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Case i: q ; 0. From the description of the injective hull R of the module M (Lemma 12) there
follows that in this case either V = Q or V = R. Case 2: q = 0. Then from Lemma 13 either
u = M, or V = R, or V = N. Thus, one has in all five indecomposable KT3-modules KT 3 such that
V'J = 0 follows from Lemma 9 (i). The theorem is proved.
Proof of Theorem 2. It follows from Lemma 2 and from Theorem 2 of [4].
.
2.
3.
4.
5.
LITERATURE CITED
A. Clifford and G. Preston, The Algebraic Theory of Semigroups, Vol. i, Am. Math. Soc., Providence (1961). C. W. Curtis and I. Reiner, Representation Theory of Finite Groups and Associative Algebras, Wiley, New York (1962). I. S. Ponizovskii, "On modules over semigroup rings of completely 0-simple semigroups," in: Modern Algebra [in Russian], Leningrad Univ., Leningrad (1981), pp. 85-94. I. S. Ponizovskii, "On algebras with a finite number of classes of indecomposable non- equivalent modules," Zap. Nauchn. gem. Leningr. Otd. Mat. Inst., 132, 122-128 (1983). I. S. Ponizovskii, "On matrix representations of semigroups," in: Eighteenth All-Union Algebra Conference. Abstracts, Kishinev (1985), p. 105.
BRUHAT DECOMPOSITION DECOMPOSITION OF ROOT SEMISIMPLE SUBGROUPS
IN THE SPECIAL LINEAR GROUP
A. V. Yakovlev UDC 519.46
It is proved that the root semisimple subgroups in the special linear group over a
field intersects at most four cosets in the Bruhat decomposition and, moreover, most
elements of the given subgroup lie in the same coset, with the remaining elements ly-
ing in distinct cosets.
In this paper we indicate which classes in the Bruhat decomposition can be intersected
by a given root semisimple subgroup in the special linear group over a field. We recall that
by a root semisimple element in the special linear group F = SL(n, K) of degree n over a field
K we mean an element that is conjugate in this group with the element d (~) = diag (s, s -I,
i, ..., i). By a root semisimple subgroup we mean a one-parameter subgroup ~={~$($)~-~, ~E K*}
where x e F. The necessary facts on the Bruhat decomposition can be found, for example, in
[ 3 ] , [ 9 ] .
It is known that, for the elements of the subgroup of one-dimensional transformations,
the element of the Weyl group, occurring in the Bruhat decomposition, does not depend on the
value of the nonunit eigenvalue of this transformation (see [4]). This fact has allowed us
to look from a more general point of view at the technique of the extraction of transvections,
applied in [i], [2] for solving problems of describing subgroups of the full linear group,
containing the group of diagonal matrices. The same result has been obtained for microweight
elements in the special linear group, i.e., for elements that are conjugate with diag(g .....
s, i , . . . , I ) [ 6 ] .
Translated from Zapiski Nauchnykh Seminarov Leningradskogo Otdeleniya Matematicheskogo Instituta im. V. A. Steklova AN SSSR, Vol. 160, pp. 239-246, 1987.
3178 0090-4104/90/5203-3178512.50 �9 1990 Plenum Publishing Corporation
However, already from [5] it is clear that in the case of two-dimensional transforma-
tions, a given subgroup may intersect more than two classes. We have succeeded to establish
that, nevertheless, in this case a given root semisimple subgroup lies almost entirely in
one class and only for at most three values of the parameter, including also the identity
i, the element xdl2(g)x -I is in other classes. We describe explicitly all the possibilities
that occur here. We mention that from the obtained result there follows the possible form
of the Bruhat decomposition of long root semisimple subgroups in the symplectic group, having
the same form as the root semisimple subgroups in F.
A similar description presents interest in connection with the problem of the description
of the subgroups of the special linear and symplectic groups, containing the group of diagonal
matrices. For example, it becomes clear the nature of the outwardly artificial methods in
the computations that serve the purpose of discovering the transvections in a symplectic
group [7]. We mention one more result, closely related to the problem solved here. In [8]
it has been established how a given root subgroup intersects the normalizer of the maximal
torus, in our case, the group of monomial matrices.
Formulation of the Fundamental Result
THEOREM. Let x e SL(n, K). A given root semisimple subgroup U x intersects at most four
double classes BwB and, moreover, most of its elements xdl2(s)x -l lie in the same class (the
generic case), while the remaining classes contain each at most one element (the degenerate
case). All the p~ssibilities are given in Table 1 (we indicate only the elements of the Weyl
group, generating the classes). We use the following notations: wil,..o,i k is the matrix
of permutation o = (i I ..... ik), rearranging cyclically il ..... ik, i.e., the matrix whose
(i, j)-entry is the element 6i,o(j) ; e is the identity matrix. We mention that in the formu-
lation of the theorem the relations between the indices are not indicated since this would
lead to a considerable extension of the table and would diminish its clarity. All the occur
ing variants are explicitly indicated in the proof.
Bruhat Decomposition of Two-Dimensional Transformations
We precede the proof of the theorem by the investigation of a somewhat more general situa-
tion~ Let d = diag(~, D, 1 ..... I). We establish the manner in which an element of the
Weyl group appears in the Bruhat decomposition of the two-dimensional transformation y = xdx -I
as a function of s and ~. We use the following standard notations: e is the identity matrix,
eij is the matrix whose unique nonzero element is equal to 1 and is in the i-th row and j-th
column, and tij($) = e + geij. If x = d0u0w0v0 is the reduced Bruhat right decomposition
of the matrix x, x e GL(n, K), then the element of the Weyl group in the decomposition of
the transformation y will coincide with the permutation in the decomposition of the matrix
z = w0v0dvolwo I and we restrict ourselves to the consideration of the latter. We mention that
the matrix v0dv~ I differs from the identity matrix only by the elements of the first two rows.
We denote them by a~, ..., a n and bl, ..., bn, respectively. If the elements of the matrix -I !
v 0 are denoted by vij, then it can be easily seen that
3179
TABLE 1
No. generic case degenerate case
(*)
In turn, the matrix z differs from the identity matrix only by the elements of the rows with
indices w0(1) and w0(2).
i. The case ~(4)<u~Ci'.
We set tff~(~= p, %~(s . The matrix z = (zij) is
Here i, j, r, s = i, ..., n and r ~ p, q. Since the multiplication of the given matrix on
the left and on the right by an upper triangular matrix does not change the element of the
Weyl group, occurring in its Bruhat decomposition, we consider the matrix z I = ~ ~ to4~-a~>
~,4.<~,<@~ , �9 In zz, in the columns with indices p + i, ..., q - l in the p-th row and
in the columns with the indices q + i, .. ~ n in the p-th and q-th rows we have zeros, the
remaining elements being the same as in the matrix z.
Now it is necessary to distinguish several cases.
i.i. In the matrix zz we have ~4=..=~p-~.=~ ..... }~.4=0
of linear equations with respect to g and q:
[ - u ' ~.K
This is equivalent to the system
~/--9/.=0. In this case, for any e and q the Here nontrivial solutions exist only for ~k- ~
matrix w is the identity matrix.
1.2. Assume that in the q-th row of the matrix zl there exists an element ~r ~ 0 such
that ~I ..... ~-4=~ ..... )~-4=0 and r < p (this, just as in the case i.i, depends only on the
3180
matrix v0). We multiply z~ o n the left by ~p~(-#~ ~) �9 We obtain the matrix z=, in the p-th
row of which one has the elements Sk=Ak-#$~#k ~ k=~,..~. We have two possibilities:
1.2.1. Among ~, ..., yp_~ there exist nonzero ones. Let s be the smallest of indices
for which Ys ~ 0. Then from [5], taking into account that 7p, E ~ 0, we obtain the value
: ~ = ~ p �9 Condition ~s ~ 0, is equivalent to ~)~-~#~0 and, introducing the cor- i I I I
responding values from (*), we obtain ~kg~-~k~0, Thus, the fact that Ys r 0 depends
only on v0.
1.2.2. If, however, y~ ..... ~p are zero (this depends again only on v0), then from
[5] we obtain that w = Wrq and case 1.2 has been completely examined.
1.3. If in the p-th row of the matrix z~ there is an element ~ ..... ~.~=# ..... ~_~=0~ #~0
for s > r (depends only on vo), then we have to consider three cases:
1.3.1 s < p. We multiply z I by ~ t~) ~ ~(-~4~) on the right and by its inverse
on the left. The result will be the matrix z s in which only the columns with the indices r,
s, p, q differ from the corresponding columns of the identity matrix. We write down those
elements of these columns which are in the rows r, s, p, q:
i 000ii 00 i As before, we bring the matrix z s to monomial form, multiplying it on the left and on the
right by appropriate upper triangular matrices: on the left by ~p(-f~)~5~#~ ~) and on the
right by ~p~ ~)'~(~-~)~)'~ ' and finally on the right by ~5~(-/$~)~-~(~-~)~) We have
obtained, to within a diagonal factor, the permutation matrix w = WrpWsq we are interested in,
and again its form does not depend on the values of E and n-
1.3.2. p < s < q (depends exclusively on v0). Conjugating the matrix z I in the same
way as in Seco 1.3.1, we obtain a matrix of the following form:
li 0 0 0 &p 0 0 0 4 0 0 0 4
It is easy to derive that for it we have w = Wrp = Wsq.
1.3.3. s = q. We conjugate z I with the aid of the matrix ~+~-~i.<~ -4~ %~i(.~ -4 ~i) ~ and then
we multiply by L~p (- ~ ) ' ~p~ (-~ &~) on the left and by %~ (-~ gp) on the right. After
this it is obvious that w = Wrp-
1.4. If, however, in the matrix z I we have ~ ..... ~p_~=}~=. =~4=0, ~s~0~ ~<s<~, then, after
the conjugation of z I with the aid of the matrix ~ ~i(~i) and multiplication by
3181
~(-#s~1~-~p~)~ '~ " -~ on the left and by tsq(--~ ~) on the right, it becomes clear that w = W s q .
Case i has been completely examined.
2. The case ~14)>~0(~.
Assume that, by the conjugation by the matrix w 0, the elements of the first row of the
matrix v0dv~ ~ go into the elements of the q-th row of the matrix z, while the elements of
the 2nd row go into the elements of the p-th row. The matrix z will be the following:
~pi=e~i , where d~=~,d~=0, Giq,0(k)=(~-4)ViK for k~4,~, r~l / / I
, , , , h e r e f o r
In the same way as in Case i, we shall assume that gp+~=,..=~4=&~+~ ,..=ib=~+~=..,=#~=O(if neces-
sary, we multiply the matrix z on the left by appropriate upper triangular matrices).
2.1. Let ,,l,~=...=,~pq=.~4=.,,=pp.~=O this, as before, depends only on the matrix v 0.
2.1.1. We assume that ~p=(~-~)~O . Then we multiply z on the right by ~J
and on the left by E ~pi(&pf/~i ) ; we obtain a matrix with a unique nonzero off-diagonal
element:
which, after multiplication by ~p~p{Ap)- on the left and by ~_#~#~],-4 on the right, yields
a matrix that differs from Wpq by a diagonal factor.
2.1.2. If, however, ~p = 0, then, depending on whether the equality ~p+4=...=#~-4 = 0 holds
or not, we obtain the permutation Wsq or e. However, the validity of the equality for ~ = I and also for v~ = 0 depends only on the matrix v 0.
2.2. We assume now that &~ .... =A~4=~=...=~=O~&~@O. The fact that the first r -- 1 ele-
ments of the p-th and q-th rows vanish simultaneously depends exclusively on the matrix v0;
i (g-~)i~(~q)~;=~0, here w0(k) = however, the condition ~0~ #~=0 (in other words, F~k~0, I -- ! _
r) will be satisfied either for ~k-9~-0 for all e and ~ but if ~90 then only for
6=(~k-9~k(~-~)).(~i) -4 Let s be the smallest index for which Ss ~ 0. As in [5], we shall
consider several cases.
2.2.1. s < p. The condition ~+4=. ~#s=0
appear in the following manner:
forms a homogeneous system, whose equations
/ / 1
If the pairs (~r~ are proportional for the considered j and vzj ~ 0, then the system _ I l / , ~.~
is consistent for ~-(q~i'~ii(4-{)'(9~i) ; otherwise, the consistency of the system depends only !
on the matrix v 0. In [5] it is shown that if )p=(~-~)~=0 then the element of the Weyl
q§ group we are interested in is %r ; otherwise w = Wrpsq. We note that for t
3182
condition $p = 0 is satisfied, by virtue of what has been said in 2.2, t ~! - - J (4-~))'($~f~ , i .e . , only for @~k-~4k.
2.2.2. s = p, according to [5], yields w = Wrp q and is encounterd for ~# 0
therefore, only for c and q that satisfy the relations from 2.2; moreover,
!
for ~: ~= (t~/k- ~ ~'k
and,
' = 0, i.e. because of the matrix v 0 or for c = q 2.2.3. p < s < q occurs either for vi2
in the situation described in case 2.2.1. The unknown here turns out to be ~=~p~
2.2.4. Finally, s = q can arise under the same conditions as in case 2.2.3; the element
of the Weyl group will be the transposition w = Wrp.
2.3. Assume that the matrix z satisfies the following conditions:
~,~=.,.=:c~..~=#4=...=j~_~=O , ),~-~0~ ,~<p.
The possible form of the elements of the Weyl group for this situation is found in Sec. 3
of [5]. We shall find out what determines the appearance of a certain permutation for these
elements.
We multiply z on the left by ~pr �9 In the p-th row of the obtained matrix we
have the elements ~=a~-#$~#~ and, moreover, ~i = .-- = Yr = 0. Assume, as usually, that s
is the smallest index for which u ~ 0. We have two possibilities:
2.3.1. s < p. The result in this case depends on the value of the element ~=gp-~pg~#~.
If yp ~ 0, then the element of the Weyl group is w = WrqWsp; if, however, yp = 0, then w =
Wrqsp. The equality yp = 0 can be written in the following manner:
~P =0 I (r~-4) 'O';k ~ !=0,
if k=~(~) This is equivalent to the equation ~(~q)~kC~-~-O~=O, We mention that
the left-hand side of this equation cannot be identically equal to zero since then it turns
out that also #~=0.
2.3.2. s = p. As before, the result depends on ~p. If yp ~ 0, then w = Wrq , otherwise
w = Wrp q. In conclusion we note that the vanishing of the elements yj, j = r + i, .... s - I,
is equivalent to the simultaneous vanishing of the determinants
% <t
and depends only on the matrix v 0.
Proof of the Theorem
We apply the just obtained results to the case q = c -z. For the sake of brevity, we
shall omit mentioning the obvious degeneration for c = i. We need the notation 6i=-~
Everywhere we shall assume that ~<s<5~<p<~<~<~.
3183
The case described at i.i is in the first row of Table i. From 1.2.1, where the generic
case is WrqWsp, we find ourselves in the sixth row, while from 1.2.2 (the generic case is
Wrq) is row 2. From 1.3.1, where WrpWsq degenerates to WrpWszq, we fall in row 6 and 1.3.2
gives again the result of the sixth row for WrpWsq. The cases 1.3.3 and 1.4 give Wrp and
Wsq , respectively, in the second row of the table.
We note that for w0(1) < w0(2) the degenerations occur only in the trivial case.
T The results of 2.1.1 and 2.1.2 for v12 ~ 0 yield the third row. In this case the degenera-
tion of Wsq to Wsz q occurs for ~ = ~-I = --i. If, however, vz2 = 0, then we obtain the result
indicated either in the second or in the first row.
Now we consider the variants, occurring in 2.2. If Vlk' = vz2' = 0, then, depending on
the matrix v0, we obtain the generic case WrpWsq with degeneration for ~ = s~ to WrpWsl q
(2.2.1) or to WrpW~q (2.2.3), or to Wrp (2.2.4). Thus, we obtain the rows 7 or 8. No other
generic case can occur in the case described in 2.2.3: WrpW~q with degenerator for WrpW~q
(2.2.3) or to Wrp (2.2.4), which again gives the results indicated in rows 7 and 8.
We proceed to the consideration of the situation from 2.3. The generic case WrpWsq
(2.3.1) may degenerate for ~=(g~#-~ to Wrqsp (2.3.1) while if ~=~-~ then we find our-
selves in 2.2.1, while the result, equal to Wrpsq, gives us the ninth row of the formulation.
This same generic case for ~=~=g~ =-~ gives us, according to 2.2.1, WrpWsq (row 7) or, if
there are sufficiently many zero elements in the q-th row of the matrix v0dv~ I, then from
2.2.3 we conclude that for the same value of g we have a degeneration to Wr~Wpq (row 7) and,
possibly, according to 2.2.4, to Wrp (row 8).
Finally, from 2.3.2 the generic case, equal to Wrq, is possible, which, for g=(s
degenerates to Wrqp, while for g=g~@~ to Wrp q (2.2.2). This is the result of row 4. If, how-
ever, g=~:-~ then in this case the degeneration of the transposition Wrq will be either
Wr~Wpq (2.2.3) or Wrp (2.2.4). We have obtained rows 5 and 3 from the formulation of the
theorem and the proof is concluded.
LITERATURE CITED
i. Z.I. Borevich, "The description of the subgroups of the general linear group that con- tain the group of diagonal matrices," Zap. Nauchn. Sem. Leningr. Otd. Mat. Inst., 64,
12-29 (1976). 2. Z.I. Bor~vich and N. A. Vavilov, "Subgroups of the general linear group over a semilocal
ring that contain a group of diagonal matrices," Trudy Mat. Inst. Akad. Nauk SSSR, 148,
43-57 (1978). 3. N. Bourbaki, Groupes et Algebres de Lie, Chaps. 4-6, Hermann, Paris (1968). 4. N.A. Vavilov, "The Bruhat decomposition of one-dimensional transformations," Vestn.
Leningr. Univ. Ser. I, No. 3, 14-20 (1986). 5. N.A. Vavilov, "The Bruhat decomposition of two-dimensional transformations," Vestn.
Leningr. Univ. Ser. I, No. 2, 3-8 (1987). 6. N.A. Vavilov, "The Bruhat decomposition of weight elements in Chevalley groups," in:
Eighteenth All-Union Algebra Conference. Abstracts of Communications, Part I, Kishinev (1985), p. 75.
7. N.A. Vavilov and E. V. Dybkova, "Subgroups of the general symplectic group containing the group of diagonal matrices," Zap. Nauchn. Sem. Leningr. Otd. Mat. Inst., 103, 31-47
(1980).
3184
,
9 .
A. E. Zalesski, Semisimple root elements of algebraic groups. Preprint Inst. Mat. Akad Nauk BSSR, No. 13(93), Minsk (1980). J. E. Humphreys, Arithmetic Groups, Lecture Notes in Math., No. 789, Springer, Berlin (198o).
INVESTIGATION ON THE BESM-6 COMPUTER OF THE STRUCTURE OF THE
NILPOTENT SERIES FOR THE METABELIAN 2-GENERATED GROUP OF
EXPONENT 27
A . I. Skopin UDC 519.~5
A special symbolic form for the notation of the elements of a 2-generated metabelian
group is realized on a computer, with the aid of which for the exponent 27 one car-
ries out the search of the relations in the factors of the lower central series. The
first 36 factors are investigated.
This paper is based on the LOMI preprint [i], published by the author on the same topic
and containing many technical details. Here the technical details, referring mainly to the
description of the programming methods, have been omitted and only the algebraic aspect of
the problem has been retained.
We study the additively written group G, having the following definition:
~--<x,yl (02) 2--0, 27 ~=0>.
We consider the nilpotent series of this group,
and we wish to give an explicit description (in terms of generators and defining relations)
of the factors M n = Gn/G n+1 of this series. A similar investigation (but "by hand") has been
carried out earlier for the exponents 8 and 9 (see [2]).
It is known (see, for example, [3]) that if in the definition of the group G the condi-
tion 27G = 0 is omitted, then for the free metabelian group G, defined by the single condition
(G2) = = 0, with generators x, y, the double sequence of monomials
Vk =r~ y .~ , -k yk-~ , ~ = i , 2 . . . . ; k = i , . . . , ~ . - i ( i )
forms (in the expression of the naturally used additive terminology) a basis, which will be
called F. Hall's basis of monomials. However, by adding the condition 27G = 0, i.e., in the
group exponent 27, investigated by us, the sequence (I) is a system of generators of this
group and we have to find relations for these generators.
In the first section we describe the obtained results: we enumerate the relations in
the factors M n, n <_ 36. (In order not to complicate the writing, we preserve without modifica-
Translated from Zapiski Nauchnykh Seminarov Leningradskogo Otdeleniya Matematicheskogo Instituta im. Vo A. Steklova AN SSSR, Vol. 160, pp. 247-256, 1987.
0090-4104/90/5203-3185512.50 �9 1990 Plenum Publishing Corporation 3185