The Hamilton cycle space of random graphs
Abstract
The cycle space of a graph G, denoted C(G), is a vector space over F2, spanned by all incidence vectors of edge-sets of cycles of G. If G has n vertices, then Cn(G) denotes the subspace of C(G), spanned by the incidence vectors of Hamilton cycles of G. A classical result in the theory of random graphs asserts that for G G(n,p), asymptotically almost surely the necessary condition δ(G) ≥ 2 is also sufficient to ensure Hamiltonicity. Resolving a problem of Christoph, Nenadov, and Petrova, we augment this result by proving that for G G(n,p), with n being odd, asymptotically almost surely the condition δ(G) ≥ 3 (observed to be necessary by Heinig) is also sufficient for ensuring Cn(G) = C(G). That is, not only does G typically have a Hamilton cycle, but its Hamilton cycles are typically rich enough to span its cycle space.
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