[Paper Review] Multiplicity preservation for orthogonal-symplectic and unitary dual pair correspondences
This paper proves multiplicity preservation for theta correspondences in orthogonal-symplectic and unitary dual pairs over non-archimedean local fields of characteristic zero. Using geometric invariant theory and Gelfand-Kazhdan criteria for distributions, the authors establish that the dimension of the space of $ω_{ψ}$-invariant functionals on $π \otimes \pi'$ is at most one, confirming the multiplicity one property for these dual pair correspondences.
Over a non-archimedean local field of characteristic zero, we prove the multiplicity preservation for orthogonal-symplectic dual pair correspondences and unitary dual pair correspondences.
Motivation & Objective
- To establish the multiplicity one property for theta correspondences in orthogonal-symplectic and unitary dual pairs over non-archimedean local fields of characteristic zero.
- To extend Waldspurger’s result (for odd residue characteristic) and Howe’s archimedean result to the general non-archimedean setting.
- To prove that the space of $ω_{ψ}$-invariant functionals on $π \otimes \pi'$ has dimension at most one for any genuine irreducible admissible smooth representations $π$ and $π'$.
Proposed method
- Constructs the metaplectic cover $ω_{ψ}$ of the symplectic group acting on a Heisenberg group via the oscillator representation.
- Introduces extended groups $̄{G}$, $̄{G}'$, and $̄{Sp}(\mathbf{E})$ to handle the action of $-1$ and stabilize orbits under the group action.
- Uses the Gelfand-Kazhdan criterion for distributions on totally disconnected groups to reduce the multiplicity problem to invariance of generalized functions under a larger group.
- Applies a geometric result showing that $G$-orbits in $\mathbf{E}'$ are stable under $\breve{G}$, which implies invariance of bi-$\mathbf{G}$-invariant generalized functions under $\{\pm 1\} \ltimes (\breve{\mathbf{G}} \times \breve{\mathbf{G}})$.
- Leverages the fact that the contragredient of the oscillator representation is isomorphic to its dual, allowing symmetry in the Hom space to conclude the bound.
- Applies the Gelfand-Kazhdan criterion to the group $\mathbf{J} = \mathbf{G} \ltimes \mathbf{H}$ to show that $\dim \mathrm{Hom}_{\mathbf{G}}(\Pi, \mathbb{C}) \cdot \dim \mathrm{Hom}_{\mathbf{G}}(\Pi^\vee, \mathbb{C}) \leq 1$ for irreducible representations $\Pi$ of $\mathbf{J}$.
Experimental results
Research questions
- RQ1Does the theta correspondence between orthogonal-symplectic and unitary dual pairs preserve multiplicity one over non-archimedean local fields of characteristic zero?
- RQ2Can the multiplicity one property be established uniformly across all classical groups in the dual pair setting?
- RQ3How does the action of the extended group $\breve{G}$ affect the stability of orbits in the dual pair construction?
Key findings
- The dimension of the space of $\widetilde{G} \times \widetilde{G}'$-invariant functionals on $\omega_{\psi} \otimes \pi \otimes \pi'$ is at most one for any genuine irreducible admissible smooth representations $\pi$ and $\pi'$.
- The result confirms the multiplicity one conjecture for orthogonal-symplectic and unitary dual pair correspondences in the non-archimedean setting with characteristic zero.
- The proof relies on the invariance of bi-$\mathbf{G}$-invariant generalized functions under the action of $\{\pm 1\} \ltimes (\breve{\mathbf{G}} \times \breve{\mathbf{G}})$, established via geometric orbit stability.
- The orbit stability result follows from the existence of an element in $\breve{G} \setminus G$ that negates a given $x \in \tilde{\mathfrak{g}}$ and preserves a flag $F$, implying $\breve{G}$-stability of $G$-orbits.
- The Gelfand-Kazhdan criterion is applied to the group $\mathbf{J} = \mathbf{G} \ltimes \mathbf{H}$ to bound the product of dimensions of Hom spaces to at most one.
- The final conclusion $\dim \mathrm{Hom}_{\widetilde{G} \times \widetilde{G}'}(\omega_{\psi}, \pi \otimes \pi') \leq 1$ is derived by symmetry and duality, using the fact that $\omega_{\psi}^\vee \cong \omega_{\psi}$ and $\dim \mathrm{Hom}_{\mathbf{G}}(\omega_{\psi} \otimes \pi^\vee \otimes \pi^{\prime\vee}, \mathbb{C}) = \dim \mathrm{Hom}_{\mathbf{G}}(\omega_{\psi}^\vee \otimes \pi \otimes \pi^{\prime}, \mathbb{C})$.
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This review was created by AI and reviewed by human editors.