There are several different definitions of the barbell graph.
Most commonly and in this work, the -barbell graph is the simple graph obtained by connecting two copies of a complete graph by a bridge (Ghosh et al. 2006, Herbster and Pontil 2006). The 3-barbell graph is isomorphic to the kayak paddle graph .
Precomputed properties of barbell graphs are available in the Wolfram Language as GraphData["Barbell", n].
Barbell graphs are geodetic.
By definition, the -barbell graph has cycle polynomial is given by
(1)
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where is the cycle polynomial of the complete graph . Its graph circumference is therefore .
The -barbell graph has chromatic polynomial and independence polynomial
(2)
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(3)
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and the latter has recurrence equation
(4)
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Wilf (1989) adopts the alternate barbell convention by defining the -barbell graph to consist of two copies of connected by an -path.
Northrup (2002) calls the graphs obtained by joining bridges on either side of a 2-path graph "barbell graphs." This version might perhaps be better called a "double flower graph."