn=0-8218-1095-2 | zbl=1068.11023 | mr = 2104929 }}
+* {{cite book | first=Falko | last=Lorenz | title=Algebra.  Volume II: Fields with Structure, Algebras and Advanced Topics | year=2008 | publisher=Springer | isbn=978-0-387-72487-4 | zbl=1130.12001 }}
+===Further reading===
+* {{cite book | title=Structure of Algebras | volume=24 | series=Colloquium Publications | first=A.A. | last=Albert | authorlink=Abraham Adrian Albert | edition=7th revised reprint | publisher=American Mathematical Society | year=1939 | isbn=0-8218-1024-3 | zbl=0023.19901 }}
+* {{cite book | last1=Gille | first1=Philippe | last2=Szamuely | first2=Tamás | title=Central simple algebras and Galois cohomology | series=Cambridge Studies in Advanced Mathematics | volume=101 | location=Cambridge | publisher=[[Cambridge University Press]] | year=2006 | isbn=0-521-86103-9 | zbl=1137.12001 }}
+[[Category:Algebras]]
+[[Category:Ring theory]]

Algebraic equation: Difference between revisions

Revision as of 17:44, 10 January 2014

Contents

Properties

Splitting field

Generalization

See also

References

Further reading

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Algebraic equation: Difference between revisions

Revision as of 17:44, 10 January 2014

Properties

Splitting field

Generalization

See also

References

Further reading

Navigation menu

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