The Longest Common Substring (LCS) and Longest Palindromic Substring (LPS) problems are fundamental challenges in string processing, traditionally solved in linear time using classical computation through suffix trees. Recent breakthroughs by Le Gall and Seddighin [1] introduced sublinear quantum query algorithms, while Akmal and Jin [2] further improved the LCS complexity to O ˜ ( n 2 / 3 ) . While these results are remarkable in the quantum query model , their practical implementation on real quantum hardware remains elusive. In this paper, we bridge this gap by presenting the first O ˜ ( n ) quantum algorithms for both LCS and LPS in the circuit model of computation . Our circuits are explicitly constructed and analyzed in terms of size and depth, achieving polylogarithmic overheads while preserving the O ˜ ( n ) depth bound. This provides, for the first time, concrete circuit-level blueprints and resource estimates for quantum solutions to LCS and LPS.
Longest Common Substring and Longest Palindromic Substring in O~(n) Time
The Longest Common Substring (LCS) and Longest Palindromic Substring (LPS) are classical problems in computer science, representing fundamental challenges in string processing. Both problems can be solved in linear time using a classical model of computation, by means of very similar algorithms, both relying on the use of suffix trees. Very recently, two sublinear algorithms for LCS and LPS in the quantum query model have been presented by Le Gall and Seddighin~\cite{GallS23}, requiring O~(n5/6) and O~(n) queries, respectively. However, while the query model is fascinating from a theoretical standpoint, its practical applicability becomes limited when it comes to crafting algorithms meant for actual execution on real hardware. In this paper we present, for the first time, a O~(n) quantum algorithm for both LCS and LPS working in the circuit model of computation. Our solutions are simpler than previous ones and can be easily translated into quantum procedures. We also present actual implementations of the two algorithms as quantum circuits working in O(nlog5(n)) and O(nlog4(n)) time, respectively.