The induced-representation multiplicity formula for Bessel and Fourier–Jacobi models

Let

σV=sV,1σV,1××sV,lVσV,lV,σW=sW,1σW,1××sW,lWσW,lW,\sigma_V=|\cdot|^{s_{V,1}}\sigma_{V,1}\times\cdots\times|\cdot|^{s_{V,l_V}}\sigma_{V,l_V},\qquad \sigma_W=|\cdot|^{s_{W,1}}\sigma_{W,1}\times\cdots\times|\cdot|^{s_{W,l_W}}\sigma_{W,l_W},

where σV,i\sigma_{V,i} and σW,i\sigma_{W,i} are irreducible tempered representations and sV,i,sW,iCs_{V,i},s_{W,i}\in\mathbb C satisfy

Re(sV,1)Re(sV,lV)>0,Re(sW,1)Re(sW,lW)>0.\operatorname{Re}(s_{V,1})\geq\cdots\geq\operatorname{Re}(s_{V,l_V})>0,\qquad \operatorname{Re}(s_{W,1})\geq\cdots\geq\operatorname{Re}(s_{W,l_W})>0.

Let πV0\pi_{V_0} and πW0\pi_{W_0} be irreducible tempered representations in the Bessel cases, and let π~W0\widetilde\pi_{W_0} be an irreducible tempered representation in the Fourier–Jacobi cases.

Induced-representation multiplicity formula. In the Bessel cases, for possibly reducible induced representations

πV=σVπV0,πW=σWπW0,\pi_V=\sigma_V\rtimes\pi_{V_0},\qquad \pi_W=\sigma_W\rtimes\pi_{W_0},

one has

m(πVπW)=m(πV0πW0).m(\pi_V\boxtimes\pi_W)=m(\pi_{V_0}\boxtimes\pi_{W_0}).

In the Fourier–Jacobi cases, for possibly reducible induced representations

πV=σVπV0,π~W=σWπ~W0,\pi_V=\sigma_V\rtimes\pi_{V_0},\qquad \widetilde\pi_W=\sigma_W\rtimes\widetilde\pi_{W_0},

one has

m(πV(π~WωW,ψF))=m(πV0(π~W0ωW0,ψF)).m\bigl(\pi_V\boxtimes(\widetilde\pi_W\otimes\omega_{W,\psi_F})\bigr) =m\bigl(\pi_{V_0}\boxtimes(\widetilde\pi_{W_0}\otimes\omega_{W_0,\psi_F})\bigr).

The formula is the uniform reduction underlying the paper's treatment of Archimedean Bessel and Fourier–Jacobi multiplicities. Its proof is the main result of the article in the Archimedean setting, while the corresponding general non-Archimedean uniform approach is described as forthcoming.

Sources & referencesView supporting material

Primary source

Cheng Chen, “Multiplicity formula for induced representations: Bessel and Fourier-Jacobi models over Archimedean local fields”, arXiv:2308.02912 (2023).

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