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{{Lie groups}}
{{Lie groups}}


In [[mathematics]], a [[Lie algebra]] <math>\mathfrak{g}</math> is '''solvable''' if its [[derived series]] terminates in the zero subalgebra. The ''derived Lie algebra'' is the subalgebra of <math>\mathfrak{g}</math>, denoted
In [[mathematics]], a [[Lie algebra]] <math>\mathfrak{g}</math> is '''solvable''' if its derived series terminates in the zero subalgebra. The ''derived Lie algebra'' of the Lie algebra <math>\mathfrak{g}</math> is the subalgebra of <math>\mathfrak{g}</math>, denoted


:<math>[\mathfrak{g},\mathfrak{g}]</math>
:<math>[\mathfrak{g},\mathfrak{g}]</math>


that consists of all linear combinations of [[Lie bracket]]s of pairs of elements of <math>\mathfrak{g}</math>. The derived series is the sequence of subalgebras
that consists of all linear combinations of [[Lie bracket]]s of pairs of elements of <math>\mathfrak{g}</math>. The ''derived series'' is the sequence of subalgebras


:<math> \mathfrak{g} \geq [\mathfrak{g},\mathfrak{g}] \geq [[\mathfrak{g},\mathfrak{g}],[\mathfrak{g},\mathfrak{g}]] \geq [[[\mathfrak{g},\mathfrak{g}],[\mathfrak{g},\mathfrak{g}]],[[\mathfrak{g},\mathfrak{g}],[\mathfrak{g},\mathfrak{g}]]] \geq ...</math>
:<math> \mathfrak{g} \geq [\mathfrak{g},\mathfrak{g}] \geq [[\mathfrak{g},\mathfrak{g}],[\mathfrak{g},\mathfrak{g}]] \geq [[[\mathfrak{g},\mathfrak{g}],[\mathfrak{g},\mathfrak{g}]],[[\mathfrak{g},\mathfrak{g}],[\mathfrak{g},\mathfrak{g}]]] \geq ...</math>


If the derived series eventually arrives at the zero subalgebra, then the Lie algebra is solvable.<ref name=Humphreys_1>{{harvnb|Humphreys|1972}}</ref> The derived series for Lie algebras is analogous to the derived series for [[commutator subgroup]]s in [[group theory]].
If the derived series eventually arrives at the zero subalgebra, then the Lie algebra is called solvable.<ref name=Humphreys_1>{{harvnb|Humphreys|1972}}</ref> The derived series for Lie algebras is analogous to the [[derived series]] for [[commutator subgroup]]s in [[group theory]], and solvable Lie algebras are analogs of [[solvable group]]s.


Any [[nilpotent Lie algebra]] is [[a fortiori]] solvable but the converse is not true. The solvable Lie algebras and the [[semisimple Lie algebra]]s form two large and generally complementary classes, as is shown by the [[Levi decomposition]].
Any [[nilpotent Lie algebra]] is [[a fortiori]] solvable but the converse is not true. The solvable Lie algebras and the [[semisimple Lie algebra]]s form two large and generally complementary classes, as is shown by the [[Levi decomposition]]. The solvable Lie algebras are precisely those that can be obtained from [[Lie algebra extension|semidirect products]], starting from 0 and adding one dimension at a time.<ref name="Knapp_1"/>


A maximal solvable subalgebra is called a [[Borel subalgebra]]. The largest solvable [[ideal (Lie algebra)|ideal]] of a Lie algebra is called the [[Radical of Lie algebra|radical]].
A maximal solvable subalgebra is called a [[Borel subalgebra]]. The largest solvable [[ideal (Lie algebra)|ideal]] of a Lie algebra is called the [[Radical of Lie algebra|radical]].
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*:<math>\mathfrak{g} = \mathfrak{g}_0 \supset \mathfrak{g}_1 \supset ... \mathfrak{g}_r = 0,</math>
*:<math>\mathfrak{g} = \mathfrak{g}_0 \supset \mathfrak{g}_1 \supset ... \mathfrak{g}_r = 0,</math>
:such that <math>\mathfrak{g}_{i+1}</math> is an ideal in <math>\mathfrak{g}_i</math> and <math>\mathfrak{g}_i/\mathfrak{g}_{i+1}</math> is abelian.<ref name= Fulton_1>{{harvnb|Fulton|Harris|1991}}</ref>
:such that <math>\mathfrak{g}_{i+1}</math> is an ideal in <math>\mathfrak{g}_i</math> and <math>\mathfrak{g}_i/\mathfrak{g}_{i+1}</math> is abelian.<ref name= Fulton_1>{{harvnb|Fulton|Harris|1991}}</ref>
*(vii) <math>\mathfrak{g}</math> is solvable if and only if its [[Killing form]] <math>B</math> satisfies <math>B(X,Y)=0</math> for all {{mvar|X}} in <math>\mathfrak{g}</math> and {{mvar|Y}} in <math>[\mathfrak{g}, \mathfrak{g}]</math>.<ref>{{harvnb|Knapp|2002}} Proposition 1.46.</ref> This is [[Cartan's criterion#Cartan's criterion for solvability|Cartan's criterion for solvability]].
*(vii) The [[Killing form]] <math>B</math> of <math>\mathfrak{g}</math> satisfies <math>B(X,Y)=0</math> for all {{mvar|X}} in <math>\mathfrak{g}</math> and {{mvar|Y}} in <math>[\mathfrak{g}, \mathfrak{g}]</math>.<ref>{{harvnb|Knapp|2002}} Proposition 1.46.</ref> This is [[Cartan's criterion#Cartan's criterion for solvability|Cartan's criterion for solvability]].


== Properties ==
== Properties ==
[[Lie's Theorem]] states that if <math>V</math> is a finite-dimensional vector space over an algebraically closed field <math>K</math> of [[Characteristic (field theory)|characteristic zero]], and <math>\mathfrak{g}</math> is a solvable linear Lie algebra over a subfield <math>k</math> of <math>K</math>, and if <math>\pi</math> is a '''representation''' of <math>\mathfrak{g}</math> over <math>V</math>, then there exists a simultaneous [[eigenvector]] <math>v \in V</math> of the matrices <math>\pi(X)</math> for all elements <math>X \in \mathfrak{g}</math>. More generally, the result holds if all [[eigenvalue]]s of <math>\pi(X)</math> lie in <math>K</math> for all <math>X \in \mathfrak{g}</math>.<ref>{{harvnb|Knapp|2002}} Theorem 1.25.</ref>
[[Lie's Theorem]] states that if <math>V</math> is a finite-dimensional vector space over an algebraically closed field of [[Characteristic (field theory)|characteristic zero]], and <math>\mathfrak{g}</math> is a solvable Lie algebra, and if <math>\pi</math> is a [[Lie algebra representation|representation]] of <math>\mathfrak{g}</math> over <math>V</math>, then there exists a simultaneous [[eigenvector]] <math>v \in V</math> of the endomorphisms <math>\pi(X)</math> for all elements <math>X \in \mathfrak{g}</math>.<ref>{{harvnb|Knapp|2002}} Theorem 1.25.</ref>


*Every Lie subalgebra, quotient and extension{{what|reason=By a solvable Lie algebra?|date=October 2015}} of a solvable [[Lie algebra]] is solvable.
*Every Lie subalgebra and quotient of a solvable Lie algebra are solvable.<ref name="Serre def">{{harvnb|Serre|2001|loc=Ch. I, § 6, Definition 2.}}</ref>
*Given a Lie algebra <math>\mathfrak g</math> and an ideal <math>\mathfrak h</math> in it,
*A solvable nonzero Lie algebra has a nonzero abelian ideal, the last nonzero term in the derived series.<ref name=Knapp_1/>
*:<math>\mathfrak{g}</math> is solvable if and only if both <math>\mathfrak h</math> and <math>\mathfrak{g}/\mathfrak h</math> are solvable.<ref name="Serre def" /><ref name=Knapp_1/>
*A homomorphic image of a solvable Lie algebra is solvable.<ref name=Knapp_1>{{harvnb|Knapp|2002}}</ref>
:The analogous statement is true for nilpotent Lie algebras provided <math>\mathfrak h</math> is contained in the center. Thus, an extension of a solvable algebra by a solvable algebra is solvable, while a ''central'' extension of a nilpotent algebra by a nilpotent algebra is nilpotent.
*If <math>\mathfrak{a}</math> is a solvable ideal in <math>\mathfrak{g}</math> and <math>\mathfrak{g}/\mathfrak{a}</math> is solvable, then <math>\mathfrak{g}</math> is solvable.<ref name=Knapp_1/>
*A solvable nonzero Lie algebra has a nonzero abelian ideal, the last nonzero term in the derived series.<ref name=Knapp_1>{{harvnb|Knapp|2002}}</ref>
*If <math>\mathfrak{g}</math> is finite-dimensional, then there is a unique solvable ideal <math>\mathfrak{r} \sub \mathfrak{g}</math> containing all solvable ideals in <math>\mathfrak{g}</math>. This ideal is the '''radical''' of <math>\mathfrak{g}</math>, denoted <math>{\rm rad} \mathfrak{g}</math>.<ref name=Knapp_1/>
*If <math>\mathfrak{a}, \mathfrak{b} \sub \mathfrak{g}</math> are solvable ideals, then so is <math>\mathfrak{a} + \mathfrak{b}</math>.<ref name=Humphreys_1/>
* If <math>\mathfrak{a}, \mathfrak{b} \sub \mathfrak{g}</math> are solvable ideals, then so is <math>\mathfrak{a} + \mathfrak{b}</math>.<ref name=Humphreys_1/> Consequently, if <math>\mathfrak{g}</math> is finite-dimensional, then there is a unique solvable ideal <math>\mathfrak{r} \sub \mathfrak{g}</math> containing all solvable ideals in <math>\mathfrak{g}</math>. This ideal is the '''[[radical of a Lie algebra|radical]]''' of <math>\mathfrak{g}</math>.<ref name=Knapp_1/>
*A solvable Lie algebra <math>\mathfrak{g}</math> has a unique largest nilpotent ideal <math>\mathfrak{n}</math>, the set of all <math>X \in \mathfrak{g}</math> such that <math>{\rm ad}_X</math> is nilpotent. If {{mvar|D}} is any derivation of <math>\mathfrak{g}</math>, then <math>D(\mathfrak{g}) \sub \mathfrak{n}</math>.<ref>{{harvnb|Knapp|2002}} Proposition 1.40.</ref>
*A solvable Lie algebra <math>\mathfrak{g}</math> has a unique largest nilpotent ideal <math>\mathfrak{n}</math>, called the [[Nilradical of a Lie algebra|nilradical]], the set of all <math>X \in \mathfrak{g}</math> such that <math>{\rm ad}_X</math> is nilpotent. If {{mvar|D}} is any derivation of <math>\mathfrak{g}</math>, then <math>D(\mathfrak{g}) \sub \mathfrak{n}</math>.<ref>{{harvnb|Knapp|2002}} Proposition 1.40.</ref>


==Completely solvable Lie algebras==
==Completely solvable Lie algebras==


A Lie algebra <math>\mathfrak{g}</math> is called '''completely solvable''' or '''split solvable''' if it has an elementary sequence{{definition|date=October 2015}} of ideals in <math>\mathfrak{g}</math> from <math>0</math> to <math>\mathfrak{g}</math>. A finite-dimensional nilpotent Lie algebra is completely solvable, and a completely solvable Lie algebra is solvable. Over an algebraically closed field a solvable Lie algebra is completely solvable, but the <math>3</math>-dimensional real Lie algebra of the group of Euclidean isometries of the plane is solvable but not completely solvable.
A Lie algebra <math>\mathfrak{g}</math> is called '''completely solvable''' or '''split solvable''' if it has an elementary sequence{(V) As above definition} of ideals in <math>\mathfrak{g}</math> from <math>0</math> to <math>\mathfrak{g}</math>. A finite-dimensional nilpotent Lie algebra is completely solvable, and a completely solvable Lie algebra is solvable. Over an algebraically closed field a solvable Lie algebra is completely solvable, but the <math>3</math>-dimensional real Lie algebra of the group of Euclidean isometries of the plane is solvable but not completely solvable.


A solvable Lie algebra <math>\mathfrak{g}</math> is split solvable if and only if the eigenvalues of <math>{\rm ad}_X</math> are in <math>k</math> for all <math>X</math> in <math>\mathfrak{g}</math>.<ref name=Knapp_1/>
A solvable Lie algebra <math>\mathfrak{g}</math> is split solvable if and only if the eigenvalues of <math>{\rm ad}_X</math> are in <math>k</math> for all <math>X</math> in <math>\mathfrak{g}</math>.<ref name=Knapp_1/>


== Examples ==
== Examples ==

* A [[Semisimple Lie algebra|semisimple]] Lie algebra is never solvable.<ref name=Humphreys_1/>
=== Abelian Lie algebras ===
* Every [[abelian Lie algebra]] is solvable.
Every [[abelian Lie algebra]] <math>\mathfrak{a}</math> is solvable by definition, since its commutator <math>[\mathfrak{a},\mathfrak{a}] = 0</math>. This includes the Lie algebra of diagonal matrices in <math>\mathfrak{gl}(n)</math>, which are of the form<blockquote><math>\left\{ \begin{bmatrix}
* Every [[nilpotent Lie algebra]] is solvable.
* & 0 & 0 \\
* Let <math>\mathfrak{b}_k</math> be the subalgebra of <math>{\rm gl}_k</math> consisting of upper triangular matrices. Then <math>\mathfrak{b}_k</math> is solvable.
0 & * & 0 \\
* Let <math>\mathfrak{g}</math> be the set of matrices on the form
0 & 0 & *
:<math>X = \left(\begin{matrix}0 & \theta & x\\ -\theta & 0 & y\\ 0 & 0 & 0\end{matrix}\right), \quad \theta, x, y \in \mathbb{R}.</math>
\end{bmatrix} \right\}</math></blockquote>for <math>n = 3</math>. The Lie algebra structure on a vector space <math>V</math> given by the trivial bracket <math>[m,n] = 0</math> for any two matrices <math>m,n \in \text{End}(V)</math> gives another example.
:Then <math>\mathfrak{g}</math> is solvable, but not split solvable.<ref name=Knapp_1/> It is isomorphic with the Lie algebra of the group of translations and rotations in the plane.

=== Nilpotent Lie algebras ===
Another class of examples comes from [[nilpotent Lie algebra]]s since the adjoint representation is solvable. Some examples include the upper-diagonal matrices, such as the class of matrices of the form<blockquote><math>\left\{ \begin{bmatrix}
0 & * & * \\
0 & 0 & * \\
0 & 0 & 0
\end{bmatrix} \right\}</math></blockquote>called the Lie algebra of '''strictly upper triangular matrices'''. In addition, the Lie algebra of '''upper diagonal matrices''' in <math>\mathfrak{gl}(n)</math> form a solvable Lie algebra. This includes matrices of the form<blockquote><math>\left\{ \begin{bmatrix}
* & * & * \\
0 & * & * \\
0 & 0 & *
\end{bmatrix} \right\}</math></blockquote>and is denoted <math>\mathfrak{b}_k</math>.

=== Solvable but not split-solvable ===
Let <math>\mathfrak{g}</math> be the set of matrices on the form<blockquote><math>X = \left(\begin{matrix}0 & \theta & x\\ -\theta & 0 & y\\ 0 & 0 & 0\end{matrix}\right), \quad \theta, x, y \in \mathbb{R}.</math></blockquote>Then <math>\mathfrak{g}</math> is solvable, but not split solvable.<ref name="Knapp_1" /> It is isomorphic with the Lie algebra of the group of translations and rotations in the plane.

=== Non-example ===
A [[semisimple Lie algebra]] <math>\mathfrak{l}</math> is never solvable since its [[Radical of a Lie algebra|radical]] <math>\text{Rad}(\mathfrak{l})</math>, which is the largest solvable ideal in <math>\mathfrak{l}</math>, is trivial.<ref name="Humphreys_1" /> <sup>page 11</sup>


==Solvable Lie groups==
==Solvable Lie groups==
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*[[Solvmanifold]]
*[[Solvmanifold]]
*[[Dixmier mapping]]
*[[Dixmier mapping]]

==External links==
*[http://eom.springer.de/l/l058520.htm EoM article ''Lie algebra, solvable'']
*[http://eom.springer.de/l/l058690.htm EoM article ''Lie group, solvable'']


==Notes==
==Notes==
{{reflist}}
{{Reflist}}


==References==
==References==
*{{cite book|ref=harv|last1=Fulton|last2=Harris|first1=W.|first2=J.|year=1991|publisher=Springer-Verlag|location=New York|series=Graduate Texts in Mathematics|volume=129|isbn=978-0-387-97527-6|mr=1153249|authorlink1=William Fulton (mathematician)|authorlink2=Joe Harris (mathematician)|title=Representation theory. A first course}}
*{{cite book|last1=Fulton|last2=Harris|first1=W.|first2=J.|year=1991|publisher=Springer-Verlag|location=New York|series=Graduate Texts in Mathematics|volume=129|isbn=978-0-387-97527-6|mr=1153249|authorlink1=William Fulton (mathematician)|authorlink2=Joe Harris (mathematician)|title=Representation theory. A first course}}
*{{cite book|ref=harv|last=Humphreys|first=James E.|title=Introduction to Lie Algebras and Representation Theory|series=Graduate Texts in Mathematics|volume=9|publisher=Springer-Verlag|location=New York|year=1972|isbn=0-387-90053-5|url-access=registration|url=https://archive.org/details/introductiontoli00jame}}
*{{cite book|last=Humphreys|first=James E.|title=Introduction to Lie Algebras and Representation Theory|series=Graduate Texts in Mathematics|volume=9|publisher=Springer-Verlag|location=New York|year=1972|isbn=0-387-90053-5|url-access=registration|url=https://archive.org/details/introductiontoli00jame}}
*{{cite book|ref=harv|authorlink=A. W. Knapp|last=Knapp|first=A. W.|title=Lie groups beyond an introduction|isbn=0-8176-4259-5|publisher=Birkhäuser|series=Progress in Mathematics|volume=120|edition=2nd|year=2002|location=Boston·Basel·Berlin}}.
*{{cite book|author-link=A. W. Knapp|last=Knapp|first=A. W.|title=Lie groups beyond an introduction|isbn=0-8176-4259-5|publisher=Birkhäuser|series=Progress in Mathematics|volume=120|edition=2nd|year=2002|location=Boston·Basel·Berlin}}.
*{{cite book|first=Jean-Pierre|last=Serre|title=Complex Semisimple Lie Algebras|publisher=Springer|location=Berlin|year=2001|isbn=3-5406-7827-1}}

==External links==
*[https://encyclopediaofmath.org/wiki/Lie_algebra,_solvable EoM article ''Lie algebra, solvable'']
*[https://encyclopediaofmath.org/wiki/Lie_group,_solvable EoM article ''Lie group, solvable'']

{{Authority control}}


[[Category:Properties of Lie algebras]]
[[Category:Properties of Lie algebras]]

Latest revision as of 19:14, 8 August 2024

In mathematics, a Lie algebra is solvable if its derived series terminates in the zero subalgebra. The derived Lie algebra of the Lie algebra is the subalgebra of , denoted

that consists of all linear combinations of Lie brackets of pairs of elements of . The derived series is the sequence of subalgebras

If the derived series eventually arrives at the zero subalgebra, then the Lie algebra is called solvable.[1] The derived series for Lie algebras is analogous to the derived series for commutator subgroups in group theory, and solvable Lie algebras are analogs of solvable groups.

Any nilpotent Lie algebra is a fortiori solvable but the converse is not true. The solvable Lie algebras and the semisimple Lie algebras form two large and generally complementary classes, as is shown by the Levi decomposition. The solvable Lie algebras are precisely those that can be obtained from semidirect products, starting from 0 and adding one dimension at a time.[2]

A maximal solvable subalgebra is called a Borel subalgebra. The largest solvable ideal of a Lie algebra is called the radical.

Characterizations

[edit]

Let be a finite-dimensional Lie algebra over a field of characteristic 0. The following are equivalent.

  • (i) is solvable.
  • (ii) , the adjoint representation of , is solvable.
  • (iii) There is a finite sequence of ideals of :
  • (iv) is nilpotent.[3]
  • (v) For -dimensional, there is a finite sequence of subalgebras of :
with each an ideal in .[4] A sequence of this type is called an elementary sequence.
  • (vi) There is a finite sequence of subalgebras of ,
such that is an ideal in and is abelian.[5]
  • (vii) The Killing form of satisfies for all X in and Y in .[6] This is Cartan's criterion for solvability.

Properties

[edit]

Lie's Theorem states that if is a finite-dimensional vector space over an algebraically closed field of characteristic zero, and is a solvable Lie algebra, and if is a representation of over , then there exists a simultaneous eigenvector of the endomorphisms for all elements .[7]

  • Every Lie subalgebra and quotient of a solvable Lie algebra are solvable.[8]
  • Given a Lie algebra and an ideal in it,
    is solvable if and only if both and are solvable.[8][2]
The analogous statement is true for nilpotent Lie algebras provided is contained in the center. Thus, an extension of a solvable algebra by a solvable algebra is solvable, while a central extension of a nilpotent algebra by a nilpotent algebra is nilpotent.
  • A solvable nonzero Lie algebra has a nonzero abelian ideal, the last nonzero term in the derived series.[2]
  • If are solvable ideals, then so is .[1] Consequently, if is finite-dimensional, then there is a unique solvable ideal containing all solvable ideals in . This ideal is the radical of .[2]
  • A solvable Lie algebra has a unique largest nilpotent ideal , called the nilradical, the set of all such that is nilpotent. If D is any derivation of , then .[9]

Completely solvable Lie algebras

[edit]

A Lie algebra is called completely solvable or split solvable if it has an elementary sequence{(V) As above definition} of ideals in from to . A finite-dimensional nilpotent Lie algebra is completely solvable, and a completely solvable Lie algebra is solvable. Over an algebraically closed field a solvable Lie algebra is completely solvable, but the -dimensional real Lie algebra of the group of Euclidean isometries of the plane is solvable but not completely solvable.

A solvable Lie algebra is split solvable if and only if the eigenvalues of are in for all in .[2]

Examples

[edit]

Abelian Lie algebras

[edit]

Every abelian Lie algebra is solvable by definition, since its commutator . This includes the Lie algebra of diagonal matrices in , which are of the form

for . The Lie algebra structure on a vector space given by the trivial bracket for any two matrices gives another example.

Nilpotent Lie algebras

[edit]

Another class of examples comes from nilpotent Lie algebras since the adjoint representation is solvable. Some examples include the upper-diagonal matrices, such as the class of matrices of the form

called the Lie algebra of strictly upper triangular matrices. In addition, the Lie algebra of upper diagonal matrices in form a solvable Lie algebra. This includes matrices of the form

and is denoted .

Solvable but not split-solvable

[edit]

Let be the set of matrices on the form

Then is solvable, but not split solvable.[2] It is isomorphic with the Lie algebra of the group of translations and rotations in the plane.

Non-example

[edit]

A semisimple Lie algebra is never solvable since its radical , which is the largest solvable ideal in , is trivial.[1] page 11

Solvable Lie groups

[edit]

Because the term "solvable" is also used for solvable groups in group theory, there are several possible definitions of solvable Lie group. For a Lie group , there is

  • termination of the usual derived series of the group (as an abstract group);
  • termination of the closures of the derived series;
  • having a solvable Lie algebra

See also

[edit]

Notes

[edit]
  1. ^ a b c Humphreys 1972
  2. ^ a b c d e f Knapp 2002
  3. ^ Knapp 2002 Proposition 1.39.
  4. ^ Knapp 2002 Proposition 1.23.
  5. ^ Fulton & Harris 1991
  6. ^ Knapp 2002 Proposition 1.46.
  7. ^ Knapp 2002 Theorem 1.25.
  8. ^ a b Serre 2001, Ch. I, § 6, Definition 2.
  9. ^ Knapp 2002 Proposition 1.40.

References

[edit]
  • Fulton, W.; Harris, J. (1991). Representation theory. A first course. Graduate Texts in Mathematics. Vol. 129. New York: Springer-Verlag. ISBN 978-0-387-97527-6. MR 1153249.
  • Humphreys, James E. (1972). Introduction to Lie Algebras and Representation Theory. Graduate Texts in Mathematics. Vol. 9. New York: Springer-Verlag. ISBN 0-387-90053-5.
  • Knapp, A. W. (2002). Lie groups beyond an introduction. Progress in Mathematics. Vol. 120 (2nd ed.). Boston·Basel·Berlin: Birkhäuser. ISBN 0-8176-4259-5..
  • Serre, Jean-Pierre (2001). Complex Semisimple Lie Algebras. Berlin: Springer. ISBN 3-5406-7827-1.
[edit]