Jump to content

Kac–Moody algebra: Difference between revisions

From Wikipedia, the free encyclopedia
Content deleted Content added
References: * The link to the Wikipedia page of Antony Wassermann
Introduction: Unified notation.
Tags: Mobile edit Mobile web edit
 
(40 intermediate revisions by 16 users not shown)
Line 1: Line 1:
In [[mathematics]], a '''Kac–Moody algebra''' (named for [[Victor Kac]] and [[Robert Moody]], who independently discovered them) is a [[Lie algebra]], usually infinite-dimensional, that can be defined by generators and relations through a [[generalized Cartan matrix]]. These algebras form a generalization of finite-dimensional [[semisimple Lie algebra]]s, and many properties related to the structure of a Lie algebra such as its [[root system]], [[representation of a Lie algebra|irreducible representations]], and connection to [[flag manifold]]s have natural analogues in the Kac–Moody setting.
{{Short description|Lie algebra that can be defined by generators and relations through a generalized Cartan matrix}}
In [[mathematics]], a '''Kac–Moody algebra''' (named for [[Victor Kac]] and [[Robert Moody]], who independently and simultaneously discovered them in 1968{{sfn|Zhe-xian|1991|loc=Preface}}) is a [[Lie algebra]], usually infinite-dimensional, that can be defined by generators and relations through a [[generalized Cartan matrix]]. These algebras form a generalization of finite-dimensional [[semisimple Lie algebra]]s, and many properties related to the structure of a Lie algebra such as its [[root system]], [[representation of a Lie algebra|irreducible representations]], and connection to [[flag manifold]]s have natural analogues in the Kac–Moody setting.


A class of '''Kac–Moody algebras''' called '''[[affine Lie algebra]]s''' is of particular importance in mathematics and [[theoretical physics]], especially [[two-dimensional conformal field theory]] and the theory of [[exactly solvable model]]s. Kac discovered an elegant proof of certain combinatorial identities, the [[Macdonald identities]], which is based on the representation theory of affine Kac–Moody algebras. Howard Garland and [[James Lepowsky]] demonstrated that [[Rogers–Ramanujan identities]] can be derived in a similar fashion.<ref>(?) {{cite journal |first=H. |last=Garland |first2=J. |last2=Lepowsky |title=Lie algebra homology and the Macdonald-Kac formulas |journal=[[Inventiones Mathematicae|Invent. Math.]] |volume=34 |issue=1 |year=1976 |pages=37–76 |doi=10.1007/BF01418970 |bibcode=1976InMat..34...37G }}</ref>
A class of Kac–Moody algebras called '''[[affine Lie algebra]]s''' is of particular importance in mathematics and [[theoretical physics]], especially [[two-dimensional conformal field theory]] and the theory of [[exactly solvable model]]s. Kac discovered an elegant proof of certain combinatorial identities, the [[Macdonald identities]], which is based on the representation theory of affine Kac–Moody algebras. Howard Garland and [[James Lepowsky]] demonstrated that [[Rogers–Ramanujan identities]] can be derived in a similar fashion.<ref>(?) {{cite journal |first1=H. |last1=Garland |first2=J. |last2=Lepowsky |title=Lie algebra homology and the Macdonald–Kac formulas |journal=[[Inventiones Mathematicae|Invent. Math.]] |volume=34 |issue=1 |year=1976 |pages=37–76 |doi=10.1007/BF01418970 |bibcode=1976InMat..34...37G |s2cid=122385055 }}</ref>


== History of Kac–Moody algebras ==
== History of Kac–Moody algebras ==
The initial construction by [[Élie Cartan]] and [[Wilhelm Killing]] of finite dimensional [[simple Lie algebra]]s from the [[Cartan integer]]s was type dependent. In 1966 [[Jean-Pierre Serre]] showed that relations of [[Claude Chevalley]] and [[Harish-Chandra]],<ref name="H-C">{{cite journal |last=Harish-Chandra |title=On some applications of the universal enveloping algebra of a semisimple Lie algebra |journal=[[Transactions of the American Mathematical Society|Trans. Amer. Math. Soc.]] |volume=70 |issue=1 |year=1951 |pages=28–28 |doi= 10.1090/S0002-9947-1951-0044515-0|jstor=1990524 }}</ref> with simplifications by [[Nathan Jacobson]],<ref name="Ja">{{cite book |last=Jacobson |first=N. |title=Lie algebras |series=Interscience Tracts in Pure and Applied Mathematics |volume=10 |publisher=Interscience Publishers (a division of John Wiley & Sons) |location=New York-London |year=1962 }}</ref> give a defining presentation for the [[Lie algebra]].<ref name="Se">{{cite book |last=Serre |first=J.-P. |title=Algèbres de Lie semi-simples complexes |language=French |publisher=W. A. Benjamin |location=New York-Amsterdam |year=1966 }}</ref> One could thus describe a simple Lie algebra in terms of generators and relations using data from the matrix of Cartan integers, which is naturally [[positive-definite matrix|positive definite]].
The initial construction by [[Élie Cartan]] and [[Wilhelm Killing]] of finite dimensional [[simple Lie algebra]]s from the [[Cartan integer]]s was type dependent. In 1966 [[Jean-Pierre Serre]] showed that relations of [[Claude Chevalley]] and [[Harish-Chandra]],<ref name="H-C">{{cite journal |last=Harish-Chandra |title=On some applications of the universal enveloping algebra of a semisimple Lie algebra |journal=[[Transactions of the American Mathematical Society|Trans. Amer. Math. Soc.]] |volume=70 |issue=1 |year=1951 |pages=28–96 |doi= 10.1090/S0002-9947-1951-0044515-0|jstor=1990524 |doi-access=free }}</ref> with simplifications by [[Nathan Jacobson]],<ref name="Ja">{{cite book |last=Jacobson |first=N. |title=Lie algebras |series=Interscience Tracts in Pure and Applied Mathematics |volume=10 |publisher=Interscience Publishers (a division of John Wiley & Sons) |location=New York-London |year=1962 }}</ref> give a defining presentation for the [[Lie algebra]].<ref name="Se">{{cite book |last=Serre |first=J.-P. |title=Algèbres de Lie semi-simples complexes |language=fr |publisher=W. A. Benjamin |location=New York-Amsterdam |year=1966 }}</ref> One could thus describe a simple Lie algebra in terms of generators and relations using data from the matrix of Cartan integers, which is naturally [[positive-definite matrix|positive definite]].


"Almost simultaneously in 1967, Victor Kac in the USSR and [[Robert Moody]] in Canada developed what was to become [[Kac-Moody algebra]]. Kac and Moody noticed that if [[Wilhelm Killing]]'s conditions were relaxed, it was still possible to associate to the [[Cartan matrix]] a Lie algebra which, necessarily, would be infinite dimensional." - A.J. Coleman<ref>Coleman, A. John, "The Greatest Mathematical Paper of All Time," ''[http://www.math.umd.edu/~jda/744/coleman.pdf The Mathematical Intelligencer],'' vol. 11, no. 3, pp.&nbsp;29–38.</ref>
"Almost simultaneously in 1967, [[Victor Kac]] in the USSR and [[Robert Moody]] in Canada developed what was to become Kac–Moody algebra. Kac and Moody noticed that if [[Wilhelm Killing]]'s conditions were relaxed, it was still possible to associate to the [[Cartan matrix]] a Lie algebra which, necessarily, would be infinite dimensional." A. J. Coleman<ref>Coleman, A. John, "The Greatest Mathematical Paper of All Time," ''[https://www.math.umd.edu/~jda/744/coleman.pdf The Mathematical Intelligencer],'' vol. 11, no. 3, pp.&nbsp;29–38.</ref>


In his 1967 thesis, [[Robert Moody]] considered Lie algebras whose [[Cartan matrix]] is no longer positive definite.<ref name="M1">{{cite journal |last=Moody |first=R. V. |title=Lie algebras associated with generalized cartan matrices |journal=Bull. Amer. Math. Soc. |volume=73 |issue= 2|year=1967 |pages=217–222 |url=http://www.ams.org/journals/bull/1967-73-02/S0002-9904-1967-11688-4/S0002-9904-1967-11688-4.pdf |doi=10.1090/S0002-9904-1967-11688-4 }}</ref><ref name="M2">Moody 1968, ''A new class of Lie algebras''</ref> This still gave rise to a Lie algebra, but one which is now infinite dimensional. Simultaneously, '''Z'''-[[graded Lie algebra]]s were being studied in Moscow where [[I. L. Kantor]] introduced and studied a general class of Lie algebras including what eventually became known as '''Kac–Moody algebras'''.<ref name="Kan">{{cite journal |last=Kantor |first=I. L. |title=Graded Lie algebras |language=Russian |journal=Trudy Sem. Vektor. Tenzor. Anal. |volume=15 |issue= |year=1970 |pages=227–266 |doi= }}</ref> [[Victor Kac]] was also studying simple or nearly simple Lie algebras with polynomial growth. A rich mathematical theory of infinite dimensional Lie algebras evolved. An account of the subject, which also includes works of many others is given in (Kac 1990).<ref>Kac, 1990</ref> See also (Seligman 1987).<ref name="Sel">{{cite journal |last=Seligman |first=George B. |title=Book Review: Infinite dimensional Lie algebras |journal=Bull. Amer. Math. Soc. |series=N.S. |volume=16 |year=1987 |issue=1 |pages=144–150 |doi=10.1090/S0273-0979-1987-15492-9 }}</ref>
In his 1967 thesis, [[Robert Moody]] considered Lie algebras whose [[Cartan matrix]] is no longer positive definite.<ref name="M1">{{cite journal |last=Moody |first=R. V. |title=Lie algebras associated with generalized cartan matrices |journal=Bull. Amer. Math. Soc. |volume=73 |issue= 2|year=1967 |pages=217–222 |url=https://www.ams.org/journals/bull/1967-73-02/S0002-9904-1967-11688-4/S0002-9904-1967-11688-4.pdf |doi=10.1090/S0002-9904-1967-11688-4 |doi-access=free }}</ref><ref name="M2">Moody 1968, ''A new class of Lie algebras''</ref> This still gave rise to a Lie algebra, but one which is now infinite dimensional. Simultaneously, '''Z'''-[[graded Lie algebra]]s were being studied in Moscow where [[I. L. Kantor]] introduced and studied a general class of Lie algebras including what eventually became known as Kac–Moody algebras.<ref name="Kan">{{cite journal |last=Kantor |first=I. L. |title=Graded Lie algebras |language=ru |journal=Trudy Sem. Vektor. Tenzor. Anal. |volume=15 |year=1970 |pages=227–266 }}</ref> [[Victor Kac]] was also studying simple or nearly simple Lie algebras with polynomial growth. A rich mathematical theory of infinite dimensional Lie algebras evolved. An account of the subject, which also includes works of many others is given in (Kac 1990).<ref>Kac, 1990</ref> See also (Seligman 1987).<ref name="Sel">{{cite journal |last=Seligman |first=George B. |title=Book Review: Infinite dimensional Lie algebras |journal=Bull. Amer. Math. Soc. |series=N.S. |volume=16 |year=1987 |issue=1 |pages=144–150 |doi=10.1090/S0273-0979-1987-15492-9 |doi-access=free }}</ref>


==Definition==
== Introduction ==
Given an ''n''&times;''n'' [[generalized Cartan matrix]] <math>C = \begin{pmatrix} c_{ij}\end{pmatrix}</math>, one can construct a Lie algebra <math>\mathfrak{g}'(C)</math> defined by [[generating set|generators]] <math>e_i</math>, <math>h_i</math>, and <math>f_i \left(i \in \{1, \ldots, n\}\right)</math> and relations given by:
A Kac–Moody algebra may be defined by first giving the following:
*<math>\left[h_i, h_j\right] = 0\ </math> for all <math>i, j \in \{1, \ldots, n\}</math>;
# An ''n''&times;''n'' [[generalized Cartan matrix]] {{nowrap|1=''C'' = (''c<sub>ij''</sub>)}} of [[rank (linear algebra)|rank]] ''r''.
*<math>\left[h_i, e_j\right] = c_{ij}e_j</math>;
# A [[vector space]] <math>\mathfrak{h}</math> over the [[complex number]]s of dimension 2''n''&nbsp;&minus;&nbsp;''r''.
*<math>\left[h_i, f_j\right] = -c_{ij}f_j</math>;
# A set of ''n'' [[linearly independent]] elements <math>\alpha_i^\vee\ </math> of <math>\mathfrak{h}</math> and a set of ''n'' linearly independent elements <math>\alpha_i</math> of the [[dual space]] <math>\mathfrak{h}^*</math>, such that <math>\alpha_i(\alpha_j^\vee) = c_{ji}</math>. The <math>\alpha_i</math> are analogue to the [[Root system of a semi-simple Lie algebra|simple roots]] of a semi-simple Lie algebra, and the <math>\alpha_i^\vee</math> to the simple coroots.
*<math>\left[e_i, f_j\right] = \delta_{ij}h_i </math>, where <math> \delta_{ij}</math> is the Kronecker delta;
*If <math>i \neq j</math> (so <math>c_{ij} \leq 0</math>) then <math>\textrm{ad}(e_i)^{1-c_{ij}}(e_j) = 0</math> and <math>\operatorname{ad}(f_i)^{1-c_{ij}}(f_j) = 0</math>, where <math>\operatorname{ad}: \mathfrak{g}\to\operatorname{End}(\mathfrak{g}),\operatorname{ad}(x)(y) = [x, y],</math> is the [[Adjoint representation of a Lie algebra|adjoint representation]] of <math>\mathfrak{g}</math>.


The Kac–Moody algebra is then the Lie algebra <math>\mathfrak{g}</math> defined by [[generating set|generators]] <math>e_i</math> and <math>f_i</math> (<math>i \in \{1,\ldots,n\}</math>) and the elements of <math>\mathfrak{h}</math> and relations
Under a "symmetrizability" assumption, <math>\mathfrak{g}'(C)</math> identifies with the derived subalgebra <math>\mathfrak{g}'(C) = [\mathfrak{g}(C), \mathfrak{g}(C)]</math> of the affine Kac-Moody algebra <math>\mathfrak{g}(C)</math> defined below.<ref name="Kac">Kac 1990, ''Infinite dimensional Lie Algebras, Third Edition''</ref>

*<math>[h,h'] = 0\ </math> for <math>h,h' \in \mathfrak{h}</math>;
== Definition ==
*<math>[h,e_i] = \alpha_i(h)e_i</math>, for <math>h \in \mathfrak{h}</math>;
Assume we are given an <math>n \times n</math> [[generalized Cartan matrix]] {{nowrap|1=''C'' = (''c<sub>ij</sub>'')}} of [[rank (linear algebra)|rank]] ''r''. For every such <math>C</math>, there exists a unique up to isomorphism ''realization'' of <math>C</math>, i.e. a triple <math>(\mathfrak{h}, \{\alpha_i\}_{i = 1}^n, \{\alpha_i^\vee\}_{i = 1}^n, </math>) where <math>\mathfrak{h}</math> is a complex vector space, <math>\{\alpha_i^\vee\}_{i = 1}^n</math> is a subset of elements of <math>\mathfrak{h}</math>, and <math>\{\alpha_i\}_{i = 1}^n</math> is a subset of the [[dual space]] <math>\mathfrak{h}^*</math> satisfying the following three conditions:<ref name="KacProp">Kac 1990, ''Infinite dimensional Lie algebras'', Proposition 1.1</ref>
*<math>[h,f_i] = -\alpha_i(h)f_i</math>, for <math>h \in \mathfrak{h}</math>;

*<math>[e_i,f_j] = \delta_{ij}\alpha_i^\vee </math>, where <math> \delta_{ij}</math> is the Kronecker delta;
# The vector space <math>\mathfrak{h}</math> has dimension 2''n''&nbsp;&minus;&nbsp;''r''
*If <math>i \neq j</math> (so <math>c_{ij} \leq 0</math>) then <math>\textrm{ad}(e_i)^{1-c_{ij}}(e_j) = 0</math> and <math>\textrm{ad}(f_i)^{1-c_{ij}}(f_j) = 0</math>, where <math>\textrm{ad}: \mathfrak{g}\to\textrm{End}(\mathfrak{g}),\textrm{ad}(x)(y)=[x,y],</math> is the [[Adjoint representation of a Lie algebra|adjoint representation]] of <math>\mathfrak{g}</math>.
# The sets <math>\{\alpha_i\}_{i = 1}^n</math> and <math>\{\alpha_i^\vee\}_{i = 1}^n</math> are linearly independent and
# For every <math>1 \leq i, j \leq n, \alpha_i\left(\alpha_j^\vee\right) = C_{ji}</math>.

The <math>\alpha_i</math> are analogue to the [[root system of a semi-simple Lie algebra|simple roots]] of a semi-simple Lie algebra, and the <math>\alpha_i^\vee</math> to the simple coroots.

Then we define the ''Kac-Moody algebra'' associated to <math>C</math> as the Lie algebra <math>\mathfrak{g} := \mathfrak{g}(C)</math> defined by [[generating set|generators]] <math>e_i</math> and <math>f_i \left(i \in \{1, \ldots, n\}\right)</math> and the elements of <math>\mathfrak{h}</math> and relations
*<math>\left[h, h'\right] = 0\ </math> for <math>h,h' \in \mathfrak{h}</math>;
*<math>\left[h, e_i\right] = \alpha_i(h)e_i</math>, for <math>h \in \mathfrak{h}</math>;
*<math>\left[h, f_i\right] = -\alpha_i(h)f_i</math>, for <math>h \in \mathfrak{h}</math>;
*<math>\left[e_i, f_j\right] = \delta_{ij}\alpha_i^\vee </math>, where <math> \delta_{ij}</math> is the Kronecker delta;
*If <math>i \neq j</math> (so <math>c_{ij} \leq 0</math>) then <math>\textrm{ad}(e_i)^{1-c_{ij}}(e_j) = 0</math> and <math>\operatorname{ad}(f_i)^{1-c_{ij}}(f_j) = 0</math>, where <math>\operatorname{ad}: \mathfrak{g}\to\operatorname{End}(\mathfrak{g}),\operatorname{ad}(x)(y) = [x, y],</math> is the [[Adjoint representation of a Lie algebra|adjoint representation]] of <math>\mathfrak{g}</math>.


A [[real number|real]] (possibly infinite-dimensional) [[Lie algebra]] is also considered a Kac–Moody algebra if its [[complexification]] is a Kac–Moody algebra.
A [[real number|real]] (possibly infinite-dimensional) [[Lie algebra]] is also considered a Kac–Moody algebra if its [[complexification]] is a Kac–Moody algebra.
Line 30: Line 44:
If <math>x\neq 0</math> is an element of <math>\mathfrak{g}</math> such that
If <math>x\neq 0</math> is an element of <math>\mathfrak{g}</math> such that


:<math>\forall h\in\mathfrak{h}, [h,x]=\lambda(h)x</math>
:<math>\forall h\in\mathfrak{h}, [h, x] = \lambda(h)x</math>


for some <math>\lambda\in\mathfrak{h}^*\backslash\{0\}</math>, then <math>x</math> is called a '''root vector''' and <math>\lambda</math> is a '''root''' of <math>\mathfrak{g}</math>. (The zero functional is not considered a root by convention.) The set of all roots of <math>\mathfrak{g}</math> is often denoted by <math>\Delta</math> and sometimes by <math>R</math>. For a given root <math>\lambda</math> one denotes by <math>\mathfrak{g}_\lambda</math> the '''root space''' of <math>\lambda</math>, that is
for some <math>\lambda\in\mathfrak{h}^*\backslash\{0\}</math>, then <math>x</math> is called a '''root vector''' and <math>\lambda</math> is a '''root''' of <math>\mathfrak{g}</math>. (The zero functional is not considered a root by convention.) The set of all roots of <math>\mathfrak{g}</math> is often denoted by <math>\Delta</math> and sometimes by <math>R</math>. For a given root <math>\lambda</math>, one denotes by <math>\mathfrak{g}_\lambda</math> the '''root space''' of <math>\lambda</math>; that is,


:<math>\mathfrak{g}_\lambda = \{x\in\mathfrak{g}:\forall h\in\mathfrak{h}, [h,x] = \lambda(h)x\}</math>.
:<math>\mathfrak{g}_\lambda = \{x\in\mathfrak{g}:\forall h\in\mathfrak{h}, [h,x] = \lambda(h)x\}</math>.


It follows from the defining relations of <math>\mathfrak{g}</math> that <math>e_i\in\mathfrak{g}_{\alpha_i}</math> and <math>f_i\in\mathfrak{g}_{-\alpha_i}</math>. Also, if <math>x_1\in\mathfrak{g}_{\lambda_1}</math> and <math>x_2\in\mathfrak{g}_{\lambda_2}</math>, then <math>[x_1,x_2]\in\mathfrak{g}_{\lambda_1+\lambda_2}</math> by the [[Jacobi identity]].
It follows from the defining relations of <math>\mathfrak{g}</math> that <math>e_i\in\mathfrak{g}_{\alpha_i}</math> and <math>f_i\in\mathfrak{g}_{-\alpha_i}</math>. Also, if <math>x_1\in\mathfrak{g}_{\lambda_1}</math> and <math>x_2\in\mathfrak{g}_{\lambda_2}</math>, then <math>\left[x_1, x_2\right]\in\mathfrak{g}_{\lambda_1+\lambda_2}</math> by the [[Jacobi identity]].


A fundamental result of the theory is that any Kac–Moody algebra can be decomposed into the [[direct sum]] of <math>\mathfrak{h}</math> and its root spaces, that is
A fundamental result of the theory is that any Kac–Moody algebra can be decomposed into the [[direct sum]] of <math>\mathfrak{h}</math> and its root spaces, that is


:<math> \mathfrak{g} = \mathfrak{h}\oplus\bigoplus_{\lambda\in\Delta} \mathfrak{g}_\lambda</math>,
:<math>\mathfrak{g} = \mathfrak{h}\oplus\bigoplus_{\lambda\in\Delta} \mathfrak{g}_\lambda</math>,


and that every root <math>\lambda</math> can be written as <math>\lambda = \sum_{i=1}^n z_i\alpha_i</math> with all the <math>z_i</math> being [[integers]] of the same [[Sign (mathematics)|sign]].
and that every root <math>\lambda</math> can be written as <math>\lambda = \sum_{i=1}^n z_i\alpha_i</math> with all the <math>z_i</math> being [[integers]] of the same [[Sign (mathematics)|sign]].
Line 47: Line 61:
Properties of a Kac–Moody algebra are controlled by the algebraic properties of its generalized Cartan matrix ''C''. In order to classify Kac–Moody algebras, it is enough to consider the case of an ''indecomposable'' matrix ''C'', that is, assume that there is no decomposition of the set of indices ''I'' into a disjoint union of non-empty subsets ''I''<sub>1</sub> and ''I''<sub>2</sub> such that ''C''<sub>''ij''</sub> = 0 for all ''i'' in ''I''<sub>1</sub> and ''j'' in ''I''<sub>2</sub>. Any decomposition of the generalized Cartan matrix leads to the direct sum decomposition of the corresponding Kac–Moody algebra:
Properties of a Kac–Moody algebra are controlled by the algebraic properties of its generalized Cartan matrix ''C''. In order to classify Kac–Moody algebras, it is enough to consider the case of an ''indecomposable'' matrix ''C'', that is, assume that there is no decomposition of the set of indices ''I'' into a disjoint union of non-empty subsets ''I''<sub>1</sub> and ''I''<sub>2</sub> such that ''C''<sub>''ij''</sub> = 0 for all ''i'' in ''I''<sub>1</sub> and ''j'' in ''I''<sub>2</sub>. Any decomposition of the generalized Cartan matrix leads to the direct sum decomposition of the corresponding Kac–Moody algebra:


: <math>\mathfrak{g}(C)\simeq\mathfrak{g}(C_1)\oplus\mathfrak{g}(C_2),</math>
: <math>\mathfrak{g}(C) \simeq \mathfrak{g}\left(C_1\right) \oplus \mathfrak{g}\left(C_2\right),</math>


where the two Kac–Moody algebras in the right hand side are associated with the submatrices of ''C'' corresponding to the index sets ''I''<sub>1</sub> and ''I''<sub>2</sub>.
where the two Kac–Moody algebras in the right hand side are associated with the submatrices of ''C'' corresponding to the index sets ''I''<sub>1</sub> and ''I''<sub>2</sub>.
Line 58: Line 72:
*Since the diagonal entries of ''C'' and ''S'' are positive, ''S'' cannot be [[negative definite matrix|negative definite]] or negative semidefinite.
*Since the diagonal entries of ''C'' and ''S'' are positive, ''S'' cannot be [[negative definite matrix|negative definite]] or negative semidefinite.


Symmetrizable indecomposable generalized Cartan matrices of finite and affine type have been completely classified. They correspond to [[Dynkin diagram]]s and [[affine Dynkin diagram]]s. Little is known about the Kac–Moody algebras of indefinite type, although the groups corresponding to these Kac–Moody algebras were constructed over arbitrary fields by Jacques Tits.<ref>{{cite journal |last=Tits |first=J. |title =Uniqueness and presentation of Kac–Moody groups over fields|journal=[[Journal of Algebra]] |volume=105 |pages=542–573 |year=1987 |doi=10.1016/0021-8693(87)90214-6}}</ref>
Symmetrizable indecomposable generalized Cartan matrices of finite and affine type have been completely classified. They correspond to [[Dynkin diagram]]s and [[affine Dynkin diagram]]s. Little is known about the Kac–Moody algebras of indefinite type, although the groups corresponding to these Kac–Moody algebras were constructed over arbitrary fields by Jacques Tits.<ref>{{cite journal |last=Tits |first=J. |title =Uniqueness and presentation of Kac–Moody groups over fields|journal=[[Journal of Algebra]] |volume=105 |issue=2 |pages=542–573 |year=1987 |doi=10.1016/0021-8693(87)90214-6|doi-access=free }}</ref>


Among the Kac–Moody algebras of indefinite type, most work has focused on those '''hyperbolic type''', for which the matrix ''S'' is indefinite, but for each proper subset of ''I'', the corresponding submatrix is positive definite or positive semidefinite. Hyperbolic Kac–Moody algebras have rank at most 10, and they have been completely classified.<ref>{{cite journal |last=Carbone |first=L. |last2=Chung |first2=S. |last3=Cobbs |first3=C. |last4=McRae |first4=R. |last5=Nandi |first5=D. |last6=Naqvi |first6=Y. |last7=Penta |first7=D. |title=Classification of hyperbolic Dynkin diagrams, root lengths and Weyl group orbits |journal=[[Journal of Physics A|J. Phys. A: Math. Theor.]] |volume=43 |issue=15 |pages=155–209 |year=2010 |doi=10.1088/1751-8113/43/15/155209 |arxiv=1003.0564 |bibcode=2010JPhA...43o5209C }}</ref> There are infinitely many of rank 2, and 238 of ranks between 3 and 10, listed at
Among the Kac–Moody algebras of indefinite type, most work has focused on those '''hyperbolic type''', for which the matrix ''S'' is indefinite, but for each proper subset of ''I'', the corresponding submatrix is positive definite or positive semidefinite. Hyperbolic Kac–Moody algebras have rank at most 10, and they have been completely classified.<ref>{{cite journal |last1=Carbone |first1=L. |last2=Chung |first2=S. |last3=Cobbs |first3=C. |last4=McRae |first4=R. |last5=Nandi |first5=D. |last6=Naqvi |first6=Y. |last7=Penta |first7=D. |title=Classification of hyperbolic Dynkin diagrams, root lengths and Weyl group orbits |journal=[[Journal of Physics A|J. Phys. A: Math. Theor.]] |volume=43 |issue=15 |pages=155–209 |year=2010 |doi=10.1088/1751-8113/43/15/155209 |arxiv=1003.0564 |bibcode=2010JPhA...43o5209C |s2cid=16946456 }}</ref> There are infinitely many of rank 2, and [[Dynkin diagram#238 Hyperbolic groups (compact and noncompact)|238 of ranks between 3 and 10]].
[[Dynkin_diagram#238_Hyperbolic_groups_.28compact_and_noncompact.29 |
hyperbolic groups: compact and noncompact]].


==See also==
==See also==
*[[Weyl–Kac character formula]]
*[[Weyl–Kac character formula]]
*[[Generalized Kac–Moody algebra]]
*[[Generalized Kac–Moody algebra]]
*[[Integrable module]]
*[[Monstrous moonshine]]
<!--
<!--
==Notes==
==Notes==
{{Reflist}}-->
<references />-->


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


==References==
==References==
{{refbegin|2}}
*{{cite journal |last1=Berman |first1=Stephen |last2=Parshall |first2=Karen Hunger |date=13 January 2002 |title=Victor Kac and Robert Moody: Their Paths to Kac-Moody Lie Algebras |journal=[[The Mathematical Intelligencer]] |volume=24 |pages=50–60 |doi=10.1007/BF03025312|s2cid=120670625 }}
*[[Robert Moody|Robert V. Moody]], ''A new class of Lie algebras'', [[Journal of Algebra]], '''10''' (1968), 211–230. {{doi|10.1016/0021-8693(68)90096-3}} {{MR|0229687}}
*[[Robert Moody|Robert V. Moody]], ''A new class of Lie algebras'', [[Journal of Algebra]], '''10''' (1968), 211–230. {{doi|10.1016/0021-8693(68)90096-3}} {{MR|0229687}}
*[[Victor Kac]], ''Infinite dimensional Lie algebras'', 3rd edition, Cambridge University Press (1990) {{ISBN|0-521-46693-8}} [https://books.google.com/books?id=kuEjSb9teJwC&lpg=PP1&dq=Victor%20G.%20Kac&pg=PP1#v=onepage&q&f=false]
*[[Victor Kac]], ''Infinite dimensional Lie algebras'', 3rd edition, Cambridge University Press (1990) {{ISBN|0-521-46693-8}} [https://books.google.com/books?id=kuEjSb9teJwC&dq=Victor%20G.%20Kac&pg=PP1]
*[[Antony Wassermann]], [https://arxiv.org/abs/1004.1287 Lecture notes on Kac–Moody and Virasoro algebras]
*[[Antony Wassermann]], [https://arxiv.org/abs/1004.1287 Lecture notes on Kac–Moody and Virasoro algebras]
*{{springer|id=K/k055050|author=|title=Kac–Moody algebra}}
*{{springer|id=K/k055050|author=|title=Kac–Moody algebra}}
* Victor G. Kac, ''Simple irreducible graded Lie algebras of finite growth'' Math. USSR Izv., 2 (1968) pp.&nbsp;1271–1311, Izv. Akad. Nauk USSR Ser. Mat., 32 (1968) pp.&nbsp;1923–1967
* Victor G. Kac, ''Simple irreducible graded Lie algebras of finite growth'' Math. USSR Izv., 2 (1968) pp.&nbsp;1271–1311, Izv. Akad. Nauk USSR Ser. Mat., 32 (1968) pp.&nbsp;1923–1967
*{{cite book|editor-last1=Sthanumoorthy|editor-first1=N.|editor-last2=Misra|editor-first2=Kailash C.|title=Kac-Moody Lie Algebras and Related Topics|date=2004|publisher=[[American Mathematical Society|AMS]]|isbn=0-8218-3337-5}}
*[[Shrawan Kumar]], ''Kac–Moody Groups, their Flag Varieties and Representation Theory'', 1st edition, Birkhäuser (2002). {{ISBN|3-7643-4227-7}}.
*[[Shrawan Kumar (mathematician)|Shrawan Kumar]], ''Kac–Moody Groups, their Flag Varieties and Representation Theory'', 1st edition, Birkhäuser (2002). {{ISBN|3-7643-4227-7}}.
*{{cite book|last=Zhe-xian|first=Wan|title=Introduction to Kac-Moody Algebra|date=1991|publisher=[[World Scientific]]|isbn=981-02-0224-5}}
{{refend}}


==External links==
==External links==
* [http://www.emis.de/journals/SIGMA/Kac-Moody_algebras.html SIGMA: Special Issue on Kac-Moody Algebras and Applications]
* [http://www.emis.de/journals/SIGMA/Kac-Moody_algebras.html SIGMA: Special Issue on Kac–Moody Algebras and Applications]
{{String theory topics |state=collapsed}}
{{String theory topics |state=collapsed}}
{{Authority control}}


{{DEFAULTSORT:Kac-Moody Algebra}}
{{DEFAULTSORT:Kac-Moody Algebra}}
[[Category:Lie algebras]]
[[Category:Lie algebras]]
[[Category:Moonshine theory]]

Latest revision as of 18:26, 3 August 2024

In mathematics, a Kac–Moody algebra (named for Victor Kac and Robert Moody, who independently and simultaneously discovered them in 1968[1]) is a Lie algebra, usually infinite-dimensional, that can be defined by generators and relations through a generalized Cartan matrix. These algebras form a generalization of finite-dimensional semisimple Lie algebras, and many properties related to the structure of a Lie algebra such as its root system, irreducible representations, and connection to flag manifolds have natural analogues in the Kac–Moody setting.

A class of Kac–Moody algebras called affine Lie algebras is of particular importance in mathematics and theoretical physics, especially two-dimensional conformal field theory and the theory of exactly solvable models. Kac discovered an elegant proof of certain combinatorial identities, the Macdonald identities, which is based on the representation theory of affine Kac–Moody algebras. Howard Garland and James Lepowsky demonstrated that Rogers–Ramanujan identities can be derived in a similar fashion.[2]

History of Kac–Moody algebras

[edit]

The initial construction by Élie Cartan and Wilhelm Killing of finite dimensional simple Lie algebras from the Cartan integers was type dependent. In 1966 Jean-Pierre Serre showed that relations of Claude Chevalley and Harish-Chandra,[3] with simplifications by Nathan Jacobson,[4] give a defining presentation for the Lie algebra.[5] One could thus describe a simple Lie algebra in terms of generators and relations using data from the matrix of Cartan integers, which is naturally positive definite.

"Almost simultaneously in 1967, Victor Kac in the USSR and Robert Moody in Canada developed what was to become Kac–Moody algebra. Kac and Moody noticed that if Wilhelm Killing's conditions were relaxed, it was still possible to associate to the Cartan matrix a Lie algebra which, necessarily, would be infinite dimensional." – A. J. Coleman[6]

In his 1967 thesis, Robert Moody considered Lie algebras whose Cartan matrix is no longer positive definite.[7][8] This still gave rise to a Lie algebra, but one which is now infinite dimensional. Simultaneously, Z-graded Lie algebras were being studied in Moscow where I. L. Kantor introduced and studied a general class of Lie algebras including what eventually became known as Kac–Moody algebras.[9] Victor Kac was also studying simple or nearly simple Lie algebras with polynomial growth. A rich mathematical theory of infinite dimensional Lie algebras evolved. An account of the subject, which also includes works of many others is given in (Kac 1990).[10] See also (Seligman 1987).[11]

Introduction

[edit]

Given an n×n generalized Cartan matrix , one can construct a Lie algebra defined by generators , , and and relations given by:

  • for all ;
  • ;
  • ;
  • , where is the Kronecker delta;
  • If (so ) then and , where is the adjoint representation of .

Under a "symmetrizability" assumption, identifies with the derived subalgebra of the affine Kac-Moody algebra defined below.[12]

Definition

[edit]

Assume we are given an generalized Cartan matrix C = (cij) of rank r. For every such , there exists a unique up to isomorphism realization of , i.e. a triple ) where is a complex vector space, is a subset of elements of , and is a subset of the dual space satisfying the following three conditions:[13]

  1. The vector space has dimension 2n − r
  2. The sets and are linearly independent and
  3. For every .

The are analogue to the simple roots of a semi-simple Lie algebra, and the to the simple coroots.

Then we define the Kac-Moody algebra associated to as the Lie algebra defined by generators and and the elements of and relations

  • for ;
  • , for ;
  • , for ;
  • , where is the Kronecker delta;
  • If (so ) then and , where is the adjoint representation of .

A real (possibly infinite-dimensional) Lie algebra is also considered a Kac–Moody algebra if its complexification is a Kac–Moody algebra.

Root-space decomposition of a Kac–Moody algebra

[edit]

is the analogue of a Cartan subalgebra for the Kac–Moody algebra .

If is an element of such that

for some , then is called a root vector and is a root of . (The zero functional is not considered a root by convention.) The set of all roots of is often denoted by and sometimes by . For a given root , one denotes by the root space of ; that is,

.

It follows from the defining relations of that and . Also, if and , then by the Jacobi identity.

A fundamental result of the theory is that any Kac–Moody algebra can be decomposed into the direct sum of and its root spaces, that is

,

and that every root can be written as with all the being integers of the same sign.

Types of Kac–Moody algebras

[edit]

Properties of a Kac–Moody algebra are controlled by the algebraic properties of its generalized Cartan matrix C. In order to classify Kac–Moody algebras, it is enough to consider the case of an indecomposable matrix C, that is, assume that there is no decomposition of the set of indices I into a disjoint union of non-empty subsets I1 and I2 such that Cij = 0 for all i in I1 and j in I2. Any decomposition of the generalized Cartan matrix leads to the direct sum decomposition of the corresponding Kac–Moody algebra:

where the two Kac–Moody algebras in the right hand side are associated with the submatrices of C corresponding to the index sets I1 and I2.

An important subclass of Kac–Moody algebras corresponds to symmetrizable generalized Cartan matrices C, which can be decomposed as DS, where D is a diagonal matrix with positive integer entries and S is a symmetric matrix. Under the assumptions that C is symmetrizable and indecomposable, the Kac–Moody algebras are divided into three classes:

Symmetrizable indecomposable generalized Cartan matrices of finite and affine type have been completely classified. They correspond to Dynkin diagrams and affine Dynkin diagrams. Little is known about the Kac–Moody algebras of indefinite type, although the groups corresponding to these Kac–Moody algebras were constructed over arbitrary fields by Jacques Tits.[14]

Among the Kac–Moody algebras of indefinite type, most work has focused on those hyperbolic type, for which the matrix S is indefinite, but for each proper subset of I, the corresponding submatrix is positive definite or positive semidefinite. Hyperbolic Kac–Moody algebras have rank at most 10, and they have been completely classified.[15] There are infinitely many of rank 2, and 238 of ranks between 3 and 10.

See also

[edit]

Citations

[edit]
  1. ^ Zhe-xian 1991, Preface.
  2. ^ (?) Garland, H.; Lepowsky, J. (1976). "Lie algebra homology and the Macdonald–Kac formulas". Invent. Math. 34 (1): 37–76. Bibcode:1976InMat..34...37G. doi:10.1007/BF01418970. S2CID 122385055.
  3. ^ Harish-Chandra (1951). "On some applications of the universal enveloping algebra of a semisimple Lie algebra". Trans. Amer. Math. Soc. 70 (1): 28–96. doi:10.1090/S0002-9947-1951-0044515-0. JSTOR 1990524.
  4. ^ Jacobson, N. (1962). Lie algebras. Interscience Tracts in Pure and Applied Mathematics. Vol. 10. New York-London: Interscience Publishers (a division of John Wiley & Sons).
  5. ^ Serre, J.-P. (1966). Algèbres de Lie semi-simples complexes (in French). New York-Amsterdam: W. A. Benjamin.
  6. ^ Coleman, A. John, "The Greatest Mathematical Paper of All Time," The Mathematical Intelligencer, vol. 11, no. 3, pp. 29–38.
  7. ^ Moody, R. V. (1967). "Lie algebras associated with generalized cartan matrices" (PDF). Bull. Amer. Math. Soc. 73 (2): 217–222. doi:10.1090/S0002-9904-1967-11688-4.
  8. ^ Moody 1968, A new class of Lie algebras
  9. ^ Kantor, I. L. (1970). "Graded Lie algebras". Trudy Sem. Vektor. Tenzor. Anal. (in Russian). 15: 227–266.
  10. ^ Kac, 1990
  11. ^ Seligman, George B. (1987). "Book Review: Infinite dimensional Lie algebras". Bull. Amer. Math. Soc. N.S. 16 (1): 144–150. doi:10.1090/S0273-0979-1987-15492-9.
  12. ^ Kac 1990, Infinite dimensional Lie Algebras, Third Edition
  13. ^ Kac 1990, Infinite dimensional Lie algebras, Proposition 1.1
  14. ^ Tits, J. (1987). "Uniqueness and presentation of Kac–Moody groups over fields". Journal of Algebra. 105 (2): 542–573. doi:10.1016/0021-8693(87)90214-6.
  15. ^ Carbone, L.; Chung, S.; Cobbs, C.; McRae, R.; Nandi, D.; Naqvi, Y.; Penta, D. (2010). "Classification of hyperbolic Dynkin diagrams, root lengths and Weyl group orbits". J. Phys. A: Math. Theor. 43 (15): 155–209. arXiv:1003.0564. Bibcode:2010JPhA...43o5209C. doi:10.1088/1751-8113/43/15/155209. S2CID 16946456.

References

[edit]
[edit]