The Universal R-matrix for 𝔘h𝔟+

Arun Ram
Department of Mathematics and Statistics
University of Melbourne
Parkville, VIC 3010 Australia
aram@unimelb.edu.au

Last updates: 28 June 2011

The Universal R-matrix of 𝔘h𝔟+

1.1 Recall that D(𝔘h𝔟+) is the Hopf algebra given by generators X,H,H∗,Y with multiplication and comultiplication given by [ H , X ]=2X, [ H∗ , Y ]= - h 2 Y, Δ(H)= H⊗1+1⊗H, Δ(X)= X⊗ e h 4 H + e - h 4 H ⊗X, Δ(H∗)= H∗⊗1+1⊗H∗, Δ(Y)= Y⊗1+e-2H∗⊗Y. Let E= e h 4 H X . Then Δ(E)= 1⊗E+ e h 2 H ,and E e h 2 H = e h 2 (H-2) e h 4 H X = e-h e h 2 H E, since XH=(H-2)X.

2.2 Recall that there is a grading on 𝔘h𝔟+ given by setting deg(H)=0 and deg(X)=1. This grading induces a grading on (𝔘h𝔟+)∗ given by deg(H∗)=0 and deg(Y)=1. The inner product between 𝔘h𝔟+ and (𝔘h𝔟+)∗ respects this grading. It follows that ⟨ (H∗)r , Es ⟩= ⟨ H∗⊗⋯∗ , Δ(r) (E)s ⟩=0 for all r,s≥1 since the left hand component of the inner product has degree zero and the right hand component of the inner product has degree s. Using this observation we have that ⟨ (H∗)r Yk , HrEk ⟩ = ⟨ (H∗)r ⊗Yk , Δ(H∗)r Δ(Ek) ⟩ = ⟨ (H∗)r ⊗Yk , (H⊗1+1⊗H) r ( 1⊗E+ E⊗ e h 2 H ) k ⟩ = r! ⟨ (H∗)r ⊗Hk , (Hr⊗1) (1⊗Ek) ⟩ = ⟨ Yk , Ek ⟩ . Let us evaluate this inner product ⟨ Yk , Ek ⟩ = ⟨ Y⊗⋯⊗Y , ( 1⊗⋯E+1⊗⋯⊗E ⊗ e h 2 H ⊗⋯⊗ e h 2 H ) k ⟩ = ⟨ Y⊗⋯⊗Y , ∑ π∈Sk (e-h) l(π) E ⊗ e h 2 H E ⊗ ( e h 2 H ) 2 E ⊗⋯ ⊗ ( e h 2 H ) k-1 E ⟩ = ⟨ Y⊗⋯⊗Y , ∑ π∈Sk (e-h) l(π) E⊗E⊗⋯⊗E ⟩ = ∑ p∈Sk (e-h) l(π) . Let q=eh⁄2 and recall that ∑ π∈Sk ql(π) = [ k ; q ]! where [ k ; q ]= (qk-1)⁄ (q-1) and [ k ; q ]!= [ k ; q ] [ k-1 ; q ] ⋯ [ 1 ; q ] . Thus ⟨ Yk , Ek ⟩ = [ k ; q-2 ]!, and ⟨ (H∗)r Yk , HrEk ⟩ = r! [ k ; q-2 ]!. It follows easil by degree counts and arguments as above that ⟨ (H∗)r Yk , HsEl ⟩ =0, if r≠s or k≠l. Thus, the bases 1 r! [ k ; q-2 ] (H∗)rYk and HsEl are dual bases in (𝔘h𝔟+)∗ and D ( 𝔘h𝔟+ ) respectively.

2.3 It follows that the universal R-matrix for D ( 𝔘h𝔟+ ) is given by R= ∑ r,k≥0 1 r! [ k ; q-2 ] HrEk⊗ (H∗)r Yk.

2.4 We shall write the universal R-matrix in terms of the generators Y ‾ , X,J1 and J2 so that we may project this R-matrix modulo the ideal in 𝔘h𝔟+ generated by J2 in order to get an R-matrix for 𝔘h𝔰𝔩(2) . Recall that in the notations of section 1 we had Y ˆ = YeH∗ and Y ‾ = Y ˆ e h 2 - e - h 2 = Y ˆ q-q-1 . Since Y ‾ = H∗ = ( H∗+h⁄2 ) Y ‾ , it follows that Y ‾ e-H∗ = e - (H∗+h⁄2) Y , and we have Yk = ( Y ‾ e-H∗ (q-q-1) ) k = (q-q-1)k Y ‾ e-H∗ Y ‾ e-H∗ ⋯ Y ‾ e-H∗ = (q-q-1)k e-kH∗ (q-1) k 2 Y ‾ k. In a similar fashion, using the fact that E= e h 4 H X and XH=(H-2)X

we have that Ek = e h 4 H X e h 4 H X⋯ e h 4 H X = e k-1 2 h 2 e kh 4 H Xk. Now we may rewrite the R-matrix as follows R = ∑ r,k≥0 1 r! [ k ; q-2 ] HrEk⊗ (H∗)r Yk = ∑ r,k 1 r! [ k ; q-2 ] Hr q k-1 2 e kh 4 H Xk⊗ (H∗)r (q-q-1)k e-kH∗ (q-1) k 2 Y ‾ k = ∑ r,k≥0 (q-q-1)k (q-1) k 2 q - k-1 2 r! [ k ; q-2 ] Hr e kh 4 H Xk⊗ (H∗)r e-kH∗ Y ‾ k. Recall that H∗= h 4 (J1+J2) . Thus (H∗)r e-kH∗ = ( h 4 (J1+J2) ) r e kh 4 (J1+J2) , Hr e kh 4 H = (J1-J2)r e kh 4 (J1-J2) . Now we may project modulo the ideal of 𝔘h𝔟+ generated by J2 and write the universal R-matrix for 𝔘h𝔰𝔩(2) in the form R = ∑ r,k≥0 (q-q-1)k (q-1) k 2 q - k-1 2 r! [ k ; q-2 ] Hr e kh 4 H Xk⊗ (H∗)r e-kH∗ Y ‾ k = ∑ r,k≥0 (q-q-1)k (q-1) k 2 q - k-1 2 r! [ k ; q-2 ] J1r e kh 4 J1 Xk ⊗ ( h 4 J1 ) r e - kh 4 J1 Y ‾ k = ∑ r,k≥0 (q-q-1)k (q-1) k 2 q - k-1 2 r! [ k ; q-2 ] exp ( h 4 (J1⊗J1) + kh 4 ( J1⊗1+1⊗J1 ) ) Xk⊗ Y ‾ k.

References

The fact that 𝔘h𝔰𝔩(2) is a quotient of the double of 𝔘h𝔟+ is stated in §13 of [D] along with the formula for the universal R-matrix of 𝔘h𝔰𝔩(2)

[Bou] N. Bourbaki, Lie groups and Lie algebras, Chapters I-III, Springer-Verlag, 1989.

[D] V.G. Drinfeld, Quantum Groups, Vol. 1 of Proccedings of the International Congress of Mathematicians (Berkeley, Calif., 1986). Amer. Math. Soc., Providence, RI, 1987, pp. 198–820. MR0934283

The theorem that a Lie bialgebra structure determinse a co-Poisson Hopf algebra structure on its enveloping algebra is due to Drinfel'd and appears as Theorem 1 in the following article.

[D1] V.G. Drinfel'd, Hopf algebras and the quantum Yang-Baxter equation, Soviet Math. Dokl. 32 (1985), 254–258. MR0802128

Derivations of the double and the universal R-matrix for 𝔘h𝔰𝔩(n) appear in [R] and [B]. Our derivation of 𝔘h𝔰𝔩(2) follows the example given in [B].

[B] N. Burroughs, The universal R-matrix for Uqsl(3) and beyond!, Comm. Math. Phys. 127 (1990), 109–128. MR1036117

[R] M. Rosso, An analogue of P.B.W. theorem and the universal R-matrix for Uhsl(N+1) Uhsl(N+1)., Quantum groups (Clausthal, 1989), Comm. Math. Phys. 124 (1989), no. 2, 307–318. MR1012870

[DHL] H.-D. Doebner, Hennig, J. D. and W. Lücke, Mathematical guide to quantum groups, Quantum groups (Clausthal, 1989), Lecture Notes in Phys., 370, Springer, Berlin, 1990, pp. 29–63. MR1201823

There is a very readable and informative chapter on Lie algebra cohomolgy in the forthcoming book

[HGW] R. Howe, R. Goodman, and N. Wallach, Representations and Invariants of the Classical Groups, manuscript, 1993.

The following book is a standard introductory book on Lie algebras; a book which remains a standard reference. This book has been released for a very reasonable price by Dover publishers. There is a short description of Lie algebra cohomology in Chapt. III §11, pp.93-96.

[J] N. Jacobson, Lie algebras, Interscience Publishers, New York, 1962.

A very readable and complete text on Lie algebra cohomology is

[Kn] A. Knapp, Lie groups, Lie algebras and cohomology, Mathematical Notes 34, Princeton University Press, 1998. MR0938524

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