Lie groups and Lie algebras
Classical groups General linear GL(n) Special linear SL(n) Orthogonal O(n) Special orthogonal SO(n) Unitary U(n) Special unitary SU(n) Symplectic Sp(n)
Simple Lie groups Classical An Bn Cn Dn Exceptional G2 F4 E6 E7 E8
Other Lie groups Circle Lorentz Poincaré Conformal group Diffeomorphism Loop Euclidean
Lie algebras Lie group–Lie algebra correspondence Exponential map Adjoint representation Killing form Index Simple Lie algebra Loop algebra Affine Lie algebra
Semisimple Lie algebra Dynkin diagrams Cartan subalgebra Root system Weyl group Real form Complexification Split Lie algebra Compact Lie algebra
Representation theory Lie group representation Lie algebra representation Representation theory of semisimple Lie algebras Representations of classical Lie groups Theorem of the highest weight Borel–Weil–Bott theorem
Lie groups in physics Particle physics and representation theory Lorentz group representations Poincaré group representations Galilean group representations
Scientists Sophus Lie Henri Poincaré Wilhelm Killing Élie Cartan Hermann Weyl Claude Chevalley Harish-Chandra Armand Borel
Glossary Table of Lie groups
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In the theory of algebraic groups, a Borel subgroup of an algebraic group G is a maximal Zariski closed and connected solvable algebraic subgroup. For example, in the general linear group GL_n (n x n invertible matrices), the subgroup of invertible upper triangular matrices is a Borel subgroup.

For groups realized over algebraically closed fields, there is a single conjugacy class of Borel subgroups.

Borel subgroups are one of the two key ingredients in understanding the structure of simple (more generally, reductive) algebraic groups, in Jacques Tits' theory of groups with a (B, N) pair. Here the group B is a Borel subgroup and N is the normalizer of a maximal torus contained in B.

The notion was introduced by Armand Borel, who played a leading role in the development of the theory of algebraic groups.

Parabolic subgroups

Subgroups between a Borel subgroup B and the ambient group G are called parabolic subgroups. Parabolic subgroups P are also characterized, among algebraic subgroups, by the condition that G/P is a complete variety. Working over algebraically closed fields, the Borel subgroups turn out to be the minimal parabolic subgroups in this sense. Thus B is a Borel subgroup when the homogeneous space G/B is a complete variety which is "as large as possible".

For a simple algebraic group G, the set of conjugacy classes of parabolic subgroups is in bijection with the set of all subsets of nodes of the corresponding Dynkin diagram; the Borel subgroup corresponds to the empty set and G itself corresponding to the set of all nodes. (In general, each node of the Dynkin diagram determines a simple negative root and thus a one-dimensional 'root group' of G. A subset of the nodes thus yields a parabolic subgroup, generated by B and the corresponding negative root groups. Moreover, any parabolic subgroup is conjugate to such a parabolic subgroup.) The corresponding subgroups of the Weyl group of G are also called parabolic subgroups, see Parabolic subgroup of a reflection group.

Example

Let ${\displaystyle G=GL_{4}(\mathbb {C} )}$. A Borel subgroup ${\displaystyle B}$ of ${\displaystyle G}$ is the set of upper triangular matrices

${\displaystyle \left\{A={\begin{bmatrix}a_{11}&a_{12}&a_{13}&a_{14}\\0&a_{22}&a_{23}&a_{24}\\0&0&a_{33}&a_{34}\\0&0&0&a_{44}\end{bmatrix)):\det(A)\neq 0\right\))$

and the maximal proper parabolic subgroups of ${\displaystyle G}$ containing ${\displaystyle B}$ are

${\displaystyle \left\((\begin{bmatrix}a_{11}&a_{12}&a_{13}&a_{14}\\0&a_{22}&a_{23}&a_{24}\\0&a_{32}&a_{33}&a_{34}\\0&a_{42}&a_{43}&a_{44}\end{bmatrix))\right\},{\text{ ))\left\((\begin{bmatrix}a_{11}&a_{12}&a_{13}&a_{14}\\a_{21}&a_{22}&a_{23}&a_{24}\\0&0&a_{33}&a_{34}\\0&0&a_{43}&a_{44}\end{bmatrix))\right\},{\text{ ))\left\((\begin{bmatrix}a_{11}&a_{12}&a_{13}&a_{14}\\a_{21}&a_{22}&a_{23}&a_{24}\\a_{31}&a_{32}&a_{33}&a_{34}\\0&0&0&a_{44}\end{bmatrix))\right\))$

Also, a maximal torus in ${\displaystyle B}$ is

${\displaystyle \left\((\begin{bmatrix}a_{11}&0&0&0\\0&a_{22}&0&0\\0&0&a_{33}&0\\0&0&0&a_{44}\end{bmatrix)):a_{11}\cdot a_{22}\cdot a_{33}\cdot a_{44}\neq 0\right\))$

This is isomorphic to the algebraic torus ${\displaystyle (\mathbb {C} ^{*})^{4}={\text{Spec))(\mathbb {C} [x^{\pm 1},y^{\pm 1},z^{\pm 1},w^{\pm 1}])}$.^[1]

Lie algebra

For the special case of a Lie algebra ${\displaystyle {\mathfrak {g))}$ with a Cartan subalgebra ${\displaystyle {\mathfrak {h))}$, given an ordering of ${\displaystyle {\mathfrak {h))}$, the Borel subalgebra is the direct sum of ${\displaystyle {\mathfrak {h))}$ and the weight spaces of ${\displaystyle {\mathfrak {g))}$ with positive weight. A Lie subalgebra of ${\displaystyle {\mathfrak {g))}$ containing a Borel subalgebra is called a parabolic Lie algebra.