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arXiv:quant-ph/0407247 · Physics Letters A

Deciding separability with a fixed error

David Pérez-Garcı́a

Published Aug 17, 2004• 11 citations
arXivHTMLPDF
DOI
10.1016/j.physleta.2004.07.059

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We study the relative power of public randomness and quantum communication in the multiparty Simultaneous Message Passing (SMP) model. By analyzing a total Boolean function and a relational problem, we establish polynomial and exponential separations between classical public-coin protocols and quantum protocols without shared randomness or prior entanglement. We first introduce XOR Equality, a total Boolean function in which each of kkk players receives an unrestricted string xj∈{0,1}nx_j\in\{0,1\}^nxj​∈{0,1}n, and the referee must decide whether x1⊕⋯⊕xk=0nx_1\oplus\cdots\oplus x_k=0^nx1​⊕⋯⊕xk​=0n. For k≥8k\ge8k≥8 and worst-case error at most 1/31/31/3, we prove quantum lower bounds of Ω(min⁡{n,k2})Ω(\min\{n,k^2\})Ω(min{n,k2}) on total communication and Ω(min⁡{n/k,k})Ω(\min\{n/k,k\})Ω(min{n/k,k}) on maximum message length. A classical public-coin protocol uses two bits per player with error at most 1/41/41/4. For n=k2n=k^2n=k2 and worst-case error at most 1/31/31/3, we prove that quantum protocols require maximum message length Ω(n)Ω(\sqrt n)Ω(n​) qubits, whereas two public-coin bits per player suffice. We then turn to relations, for which we obtain exponential separations. Specifically, we study Multiparty Index Coordination, a kkk-player generalization of the two-player relation studied by Gavinsky, Kempe, Regev, and de Wolf (STOC 2006). We prove an unambiguous quantum lower bound of Ω(n1−1/k)Ω(n^{1-1/k})Ω(n1−1/k) on maximum message length, matched by a classical private-coin protocol. For any fixed error ε∈(0,1/8)\varepsilon\in(0,1/8)ε∈(0,1/8), we also prove a bounded-error quantum lower bound of Ω(n(k−1)/(k+1))Ω(n^{(k-1)/(k+1)})Ω(n(k−1)/(k+1)) while we show that public-coin protocols solve the relation unambiguously with maximum message length O(log⁡n)O(\log n)O(logn), giving exponential separations in both regimes. The implicit constants are independent of kkk, and both quantum lower bounds become linear when k≥clog⁡nk\ge c\log nk≥clogn for any fixed c>0c>0c>0.