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On relating one-way classical and quantum communication complexities
Communication complexity is the amount of communication needed to compute a function when the function inputs are distributed over multiple parties. In its simplest form, one-way communication complexity, Alice and Bob compute a function \(f(x,y)\), where \(x\) is given to Alice and \(y\) is given t...
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Published in: | arXiv.org 2023-05 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
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Summary: | Communication complexity is the amount of communication needed to compute a function when the function inputs are distributed over multiple parties. In its simplest form, one-way communication complexity, Alice and Bob compute a function \(f(x,y)\), where \(x\) is given to Alice and \(y\) is given to Bob, and only one message from Alice to Bob is allowed. A fundamental question in quantum information is the relationship between one-way quantum and classical communication complexities, i.e., how much shorter the message can be if Alice is sending a quantum state instead of bit strings? We make some progress towards this question with the following results. Let \(f: \mathcal{X} \times \mathcal{Y} \rightarrow \mathcal{Z} \cup \{\bot\}\) be a partial function and \(\mu\) be a distribution with support contained in \(f^{-1}(\mathcal{Z})\). Denote \(d=|\mathcal{Z}|\). Let \(\mathsf{R}^{1,\mu}_\epsilon(f)\) be the classical one-way communication complexity of \(f\); \(\mathsf{Q}^{1,\mu}_\epsilon(f)\) be the quantum one-way communication complexity of \(f\) and \(\mathsf{Q}^{1,\mu, *}_\epsilon(f)\) be the entanglement-assisted quantum one-way communication complexity of \(f\), each with distributional error (average error over \(\mu\)) at most \(\epsilon\). We show: 1) If \(\mu\) is a product distribution, \(\eta > 0\) and \(0 \leq \epsilon \leq 1-1/d\), then, $$\mathsf{R}^{1,\mu}_{2\epsilon -d\epsilon^2/(d-1)+ \eta}(f) \leq 2\mathsf{Q}^{1,\mu, *}_{\epsilon}(f) + O(\log\log (1/\eta))\enspace.$$ 2)If \(\mu\) is a non-product distribution and \(\mathcal{Z}=\{ 0,1\}\), then \(\forall \epsilon, \eta > 0\) such that \(\epsilon/\eta + \eta < 0.5\), $$\mathsf{R}^{1,\mu}_{3\eta}(f) = O(\mathsf{Q}^{1,\mu}_{{\epsilon}}(f) \cdot \mathsf{CS}(f)/\eta^3)\enspace,$$ where \[\mathsf{CS}(f) = \max_{y} \min_{z\in\{0,1\}} \vert \{x~|~f(x,y)=z\} \vert \enspace.\] |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.2107.11623 |