Fourier duality for quantum volumes under symplectic reduction
Establish that the T-equivariant quantum volume Π_X^{eq}(−[ω]−λ⋅μ) of a Hamiltonian T-space X and the quantum volume Π_{X//_t T}(−[ω_red]) of the symplectic (or GIT) reduction X//_t T are related by Fourier transformation with respect to λ ∈ Lie(T) and t ∈ Lie(T)^*, where [ω_red] denotes the class of the reduced symplectic form and ω−λ⋅μ is the Duistermaat–Heckman form. Concretely, demonstrate a Fourier duality Π_X^{eq}(−[ω]−λ⋅μ) ↔ Π_{X//_t T}(−[ω_red]) consistent with the identifications of parameters and the reduction data.
References
We propose the following naive conjecture.
The equivariant quantum volume \Pi{\rm eq}X(-[]) of X and the quantum volume \Pi{X/!/t T}(-[\omega{\rm red}]) of the reduction are related by Fourier transformation:
\Pi{\rm eq}X(-[]) \quad \underset{\rm FT}{\longleftrightarrow}
\quad \Pi{X/!/t T}(-[\omega{\rm red}]),
where \Pi_X{\rm eq}(-[]) is viewed as a function of \lambda\inLie(T) and \Pi_{X/!/t T}(-[\omega{\rm red}]) is viewed as a function of t\in Lie*(T); =\omega - \lambda \cdot \mu is the Duistermaat-Heckman form eq:DH and \omega_{\rm red} is the reduced symplectic form on X/!/_t T = \mu{-1}(t)/T.