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In , a unipotent element r of a ring R is one such that r − 1 is a nilpotent element; in other words, ( r − 1) n is zero for some n.

In particular, a M is a unipotent matrix if and only if its characteristic polynomial P( t) is a power of t − 1. Thus all the of a unipotent matrix are 1.

The term quasi-unipotent means that some power is unipotent, for example for a diagonalizable matrix with eigenvalues that are all roots of unity.

In the theory of , a group element is unipotent if it acts unipotently in a certain natural group representation. A unipotent affine algebraic group is then a group with all elements unipotent.


Definition

Definition with matrices
Consider the group \mathbb{U}_n of upper-triangular matrices with 1's along the diagonal, so they are the group of matrices
\mathbb{U}_n = \left\{
\begin{bmatrix} 1 & * & \cdots & * & * \\ 0 & 1 & \cdots & * & * \\ \vdots & \vdots & &\vdots & \vdots \\ 0& 0& \cdots & 1 &* \\ 0 & 0 & \cdots & 0 & 1 \end{bmatrix} \right\}. Then, a unipotent group can be defined as a of some \mathbb{U}_n. Using scheme theory the group \mathbb{U}_n can be defined as the
\text{Spec}\left(
\frac{\mathbb{C}\!\leftx_{11},x_{12},\ldots,}{
   (x_{ii} = 1, x_{i > j} = 0)
     
} \right) and an affine group scheme is unipotent if it is a closed group scheme of this scheme.


Definition with ring theory
An element x of an affine is unipotent when its associated right translation operator, r x, on the affine coordinate ring A G of G is locally unipotent as an element of the ring of of AG. (Locally unipotent means that its restriction to any finite-dimensional stable subspace of A G is unipotent in the usual ring-theoretic sense.)

An affine algebraic group is called unipotent if all its elements are unipotent. Any unipotent algebraic group is to a closed subgroup of the group of upper triangular matrices with diagonal entries 1, and conversely any such subgroup is unipotent. In particular any unipotent group is a , though the converse is not true (counterexample: the diagonal matrices of GL n( k)).

For example, the standard representation of \mathbb{U}_n on k^n with standard basis e_i has the fixed vector e_1.


Definition with representation theory
If a unipotent group acts on an , all its orbits are closed, and if it acts linearly on a finite-dimensional then it has a non-zero fixed vector. In fact, the latter property characterizes unipotent groups. In particular, this implies there are no non-trivial semisimple representations.


Examples

Un
Of course, the group of matrices \mathbb{U}_n is unipotent. Using the lower central series
\mathbb{U}_n = \mathbb{U}_n^{(0)} \supset \mathbb{U}_n^{(1)} \supset \mathbb{U}_n^{(2)} \supset \cdots \supset \mathbb{U}_n^{(m)} = e
where
\mathbb{U}_n^{(1)} = \mathbb{U}_n,\mathbb{U}_n and \mathbb{U}_n^{(2)} = \mathbb{U}_n,
there are associated unipotent groups. For example, on n = 4, the central series are the matrix groups
\mathbb{U}_4 = \left\{
\begin{bmatrix} 1 & * & * & * \\ 0 & 1 & * & * \\ 0 & 0 & 1 & * \\ 0 & 0 & 0 & 1 \end{bmatrix} \right\}, \mathbb{U}_4^{(1)} = \left\{ \begin{bmatrix} 1 & 0 & * & * \\ 0 & 1 & 0 & * \\ 0 & 0 & 1 & 0 \\ 0 & 0 & 0 & 1 \end{bmatrix} \right\}, \mathbb{U}_4^{(2)} = \left\{ \begin{bmatrix} 1 & 0 & 0 & * \\ 0 & 1 & 0 & 0 \\ 0 & 0 & 1 & 0 \\ 0 & 0 & 0 & 1 \end{bmatrix} \right\}, and \mathbb{U}_4^{(3)} = \left\{ \begin{bmatrix} 1 & 0 & 0 & 0 \\ 0 & 1 & 0 & 0 \\ 0 & 0 & 1 & 0 \\ 0 & 0 & 0 & 1 \end{bmatrix} \right\} given some induced examples of unipotent groups.


Gan
The additive group \mathbb{G}_a is a unipotent group through the embedding
a \mapsto \begin{bmatrix}
1 & a\\ 0 & 1 \end{bmatrix} Notice the matrix multiplication gives
\begin{bmatrix}
1 & a \\ 0 & 1 \end{bmatrix} \cdot \begin{bmatrix} 1 & b \\ 0 & 1 \end{bmatrix} = \begin{bmatrix} 1 & a + b \\ 0 & 1 \end{bmatrix} hence this is a group embedding. More generally, there is an embedding \mathbb{G}_a^n \to \mathbb{U}_{n+1} from the map
(a_1,\ldots, a_n) \,\mapsto \begin{bmatrix}
1 & a_1 & a_2 & \cdots & a_{n-1} &a_n \\ 0 & 1 & 0 & \cdots & 0 & 0 \\ \vdots & \vdots & \vdots & & \vdots & \vdots \\ 0 & 0 & 0 & \cdots &1 & 0 \\ 0 & 0 & 0 & \cdots &0 & 1 \end{bmatrix}

Using scheme theory, \mathbb{G}_a is given by the

\mathcal{O}:\textbf{Sch}^{op} \to \textbf{Sets}
where
(X,\mathcal{O}_X) \mapsto \mathcal{O}_X(X)


Kernel of the Frobenius
Consider the functor \mathcal{O} on the \textbf{Sch}/\mathbb{F}_p, there is the subfunctor \alpha_p where
\alpha_p(X) = \{ x \in \mathcal{O}(X) : x^p = 0 \}
so it is given by the kernel of the Frobenius endomorphism.


Classification of unipotent groups over characteristic 0
Over characteristic 0 there is a nice classification of unipotent algebraic groups with respect to nilpotent Lie algebras. Recall that a nilpotent Lie algebra is a subalgebra of some \mathfrak{gl}_n such that the iterated adjoint action eventually terminates to the zero-map. In terms of matrices, this means it is a subalgebra \mathfrak{g} of \mathfrak{n}_n, the matrices with a_{ij} = 0 for i \leq j.

Then, there is an equivalence of categories of finite-dimensional nilpotent Lie algebras and unipotent algebraic groups.page 261 This can be constructed using the Baker–Campbell–Hausdorff series H(X,Y), where given a finite-dimensional nilpotent Lie algebra, the map

H:\mathfrak{g}\times\mathfrak{g} \to \mathfrak{g} \text{ where } (X,Y)\mapsto H(X,Y)
gives a Unipotent algebraic group structure on \mathfrak{g}.

In the other direction the exponential map takes any nilpotent square matrix to a unipotent matrix. Moreover, if U is a commutative unipotent group, the exponential map induces an from the Lie algebra of U to U itself.


Remarks
Unipotent groups over an algebraically closed field of any given dimension can in principle be classified, but in practice the complexity of the classification increases rapidly with the dimension, so some tend to give up somewhere around dimension 6.


Unipotent radical
The unipotent radical of an G is the set of unipotent elements in the radical of G. It is a connected unipotent normal subgroup of G, and contains all other such subgroups. A group is called reductive if its unipotent radical is trivial. If G is reductive then its radical is a torus.


Decomposition of algebraic groups
Algebraic groups can be decomposed into unipotent groups, multiplicative groups, and abelian varieties, but the statement of how they decompose depends upon the characteristic of their base field.


Characteristic 0
Over characteristic 0 there is a nice decomposition theorem of a commutative algebraic group G relating its structure to the structure of a linear algebraic group and an . There is a short exact sequence of groupspage 8
0 \to M\times U \to G \to A \to 0
where A is an abelian variety, M is of multiplicative type (meaning, M is, geometrically, a product of tori and algebraic groups of the form \mu_n) and U is a unipotent group.


Characteristic p
When the characteristic of the base field is p there is an analogous statement for an algebraic group G: there exists a smallest subgroup H such that

  1. G/H is a unipotent group
  2. H is an extension of an abelian variety A by a group M of multiplicative type.
  3. M is unique up to commensurability in G and A is unique up to .


Jordan decomposition
Any element g of a linear algebraic group over a can be written uniquely as the product g = g u g s of commuting unipotent and elements g u and g s. In the case of the group GL n( C), this essentially says that any invertible matrix is conjugate to the product of a diagonal matrix and an upper triangular one, which is (more or less) the multiplicative version of the Jordan–Chevalley decomposition.

There is also a version of the Jordan decomposition for groups: any commutative linear algebraic group over a perfect field is the product of a unipotent group and a semisimple group.


See also

  • A. Borel, Linear algebraic groups,

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