#K-theoretic Schur P/Q polynomials
In [IN13], T. Ikeda and H. Naruse introduce \(K\)-theoretic analogs of the Schur \(P\) and Schur \(Q\) functions, as well as factorial versions of these. The factorial versions are denoted \(\schurKP_{\lambda}(\xvec|b)\) and \(\schurKQ_{\lambda}(\xvec|b),\) where \(b = (b_1,b_2,\dotsc)\) is a vector of parameters. When all these are set to \(0,\) we obtain \(\schurKP_{\lambda}(\xvec)\) and \(\schurKQ_{\lambda}(\xvec).\) These are \(K\)-theoretic analogs of \(\schurP_{\lambda}(\xvec)\) and \(\schurQ_{\lambda}(\xvec).\) Ikeda and Naruse give several formulas for these functions, including a ratio-of-Pfaffians formula, a shifted set-valued tableau formula, and an excited Young diagram formula.
They give a presentation for equivariant \(K\)-theory classes of the orthogonal and Lagrangian Grassmannian.
E. Marberg and B. Pawlowski give \(K\)-theory formulas for orthogonal and symplectic orbit closures [MP20]. Their stable Grothendieck analogues for fixed-point-free involutions expand positively in \(K\)-theoretic Schur \(P\)-functions, and related involution families are connected to \(K\)-theoretic Schur \(Q\)-functions. S. Iwao gives a boson–fermion correspondence for dual \(K\)-theoretic \(P\)- and \(Q\)-functions [Iwa27]. The construction uses \(\beta\)-deformed neutral fermions and vertex operators, and recovers generating functions for the dual \(K\)-theoretic Schur \(P\)- and \(Q\)-functions.
J. B. Lewis and E. Marberg prove the Nakagawa–Naruse conjecture that the dual \(K\)-theoretic Schur \(P\)- and \(Q\)-functions are generating functions for shifted plane partitions [LM24]. They also describe the images of these functions under the involution \(\omega\) and verify an Ikeda–Naruse basis conjecture for the \(GQ\)-functions.
Y.-C. Chiu and E. Marberg prove identities expanding \(K\)-theoretic Schur \(Q\)-functions in terms of \(K\)-theoretic Schur \(P\)-functions [CM24]. Their main formula is a signed finite expansion, and they characterize when its coefficients lie in \(\setN[\beta]\); see [Thm. 1.1 and Cor. 1.2, CM24]. Their formulas extend to skew and dual versions, and they also prove a shifted skew Cauchy identity for symmetric Grothendieck polynomials. E. Marberg proves that the \(K\)-Stanley symmetric functions of classical types expand positively into these \(K\)-theoretic Schur \(P\)- and \(Q\)-functions [Mar25].
Example (A \(Q\)-to-\(P\) expansion).
In the notation of [Thm. 1.1, CM24], the coefficient of \(\schurKP_\lambda\) in \(\schurKQ_\mu\) is obtained by summing over strict partitions \(\lambda \supseteq \mu\) with \(\ell(\lambda)=\ell(\mu)\) such that the shifted skew diagram \(\lambda/\mu\) has at most one box in each row. The coefficient is \[2^{\ell(\mu)}(-1)^{\operatorname{col}(\lambda/\mu)} \left(-\frac{\beta}{2}\right)^{|\lambda/\mu|},\] where \(\operatorname{col}(\lambda/\mu)\) is the number of occupied shifted columns. For \(\mu=(3,2),\) the only strict partitions which contribute are \((3,2),\) \((4,2),\) and \((4,3),\) so \[\schurKQ_{(3,2)} =4\schurKP_{(3,2)} +2\beta\schurKP_{(4,2)} -\beta^2\schurKP_{(4,3)}.\] The negative term occurs because the two boxes of the shifted skew diagram \((4,3)/(3,2)\) lie in the same shifted column. In contrast, every part of \((4,2)\) differs from the next by at least two, and the same rule gives only nonnegative \(\beta\)-coefficients: \[\schurKQ_{(4,2)} =4\schurKP_{(4,2)} +2\beta\schurKP_{(4,3)} +2\beta\schurKP_{(5,2)} +\beta^2\schurKP_{(5,3)}.\]
#Properties
The fundamental quasisymmetric expansion of \(\schurKP_{\lambda}(\xvec)\) and \(\schurKQ_{\lambda}(\xvec)\) can be found in [HKPW+17].
T. Nobukawa and T. Shimazaki compute special values of skew \(K\)-theoretic Schur \(P\)- and \(Q\)-functions [NS24]. For strict partitions \(\lambda \supset \mu,\) their main evaluation gives \(\schurKP_{\lambda/\mu}(\beta,\dotsc,\beta\mid -\beta^{-1}) = \schurKQ_{\lambda/\mu}(\beta,\dotsc,\beta\mid -\beta^{-1}) = \beta^{|\lambda/\mu|}\) in their notation. The proof uses sign-reversing involutions on shifted set-valued tableaux and implies oddness results for the corresponding tableau counts.
#Littlewood–Richardson rule
The Littlewood–Richardson rule for \(\schurKP_{\lambda}(\xvec)\) is due to Clifford–Thomas–Yong [CTY14]. Their result is based on a Pieri rule due to A. Buch and V. Ravikumar, [BR12].
Problem (Littlewood–Richardson rule).
Find a Littlewood–Richardson rule for \(\schurKQ_{\lambda}(\xvec).\)
Bibliography
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