Moyal deformation of the classical arrival time

The quantum time of arrival (TOA) problem requires a statistics of measured arrival times given only a particle's initial state. Following the standard framework of quantum theory, the problem translates into finding an appropriate quantum image of the classical arrival time $\mathcal{T}_C(q,p)$, usually in operator form $\hat{\mathrm{T}}$. In this paper, we consider the problem anew within the phase space formulation of quantum mechanics. The resulting quantum image is a real-valued and time-reversal symmetric function $\mathcal{T}_M(q,p)$ in formal series of $\hbar^2$ with the classical arrival time as the leading term. It is obtained from the Moyal bracket relation with the system Hamiltonian and is hence interpreted as a Moyal deformation of the classical TOA. Finally, we show that $\mathcal{T}_M(q,p)$ is isomorphic to the rigged Hilbert space TOA operator constructed recently in [Eur. Phys. J. Plus \textbf{138}, 153 (2023)] independent of canonical quantization.