Abstract
We construct algebra homomorphisms from affine Yangians to the current algebras of rectangular W-algebras both in type A. The construction is given via the coproduct and the evaluation map for the affine Yangians. As a consequence, we show that parabolic inductions for representations of the rectangular W-algebras can be regarded as tensor product representations of the affine Yangians under the homomorphisms. The same method is applicable also to the super-setting.
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References
Alday, L.F., Gaiotto, D., Tachikawa, Y.: Liouville correlation functions from four-dimensional gauge theories. Lett. Math. Phys. 91(2), 167–197 (2010)
Arakawa, T.: Representation theory of \({\mathscr {W}}\)-algebras. Invent. Math. 169(2), 219–320 (2007)
Arakawa, T.: Introduction to W-algebras and their representation theory, Perspectives in Lie theory, Springer INdAM Ser., vol. 19, pp. 179–250. Springer, Cham (2017)
Arakawa, T.: Representation theory of \(W\)-algebras and Higgs branch conjecture. In: Proceedings of the International Congress of Mathematicians—Rio de Janeiro 2018. vol. II. Invited lectures. pp. 1263–1281. World Sci. Publ., Hackensack, NJ (2018)
Arakawa, T., Molev, A.: Explicit generators in rectangular affine \({\cal{W}}\)-algebras of type \(A\). Lett. Math. Phys. 107(1), 47–59 (2017)
Braverman, A., Feigin, B., Finkelberg, M., Rybnikov, L.: A finite analog of the AGT relation I: Finite \(W\)-algebras and Quasimaps spaces. Comm. Math. Phys. 308(2), 457–478 (2011)
Braverman, A., Finkelberg, M., Nakajima, H.: Instanton moduli spaces and \({\mathscr {W}}\)-algebras, Astérisque (385), vii+128 (2016)
Brundan, J., Kleshchev, A.: Shifted Yangians and finite \(W\)-algebras. Adv. Math. 200(1), 136–195 (2006)
Brundan, J., Kleshchev, A.: Representations of shifted Yangians and finite \(W\)-algebras. Mem. Amer. Math. Soc. 196(918), viii+107 (2008)
Briot, C., Ragoucy, E.: \({\cal{W}}\)-superalgebras as truncations of super-Yangians. J. Phys. A 36(4), 1057–1081 (2003)
Creutzig, T., Hikida, Y.: Rectangular W-algebras, extended higher spin gravity and dual coset CFTs. J. High Energy Phys. 2, 147 (2019). front matter + 30
Creutzig, T., Hikida, Y.: Rectangular \(W\) algebras and superalgebras and their representations. Phys. Rev. D 100(8), 086008 (2019)
Eberhardt, L., Procházka, T.: The matrix-extended \({\cal{W}}_{1+\infty }\) algebra. J. High Energy Phys. 12, 175 (2019)
Feigin, B., Finkelberg, M., Negut, A., Rybnikov, L.: Yangians and cohomology rings of Laumon spaces. Selecta Math. (N.S.) 17(3), 573–607 (2011)
Feigin, B., Frenkel, E.: Quantization of the Drinfeld-Sokolov reduction. Phys. Lett. B 246(1–2), 75–81 (1990)
Finkelberg, M., Tsymbaliuk, A.: Multiplicative slices, relativistic Toda and shifted quantum affine algebras. Representations and nilpotent orbits of Lie algebraic systems, Progr. Math., vol. 330, pp. 133–304. Birkhäuser/Springer, Cham (2019)
Frenkel, E., Ben-Zvi, D.: Vertex algebras and algebraic curves. Mathematical Surveys and Monographs, vol. 88, 2nd edn. American Mathematical Society, Providence, RI (2004)
Genra, N.: Screening operators for \({mathcal W }\)-algebras. Selecta Math. (N.S.) 23(3), 2157–2202 (2017)
Genra, N.: Screening operators and parabolic inductions for affine \({\cal{W}}\)-algebras (with an appendix by Shigenori Nakatsuka). Adv. Math. 369, 107179 (2020). 62 pages
Guay, N.: Affine Yangians and deformed double current algebras in type A. Adv. Math. 211(2), 436–484 (2007)
Guay, N., Nakajima, H., Wendlandt, C.: Coproduct for Yangians of affine Kac-Moody algebras. Adv. Math. 338, 865–911 (2018)
Guay, N., Regelskis, V., Wendlandt, C.: Vertex representations for Yangians of Kac-Moody algebras. J. Éc. Polytech. Math. 6, 665–706 (2019)
Kac, V., Roan, S.-S., Wakimoto, M.: Quantum reduction for affine superalgebras. Comm. Math. Phys. 241(2–3), 307–342 (2003)
Kodera, R.: Braid group action on affine Yangian. SIGMA Symmetry Integrability Geom. Methods Appl. 15, 020 (2019). 28 pages
Kodera, R.: On Guay’s evaluation map for affine Yangians. Algebr. Represent. Theory 24(1), 253–267 (2021). correction 269–272. arXiv:1806.09884
Maulik, D., Okounkov, A.: Quantum groups and quantum cohomology. Astérisque (408) (2019). ix+209
Nakajima, H.: Handsaw quiver varieties and finite \(W\)-algebras. Mosc. Math. J. 12(3), 633–666, 669–670 (2012)
Nakatsuka, S.: On Miura maps for \({\cal{W}}\)-superalgebras. arXiv:2005.10472
Negut, A.: Toward AGT for parabolic sheaves. arXiv:1911.02963, to appear in IMRN, https://doi.org/10.1093/imrn/rnaa308
Negut, A.: Deformed \(W\)-algebras in type A for rectangular nilpotent. arXiv:2004.02737
Peng, Y.-N.: Finite \(W\)-superalgebras and truncated super Yangians. Lett. Math. Phys. 104(1), 89–102 (2014)
Peng, Y.-N.: Finite \(W\)-superalgebras via super Yangians. Adv. Math. 377, 107459 (2021). 60 pages
Ragoucy, E., Sorba, P.: Yangian realisations from finite \({\cal{W}}\)-algebras. Comm. Math. Phys. 203(3), 551–572 (1999)
Rapčák, M.: On extensions of \(\widehat{{\mathfrak{gl}}(m|n)}\) Kac-Moody algebras and Calabi-Yau singularities. J. High Energy Phys. (1), 042 (2020). 34 pages
Schiffmann, O., Vasserot, E.: Cherednik algebras, W-algebras and the equivariant cohomology of the moduli space of instantons on \(\mathbf{A}^2\). Publ. Math. Inst. Hautes Études Sci. 118, 213–342 (2013)
Ueda, M.: Construction of affine super Yangian. arXiv:1911.06666, to appear in Publ. RIMS
Ueda, M.: Affine super Yangians and rectangular \(W\)-superalgebras, arXiv:2002.03479
Varagnolo, M., Vasserot, E.: K-theoretic Hall algebras, quantum groups and super quantum groups. arXiv:2011.01203
Acknowledgements
The authors are grateful to Tomoyuki Arakawa, Boris Feigin, Ryo Fujita, Naoki Genra, Toshiro Kuwabara, Andrew Linshaw, Hiraku Nakajima, Shigenori Nakatsuka, Andrei Negut, Masatoshi Noumi, Shoma Sugimoto, Husileng Xiao, Yasuhiko Yamada, and Shintarou Yanagida for valuable discussions and suggestions. They also thank the referees for many helpful comments to improve the paper. Some part of results of this paper were presented by the first named author in Workshop on 3d Mirror Symmetry and AGT Conjecture held on October 21–25, 2019, at Institute for Advanced Study in Mathematics, Zhejiang University, Hangzhou. He thanks their hospitality. The first named author was supported by JSPS KAKENHI Grant Number 18K13390, 21K03155. His work was also supported in part by JSPS Bilateral Joint Projects (JSPS-RFBR collaboration) “Elliptic algebras, vertex operators and link invariants” from MEXT, Japan. The second named author was supported by Grant-in-Aid for JSPS Fellows 20J12072.
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Appendices
Appendix A
Lemma A.1 and Proposition A.2 are statements on the rectangular W-algebra \({\mathcal {W}}^{\kappa }({\mathfrak {g}},f)\) for \(n \ge 1\) and for \(n \ge 2\), respectively.
Lemma A.1
We have
In particular, we have
The following assertion slightly refines Proposition 4.5. It can be regarded as an analog of Proposition 6.3.
Proposition A.2
Assume \(l \ge 2,\) \(n \ge 2\) and \(\alpha \ne 0\). Then, \({\mathfrak {U}}({\mathcal {W}}^{\kappa }({\mathfrak {g}},f))\) is topologically generated by
Proof
We will gradually construct the elements \(W_{i,j}^{(1)}(m)\), \(W_{i,j}^{(2)}(m)\) for \(i,j=1,\ldots ,n\) and \(m \in {\mathbb {Z}}\). They are topological generators of \({\mathfrak {U}}({\mathcal {W}}^{\kappa }({\mathfrak {g}},f))\) when \(n \ge 2\) and \(\alpha \ne 0\) by Proposition 4.5. The argument below is essentially the same as the one in [37].
-
\(W_{i,j}^{(1)}(m)\) for \(i \ne j\): they are generated from
$$\begin{aligned} \left\{ W_{n,1}^{(1)}(1),\ W_{1,n}^{(1)}(-1),\ W_{i,i+1}^{(1)}(0),\ W_{i+1,i}^{(1)}(0) \mid i=1,\ldots ,n-1 \right\} \end{aligned}$$by the commutation relation (4.4).
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\(W_{i,i}^{(2)}(0) - W_{j,j}^{(2)}(0)\) for \(i \ne j\): we have
$$\begin{aligned} \begin{aligned} {[}W_{i,i+1}^{(2)}(0), W_{i+1,i}^{(1)}(0)] = W_{i,i}^{(2)}(0) - W_{i+1,i+1}^{(2)}(0) \end{aligned} \end{aligned}$$for \(i=1,\ldots ,n-1\).
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\(W_{i,j}^{(2)}(m)\) for \(i \ne j\): we have
$$\begin{aligned} \begin{aligned} {[}W_{i,i}^{(2)}(0) - W_{j,j}^{(2)}(0), W_{i,j}^{(1)}(m)] = 2 W_{i,j}^{(2)}(m) + m(l-1)\alpha W_{i,j}^{(1)}(m) \end{aligned} \end{aligned}$$for \(i \ne j\).
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\(W_{i,i}^{(2)}(m)-W_{j,j}^{(2)}(m)\) for \(i \ne j\): we have
$$\begin{aligned} \begin{aligned} {[}W_{i,j}^{(2)}(m), W_{j,i}^{(1)}(0)] = W_{i,i}^{(2)}(m)-W_{j,j}^{(2)}(m) \end{aligned} \end{aligned}$$for \(i \ne j\).
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\(W_{i,i}^{(1)}(m)\): we have
$$\begin{aligned} \begin{aligned} {[}W_{j,i}^{(2)}(m-1), W_{i,j}^{(1)}(1)] = W_{j,j}^{(2)}(m)-W_{i,i}^{(2)}(m) - (l-1)\alpha W_{i,i}^{(1)}(m) \end{aligned} \end{aligned}$$for \(i \ne j\).
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\(W_{i,i}^{(2)}(m)\): we have
$$\begin{aligned}&{[}W_{i,i}^{(2)}(m) - W_{j,j}^{(2)}(m), W_{i,i}^{(2)}(m') - W_{j,j}^{(2)}(m')] \\&\quad = (m'-m)\alpha \Big ( W_{i,i}^{(2)}(m+m') + W_{j,j}^{(2)}(m+m') \Big ) + P \end{aligned}$$for \(i \ne j\), where P is an element of \({\mathfrak {U}}({\mathcal {W}}^{\kappa }({\mathfrak {g}},f))\) which is generated by \(W_{a,b}^{(1)}(m'')\) and \(W_{c,d}^{(2)}(m''')\) for various \(a,b,c,d,m'',m'''\) with \(c \ne d\). Hence, under the assumption \(\alpha \ne 0\), we see that all the elements of the form \(W_{i,i}^{(2)}(m) + W_{j,j}^{(2)}(m)\) for \(i \ne j\) and \(m \in {\mathbb {Z}}\) belong to the image of \(\Phi _{l}\). Thus, \(W_{i,i}^{(2)}(m)\) for any i and m belong to the image of \(\Phi _{l}\) since so do \(W_{i,i}^{(2)}(m) - W_{j,j}^{(2)}(m)\).
\(\square \)
Assume \(\alpha \ne 0\). Let us prove the surjectivity of \(\Phi _{l}\), the latter statement of Theorem 9.2. By (9.1) with the commutation relation (4.4), we see that the image of \(\Phi _{l}\) contains \(W_{i,j}^{(1)}(m)\) and \(W_{i,i}^{(1)}(m)-W_{j,j}^{(1)}(m)\) for \(i \ne j\) and \(m \in {\mathbb {Z}}\). The image of \(\Phi _{l}\) contains \(W_{i,i}^{(1)}(0)\) for any i since we have
We show that the image of \(\Phi _{l}\) contains \(W_{i,i}^{(1)}(m)\) for any i and \(m \ne 0\). The formula (11.1) for \(i = 0\) shows that the image of \(\Phi _{l}\) contains
Hence, the assertion follows from
If \(l=1\), this completes the proof. Suppose \(l \ge 2\). By Proposition 9.3 together with the fact that the image of \(\Phi _{l}\) contains \(W_{i,j}^{(1)}(m)\) for any i, j, m, the image of \(\Phi _{l}\) contains
The proof is complete by Proposition A.2.
Remark A.3
A proof of the surjectivity of \(\Phi _{1} = {{\,\mathrm{ev}\,}}\) was initially given by the first named author in [24] by a different method. The above argument, just computing (A.2), supplies a much simpler proof (the computation of (A.1) for \(l=1\) has already appeared in [24]).
Appendix B
Lemma B.1
We have
Lemma B.2
For \(i < j\), we have
and
Proof of Proposition11.1
We may assume \(i < j\). Then, by Lemma B.1, B.2, and (11.2), we have
This is equal to 0 by Lemma A.1. \(\square \)
Appendix C
The equality (11.2) is deduced from the following. We omit its proof.
Lemma C.1
For \(i < j\), we have
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Kodera, R., Ueda, M. Coproduct for affine Yangians and parabolic induction for rectangular W-algebras. Lett Math Phys 112, 3 (2022). https://doi.org/10.1007/s11005-021-01500-3
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DOI: https://doi.org/10.1007/s11005-021-01500-3