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Three‐Phase Barker Arrays
Authors:Jason P Bell  Jonathan Jedwab  Mahdad Khatirinejad  Kai‐Uwe Schmidt
Affiliation:1. Department of Pure Mathematics, University of Waterloo, Waterloo, Canada;2. Department of Mathematics, Simon Fraser University, Burnaby, Canada;3. Department of Mathematics, The University of British Columbia, Vancouver, Canada;4. Department of Communications and Networking, Aalto University, Aalto, Finland;5. Faculty of Mathematics, Otto‐von‐Guericke University, Universit?tsplatz 6. 2, Magdeburg, Germany
Abstract:A 3‐phase Barker array is a matrix of third roots of unity for which all out‐of‐phase aperiodic autocorrelations have magnitude 0 or 1. The only known truly two‐dimensional 3‐phase Barker arrays have size 2 × 2 or 3 × 3. We use a mixture of combinatorial arguments and algebraic number theory to establish severe restrictions on the size of a 3‐phase Barker array when at least one of its dimensions is divisible by 3. In particular, there exists a double‐exponentially growing arithmetic function T such that no 3‐phase Barker array of size urn:x-wiley:10638539:jcd21377:equation:jcd21377-math-0001 with urn:x-wiley:10638539:jcd21377:equation:jcd21377-math-0002 exists for all urn:x-wiley:10638539:jcd21377:equation:jcd21377-math-0003. For example, urn:x-wiley:10638539:jcd21377:equation:jcd21377-math-0004, urn:x-wiley:10638539:jcd21377:equation:jcd21377-math-0005, and urn:x-wiley:10638539:jcd21377:equation:jcd21377-math-0006. When both dimensions are divisible by 3, the existence problem is settled completely: if a 3‐phase Barker array of size urn:x-wiley:10638539:jcd21377:equation:jcd21377-math-0007 exists, then urn:x-wiley:10638539:jcd21377:equation:jcd21377-math-0008.
Keywords:Barker array  aperiodic autocorrelation  three‐phase  algebraic number theory
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