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A Near-Quadratic Lower Bound for the Size of Quantum Circuits of Constant Treewidth

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 Publication date 2016
and research's language is English




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We show that any quantum circuit of treewidth $t$, built from $r$-qubit gates, requires at least $Omega(frac{n^{2}}{2^{O(rcdot t)}cdot log^4 n})$ gates to compute the element distinctness function. Our result generalizes a near-quadratic lower bound for quantum formula size obtained by Roychowdhury and Vatan [SIAM J. on Computing, 2001]. The proof of our lower bound follows by an extension of Nev{c}iporuks method to the context of quantum circuits of constant treewidth. This extension is made via a combination of techniques from structural graph theory, tensor-network theory, and the connected-component counting method, which is a classic tool in algebraic geometry.



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It has been known for almost three decades that many $mathrm{NP}$-hard optimization problems can be solved in polynomial time when restricted to structures of constant treewidth. In this work we provide the first extension of such results to the quantum setting. We show that given a quantum circuit $C$ with $n$ uninitialized inputs, $mathit{poly}(n)$ gates, and treewidth $t$, one can compute in time $(frac{n}{delta})^{exp(O(t))}$ a classical assignment $yin {0,1}^n$ that maximizes the acceptance probability of $C$ up to a $delta$ additive factor. In particular, our algorithm runs in polynomial time if $t$ is constant and $1/poly(n) < delta < 1$. For unrestricted values of $t$, this problem is known to be complete for the complexity class $mathrm{QCMA}$, a quantum generalization of MA. In contrast, we show that the same problem is $mathrm{NP}$-complete if $t=O(log n)$ even when $delta$ is constant. On the other hand, we show that given a $n$-input quantum circuit $C$ of treewidth $t=O(log n)$, and a constant $delta<1/2$, it is $mathrm{QMA}$-complete to determine whether there exists a quantum state $mid!varphirangle in (mathbb{C}^d)^{otimes n}$ such that the acceptance probability of $Cmid!varphirangle$ is greater than $1-delta$, or whether for every such state $mid!varphirangle$, the acceptance probability of $Cmid!varphirangle$ is less than $delta$. As a consequence, under the widely believed assumption that $mathrm{QMA} eq mathrm{NP}$, we have that quantum witnesses are strictly more powerful than classical witnesses with respect to Merlin-Arthur protocols in which the verifier is a quantum circuit of logarithmic treewidth.
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