Hypercube graph explained

Hypercube graph
Vertices:

2n

Edges:

2n-1n

Automorphisms:

n!2n

Chromatic Number:2
Girth:4 if

n\ge2

Diameter:

n

Spectrum:

\{(n-2k)\binom{n{k}};k=0,\ldots,n\}

Notation:

Qn

In graph theory, the hypercube graph

Qn

is the edge graph of the

n

-dimensional hypercube, that is, it is the graph formed from the vertices and edges of the hypercube. For instance, the cube graph

Q3

is the graph formed by the 8 vertices and 12 edges of a three-dimensional cube.

Qn

has

2n

vertices,

2n-1n

edges, and is a regular graph with

n

edges touching each vertex.

The hypercube graph

Qn

may also be constructed by creating a vertex for each subset of an

n

-element set, with two vertices adjacent when their subsets differ in a single element, or by creating a vertex for each

n

-digit binary number, with two vertices adjacent when their binary representations differ in a single digit. It is the

n

-fold Cartesian product of the two-vertex complete graph, and may be decomposed into two copies of

Qn-1

connected to each other by a perfect matching.

Hypercube graphs should not be confused with cubic graphs, which are graphs that have exactly three edges touching each vertex. The only hypercube graph

Qn

that is a cubic graph is the cubical graph

Q3

.

Construction

The hypercube graph

Qn

may be constructed from the family of subsets of a set with

n

elements, by making a vertex for each possible subset and joining two vertices by an edge whenever the corresponding subsets differ in a single element. Equivalently, it may be constructed using

2n

vertices labeled with

n

-bit binary numbers and connecting two vertices by an edge whenever the Hamming distance of their labels is one. These two constructions are closely related: a binary number may be interpreted as a set (the set of positions where it has a nonzero digit), and two such sets differ in a single element whenever the corresponding two binary numbers have Hamming distance one.

Alternatively,

Qn

may be constructed from the disjoint union of two hypercubes

Qn-1

, by adding an edge from each vertex in one copy of

Qn-1

to the corresponding vertex in the other copy, as shown in the figure. The joining edges form a perfect matching.

The above construction gives a recursive algorithm for constructing the adjacency matrix of a hypercube,

An

. Copying is done via the Kronecker product

⊗ K

, so that the two copies of

Qn-1

have an adjacency matrix

12 ⊗ KAn-1

,where

1d

is the

d x d

identity matrix. Meanwhile the joining edges have an adjacency matrix

A1 ⊗ K

1
2n-1
. The sum of these two terms gives a recursive function for the adjacency matrix of a hypercube:A_ = \begin1_2\otimes_K A_+A_1\otimes_K 1_ & \text n>1\\\begin0 & 1\\1 & 0\end&\textn=1\endAnother construction of

Qn

is the Cartesian product of

n

two-vertex complete graphs

K2

. More generally the Cartesian product of copies of a complete graph is called a Hamming graph; the hypercube graphs are examples of Hamming graphs.

Examples

The graph

Q0

consists of a single vertex, while

Q1

is the complete graph on two vertices.

Q2

is a cycle of

The graph

Q3

is the 1-skeleton of a cube and is a planar graph with eight vertices and twelve edges.

The graph

Q4

is the Levi graph of the Möbius configuration. It is also the knight's graph for a toroidal

4 x 4

chessboard.[1]

Properties

Bipartiteness

Every hypercube graph is bipartite: it can be colored with only two colors. The two colors of this coloring may be found from the subset construction of hypercube graphs, by giving one color to the subsets that have an even number of elements and the other color to the subsets with an odd number of elements.

Hamiltonicity

Every hypercube

Qn

with

n>1

has a Hamiltonian cycle, a cycle that visits each vertex exactly once. Additionally, a Hamiltonian path exists between two vertices

u

and

v

if and only if they have different colors in a 2-coloring of the graph. Both facts are easy to prove using the principle of induction on the dimension of the hypercube, and the construction of the hypercube graph by joining two smaller hypercubes with a matching.

Hamiltonicity of the hypercube is tightly related to the theory of Gray codes. More precisely there is a bijective correspondence between the set of

n

-bit cyclic Gray codes and the set of Hamiltonian cycles in the An analogous property holds for acyclic

n

-bit Gray codes and Hamiltonian paths.

A lesser known fact is that every perfect matching in the hypercube extends to a Hamiltonian cycle.[2] The question whether every matching extends to a Hamiltonian cycle remains an open problem.[3]

Other properties

The hypercube graph

Qn

(for

n>1

) :
2n-2
2
perfect matchings. (this is another consequence that follows easily from the inductive construction.)

4,6,...2n

and is thus a bipancyclic graph.

n

elements, choosing a distinct unit vector for each set element, and placing the vertex corresponding to the set

S

at the sum of the vectors in

S

.

n\le3

. For larger values of

n

, the hypercube has
2n-n-1
2
n
\prod
k=2

k{n\choose

} spanning trees.
n-1
\sum
i=0

\binom{i}{\lfloori/2\rfloor}

.[4]

\sqrt{n2n}

, but the constant of proportionality is not known precisely.[5]

\{-n,-n+2,-n+4,...,n-4,n-2,n\}

and as the eigenvalues of its Laplacian matrix the numbers

\{0,2,...,2n\}

. The

k

th eigenvalue has multiplicity

\binom{n}{k}

in both cases.

h(G)=1

.

The family

Qn

for all

n>1

is a Lévy family of graphs.

Problems

The problem of finding the longest path or cycle that is an induced subgraph of a given hypercube graph is known as the snake-in-the-box problem.

Szymanski's conjecture concerns the suitability of a hypercube as a network topology for communications. It states that, no matter how one chooses a permutation connecting each hypercube vertex to another vertex with which it should be connected, there is always a way to connect these pairs of vertices by paths that do not share any directed edge.[6]

See also

References

Notes and References

  1. .
  2. .
  3. Ruskey, F. and Savage, C. Matchings extend to Hamiltonian cycles in hypercubes on Open Problem Garden. 2007.
  4. Optimal Numberings and Isoperimetric Problems on Graphs, L.H. Harper, Journal of Combinatorial Theory, 1, 385 - 393,
  5. .
  6. .