Relative root system
of a connected reductive algebraic group defined over a field k
A system \Phi _{k} (S,\ G)
of non-zero weights of the adjoint representation of a maximal k -
split torus S
of the group G
in the Lie algebra \mathfrak g
of this group (cf. Weight of a representation of a Lie algebra). The weights themselves are called the roots of G
relative to S .
The relative root system \Phi _{k} (S,\ G) ,
which can be seen as a subset of its linear envelope L
in the space X(S) \otimes _ {\mathbf Z} \mathbf R ,
where X(S)
is the group of rational characters of the torus S ,
is a root system. Let N(S)
be the normalizer and Z(S)
the centralizer of S
in G .
Then Z(S)
is the connected component of the unit of the group N(S) ;
the finite group W _{k} (S,\ G) = N(S)/Z(S)
is called the Weyl group of G
over k ,
or the relative Weyl group. The adjoint representation of N(S)
in \mathfrak g
defines a linear representation of W _{k} (S,\ G)
in L .
This representation is faithful and its image is the Weyl group of the root system \Phi _{k} (S,\ G) ,
which enables one to identify these two groups. Since two maximal k -
split tori S _{1}
and S _{2}
in G
are conjugate over k ,
the relative root systems \Phi _{k} (S _{i} ,\ G)
and the relative Weyl groups W _{k} (S _{i} ,\ G) ,
i=1,\ 2 ,
are isomorphic, respectively. Hence they are often denoted simply by \Phi _{k} (G)
and W _{k} (G) .
When G
is split over k ,
the relative root system and the relative Weyl group coincide, respectively, with the usual (absolute) root system and Weyl group of G .
Let g _ \alpha
be the weight subspace in \mathfrak g
relative to S ,
corresponding to the root \alpha \in \Phi _{k} (S,\ G) .
If G
is split over k ,
then \mathop{\rm dim}\nolimits \ g _ \alpha = 1
for any \alpha ,
and \Phi _{k} (G)
is a reduced root system; this is not so in general: \Phi _{k} (G)
does not have to be reduced and \mathop{\rm dim}\nolimits \ g _ \alpha
can be greater than 1. The relative root system \Phi _{k} (G)
is irreducible if G
is simple over k .
The relative root system plays an important role in the description of the structure and in the classification of semi-simple algebraic groups over k .
Let G
be semi-simple, and let T
be a maximal torus defined over k
and containing S .
Let X(S)
and X(T)
be the groups of rational characters of the tori S
and T
with fixed compatible order relations, let \Delta
be a corresponding system of simple roots of G
relative to T ,
and let \Delta _{0}
be the subsystem in \Delta
consisting of the characters which are trivial on S .
Moreover, let \Delta _{k}
be the system of simple roots in the relative root system \Phi _{k} (S,\ G)
defined by the order relation chosen on X(S) ;
it consists of the restrictions to S
of the characters of the system \Delta .
The Galois group \Gamma = \mathop{\rm Gal}\nolimits (k _{s} /k)
acts naturally on \Delta ,
and the set \{ \Delta ,\ \Delta _{0} , \textrm{ the action of } \Gamma \textrm{ on } \Delta \}
is called the k -
index of the semi-simple group G .
The role of the k -
index is explained by the following theorem: Every semi-simple group over k
is uniquely defined, up to a k -
isomorphism, by its class relative to an isomorphism over k _{s} ,
its k -
index and its anisotropic kernel. The relative root system \Phi _{k} (G)
is completely defined by the system \Delta _{k}
and by the set of natural numbers n _ \alpha ,
\alpha \in \Delta _{k} (
equal to 1 or 2), such that n _ \alpha \alpha \in \Phi _{k} (G)
but (n _ \alpha + 1) \alpha \notin \Phi _{k} (G) .
Conversely, \Delta _{k}
and n _ \alpha ,
\alpha \in \Delta _{k} ,
can be determined from the k -
index. In particular, two elements from \Delta \setminus \Delta _{0}
have one and the same restriction to S
if and only if they are located in the same orbit of \Gamma ;
this defines a bijection between \Delta _{k}
and the set of orbits of \Gamma
into \Delta \setminus \Delta _{0} .
If \gamma \in \Delta _{k} ,
if O _ \gamma \subset \Delta \setminus \Delta _{0}
is the corresponding orbit, if \Delta ( \gamma )
is any connected component in \Delta _{0} \cup O _ \gamma
not all vertices of which lie in \Delta _{0} ,
then n _ \gamma
is the sum of the coefficients of the roots \alpha \in \Delta ( \gamma ) \cap O _ \gamma
in the decomposition of the highest root of the system \Delta ( \gamma )
in simple roots.
If k = \mathbf R , \overline{k} = \mathbf C , then the above relative root system and relative Weyl group are naturally identified with the root system and Weyl group, respectively, of the corresponding symmetric space.
References
[1] | J. Tits, "Sur la classification des groupes algébriques semi-simples" C.R. Acad. Sci. Paris , 249 (1959) pp. 1438–1440 MR0106967 |
[2] | A. Borel, J. Tits, "Groupes réductifs" Publ. Math. IHES , 27 (1965) pp. 55–150 MR0207712 Zbl 0145.17402 |
[3] | J. Tits, "Classification of algebraic simple groups" , Algebraic Groups and Discontinuous Subgroups , Proc. Symp. Pure Math. , 9 , Amer. Math. Soc. (1966) pp. 33–62 |
Relative root system. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Relative_root_system&oldid=44284