Two New Classes of Hamiltonian Graphs Valentin Polishchuk



![Hamiltonicity of Square Grids • NP-complete in general [Itai, Papadimitriou, and Szwarcfiter ’ 82] Hamiltonicity of Square Grids • NP-complete in general [Itai, Papadimitriou, and Szwarcfiter ’ 82]](https://slidetodoc.com/presentation_image/411fdc49157783707fb83c957ab3ab81/image-4.jpg)
























![Multi-Hamiltonicity • 1 HC 2 HCs cubic [Smith], any vert – odd-deg r-regular, r Multi-Hamiltonicity • 1 HC 2 HCs cubic [Smith], any vert – odd-deg r-regular, r](https://slidetodoc.com/presentation_image/411fdc49157783707fb83c957ab3ab81/image-29.jpg)


































- Slides: 63
Two New Classes of Hamiltonian Graphs Valentin Polishchuk Helsinki Institute for Information Technology, University of Helsinki Joint work with Esther Arkin and Joseph Mitchell Applied Math and Statistics, Stony Brook University
Induced Graph Subset S of R 2 – vertices: S – edge (i, j) if |i – j | = 1
Square Grid Graph • Subset S of Z 2 • Solid grid – no “holes” – all bounded faces – unit squares
Hamiltonicity of Square Grids • NP-complete in general [Itai, Papadimitriou, and Szwarcfiter ’ 82] • Solid grids – polynomial [Umans and Lenhart ’ 96]
Tilings • Square grid – unit squares
Tilings • Square grid – unit squares • Triangular grid – unit equilateral triangles
Triangular Grid Graph Subset S vertices: S – edge (i, j) if |i – j | = 1 Hole: bounded face ≠ unit equilateral ∆
Solid Triangular Grid No holes all bounded faces – unit equilateral triangles
Previous Work • Ham. Cycle Problem – NP-complete in general • Solid grids – always Hamiltonian • no deg-1 vertices The only non-Hamiltonian solid triangular grid
Local Cut Single vertex whose removal decreases number of holes Solid ) No local cuts Our result: Triangular grids without local cuts are Hamiltonian
Idea • B: – Cycle around the outer boundary – Cycles around holes’ boundaries • Use modifications – cycles go through all internal vertices • Exists “facing” rhombus – no local cuts = graph is “thick” – merge facing cycles • Decrease number of cycles • Get Hamiltonian Cycle
L-modification
V-modification
Z-modification
Priority: L , V , Z • L • V • Z
Wedges • Sharp o – 60 turn • Wide o – 120 turn
The Main Lemma Until B passes through ALL internal vertices – either L, V, or Z may be applied small print: unless G is the Star of David
Internal vertex v not in B • A neighbor u is in B • Crossed edges – not in B – o. w. – apply L
How is u visited? WLOG, 1 is in B
L cannot be applied s is in B s How is s visited?
Sharp Wedge s s V Z
Wide Wedge L cannot be applied t is in B
Deja Vu s Rhombus – edge of B – vertex not in B – vertex in B Unless – t is a wide wedge • modification! • welcome new vertex to B
Another Wide Wedge Yet Another vertex – Yet Another rhombus Yet Another wide wedge
And so on… Star of David!
Cycle Cover → Ham. Cycle • Cycles around the outer boundary • Cycles around holes’ boundaries • Use modifications – cycles go through all internal vertices • Exists “facing” rhombus – no local cuts = graph is “thick” – merge facing cycles • Decrease number of cycles • Get Hamiltonian Cycle
Hamiltonian Cycles in High-Girth Graphs
Ham. Cycle Problem is NP-complete • Classic • Girth? – – 4 3 • NP-complete [GJ] [CLRS] [Garey, Johnson, Tarjan’ 76] – planar – cubic – girth-5 Higher girth?
Multi-Hamiltonicity • 1 HC 2 HCs cubic [Smith], any vert – odd-deg r-regular, r > 300 [Thomassen’ 98], r > 48 4 -regular? conjecture maxdeg ≥ f( maxdeg/mindeg ) bipartite, mindeg in a part = 3 • 1 HC exp(maxdeg) HCs [Thomason’ 78] [Ghandehari and Hatami] [Sheehan’ 75] [Horak and Stacho’ 00] [Thomassen’ 96] – bipartite • 1 HC cubic exp(girth) HCs or [Thomassen’ 96] bipartite, mindeg in a part = 4 Planar maxdeg 3, high-girth? >1 HC? Small # of HCs?
Our Contribution Planar maxdeg 3 arbitrarily large girth • Ham. Cycle Problem is NP-complete • Exactly 3 Ham. Cycles arbitrarly large # of vertices
The Other Tiling: Infinite Hexagonal Grid • Induced graphs – hexagonal grids Is Ham. Cycle Problem NP-hard for hexagonal grids?
Attempt to Show NP-Hardness • Same idea as for square and triangular grids [Itai, Papadimitriou, and Szwarcfiter ‘ 82, Papadimitriou and Vazirani ’ 84, PAM’ 06] • Ham. Cycle Problem – undirected planar bipartite graphs – max deg 3 G 0 Embed o o o 0 , 60 , 120 segments
(Try to) Embed in Hex Grid
Edges – Tentacles
Traversing Tentacles
Cross path connects adjacent nodes
Return path returns to one of the nodes
White Node Gadget
Middle Vertex: 2 edges…
Middle Vertex: 2 edges…
Induces 2 cross, 1 return path
Induces 2 cross, 1 return path
Induces 2 cross, 1 return path
Black Node Gadget
Middle Vertex: 2 edges…
Middle Vertex: 2 edges…
Induces 2 cross, 1 return path
Induces 2 cross, 1 return path
Induces 2 cross, 1 return path
Return Path Starts at white node Closes at black node
HC in G 0 Any node gadget adjacent to 2 cross paths 1 return path • Edges of G 0 in HC Cross paths • Edges of G 0 not in HC Return paths from white nodes
Ham Cycle is NP-hard for Hex Grid? No… didn’t show to turn a tentacle Can’t turn with these tentacles
No Longer in a Hex Grid
Subdivide (Shown) Edges Imagine: adjacent deg-2 vertices connected by length-g path Girth g
Girth g+2 Graph • Planar – turning tentacle • no longer an issue – not in a hex grid • Maxdeg 3
HC in G 0 Any node gadget adjacent to 2 cross paths 1 return path • Edges of G 0 in HC Cross paths • Edges of G 0 not in HC Return paths from white nodes
Theorem 1 For any g ≥ 6 Ham. Cycle is NP-hard in planar deg ≤ 3 non-bipartite girth-g graphs
Multi-Hamiltonicity • Planar • Bipartite • Maxdeg 3
Exactly 3 Ham. Cycles
Theorem 2 For any g ≥ 6 exists planar deg ≤ 3 non-bipartite girth-g graph with exactly 3 Ham. Cycles
Summary • Trangular grids no local cut ) Hamiltonian • maxdeg-3 planar girth-g – Ham. Cycle Problem is NP-complete – exists graphs with exactly 3 Ham. Cycles
Open • Ham. Cycle Problem in hexagonal grids