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arXiv:quant-ph/0403138 · The European Physical Journal D

Phase diagram for the Grover algorithm with static imperfections

A. A. Pomeransky, O. V. Zhirov, Dima L. Shepelyansky

Published Aug 30, 2004• 8 citations
arXivHTMLPDF
DOI
10.1140/epjd/e2004-00113-4

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Phase diagram for the Grover algorithm with static imperfections

Pomeransky, A A, Zhirov, O V, Dima L. Shepelyansky

We study effects of static inter-qubit interactions on the stability of the Grover quantum search algorithm. Our numerical and analytical results show existence of regular and chaotic phases depending on the imperfection strength $\\epsilon$. The critical border $\\epsilon_c$ between two phases drops polynomially with the number of qubits $n_q$ as $\\epsilon_c \\sim n_q^{-3/2}$. In the regular phase $(\\epsilon < \\epsilon_c)$ the algorithm remains robust against imperfections showing the efficiency gain $\\epsilon_c / \\epsilon$ for $\\epsilon \\gtrsim 2^{-n_q/2}$. In the chaotic phase $(\\epsilon > \\epsilon_c)$ the algorithm is completely destroyed.

•Jan 1, 2004•10 citations
We study effects of static inter-qubit interactions on the stability of the Grover quantum search algorithm. Our numerical and analytical results show existence of regular and chaotic phases depending on the imperfection strength epsilon\\epsilonepsilon. The critical border epsilonc\\epsilon_cepsilonc​ between two phases drops polynomially with the number of qubits nqn_qnq​ as epsiloncsimnq−3/2\\epsilon_c \\sim n_q^{-3/2}epsilonc​simnq−3/2​. In the regular phase (epsilon<epsilonc)(\\epsilon < \\epsilon_c)(epsilon<epsilonc​) the algorithm remains robust against imperfections showing the efficiency gain epsilonc/epsilon\\epsilon_c / \\epsilonepsilonc​/epsilon for epsilongtrsim2−nq/2\\epsilon \\gtrsim 2^{-n_q/2}epsilongtrsim2−nq​/2. In the chaotic phase (epsilon>epsilonc)(\\epsilon > \\epsilon_c)(epsilon>epsilonc​) the algorithm is completely destroyed.