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Twofold triple systems with cyclic 2‐intersecting Gray codes
Abstract:Given a combinatorial design urn:x-wiley:10638539:media:jcd21584:jcd21584-math-0001 with block set urn:x-wiley:10638539:media:jcd21584:jcd21584-math-0002, the block‐intersection graph (BIG) of urn:x-wiley:10638539:media:jcd21584:jcd21584-math-0003 is the graph that has urn:x-wiley:10638539:media:jcd21584:jcd21584-math-0004 as its vertex set, where two vertices urn:x-wiley:10638539:media:jcd21584:jcd21584-math-0005 and urn:x-wiley:10638539:media:jcd21584:jcd21584-math-0006 are adjacent if and only if urn:x-wiley:10638539:media:jcd21584:jcd21584-math-0007. The i‐block‐intersection graph (i‐BIG) of urn:x-wiley:10638539:media:jcd21584:jcd21584-math-0008 is the graph that has urn:x-wiley:10638539:media:jcd21584:jcd21584-math-0009 as its vertex set, where two vertices urn:x-wiley:10638539:media:jcd21584:jcd21584-math-0010 and urn:x-wiley:10638539:media:jcd21584:jcd21584-math-0011 are adjacent if and only if urn:x-wiley:10638539:media:jcd21584:jcd21584-math-0012. In this paper, several constructions are obtained that start with twofold triple systems (TTSs) with Hamiltonian 2‐BIGs and result in larger TTSs that also have Hamiltonian 2‐BIGs. These constructions collectively enable us to determine the complete spectrum of TTSs with Hamiltonian 2‐BIGs (equivalently TTSs with cyclic 2‐intersecting Gray codes) as well as the complete spectrum for TTSs with 2‐BIGs that have Hamilton paths (i.e. for TTSs with 2‐intersecting Gray codes). In order to prove these spectrum results, we sometimes require ingredient TTSs that have large partial parallel classes; we prove lower bounds on the sizes of partial parallel classes in arbitrary TTSs, and then construct larger TTSs with both cyclic 2‐intersecting Gray codes and parallel classes.
Keywords:block‐intersection graph  Gray code  hamilton cycle  partial parallel class  triple system  05B05  05B07  05C38
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