Abstract
As a spin analog of the plethystic Murnaghan–Nakayama rule for Schur functions, the plethystic Murnaghan–Nakayama rule for Schur Q-functions is established with the help of the vertex operator realization. This generalizes both the Murnaghan–Nakayama rule and the Pieri rule for Schur Q-functions. A plethystic Murnaghan–Nakayama rule for Hall–Littlewood functions is also investigated.
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Acknowledgements
We would like to thank the anonymous referee for helpful comments and correcting an error in the original statement of Proposition 4.2. The project is partially supported by Simons Foundation under Grant No. 523868, NSFC Grant 12171303, and the Humboldt foundation. The second author also thanks Max-Planck Institute for Mathematics in the Sciences, Leipzig for hospitality during the project. The third author is supported by the China Scholarship Council and he also acknowledges the hospitality of the Faculty of Mathematics of the University of Vienna, where parts of the present work were completed.
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Appendix
Appendix
Proof of (3.14):
\(B=(b_{ij})_{2n\times 2n}\) is an antisymmetric matrix obtained from \(A=(a_{ij})_{2n\times 2n}\) by rotating the first i rows and columns by the cyclic permutation \(\left( \begin{array}{ccccc} 1&{}2&{}\cdots &{}i-1&{}i\\ 2&{}3&{}\cdots &{}i&{}1\\ \end{array}\right) .\) Explicitly
Therefore \(\text {Pf(A)}=(-1)^{i-1}\text {Pf(B)}.\) It follows from (3.13) that
\(\square \)
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Cao, Y., **g, N. & Liu, N. A Spin Analog of the Plethystic Murnaghan–Nakayama Rule. Ann. Comb. 28, 655–679 (2024). https://doi.org/10.1007/s00026-023-00686-8
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DOI: https://doi.org/10.1007/s00026-023-00686-8