Quantum K Whitney relations for partial flag varieties

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Let X=Fl⁡(r1,…,rk,n)X=\operatorname{Fl}(r_1,\dots,r_k,n) be a partial flag variety with tautological bundles

0=S0⊂S1⊂⋯⊂Sk⊂Sk+1=Cn,0=\mathcal S_0\subset\mathcal S_1\subset\dots\subset\mathcal S_k\subset\mathcal S_{k+1}=\mathbb C^n,

where Sj\mathcal S_j has rank rjr_j, and let qjq_j denote the quantum parameter associated with the degree in the jjth direction. For a vector bundle EE, write λy(E)=∑i[ΛiE]yi\lambda_y(E)=\sum_i[\Lambda^iE]y^i.

Quantum K Whitney relations. For j=1,…,kj=1,\dots,k, the following relations hold in QK⁡T(X)\operatorname{QK}_T(X):

λy(Sj)⋆λy(Sj+1/Sj)=λy(Sj+1)−yrj+1−rjqj1−qjdet⁡(Sj+1/Sj)⋆(λy(Sj)−λy(Sj−1)).\lambda_y(\mathcal S_j)\star\lambda_y(\mathcal S_{j+1}/\mathcal S_j)=\lambda_y(\mathcal S_{j+1})-y^{r_{j+1}-r_j}\frac{q_j}{1-q_j}\det(\mathcal S_{j+1}/\mathcal S_j)\star(\lambda_y(\mathcal S_j)-\lambda_y(\mathcal S_{j-1})).

These relations are conjectured to give a Whitney-type presentation of the equivariant quantum K-theory ring of a partial flag variety, extending the corresponding relations in quantum cohomology and describing the quantum deformation of the product of lambda classes.

References

Primary source

Wei Gu, Leonardo C. Mihalcea, Eric Sharpe, Weihong Xu, Hao Zhang and Hao Zou, “Quantum K Whitney relations for partial flag varieties”, arXiv:2310.03826 (2024).

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