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arXiv:2511.04794

Pseudodeterministic Communication Complexity

Mika Göös, Harms, Nathaniel, Riazanov, Artur, Sofronova, Anastasia, Sokolov, Dmitry, Yuan, Weiqiang

Published Nov 6, 2025• 0 citations
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Abstract

We exhibit an $n$-bit partial function with randomized communication complexity $O(\log n)$ but such that any completion of this function into a total one requires randomized communication complexity $n^{Ω(1)}$. In particular, this shows an exponential separation between randomized and \emph{pseudodeterministic} communication protocols. Previously, Gavinsky (2025) showed an analogous separation in the weaker model of parity decision trees. We use lifting techniques to extend his proof idea to communication complexity.

DOI
10.48550/arxiv.2511.04794

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We exhibit an nnn-bit partial function with randomized communication complexity O(log⁡n)O(\log n)O(logn) but such that any completion of this function into a total one requires randomized communication complexity nΩ(1)n^{Ω(1)}nΩ(1). In particular, this shows an exponential separation between randomized and \emph{pseudodeterministic} communication protocols. Previously, Gavinsky (2025) showed an analogous separation in the weaker model of parity decision trees. We use lifting techniques to extend his proof idea to communication complexity.
We exhibit an n-bit partial function with randomized communication complexity O(logn) but such that any completion of this function into a total one requires randomized communication complexity nΩ(1). In particular, this shows an exponential separation between randomized and pseudodeterministic communication protocols. Previously, Gavinsky (2025) showed an analogous separation in the weaker model of parity decision trees. We use lifting techniques to extend his proof idea to communication complexity.
We refine Gavinsky's framework (arXiv:2608.18784) for exponential separations between quantum and randomized communication complexity of total functions and obtain larger separations: polylogarithmic quantum communication versus Ω~(n)\tildeΩ(\sqrt n)Ω~(n​) randomized communication with two quantum messages, and versus Ω(n1−ε)Ω(n^{1-\varepsilon})Ω(n1−ε) for every fixed 0<ε<10<\varepsilon<10<ε<1 with more quantum messages.
Boolean function F(x,y)F(x,y)F(x,y) for x,y∈{0,1}nx,y \in \{0,1\}^nx,y∈{0,1}n is an XOR function if F(x,y)=f(x⊕y)F(x,y)=f(x\oplus y)F(x,y)=f(x⊕y) for some function fff on nnn input bits, where ⊕\oplus⊕ is a bit-wise XOR. XOR functions are relevant in communication complexity, partially for allowing Fourier analytic technique. For total XOR functions it is known that deterministic communication complexity of FFF is closely related to parity decision tree complexity of fff. Montanaro and Osbourne (2009) observed that one-sided communication complexity Dcc→(F)D_{cc}^{\rightarrow}(F)Dcc→​(F) of FFF is exactly equal to nonadaptive parity decision tree complexity NADT⊕(f)NADT^{\oplus}(f)NADT⊕(f) of fff. Hatami et al. (2018) showed that unrestricted communication complexity of FFF is polynomially related to parity decision tree complexity of fff. We initiate the studies of a similar connection for partial functions. We show that in case of one-sided communication complexity whether these measures are equal, depends on the number of undefined inputs of fff. On the one hand, if Dcc→(F)=tD_{cc}^{\rightarrow}(F)=tDcc→​(F)=t and fff is undefined on at most O(2n−tn−t)O(\frac{2^{n-t}}{\sqrt{n-t}})O(n−t​2n−t​), then NADT⊕(f)=tNADT^{\oplus}(f)=tNADT⊕(f)=t. On the other hand, for a wide range of values of Dcc→(F)D_{cc}^{\rightarrow}(F)Dcc→​(F) and NADT⊕(f)NADT^{\oplus}(f)NADT⊕(f) (from constant to n−2n-2n−2) we provide partial functions for which Dcc→(F)<NADT⊕(f)D_{cc}^{\rightarrow}(F) < NADT^{\oplus}(f)Dcc→​(F)<NADT⊕(f). In particular, we provide a function with an exponential gap between the two measures. Our separation results translate to the case of two-sided communication complexity as well, in particular showing that the result of Hatami et al. (2018) cannot be generalized to partial functions. Previous results for total functions heavily rely on Boolean Fourier analysis and the technique does not translate to partial functions. For the proofs of our results we build a linear algebraic framework instead. Separation results are proved through the reduction to covering codes.
A longstanding question in quantum communication complexity is whether some task can be accomplished with a small amount of communication in the presence of entanglement, yet require much more quantum communication in the absence of entanglement. Separations of this nature were previously known for relational problems and, in the simultaneous message passing model, for partial functions. But it has remained unresolved whether any such separation exists for a total Boolean function. We resolve this question with an exponential separation in the one-way setting: we exhibit a family of total Boolean functions fn ⁣:{0,1}n×{0,1}n→{0,1}f_n\colon \{0,1\}^n \times \{0,1\}^n \to \{0,1\}fn​:{0,1}n×{0,1}n→{0,1} that can be computed with O(log⁡n)O(\log n)O(logn) bits of one-way classical communication given prior entanglement, but that require Ω(n1/3)Ω(n^{1/3})Ω(n1/3) qubits of one-way quantum communication without entanglement. Our function is a special case of the subgroup membership problem, first studied in the communication setting by Aaronson, Le Gall, Russell, and Tani.