Tanusree Khandai and Punita Batra Harish-Chandra Research ... · The Quantum Torus C q : Let q =(q...

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The Quantum Torus C q : Let q =(q ij ) be a r×r matrix of non-zero complex numbers satisfying the relation : q ii = 1, q ij= q ji , for all 1≤i,j≤ r. Let J q be the ideal of the non-commutative Laurent polynomial ring S [r] =C[t 1 ... t r ] n.c generated by the elements, t i t j -q ij t j t i, 1≤i,j≤r. The algebra C q := S [r] /J q is called the quantum torus of rank r associated to q. C q is said to be cyclotomic if q ij is a complex roots of unity for all i.j. The Lie tori sl l+1 (C q ) : Given M l+1 (C q ) = M l+1 (C) C q, the Lie algebra sl l+1 (C q ) is defined as : sl l+1 (C q ) = { X=( x ij ) є M l+1 (C q ) :Trace(X) є[C q , C q ]} with commutator relations: [xa, y b] = B(x, y)I([a, b]) + [x, y] (a b)/2 + (x y) [a, b]/2 [b1] [I([a, b]), I([c, d])] = I([[a, b], [c, d]]), [b2] [I([a, b]), x c] = x [[a, b], c ], [b3] where x, y є sl l+1 (C), a, b, c, d є C q , [x, y] = xy yx, x y = xy + yx 2/(l + 1)Tr(xy)I(1), [a, b] = ab ba, a b = ab + ba, and B(x, y) = 1/(l + 1)Tr(xy). Let Q + = positive integer root lattice of sl l+1 (C) ; Q - = - Q + , and Q = Q + + Q - sl l+1 (C q ) has a decomposition given by: sl l+1 (C q ) = ( sl l+1 (C q ) a ) ( sl l+ 1 (C q ) 0 ) !! he Idea T Let V be a finite-dimensional irreducible representation of sl l+1 (C q ) generated by a vector v. Then there exists a positive Borel subalgebra b(s q ) = ( n q + H(s q ) ) of sl l+1 (C q ) such that U q ( n q + H(s q )). v Cv. It follows from the representation theory of multiloop Lie algebra that there exists a finitely supported functions f : (C × ) r P + such that : h t m . v = f(a)(h) ev a (t m ) v, for all m G(s q ), where P + is the positive integral weight lattice and ev a : s q C denotes the evaluation map at the point a (C × ) r . This implies that the finite-dimensional irreducible sl l+1 (C q ) modules are tensor products of sl l+1 (C q ) -modules which are analogous to the evaluation modules defined for the multiloop Lie algebras. KNOWN RESULT : It has been shown in [1], [17] that a rank r cyclotomic torus C q is isomorphic to a tensor product: C q Q (d 1 ) ….. Q (d s ) C[z 1 1 ... z k 1 ], where Q (d i ) is a rank 2 quantum torus associated to the matrix q(i)=(q kl [i]) with q 12 [i]=ζ i = (q 21 [i]) -1 , where ζ i is a d i th root of unity for 1 i s. Set supp sl l+1 (C q ) = {(a, m) Q×Z r : sl l+1 (C q ) a m 0 } and H(C q ) = sl l+1 (C q ) 0 . : OUR OBSERVATIONS Let ß(q) := Set of maximal commutative subalgebras of C q and let Z(q) be the center of C q. For s q є ß(q), set G(s q ) = { m =(m 1 ,..,m r ) є Z r : t m 1 .. t m r = t m є s q } and let s q ß(q) be such that s q s q = Z(q). One can associate with each subalgebra s q ß(q), of a normalized cyclotomic quantum torus C q, an abelian group G(s q ) = Z r / G(s q ) of rank d 1 …. d s . Any Borel subalgebra of sl l+1 (C q ) is of the form ( n q + H(s q ) ) or (n q - H(s q ) ), where n q is the subalgebra of sl l+1 (C q ) generated by the elements of sl l+1 (C q ) a for (a, m) supp sl l+1 (C q ), with a Q ± and H(s q ) is the subalgebra of sl l+1 (C q ) generated by the elements of sl l+1 (C q ) 0 , for m G(s q ). Let V be an irreducible sl l+1 (C q )-module with finite dimensional weight spaces. Then there exists non-zero vector v V such that U q (n q + )v =0 and V = U q (sl l+1 (C q ))v , where U q (a) denotes the universal enveloping algebra of any ) q C ( 1 l+ sl nalogs of Evaluation Modules for A Suppose that c a : (C × ) r P + is a function supported at a point a(C × ) r . Let v be a non-zero vector of an irreducible finite-dimensional sl l+1 (C q ) module V such that : n q + .v = 0 and h t m .v = c a (a)(h) ev a (t m ) v. for all m G(s q ), for some s q ß(q). H(C q ) is not a commutative algebra, hence if V is a non-trivial sl l+1 (C q )-module, then dim U q (H(C q ) ) > 1, implying, h t s .v Cv for s Z r \ G(s q ). However n q + .v = 0, implies n q +. h t s .v = 0, for all s Z r . In particular, h t s .v is a highest weight vector of V for s Z r \ G(s q ). Hence there exists a positive Borel subalgebra b(c q ) with c q ß(q) such that : b(c q ). h t s .v C. h t s .v , for all s Z r \ G(s q ). Irreducibility of the module V and the fact that the center of the algebra H(C q ) acts on all the highest weight vectors by the same scalar, imply that there exists z G(s q ) such that : h t m . h t s .v = c a (a.z s )(h) ev a.z s (t m ) h t s .v , for s Z r \ G(s q ) , m G(s q ), where c a (a. z s ) = c a (a), for all s Z r \ G(s q ). Further owing to the bracket operation [b1] in H(C q ) , it is seen that the module generated by v is an irreducible sl l+1 (C q )-module if and only if c a (a) is a miniscule weight of sl l+1 (C) . Let F(s q ) be the set of all finitely supported functions f : (C × ) r P + such that f(a) is a miniscule weight for all a support of f, and let F(s q , Z(q)) be the subset of F(s q ) consisting of all functions f such that ev a (t d ) ev b (t d ), for a,b supp f and t d є Z(q), where d є Z r denotes a multi-index element . Given c a є F(s q , Z(q)) and z є G(s q ) , let (s q , c a , z ) denote the set of all finitely supported functions g є F(s q , Z(q)) for which supp g = z s . a for s є G(s q ). Then the analogs of the evaluation modules for sl l+1 (C q ) is given by V (s q ,c a ,z) which is a module generated by a highest weight vector v on which h s q acts by the function c a and h s q acts on any other highest weight vector of V (s q ,c a ,z)by a function of the form z s .c a, for s є G(s q ). Given s q ß(q) , f =i=1 c a i F( s q , Z ( q ) ) , z G(s q ) r , set : V (s q , f , z) = V (s q ,c a ,z). r a є supp f r : MAIN RESULTS * Let V be a finite dimensional modules for the Lie algebra sl l+1 (C q ). Then V is of the form V(s q, f , z), where f F(s q , Z(q)) and z G(s q ) | f | , * Let s q , c q ß(q) and f 1 F(s q , Z(q)), f 2 F(c q , Z(q) ) with |f j | = r j, j=1,2 and let z G(s q ) r 1 and h G(c q ) r 2 . Then there exists a sl l+1 (C q )-module isomorphism g : V(s q, f 1, z )V(c q, f 2, h) if and only if subalgebra a of sl l+1 (C q ) . Tanusree Khandai and Punita Batra Harish-Chandra Research Institute, India References: 1. Allison, B., Berman, S., Faulkner, J.,Pianzola, A., Realization of graded-simple algebras as loop algebras. Forum Math. 20 (2008), no. 3. 2. Allison, B., Berman, S., Faulkner, J., Pianzola, A., Multiloop realization of extended affine Lie algebras and Lie tori, Trans. Amer. Math. Soc. (to appear). 3. Berman, S., Gao, Y., Krylyuk, Y. S., Quantum tori and the structure of elliptic quasi-simple Lie algebras. J. Funct. Anal. 135 (1996), no. 2. 4. Berman, S., Szmigielski, J., Principal realization for the extended affine Lie algebra of type ${\rm sl}\sb 2$ with coordinates in a simple quantum torus with two generators. Recent developments in quantum affine algebras and related topics (Raleigh, NC, 1998), 39--67, Contemp. Math., 248, Amer. Math. Soc., Providence, RI, 1999. 5. Billig, Y., Lau, M., Thin coverings of modules, J. Algebra 316, (2007), no. 1, 147-173; 0605680v1. 6. Chari, V., Integrable representations of affine Lie-algebras. Invent. Math. 85 (1986), no. 2. 7. Chari, V., Pressley, A., New unitary representations of loop groups. Math. Ann. 275 (1986), no. 1. 8. Chari, V., Pressley, A., Weyl Modules for Classical and Quantum Affine Algebras, Represent. Theory 5 (2001) ; math.QA/0004174. 9. Chari, V., Fourier, G., Khandai, T., A Categorical Approach to Weyl modules, In Preparation. 10. Feigin, B., Loktev, S., Multi-dimensional Weyl modules and symmetric functions. Comm. Math. Phys. 251 (2004), no. 3. 11. Garland, H., The Arithmetic Theory of Loop Algebras, J. Algebra 53 (1978). 12. Gao, Y., Representations of extended affine Lie algebras coordinatized by certain quantum tori. Compositio Math. 123 (2000), no. 1. 13. Gao, Y., Vertex operators arising from the homogeneous realization for $\widehat{{\rm g}\ell_n}$. Comm. Math. Phys. 211(2000). 14. Joseph, A, The admissibility of simple bounded modules for an affine Lie algebra. Algebra. Represent. Theory 3 (2000), no. 2. 15. Kac, Victor G. Infinite-dimensional Lie algebras. Third edition. Cambridge University Press, Cambridge, 1990. 16. Lau, M., Representations of Multiloop Algebras, arXiv:0811. 2011v2 [math.RT] 17. Neeb, K. H., On the classification of rational quantum tori and the structure of their automorphism groups, Canad. Math. Bull. 51 (2008), no. 2. 18. Rao, S. Eswara, A class of integrable modules for the core of EALA coordinatized by quantum tori. J. Algebra 275 (2004), no.1. 19. Rao, S. Eswara, Unitary modules for EALAs co-ordinatized by a quantum torus. Comm. Algebra 31 (2003), no. 5. ± i . s q = c q. ii . For each highest weight vector v V(s q, f 1, z ), g (v) is a highest weight vector of V(c q, f 2, h) such that upto a scaling factor f (1,v) (s q, f 1, z ) is G(s q ) - equivariant to f (2,g (v)) (c q. f 2, h), where f (i,w) denotes the finitely supported function by which h s q acts on the highest weight vector w for some s q ß(q) . ±1 _ -1 th ±1 ± m m (a, m) є Q×Z r m є Z r m m ± The multiloop Lie algebra sl l+1 (C) s q is a subalgebra of sl l+1 (C q ) for all s q ß(q). m a є supp f × where |f| = supp f.

Transcript of Tanusree Khandai and Punita Batra Harish-Chandra Research ... · The Quantum Torus C q : Let q =(q...

Page 1: Tanusree Khandai and Punita Batra Harish-Chandra Research ... · The Quantum Torus C q : Let q =(q ij) be a r×r matrix of non-zero complex numbers satisfying the relation : q ii

The Quantum Torus Cq : Let q =(qij) be a r×r matrix of non-zero complex

numbers satisfying the relation : qii = 1, qij= qji , for all 1≤i,j≤ r.

Let Jq be the ideal of the non-commutative Laurent polynomial ring

S[r]=C[t1 ... tr]n.c generated by the elements, titj-qijtjti, 1≤i,j≤r.

The algebra Cq:= S[r]/Jq is called the quantum torus of rank r associated to q.

Cq is said to be cyclotomic if qij is a complex roots of unity for all i.j.

The Lie tori sll+1(Cq) : Given Ml+1(Cq) = Ml+1(C) Cq, the Lie algebra sll+1(Cq)

is defined as : sll+1(Cq) = { X=( x ij) є Ml+1(Cq) :Trace(X) є[Cq , Cq]}

with commutator relations:[xa, y b] = B(x, y)I([a, b]) + [x, y] (a ○ b)/2 + (x ○ y) [a, b]/2 [b1]

[I([a, b]), I([c, d])] = I([[a, b], [c, d]]), [b2]

[I([a, b]), x c] = x [[a, b], c ], [b3]

where x, y є sll+1(C), a, b, c, d є Cq ,

[x, y] = xy − yx, x ○ y = xy + yx − 2/(l + 1)Tr(xy)I(1),

[a, b] = ab − ba, a ○ b = ab + ba, and B(x, y) = 1/(l + 1)Tr(xy).

Let Q+ = positive integer root lattice of sll+1(C) ; Q- = - Q+ , and Q = Q+ + Q-

sll+1(Cq) has a decomposition given by:

sll+1(Cq) = ( sll+1(Cq)a ) ( sll+1(Cq)0 )

!!he IdeaTLet V be a finite-dimensional irreducible representation of sll+1(Cq) generated by a vector v. Then

there exists a positive Borel subalgebra b(sq) = ( nq+

H(sq) ) of sll+1(Cq) such that

Uq( nq+ H(sq)). v Cv .

It follows from the representation theory of multiloop Lie algebra that there exists a finitely supported

functions f : (C ×)r → P+ such that :

h tm . v = ∑ f(a)(h) eva (tm ) v, for all m G(sq),

where P+ is the positive integral weight lattice and eva : sq → C denotes the evaluation map at the point

a(C×)r . This implies that the finite-dimensional irreducible sll+1(Cq) –modules are tensor products of

sll+1(Cq) -modules which are analogous to the evaluation modules defined for the multiloop Lie algebras.

KNOWN RESULT : It has been shown in [1], [17] that a rank r cyclotomic torus Cq is

isomorphic to a tensor product: Cq Q (d1) ….. Q (ds) C[z11

... zk1

],

where Q (di) is a rank 2 quantum torus associated to the matrix q(i)=(qkl[i])

with q12[i]=ζi= (q21[i])-1, where ζi is a di

throot of unity for 1 ≤ i ≤ s.

Set supp sll+1(Cq) = {(a, m) Q×Zr : sll+1(Cq)am

≠ 0 } and H(Cq) = sll+1(Cq)0 .

:OUR OBSERVATIONS

Let ß(q) := Set of maximal commutative subalgebras of Cq and let Z(q) be the center of Cq.

For sq є ß(q), set G(sq) = { m =(m1,..,mr) є Zr : tm1.. tmr = tm є sq } and

let sq ß(q) be such that sq ∩ sq = Z(q).

• One can associate with each subalgebra sq ß(q), of a normalized cyclotomic

quantum torus Cq, an abelian group G(sq ) = Zr / G(sq) of rank d1…. ds.

• Any Borel subalgebra of sll+1(Cq) is of the form ( nq+ H(sq) ) or (nq

- H(sq) ),

where nq is the subalgebra of sll+1(Cq) generated by the elements of sll+1(Cq)a for

(a, m) supp sll+1(Cq), with a Q± and H(sq) is the subalgebra of sll+1(Cq)

generated by the elements of sll+1(Cq)0 , for m G(sq).

• Let V be an irreducible sll+1(Cq)-module with finite dimensional weight spaces.

Then there exists non-zero vector v V such that Uq(nq+)v =0 and

V = Uq(sll+1(Cq))v , where Uq(a) denotes the universal enveloping algebra of any

) qC(1l+slnalogs of Evaluation Modules for ASuppose that ca : (C

×)r → P+ is a function supported at a point a(C×)r . Let v be a non-zero vector of an

irreducible finite-dimensional sll+1(Cq) module V such that :

nq+.v = 0 and h tm.v = ca(a)(h) eva (tm ) v. for all m G(sq), for some sq ß(q).

H(Cq) is not a commutative algebra, hence if V is a non-trivial sll+1(Cq)-module, then

dim Uq(H(Cq) ) > 1, implying, h ts.v Cv for s Zr \ G(sq).

However nq+.v = 0, implies nq

+. h ts.v = 0, for all s Zr . In particular,

h ts.v is a highest weight vector of V for s Zr \ G(sq).

Hence there exists a positive Borel subalgebra b(cq) with cq ß(q) such that :

b(cq). h ts.v C. h ts.v , for all s Zr \ G(sq).

Irreducibility of the module V and the fact that the center of the algebra H(Cq) acts on all

the highest weight vectors by the same scalar, imply that there exists z G(sq) such that :

h tm. h ts.v = ca(a.zs)(h) eva.zs (tm ) h ts.v , for s Zr \ G(sq) , m G(sq),

where ca(a. zs) = ca(a), for all s Zr \ G(sq). Further owing to the bracket operation [b1] in H(Cq) ,

it is seen that the module generated by v is an irreducible sll+1(Cq)-module if and only if

ca(a) is a miniscule weight of sll+1(C) .

Let F(sq) be the set of all finitely supported functions f : (C×)r → P+ such that f(a) is a miniscule

weight for all a support of f, and let F(sq, Z(q)) be the subset of F(sq) consisting of all functions f

such that

eva(td) ≠ evb(t

d), for a,b supp f and td є Z(q),

where d є Zr

denotes a multi-index element .

Given ca є F(sq, Z(q)) and z є G(sq) , let (sq, ca, z ) denote the set of all finitely supported functions

g є F(sq, Z(q)) for which supp g = zs .a for s є G(sq).

Then the analogs of the evaluation modules for sll+1(Cq) is given by V (sq ,ca ,z) which is a module

generated by a highest weight vector v on which h sq acts by the function ca and h sq acts on

any other highest weight vector of V (sq ,ca ,z)by a function of the form zs.ca, for s є G(sq).

Given sq ß(q) , f =∑i=1

cai F(sq, Z(q)), z G(sq)

r ,

set : V (sq , f , z) = V (sq ,ca ,z).

r

a є supp f

r

:MAIN RESULTS

* Let V be a finite dimensional modules for the Lie algebra sll+1(Cq). Then V

is of the form V(sq, f,z), where f F(sq, Z(q)) and z G(sq)| f |

,

* Let sq , cq ß(q) and f1 F(sq, Z(q)), f2 F(cq, Z(q) ) with

|f j| = rj, j=1,2 and let z G(sq)r1 and h G(cq)

r2 . Then

there exists a sll+1(Cq)-module isomorphism

g : V(sq, f1, z )→ V(cq, f2,h) if and only if

subalgebra a of sll+1(Cq) .

Tanusree Khandai and Punita Batra

Harish-Chandra Research Institute, India

References:1. Allison, B., Berman, S., Faulkner, J.,Pianzola, A., Realization of graded-simple algebras as loop algebras. Forum Math. 20 (2008), no. 3.

2. Allison, B., Berman, S., Faulkner, J., Pianzola, A., Multiloop realization of extended affine Lie algebras and Lie tori, Trans. Amer. Math. Soc. (to appear).

3. Berman, S., Gao, Y., Krylyuk, Y. S., Quantum tori and the structure of elliptic quasi-simple Lie algebras. J. Funct. Anal. 135 (1996), no. 2.

4. Berman, S., Szmigielski, J., Principal realization for the extended affine Lie algebra of type ${\rm sl}\sb 2$ with coordinates in a simple quantum torus

with two generators. Recent developments in quantum affine algebras and related topics (Raleigh, NC, 1998), 39--67, Contemp. Math., 248, Amer. Math.

Soc., Providence, RI, 1999.

5. Billig, Y., Lau, M., Thin coverings of modules, J. Algebra 316, (2007), no. 1, 147-173; 0605680v1.

6. Chari, V., Integrable representations of affine Lie-algebras. Invent. Math. 85 (1986), no. 2.

7. Chari, V., Pressley, A., New unitary representations of loop groups. Math. Ann. 275 (1986), no. 1.

8. Chari, V., Pressley, A., Weyl Modules for Classical and Quantum Affine Algebras, Represent. Theory 5 (2001) ; math.QA/0004174.9. Chari, V., Fourier, G., Khandai, T., A Categorical Approach to Weyl modules, In Preparation.

10. Feigin, B., Loktev, S., Multi-dimensional Weyl modules and symmetric functions. Comm. Math. Phys. 251 (2004), no. 3.

11. Garland, H., The Arithmetic Theory of Loop Algebras, J. Algebra 53 (1978).12. Gao, Y., Representations of extended affine Lie algebras coordinatized by certain quantum tori. Compositio Math. 123 (2000), no. 1.

13. Gao, Y., Vertex operators arising from the homogeneous realization for $\widehat{{\rm g}\ell_n}$. Comm. Math. Phys. 211(2000).

14. Joseph, A, The admissibility of simple bounded modules for an affine Lie algebra. Algebra. Represent. Theory 3 (2000), no. 2.

15. Kac, Victor G. Infinite-dimensional Lie algebras. Third edition. Cambridge University Press, Cambridge, 1990.

16. Lau, M., Representations of Multiloop Algebras, arXiv:0811. 2011v2 [math.RT]

17. Neeb, K. H., On the classification of rational quantum tori and the structure of their automorphism groups, Canad. Math. Bull. 51 (2008), no. 2.18. Rao, S. Eswara, A class of integrable modules for the core of EALA coordinatized by quantum tori. J. Algebra 275 (2004), no.1.

19. Rao, S. Eswara, Unitary modules for EALAs co-ordinatized by a quantum torus. Comm. Algebra 31 (2003), no. 5.

±

i. sq = cq. ii. For each highest weight vector v V(sq, f1, z ), g (v) is a

highest weight vector of V(cq, f2, h) such that upto a scaling

factor f(1,v) (sq, f1, z ) is G(sq) - equivariant to f(2,g (v)) (cq. f2, h),

where f(i,w) denotes the finitely supported function by which h sq acts on the

highest weight vector w for some sq ß(q) .

±1

_

-1

th

±1

±

m

m

(a, m) є Q×Zr m є Zr

mm

±

• The multiloop Lie algebra sll+1(C) sq is a subalgebra of sll+1(Cq) for all sq ß(q).

m

a є supp f

×

where |f| = supp f.