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− | ''over a field <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l0584401.png" />'' | + | ''over a field $K$'' |
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− | A [[Lie algebra|Lie algebra]] <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l0584402.png" /> whose elements are linear transformations of a [[Vector space|vector space]] <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l0584403.png" /> over <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l0584404.png" />; addition of elements and multiplication of them by elements of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l0584405.png" /> are defined in the usual way, and the commutator <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l0584406.png" /> of two elements <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l0584407.png" /> is given by the formula | + | A [[Lie algebra]] $\mathfrak{g}$ whose elements are linear transformations of a [[vector space]] $V$ over $K$; addition of elements and multiplication of them by elements of $K$ are defined in the usual way, and the commutator $[x,y]$ of two elements $x,y \in \mathfrak{g}$ is given by the formula |
| + | $$ |
| + | [x,y] = xy - yx |
| + | $$ |
| + | ($xy$ and $yx$ are the usual products of linear transformations). The linear Lie algebra consisting of all linear transformations of $V$ is denoted by $\mathfrak{gl}(V)$. If $V = K^n$, then $\mathfrak{gl}(V)$ is naturally identified with the set of all square matrices of order $n$ over $K$ and is denoted by $\mathfrak{gl}(n,K)$. Any linear Lie algebra is a subalgebra of some Lie algebra $\mathfrak{gl}(V)$. |
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− | <table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l0584408.png" /></td> </tr></table>
| + | Examples. 1) Let $V$ be endowed with an associative algebra structure. Then all derivations (cf. [[Derivation in a ring]]) of $V$ form a linear Lie algebra. If $V$ is a Lie algebra, then for a fixed element $x \in V$ the linear transformation of $V$ adjoint to $x$, defined by the formula $y \mapsto [x,y]$, $y \in V$, is a derivation of $V$; it is denoted by $\mathrm{ad} x$. The set |
| + | $$ |
| + | \mathrm{ad} V = \{ \mathrm{ad} x : x \in V \} |
| + | $$ |
| + | is a linear algebra, called the adjoint linear Lie algebra or the Lie algebra of inner derivations of $V$. |
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− | (<img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l0584409.png" /> and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844010.png" /> are the usual products of linear transformations). The linear Lie algebra consisting of all linear transformations of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844011.png" /> is denoted by <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844012.png" />. If <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844013.png" />, then <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844014.png" /> is naturally identified with the set of all square matrices of order <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844015.png" /> over <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844016.png" /> and is denoted by <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844017.png" />. Any linear Lie algebra is a subalgebra of some Lie algebra <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844018.png" />.
| + | 2) Let $K$ be a field that is complete with respect to some non-trivial absolute value, let $V$ be a normed complete space over $K$ and let $G$ be a linear Lie group of transformations of $V$, that is, a Lie subgroup of the Lie group of all automorphisms of $V$. Then the Lie algebra of the analytic group $G$ (cf. [[Lie algebra of an analytic group]]) is naturally identified with a Lie subalgebra of $\mathfrak{gl}(V)$, that is, it is a linear Lie algebra. |
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− | Examples. 1) Let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844019.png" /> be endowed with an associative algebra structure. Then all derivations (cf. [[Derivation in a ring|Derivation in a ring]]) of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844020.png" /> form a linear Lie algebra. If <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844021.png" /> is a Lie algebra, then for a fixed element <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844022.png" /> the linear transformation of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844023.png" /> adjoint to <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844024.png" />, defined by the formula <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844025.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844026.png" />, is a derivation of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844027.png" />; it is denoted by <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844028.png" />. The set
| + | The problem of the existence of an isomorphism of an arbitrary finite-dimensional Lie algebra to some linear Lie algebra had already arisen in the first papers on group theory and Lie algebras, but it was affirmatively solved only in 1935 by Ado's theorem (see [[#References|[4]]]): Every finite-dimensional Lie algebra $\mathfrak{g}$ over a field of characteristic zero has a faithful finite-dimensional representation $\rho$ (moreover, if $\mathfrak{n}$ is the largest nilpotent ideal of $\mathfrak{g}$, then $\rho$ can be chosen so that all elements of $\rho(\mathfrak{n})$ are nilpotent, cf. also [[Representation of a Lie algebra]]). The analogue of this theorem for Lie groups does not hold, in general; for example, the [[universal covering]] of the group of real unimodular matrices of order 2 does not have a faithful linear representation. |
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− | <table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844029.png" /></td> </tr></table>
| + | See also [[Lie algebra, algebraic]]. |
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− | is a linear algebra, called the adjoint linear Lie algebra or the Lie algebra of inner derivations of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844030.png" />. 2) Let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844031.png" /> be a field that is complete with respect to some non-trivial absolute value, let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844032.png" /> be a normed complete space over <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844033.png" /> and let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844034.png" /> be a linear Lie group of transformations of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844035.png" />, that is, a Lie subgroup of the Lie group of all automorphisms of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844036.png" />. Then the Lie algebra of the analytic group <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844037.png" /> (cf. [[Lie algebra of an analytic group|Lie algebra of an analytic group]]) is naturally identified with a Lie subalgebra of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844038.png" />, that is, it is a linear Lie algebra.
| + | ====References==== |
− | | + | <table> |
− | The problem of the existence of an isomorphism of an arbitrary finite-dimensional Lie algebra to some linear Lie algebra had already arisen in the first papers on group theory and Lie algebras, but it was affirmatively solved only in 1935 by Ado's theorem (see [[#References|[4]]]): Every finite-dimensional Lie algebra <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844039.png" /> over a field of characteristic zero has a faithful finite-dimensional representation <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844040.png" /> (moreover, if <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844041.png" /> is the largest nilpotent ideal of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844042.png" />, then <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844043.png" /> can be chosen so that all elements of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/l/l058/l058440/l05844044.png" /> are nilpotent, cf. also [[Representation of a Lie algebra|Representation of a Lie algebra]]). The analogue of this theorem for Lie groups does not hold, in general; for example, the [[Universal covering|universal covering]] of the group of real unimodular matrices of order 2 does not have a faithful linear representation.
| + | <TR><TD valign="top">[1]</TD> <TD valign="top"> L.S. Pontryagin, "Topological groups" , Princeton Univ. Press (1958) (Translated from Russian)</TD></TR> |
− | | + | <TR><TD valign="top">[2]</TD> <TD valign="top"> N. Bourbaki, "Elements of mathematics. Lie groups and Lie algebras" , Addison-Wesley (1975) (Translated from French)</TD></TR> |
− | See also [[Lie algebra, algebraic|Lie algebra, algebraic]].
| + | <TR><TD valign="top">[3]</TD> <TD valign="top"> J.-P. Serre, "Lie algebras and Lie groups" , Benjamin (1965) (Translated from French)</TD></TR> |
| + | <TR><TD valign="top">[4]</TD> <TD valign="top"> I.D. Ado, "The representation of Lie algebras by matrices" ''Uspekhi Mat. Nauk'' , '''2''' : 6 (1947) pp. 159–173 (In Russian)</TD></TR> |
| + | </table> |
| | | |
− | ====References====
| + | {{TEX|done}} |
− | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> L.S. Pontryagin, "Topological groups" , Princeton Univ. Press (1958) (Translated from Russian)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> N. Bourbaki, "Elements of mathematics. Lie groups and Lie algebras" , Addison-Wesley (1975) (Translated from French)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> J.-P. Serre, "Lie algebras and Lie groups" , Benjamin (1965) (Translated from French)</TD></TR><TR><TD valign="top">[4]</TD> <TD valign="top"> I.D. Ado, "The representation of Lie algebras by matrices" ''Uspekhi Mat. Nauk'' , '''2''' : 6 (1947) pp. 159–173 (In Russian)</TD></TR></table>
| |
over a field $K$
A Lie algebra $\mathfrak{g}$ whose elements are linear transformations of a vector space $V$ over $K$; addition of elements and multiplication of them by elements of $K$ are defined in the usual way, and the commutator $[x,y]$ of two elements $x,y \in \mathfrak{g}$ is given by the formula
$$
[x,y] = xy - yx
$$
($xy$ and $yx$ are the usual products of linear transformations). The linear Lie algebra consisting of all linear transformations of $V$ is denoted by $\mathfrak{gl}(V)$. If $V = K^n$, then $\mathfrak{gl}(V)$ is naturally identified with the set of all square matrices of order $n$ over $K$ and is denoted by $\mathfrak{gl}(n,K)$. Any linear Lie algebra is a subalgebra of some Lie algebra $\mathfrak{gl}(V)$.
Examples. 1) Let $V$ be endowed with an associative algebra structure. Then all derivations (cf. Derivation in a ring) of $V$ form a linear Lie algebra. If $V$ is a Lie algebra, then for a fixed element $x \in V$ the linear transformation of $V$ adjoint to $x$, defined by the formula $y \mapsto [x,y]$, $y \in V$, is a derivation of $V$; it is denoted by $\mathrm{ad} x$. The set
$$
\mathrm{ad} V = \{ \mathrm{ad} x : x \in V \}
$$
is a linear algebra, called the adjoint linear Lie algebra or the Lie algebra of inner derivations of $V$.
2) Let $K$ be a field that is complete with respect to some non-trivial absolute value, let $V$ be a normed complete space over $K$ and let $G$ be a linear Lie group of transformations of $V$, that is, a Lie subgroup of the Lie group of all automorphisms of $V$. Then the Lie algebra of the analytic group $G$ (cf. Lie algebra of an analytic group) is naturally identified with a Lie subalgebra of $\mathfrak{gl}(V)$, that is, it is a linear Lie algebra.
The problem of the existence of an isomorphism of an arbitrary finite-dimensional Lie algebra to some linear Lie algebra had already arisen in the first papers on group theory and Lie algebras, but it was affirmatively solved only in 1935 by Ado's theorem (see [4]): Every finite-dimensional Lie algebra $\mathfrak{g}$ over a field of characteristic zero has a faithful finite-dimensional representation $\rho$ (moreover, if $\mathfrak{n}$ is the largest nilpotent ideal of $\mathfrak{g}$, then $\rho$ can be chosen so that all elements of $\rho(\mathfrak{n})$ are nilpotent, cf. also Representation of a Lie algebra). The analogue of this theorem for Lie groups does not hold, in general; for example, the universal covering of the group of real unimodular matrices of order 2 does not have a faithful linear representation.
See also Lie algebra, algebraic.
References
[1] | L.S. Pontryagin, "Topological groups" , Princeton Univ. Press (1958) (Translated from Russian) |
[2] | N. Bourbaki, "Elements of mathematics. Lie groups and Lie algebras" , Addison-Wesley (1975) (Translated from French) |
[3] | J.-P. Serre, "Lie algebras and Lie groups" , Benjamin (1965) (Translated from French) |
[4] | I.D. Ado, "The representation of Lie algebras by matrices" Uspekhi Mat. Nauk , 2 : 6 (1947) pp. 159–173 (In Russian) |