• 検索結果がありません。

LIE STRUCTURES ON f[x,,•••,x.,y]1(y3-3py-q)By Fujio KuBo

N/A
N/A
Protected

Academic year: 2021

シェア "LIE STRUCTURES ON f[x,,•••,x.,y]1(y3-3py-q)By Fujio KuBo"

Copied!
6
0
0

読み込み中.... (全文を見る)

全文

(1)

Bull. Kyushu Inst. Tech.

(Math. Natur. Sci.) No. 35, 1988, pp. 1-6

LIE STRUCTURES ON f[x,,•••,x.,y]1(y3-3py-q)

By Fujio KuBo

(Received November 27, 1987)

1. Introduction

The Poisson Lie structures have been investigated in many papers (for example Berezin [2]). Recently Kubo and Mimura [4] extended these Lie structures to

commutative associative algebras containing a finite-dimensional Lie algebra and studied Lie structures on f[x,,..., x., y]1(y2-2ay+b) (a,bEf[x,,..., jx]). In this paper we

shall investigate Lie structures on factor algebras f[xi,..., x., y]/(y3-3py-g).

2. Notationsandpreliminaries

Let L be a finite-dimensional Lie algebra over a field f of characteristic zero with a basis {xi,..., x.}. Let A be a commutative associative algebra over { with an identity 1 and have deriations di,..., d. satisfying the following conditions, for i, 1'=1,..., n,

LcA, d,(xj)=6ij, didj=djdi.

ThenaLie structure on A is defined as follow ([4]): For any elements a, bEA, the product [a, b] in A is given by

[a, b] =2i,j[xi, xj]di(a)dj(b) = 2 i,j,k ck' xkdi(a)dj(b)

where eV are the structure constants with respect to a basis {xi,..., x.} ofL. Then A is a Lie algebra with this product and this Lie algebra is denoted by

L(L; A, {d,}).

ExAMpLE (Tensor products ofLie algebras constructed above). Let L, G be finite- dimensional Lie algebras over f with basis {xi,..., x.}, {yi,..., y.}, respectively. Let A,

B be commutative associative algebras with identities such that LcA, GcB and there exist derivations ui,..., u. of A and vi,..., v. of B satisfying the conditions; uiu,• ---

ujui, v,vt=vtv,, ui(xj)=6iJ•, v.(yt) ==6,t (i, 1''-- 1,..., n; s, t=1,..., m). Consider the

Author is partially supported by Grand-in-Aid for Encouragement of Young Scientist of Ministry of Education of Japan.

(2)

commutative associative algebra C =A(g)fBand a Lie algebra M==L(g)ff+f(g),G with [a(g)1, a'(g) 1] -= [a,a'] (g)1, [1(g)b, 1Qb'] =1(21) [b, b'].

[L (g) ,f, f(gÅr ,G] == O, (a, deA, b, b'EB).

We define derivations Ui,..., U., Vi,..., V. of C by Ui (a Qb) - ui(a)Q b, V, (a (gÅr b) = a (g) v,(b)

(aE4 bE B, i:- 1,..., n, s= 1,..., m). Then for a basis {xi (g) 1, 1 (g) y,: i== 1,..., n, s=1,..., m}, we have U,(xj(g)1)=6ij, Ui(1(El)y,) =O, V,(xj)=O, V,(y,)=6,,(i,j=1,..., n: s, t=1,..., m). Further theses derivations are commutable each other. Then a Lie structure ofL(M; C, {Ui, V,}) is given by, for a, a'EA, b, b'EB,

[a (g) b, a' (g)b'] = 2,,j[x-i(g) 1, xj (g) 1] Ui(a (8)b) Uj(d (El)b')

+ ]2 ,,t[1(2i)y,, 1 (Ei) .vt] V.(a(2)b) V,(a'(g)b') = [a, a'] (Ei)bb'+aa'(g) [b, b'].

To express the structures of Lie algebras we employ some notations. Let I, K be Lie algebras with a homomorphism (S of K into the derivation algebra Der(I). Then the vector space L=I+K is made into a Lie algebra by [a+b, c+d] =([a, c] +6(d)(a)

-j(b)(c))+ [b, d] (a, cEI, h, dEK). This Lie algebra L is called a split extension of I by Kand denoted by I+,K([1: p. 22]).

Let A be a commutative associative algebra over f. Assume that A has a Lie structure whose product [,] satisfies the condition; [ab, c] = [a, c]b+a[b, c](a, b, cE A). For an element wEA, we define the product [a, b].(a, bE A) by

[a, b]. =a[b, w] -h[a, w].

Then by a simple computation this product [ , ]. makes A into a Lie algebra.

3. Lie structures on f[x,,..,,x., y]1(y3-3py-q)

Let L be a finite-dimensional Lie algebra over f with a basis {xi,..., x.} and R the polynomial algebra f[x,,..., x.]. Consider the polynomial algebra R [y] over R and take a polynomial y3-3py-q (p, qER). Let us denote by

A(p, q) -= R[y]/(y3-3py- q)

acommutative associative factor algebra, where (y3-3py-q) is the ideal of R[y]

generated by the polynomial y3 - 3py - q.

Let T(y)=y3+ay2+by+c(a,b, cER), A a factor algebra R[y]/((T(y)) and Di,..., D. derivations of A such that for i, 1'=1,,.., n, DiDj=DjDi, DilR==O/axi.

(3)

Lie structures on f[xi,,,,, x., y] 1(y3-3py-q) 3

Then we put p = (a2 - 3b)19, q = ( - 2a3 + 9ab - 27c)127. For an associative isomorphism ip: A(p, q)-ÅrA with di(y) =y+(a!3), we set d,=ip-'Diip(i=1,..., n). Then d,,..., d.

are derivations of A(p, q) such that didj=djdi, ipdi == Diip, dilR=O/Oxi(i, 1'=1,..., n), in other words di is a differential automorphism([3]). Therefore by [4, Lemma 5]

we have the following

PRoposiTioN 1. Let A, p, q, di, Di (l=1,..., n) be given above. Then a Lie algebra L(L; A, {Di}) is isomorphic to a Lie algebra L(L; A(p, q),{d,}).

Hence we shall only investigate Lie structures on A(p, q),

We first extend a derivation Olaxi on R to A(p, q). Let di,..., d. be derivations of A(p, q) such that

(*) d,l.=:DIOx,, d,dj=djd,,

di(y) = ai + biy + c,y2

(ai, bi, cieR: i, 7'=1,..., n). Since di(y3-3py-q) =(-3pai+3qb,-di(q))+3(2pb,+

qci-di(p))y+3(ai+2pci)y2 =O in A(p, q), we have the following conditions; for i, 7'=1,... n,

(1) -3pai+3qbi-di(q), (2) 2pbi+qci=di(p),

(3) ai+2pci--O.

By the condition that didj(y)=d,•di(y) and didj(y)=:(di(a,•)+aibj+2qcicj)+

(di(bj) +bibj + 2aicj + 6pc icj)y + (di(cj) + bjci + 2bicj)y2, we have the following

conditions; for i, 7' -- 1,..., n,

(4) di(aj)+aibj=dj(ai)+ajbi,

(5) di (bj)+2aic,•=dj(bi)+2ajci, (6) di(cj)+bic,•=dj(ci)+bjci.

LEMMA 2. if there exist derivations di,..., d. of A(p,q) satisfying the condition (*), then 4p3-q2Ef. Further if 4p3 =q2, then p, qE{.

PRooF. By (1), (2), (3) we have 3(4p3-g2)b, == d,(4p3-q2)/2 (i=1,...,n).

Therefore 4p3-g2Ef. Assume that 4p3 =q2 and pq#O, and takeanon-zero element hER such that p== h2, q=2h3. By(2), h(bi+cih)= di(h) for i=1,..., n, we have hef.

QE. D.

From novv on, the Lie product [f, g] (f, geR) will be calculated in L(L;R,

{o/o.xi})•

(4)

3.l. Lie structures on A(p, q); 4p3#g2

In this section we assume that 4p3lq2. We shall show that di(y)-O (i---=1,,.., n).

By the proofof Lemma 2, we have bi=O (i=1,..., n). If p=O or q==O, then by (1), (2), (3) we have ai=c,=O. If pqlO, then comparing the degrees in x, of the both sides in (2) we have ci ==O and so ai=O.

We now compute a Lie product ff, y] (fGR) of L(L;A(p, q), {di}) as follow:

[f, y] =2i,j[xi xj]di(f)d,(y) =o.

Therefore we have the following

THEoREM 3. Assume that 4p37Eq2. Then the Lie structure of L(L;A(p, q),

{di}) is given by

[f, gy]=[f, g], [f, gy2] .. [f, g]y2,

[fy,gy]= [f, g]y2, [fy,gy2]-g[f, g]+3p[f, g]y, [fy2, gy2] -q[f, g]y+3p[f, g]y2 (f, gER).

CoRoLLARy 4. (1) Lie algebras L(L;A(O, q), {d,})(q 7EO) are isomorphic to a Z3-graded Lie algebra Ro+Ri+R2 such that

[fo, gi] == [f, g]i (i-O, 1, 2), [fi,gi]-[f, g]o,

[fi, g2] =q[f, g]o, [f2, g2] -g[f, g]i•

(2) Lie algebrasL(L;A(p,O),{d,})(p7EO) are isomorphic to the split extension (Ro -F Ri) -F iR ofa Z2-graded Lie algebra Ro+R, by R, where, for f, g, hER, [fo, gi] =3p[f, g]i(i--O, 1), [fi, gi]=[f, g]o,

and the Lie homomorphism 6 of R into Der(Ro+Ri) is given by 6(h)(fo+gi)- [f, h]o+ [g, h]i•

3.2. Lie structures on A(O, O)

In this section we shall discuss about Lie structures on A(O, O) =R[y]/(y3), Let di,..., d. be derivations ofA(O, O) satisfying the condition (*). Then by (3), (4), (5), (6) we have ai=:O, di(bj)=dj(bi) for i, 1'=1,..., n. Therefore there exists an element b of R such that

(5)

Lie structures on f[xi,..., x., y] /(y3-3py-q) 5

bi=OblOxi fori=1,...,n.

We restrict the condition (6) to that di(c,•) == dj(ci) (i, .f -- 1,..., n). For example this condition holds if the degrees of ci are less than that of b. Then we can choose an element c ofR such that ci=Oc!Oxi. Therefore we have, for i, j-- 1,..., n,

di(y) = di(b)y+ d,(c)y2 d,(b)d,• (c) == d,• (h)di(c).

THEoREM 5. Let b, cER satisf.y the condition (Oh/Ox,)(Oc!Oxj) == (ab/Oxj)

(OclOxi) (i, J'=1,..., n), and deLfine derivations d,,..., d. of' A(O, O) by d,(y) == d,(b)y +d,(c)y2. Then the Lie structure Qf L(L; A(O, O),{di'i) is given by

[f, gy] == ([f, g] +g[f, b] )y +g[f, c] y2, [,L gy2] -([f, g] +2g [f, h] )y2, [fy, gy] -=([f, g] -f[g, b] +g[f, h]).v2, [fy,gy2] ==O.

[fy2, gy2] =-O (f, gER).

CoRoLLARy6. The Lie algebra L(L;A(O,O),{di})gtven in Theorem 5 is

isomorph ic to the split extension (Ro + R i ) + jR of a Z2-g ra ded Lie atg ebra Ro + Ri by R, where forf, g, hG R,

[Ro, Ro] ==O, [fi,gi] -=([f, g] -f[g, b] +g[f, b])o, [R,, R,] ==O,

and the Lie homomorphism 6 of R into Der(Ro+Ri) is given by 6(h) (f,+g,)== ([f, h]+2f[b, h] +g[c, h]),+(g[b, h]+[g, h]),.

3.3. Lie structures on A (p, g); 4p3=g2, pg40

In this section we assume that 4p3==q2, pg ifO. By Lemma 2 and the conditions (1), (2), (3) we have a,-(4p2!q2)b,, ci=(-2p/q)b, (i-1,..., n). Since di(bj)=dj(bi)

(i, J' -- 1,..., n) by (3), (4), there exists an element b of R such that bi= di(b)(i=1,..., n).

Hence we have, for i=1,..., n,

di(y) -= (4p21q)d,(b) + di(b)y - (2plq)d,(b)y2.

We now compute a Lie product [.L y](feR) of L(L; A(p, q),{d,}) as follow;

[f, y] = Z ,,i [x ,, x,•]d,( f) dj (y)

= (4p21q) [f, b] + [f, b] y - (2pl q) [f, b] y2.

Therefore we have the following

(6)

THEoRE"f7.,., Assume that 4p3=e2, pq7EO. rhen the Lie strueture ojf'

L(L; A(p, e), {di-}) is given by

U, gy] = (4p2/q)g[L b] +Åq[L g] +g[A b])År, -- Åq2piq) g[f, b]y2, '[f, gy2] == - 4pg [f, b] - (4p2/q)g [f, b] y+ ( V, g] + 2g V, b] )y2, Efy, gy] ==2p[f, g]'+(2p2tq)[f. g]".v+([f, g] - [.L g]')y2,

[fy, g.v 2] == q( [L g] -f[g, bl + 2g [L b] ) + p(3 [L g] -f [g, b] + 2g [f, b] )N +{2p2/qÅr (f[g, b] ---2g[f, bl)y2,

[fy2, gy2] =4p2[L g]"+e([.L g]+[f, g]')y+p(3[L g] -2Y, gl")y2 ,vhereL gER and [f, g]'= [L g]h (Section 2).

References

[ 1 ] R.K. Amayo and -1.N. Stewart, Infinite-dimensional Lie algebrfis, Noordhoff, Leyden, 1974, [21 F.A. Berezin, Some remarks on the associative envelope of a Lie algebra (in Russian), Funkclon. Anal. Priloz. 1 (1967), 1--14.

r3] 1. Kaplansky, An introduction to differential algebras, Actualites Sci. Ind,, Hermann. 1957.

[4] F. Kubo and F. Mimura, Lie structures on differential algebras, to appea:, Hiroshima Malh, J.

Department of Mathematics K.vushu Institute of Technelogy

参照

関連したドキュメント

In the second section, we study the continuity of the functions f p (for the definition of this function see the abstract) when (X, f ) is a dynamical system in which X is a

We study a Neumann boundary-value problem on the half line for a second order equation, in which the nonlinearity depends on the (unknown) Dirichlet boundary data of the solution..

Lang, The generalized Hardy operators with kernel and variable integral limits in Banach function spaces, J.. Sinnamon, Mapping properties of integral averaging operators,

Algebraic curvature tensor satisfying the condition of type (1.2) If ∇J ̸= 0, the anti-K¨ ahler condition (1.2) does not hold.. Yet, for any almost anti-Hermitian manifold there

In this paper, for each real number k greater than or equal to 3 we will construct a family of k-sum-free subsets (0, 1], each of which is the union of finitely many intervals

Global transformations of the kind (1) may serve for investigation of oscilatory behavior of solutions from certain classes of linear differential equations because each of

Some of the known oscillation criteria are established by making use of a technique introduced by Kartsatos [5] where it is assumed that there exists a second derivative function

The Heisenberg and filiform Lie algebras (see Example 4.2 and 4.3) illustrate some features of the T ∗ -extension, notably that not every even-dimensional metrised Lie algebra over