Paper 2026/1236

New bounds on private simultaneous quantum message passing

Abstract

In the private simultaneous message (PSM) setting, $k$ players obtain inputs $x_i\in\{0,1\}^n$ and then independently send messages to a referee, who should learn $f(x_1,...,x_k)$ but no other information about $(x_1,...,x_k)$. The PSM setting was introduced as a minimal model for secure multiparty computation. In the quantum setting, PSM has been related to non-local quantum computation (NLQC), and has several connections to the complexity of Boolean functions. The communication and correlation cost of implementing private simultaneous message passing may be much larger than the cost without privacy, and the cost of privacy in this setting remains poorly understood. Here, we give new upper and lower bounds on the PSM model, in both the quantum and classical settings. Concretely, we prove two lower bounds: 1) Nečiporuk's measure lower bounds the entanglement required for $k$-player quantum PSM with perfect correctness. This can be evaluated to give quadratic lower bounds for some explicit functions. 2) The rank of the communication matrix of $f(x_1,x_2)$ lower bounds 2-player quantum PSM with perfect privacy but imperfect correctness. This implies a previously unknown lower bound on classical PSM with imperfect correctness. When allowing both quantum communication and shared entanglement, these two bounds are the first lower bounds on quantum PSM that make use of the privacy condition. Regarding upper bounds, we show: 1) Letting $s$ be the size of a quantum circuit computing $f$, $d_f$ be the circuit depth, $k$ the number of players, $n$ the number of bits received by each player, and $\epsilon$ the correctness parameter of the PSM protocol, we obtain the upper bound $\mathsf{PSM}_k^*(f) \leq (kn +s) \cdot \log^{O( d_f)}(s/\epsilon)$. 2) The square of the Fourier 1 norm of $f$, $\Vert \hat{f}\Vert_1^2$, upper bounds the classical PSM complexity, $\mathsf{PSM}(f)\leq O(\Vert \hat{f} \Vert^2_1)$. In proving the first upper bound, we also generalize existing $T$-depth based techniques for NLQC from $2$ to $k\geq 2$ parties, and consider cases where the Clifford layers are restricted to having small light cones. These generalizations may be of independent interest.