Abstract
This paper shows that the cyclotomic quiver Hecke algebras of type A, and the gradings on these algebras, are intimately related to the classical seminormal forms. We start by classifying all seminormal bases and then give an explicit “integral” closed formula for the Gram determinants of the Specht modules in terms of the combinatorics associated with the KLR grading. We then use seminormal forms to give a deformation of the KLR algebras of type A. This makes it possible to study the cyclotomic quiver Hecke algebras in terms of the semisimple representation theory and seminormal forms. As an application we construct a new distinguished graded cellular basis of the cyclotomic KLR algebras of type A.
Similar content being viewed by others
References
Ariki, S.: On the semi-simplicity of the Hecke algebra of \((\mathbb{Z}/r\mathbb{Z})\wr \mathfrak{S}_n\). J. Algebra 169, 216–225 (1994)
Ariki, S.: On the classification of simple modules for cyclotomic Hecke algebras of type \(G(m,1, n)\) and Kleshchev multipartitions. Osaka J. Math. 38, 827–837 (2001)
Ariki, S., Koike, K.: A Hecke algebra of \(({ Z}/r{ Z})\wr {\mathfrak{S}}_n\) and construction of its irreducible representations. Adv. Math. 106, 216–243 (1994)
Ariki, S., Mathas, A., Rui, H.: Cyclotomic Nazarov-Wenzl algebras. Nagoya Math. J. 182, 47–134 (2006) (Special issue in honour of George Lusztig). arXiv:math/0506467
Brundan, J., Kleshchev, A.: Schur–Weyl duality for higher levels. Sel. Math. (N.S.) 14, 1–57 (2008)
Brundan, J., Kleshchev, A.: Blocks of cyclotomic Hecke algebras and Khovanov–Lauda algebras. Invent. Math. 178, 451–484 (2009)
Brundan, J., Kleshchev, A.: Graded decomposition numbers for cyclotomic Hecke algebras. Adv. Math. 222, 1883–1942 (2009)
Brundan, J., Kleshchev, A., Wang, W.: Graded Specht modules. J. Reine Angew. Math. 655, 61–87 (2011). arXiv:0901.0218
Brundan, J., Stroppel, C.: Highest weight categories arising from Khovanov’s diagram algebra III: category \({\cal O}\). Represent. Theory 15, 170–243 (2011). arXiv:0812.1090
Dipper, R., James, G., Mathas, A.: Cyclotomic \(q\)-Schur algebras. Math. Z. 229, 385–416 (1998)
Dipper, R., Mathas, A.: Morita equivalences of Ariki–Koike algebras. Math. Z. 240, 579–610 (2002)
Graham, J.J., Lehrer, G.I.: Cellular algebras. Invent. Math. 123, 1–34 (1996)
Hoffnung, A.E., Lauda, A.D.: Nilpotency in type \(A\) cyclotomic quotients. J. Algebraic Comb. 32, 533–555 (2010)
Hu, J., Mathas, A.: Graded cellular bases for the cyclotomic Khovanov–Lauda–Rouquier algebras of type \(A\). Adv. Math. 225, 598–642 (2010). arXiv:0907.2985
Hu, J., Mathas, A.: Cyclotomic quiver Schur algebras for linear quivers. Proc. Lond. Math. Soc. 110, 1315–1386 (2015). arXiv:1110.1699
James, G., Mathas, A.: A \(q\)-analogue of the Jantzen–Schaper theorem. Proc. Lond. Math. Soc. (3) 74, 241–274 (1997)
Hu, J., Mathas, A.: The Jantzen sum formula for cyclotomic \(q\)-Schur algebras. Trans. Am. Math. Soc. 352, 5381–5404 (2000)
James, G., Murphy, G.E.: The determinant of the Gram matrix for a Specht module. J. Algebra 59, 222–235 (1979)
Kac, V.G.: Infinite-Dimensional Lie Algebras, 3rd edn. Cambridge University Press, Cambridge (1990)
Kazhdan, D., Lusztig, G.: Representations of Coxeter groups and Hecke algebras. Invent. Math. 53, 165–184 (1979)
Khovanov, M., Lauda, A.D.: A diagrammatic approach to categorification of quantum groups. I. Represent. Theory 13, 309–347 (2009)
Khovanov, M., Lauda, A.D.: A diagrammatic approach to categorification of quantum groups II. Trans. Am. Math. Soc. 363, 2685–2700 (2011)
Kleshchev, A., Mathas, A., Ram, A.: Universal graded Specht modules for cyclotomic Hecke algebras. Proc. Lond. Math. Soc. (3) 105, 1245–1289 (2012). arXiv:1102.3519
Li, G.: Integral Basis Theorem of Cyclotomic Khovanov–Lauda–Rouquier Algebras of Type A. Ph.D. thesis, University of Sydney (2012)
Maksimau, R.: Quiver Schur algebras and Koszul duality. J. Algebra 406, 91–133 (2014). arXiv:1307.6013
Mathas, A.: Iwahori–Hecke algebras and Schur algebras of the symmetric group. In: University Lecture Series, vol. 15. American Mathematical Society, Providence (1999)
Mathas, A.: Matrix units and generic degrees for the Ariki–Koike algebras. J. Algebra 281, 695–730 (2004). arXiv:math/0108164
Mathas, A.: Seminormal forms and Gram determinants for cellular algebras. J. Reine Angew. Math. 619, 141–173 (2008) (With an appendix by Marcos Soriano). arXiv:math/0604108
Murphy, G.E.: The idempotents of the symmetric group and Nakayama’s conjecture. J. Algebra 81, 258–265 (1983)
Okounkov, A., Vershik, A.: A new approach to representation theory of symmetric groups. Sel. Math. (N.S.) 2, 581–605 (1996)
Rouquier, R.: 2-Kac–Moody algebras (2008, preprint). arXiv:0812.5023
Rouquier, R., Shan, P., Varagnolo, M., Vasserot, E.: Categorifications and cyclotomic rational double affine Hecke algebras (2013, preprint). arXiv:1305.4456
Ryom-Hansen, S.: The Schaper formula and the Lascoux, Leclerc and Thibon algorithm. Lett. Math. Phys. 64, 213–219 (2003)
Ryom-Hansen, S.: Young’s seminormal form and simple modules for \(S_n\) in characteristic \(p\), 2011. Algebras Represent. Theory 16, 15871609 (2013). arXiv:1107.3076
Serre, J.-P.: Local fields. In: Graduate Texts in Mathematics, vol. 67. Springer, New York (1979) (Translated from the French by Marvin Jay Greenberg)
Stroppel, C., Webster, B.: Quiver Schur algebras and \(q\)-Fock space (2011, preprint). arXiv:1110.1115
Young, A.: On quantitative substitutional analysis I. Proc. Lond. Math. Soc. 33, 97–145 (1900)
Yvonne, X.: A conjecture for \(q\)-decomposition matrices of cyclotomic \(v\)-Schur algebras. J. Algebra 304, 419–456 (2006)
Acknowledgments
J. Hu and A. Mathas were supported by the Australian Research Council. J. Hu author was also supported by the National Natural Science Foundation of China.
Author information
Authors and Affiliations
Corresponding author
Appendix: Seminormal forms for the linear quiver
Appendix: Seminormal forms for the linear quiver
In this appendix we show how the results in this paper work when \(e=0\) so that \(\xi \in K\) is either not a root of unity or \(\xi =1\) and K is a field of characteristic zero. In order to define a modular system we have to leave the case where the cyclotomic parameters \(Q_1,\ldots ,Q_\ell \) are integral, that is, when \(Q_l=[\kappa _l]\) for \(1\le l\le \ell \). This causes quite a few notational inconveniences, but otherwise the story is much the same as for the case when \(e>0\). We do not develop the full theory of “0-idempotent subrings” here. Rather, we show just one way of proving the results in this paper when \(e=0\).
Fix a field K and \(0\ne \xi \in K\) of quantum characteristic e. That is, either \(\xi =1\) and K is a field of characteristic zero or \(\xi ^d\ne 1\) for \(d\in \mathbb {Z}\). The multicharge \({\varvec{\kappa }}\in \mathbb {Z}^\ell \) is arbitrary.
Let \({\mathcal {O}}=\mathbb {Z}[x,\xi ]_{(x)}\) be the localisation of \(\mathbb {Z}[x,\xi ]\) at the principal ideal generated by x. Let \(\fancyscript{K}=\mathbb {Q}(x,\xi )\) be the field of fractions of \({\mathcal {O}}\). Define \(\mathcal {H}^\varLambda _n({\mathcal {O}})\) to be the cyclotomic Hecke algebra of type A with Hecke parameter \(t=\xi \), a unit in \({\mathcal {O}}\), and cyclotomic parameters
where, as before, \([k]=[k]_t\) for \(k\in \mathbb {Z}\). Then \(\mathcal {H}^\varLambda _{n}(\fancyscript{K})=\mathcal {H}^\varLambda _n({\mathcal {O}})\otimes _{\mathcal {O}}\fancyscript{K}\) is split semisimple in view of Ariki’s semisimplicity condition [1]. Moreover, by definition, \(\mathcal {H}^\varLambda _{n}(K)\cong \mathcal {H}^\varLambda _n({\mathcal {O}})\otimes _{\mathcal {O}}K\), where we consider K as an \({\mathcal {O}}\)-module by setting x act on K as multiplication by zero.
Define a new content function for \(\mathcal {H}^\varLambda _n({\mathcal {O}})\) by setting
for a node \(\gamma =(l,r,c)\). We will also need the previous definition of contents below. If \({\mathfrak t}\in {\mathop {\mathrm{Std}}\nolimits }(\mathcal {P}^{\varLambda }_{n})\) is a tableau and \(1\le k\le n\) then set \(C_k({\mathfrak t})=C_\gamma \), where \(\gamma \) is the unique node such that \({\mathfrak t}(\gamma )=k\).
As in Sect. 2.5, let \(\{m_{{\mathfrak s}{\mathfrak t}}\,|\,({\mathfrak s},{\mathfrak t})\in {\mathrm{Std}}^2(\mathcal {P}^{\varLambda }_{n})\}\) be the Murphy basis of \(\mathcal {H}^\varLambda _n({\mathcal {O}})\). Then the analogue of Lemma 2.6 is that if \(1\le r\le n\) then
for some \(r_{{\mathfrak u}{\mathfrak v}}\in {\mathcal {O}}\). As in Sect. 3.1 define a \(*\)-seminormal basis of \(\mathcal {H}^\varLambda _{n}(\fancyscript{K})\) to be a basis \(\{f_{{\mathfrak s}{\mathfrak t}}\}\) of simultaneous two-sided eigenvectors for \(L_1,\ldots ,L_n\) such that \(f_{{\mathfrak s}{\mathfrak t}}^{*}=f_{{\mathfrak t}{\mathfrak s}}\).
Define a seminormal coefficient system for \(\mathcal {H}^\varLambda _n({\mathcal {O}})\) to be a set of scalars \({\varvec{\alpha }}=\{\alpha _r({\mathfrak s})\}\) satisfying Definition 3.5(a), (b) and such that if \({\mathfrak s}\in {\mathop {\mathrm{Std}}\nolimits }(\mathcal {P}^{\varLambda }_{n})\) and \({\mathfrak u}={\mathfrak s}(r,r+1)\in {\mathop {\mathrm{Std}}\nolimits }(\mathcal {P}^{\varLambda }_{n})\) then
where \(P_r({\mathfrak s})=C_r({\mathfrak u})-C_r({\mathfrak s})\), and where \(\alpha _r({\mathfrak s})=0\) if \({\mathfrak u}\notin {\mathop {\mathrm{Std}}\nolimits }(\mathcal {P}^{\varLambda }_{n})\).
As in Theorem 3.9, each seminormal basis of \(\mathcal {H}^\varLambda _n(\fancyscript{K})\) is determined by a seminormal coefficient system \({\varvec{\alpha }}=\{\alpha _r({\mathfrak s})\}\), such that
together with a set of scalars \(\{\gamma _{{\mathfrak t}^{\varvec{\lambda }}}\,|\,{\varvec{\lambda }}\in \mathcal {P}^{\varLambda }_{n}\}\). Notice that \(I=\mathbb {Z}\), since \(e=0\), so if \(\mathbf {i}\in I^n\) then \({\mathfrak t}\in {\mathop {\mathrm{Std}}\nolimits }(\mathbf {i})\) if and only if \(c_r({\mathfrak t})=i_r\) and, in turn, this is equivalent to the constant term of \(C_r({\mathfrak t})\) being equal to \([i_r]\), for \(1\le r\le n\). Arguing as in Lemma 4.3,
With these definitions in place all of the arguments in Sect. 4 go through with only minor changes. In particular, if \(1\le r\le n\) and \(\mathbf {i}\in I^n\) then Definition 4.12 should be replaced by
and \(y^{{\mathcal {O}}}_rf_{\mathbf {i}}^{\mathcal {O}}=\big (L_r-C_r({\mathfrak t})\big )f_{\mathbf {i}}^{\mathcal {O}}\) where, as before, \(M_r=1-L_r+tL_{r+1}\). With these new definitions, if \({\mathfrak s}\in {\mathop {\mathrm{Std}}\nolimits }(\mathbf {i})\), for \(\mathbf {i}\in I^m\), and \(1\le r\le n\) then Lemma 4.19 becomes
where \({\mathfrak u}={\mathfrak s}(r,r+1)\) and
Observe that if \({\mathfrak u}={\mathfrak s}(r,r+1)\) is a standard tableau then, using (A1), the definitions imply that
Comparing this with Lemma 4.22, it is now easy to see that analogues of Proposition 4.23 and Proposition 4.24 both hold in this situation. Hence, repeating the arguments of Sect. 4.4, a suitable modification of Theorem A also holds. Similarly, the construction of the bases in Sects. 5 and Sect. 6 now goes though largely without change.
Rights and permissions
About this article
Cite this article
Hu, J., Mathas, A. Seminormal forms and cyclotomic quiver Hecke algebras of type A . Math. Ann. 364, 1189–1254 (2016). https://doi.org/10.1007/s00208-015-1242-8
Received:
Revised:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s00208-015-1242-8